100% FREE Updated: Mar 2026 Real Analysis Calculus of Multiple Variables

Functions of Two Real Variables

Comprehensive study notes on Functions of Two Real Variables for CUET PG Mathematics preparation. This chapter covers key concepts, formulas, and examples needed for your exam.

Functions of Two Real Variables

This chapter delves into the analytical study of functions involving two independent real variables, extending fundamental calculus concepts to higher dimensions. A thorough understanding of these topics is essential for advanced mathematical studies and carries significant weight in the CUET PG examination, particularly in problems related to optimization and multivariable calculus.

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Chapter Contents

| # | Topic |
|---|-------|
| 1 | Limit, Continuity, and Partial Derivatives |
| 2 | Differentiability |
| 3 | Homogeneous Functions |
| 4 | Maxima and Minima |
| 5 | Constrained Optimization |

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We begin with Limit, Continuity, and Partial Derivatives.

Part 1: Limit, Continuity, and Partial Derivatives

Functions of two real variables extend the concepts of calculus to higher dimensions, providing a framework for analyzing surfaces and complex relationships. We examine the fundamental notions of limits, continuity, and partial derivatives, which are essential for understanding multivariate calculus and are frequently tested in the CUET PG examination.

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Core Concepts

1. Functions of Two Variables

We define a real-valued function of two variables as a rule that assigns a unique real number f(x,y)f(x, y) to each ordered pair (x,y)(x, y) in some set DR2D \subset \mathbb{R}^2. The set DD is termed the domain of the function, and the set of all possible values f(x,y)f(x, y) is its range.

Quick Example: Determine the domain of f(x,y)=4x2y2f(x, y) = \sqrt{4 - x^2 - y^2}.

Step 1: Identify the constraint for the function to be real-valued.
> We require the expression under the square root to be non-negative.

4x2y204 - x^2 - y^2 \ge 0

Step 2: Rearrange the inequality to describe the domain.

x2+y24x^2 + y^2 \le 4

This describes a disk centered at the origin with radius 2, including its boundary.

Answer: The domain is the set of all (x,y)(x, y) such that x2+y24x^2 + y^2 \le 4.

:::question type="MCQ" question="The domain of the function f(x,y)=ln(xy)x2+y21f(x, y) = \frac{\ln(x-y)}{\sqrt{x^2+y^2-1}} is:" options=["x>yx > y and x2+y2>1x^2+y^2 > 1","xy>0x-y > 0 and x2+y21x^2+y^2 \ge 1","xyx \ge y and x2+y2>1x^2+y^2 > 1","x>yx > y and x2+y21x^2+y^2 \ne 1"] answer="x>yx > y and x2+y2>1x^2+y^2 > 1" hint="Consider the constraints for the logarithm and the square root in the denominator." solution="Step 1: For ln(xy)\ln(x-y) to be defined, we must have xy>0x-y > 0, which implies x>yx > y.

Step 2: For the term x2+y21\sqrt{x^2+y^2-1} in the denominator, we must have x2+y21>0x^2+y^2-1 > 0 (strictly greater than zero because it is in the denominator, so it cannot be zero). This implies x2+y2>1x^2+y^2 > 1.

Step 3: Combine both conditions.
The domain is the set of all (x,y)(x,y) such that x>yx > y and x2+y2>1x^2+y^2 > 1."
:::

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2. Limits of Functions of Two Variables

We say that the limit of f(x,y)f(x, y) as (x,y)(x, y) approaches (a,b)(a, b) is LL, denoted lim(x,y)(a,b)f(x,y)=L\lim_{(x,y) \to (a,b)} f(x,y) = L, if for every ϵ>0\epsilon > 0 there exists a δ>0\delta > 0 such that if 0<(xa)2+(yb)2<δ0 < \sqrt{(x-a)^2 + (y-b)^2} < \delta, then f(x,y)L<ϵ|f(x, y) - L| < \epsilon. This implies that f(x,y)f(x,y) must approach LL regardless of the path taken towards (a,b)(a,b).

📖 Limit Definition

The limit lim(x,y)(a,b)f(x,y)=L\lim_{(x,y) \to (a,b)} f(x,y) = L exists if f(x,y)f(x,y) approaches LL as (x,y)(x,y) approaches (a,b)(a,b) along every possible path.

2.1 Path Dependence

To demonstrate that a limit does not exist, we commonly evaluate the limit along different paths. If the limit values differ for at least two distinct paths approaching (a,b)(a,b), then the overall limit does not exist. Common paths include lines y=mxy=mx, x=0x=0, y=0y=0, or parabolas y=x2y=x^2.

Quick Example: Show that lim(x,y)(0,0)xyx2+y2\lim_{(x,y) \to (0,0)} \frac{xy}{x^2+y^2} does not exist.

Step 1: Evaluate the limit along the path y=0y=0 (the x-axis).

limx0x(0)x2+02=limx00x2=0for x0\lim_{x \to 0} \frac{x(0)}{x^2+0^2} = \lim_{x \to 0} \frac{0}{x^2} = 0 \quad \text{for } x \ne 0

Step 2: Evaluate the limit along the path x=0x=0 (the y-axis).

limy00(y)02+y2=limy00y2=0for y0\lim_{y \to 0} \frac{0(y)}{0^2+y^2} = \lim_{y \to 0} \frac{0}{y^2} = 0 \quad \text{for } y \ne 0

Step 3: Evaluate the limit along the path y=xy=x.

limx0x(x)x2+x2=limx0x22x2=12\lim_{x \to 0} \frac{x(x)}{x^2+x^2} = \lim_{x \to 0} \frac{x^2}{2x^2} = \frac{1}{2}

Step 4: Compare the results.
> Since the limit along y=xy=x is 1/21/2 and the limits along y=0y=0 and x=0x=0 are 00, the limit depends on the path.

Answer: The limit lim(x,y)(0,0)xyx2+y2\lim_{(x,y) \to (0,0)} \frac{xy}{x^2+y^2} does not exist.

⚠️ Common Mistake with Path Dependence

❌ Showing the limit is the same along a few paths (e.g., y=0y=0, x=0x=0, y=xy=x) does NOT prove the limit exists. It only suggests it might.
✅ To prove a limit exists, one must use the ϵδ\epsilon-\delta definition or a suitable theorem (e.g., Squeeze Theorem). To prove a limit does NOT exist, finding two paths yielding different limits is sufficient.

2.2 Iterated Limits

Iterated limits involve taking limits sequentially, one variable at a time. For a function f(x,y)f(x, y) as (x,y)(a,b)(x, y) \to (a, b), the two iterated limits are:

limxa(limybf(x,y))andlimyb(limxaf(x,y))\lim_{x \to a} \left( \lim_{y \to b} f(x, y) \right) \quad \text{and} \quad \lim_{y \to b} \left( \lim_{x \to a} f(x, y) \right)

If the overall limit lim(x,y)(a,b)f(x,y)\lim_{(x,y) \to (a,b)} f(x,y) exists and equals LL, then both iterated limits must also exist and be equal to LL. However, the existence and equality of iterated limits do not guarantee the existence of the overall limit.

Quick Example: For f(x,y)=x2y2x2+y2f(x, y) = \frac{x^2 - y^2}{x^2 + y^2} (for (x,y)(0,0)(x,y) \ne (0,0)) and f(0,0)=0f(0,0)=0, find the iterated limits at (0,0)(0,0). This relates to PYQ 2 & 3.

Step 1: Calculate limx0(limy0f(x,y))\lim_{x \to 0} \left( \lim_{y \to 0} f(x, y) \right).
> First, evaluate the inner limit:

limy0x2y2x2+y2=x202x2+02=x2x2=1for x0\lim_{y \to 0} \frac{x^2 - y^2}{x^2 + y^2} = \frac{x^2 - 0^2}{x^2 + 0^2} = \frac{x^2}{x^2} = 1 \quad \text{for } x \ne 0

> Now, evaluate the outer limit:
limx0(1)=1\lim_{x \to 0} (1) = 1

> So, a=1a = 1.

Step 2: Calculate limy0(limx0f(x,y))\lim_{y \to 0} \left( \lim_{x \to 0} f(x, y) \right).
> First, evaluate the inner limit:

limx0x2y2x2+y2=02y202+y2=y2y2=1for y0\lim_{x \to 0} \frac{x^2 - y^2}{x^2 + y^2} = \frac{0^2 - y^2}{0^2 + y^2} = \frac{-y^2}{y^2} = -1 \quad \text{for } y \ne 0

> Now, evaluate the outer limit:
limy0(1)=1\lim_{y \to 0} (-1) = -1

> So, b=1b = -1.

Answer: The iterated limits are a=1a=1 and b=1b=-1. Note that since aba \ne b, the overall limit lim(x,y)(0,0)f(x,y)\lim_{(x,y) \to (0,0)} f(x,y) does not exist for this function.

:::question type="MCQ" question="Let f(x,y)=xyx2+y2f(x, y) = \frac{x y}{x^2 + y^2} for (x,y)(0,0)(x, y) \ne (0, 0) and f(0,0)=0f(0, 0) = 0. Which of the following statements about the iterated limits at (0,0)(0,0) is correct?" options=["Both iterated limits exist and are equal to 0.","Both iterated limits exist and are equal to 1.","One iterated limit is 0, the other is 1.","Neither iterated limit exists."] answer="Both iterated limits exist and are equal to 0." hint="Calculate limx0(limy0f(x,y))\lim_{x \to 0} (\lim_{y \to 0} f(x,y)) and limy0(limx0f(x,y))\lim_{y \to 0} (\lim_{x \to 0} f(x,y)) separately." solution="Step 1: Calculate limx0(limy0f(x,y))\lim_{x \to 0} \left( \lim_{y \to 0} f(x, y) \right).
> Inner limit: limy0xyx2+y2=x0x2+02=0x2=0\lim_{y \to 0} \frac{xy}{x^2 + y^2} = \frac{x \cdot 0}{x^2 + 0^2} = \frac{0}{x^2} = 0 (for x0x \ne 0).
> Outer limit: limx0(0)=0\lim_{x \to 0} (0) = 0.

Step 2: Calculate limy0(limx0f(x,y))\lim_{y \to 0} \left( \lim_{x \to 0} f(x, y) \right).
> Inner limit: limx0xyx2+y2=0y02+y2=0y2=0\lim_{x \to 0} \frac{xy}{x^2 + y^2} = \frac{0 \cdot y}{0^2 + y^2} = \frac{0}{y^2} = 0 (for y0y \ne 0).
> Outer limit: limy0(0)=0\lim_{y \to 0} (0) = 0.

Step 3: Compare results.
> Both iterated limits exist and are equal to 0. However, as shown in a previous example, the overall limit does not exist for this function because the limit along y=xy=x is 1/21/2. This highlights that even if iterated limits exist and are equal, the actual limit may not exist."
:::

2.3 Polar Coordinates for Limits

Converting to polar coordinates can simplify limit calculations, especially for functions involving x2+y2x^2+y^2 terms or when approaching the origin (0,0)(0,0). We substitute x=rcosθx = r \cos \theta and y=rsinθy = r \sin \theta. As (x,y)(0,0)(x, y) \to (0, 0), r0+r \to 0^+. If the expression in polar coordinates simplifies to a function of rr that approaches a single value as r0r \to 0, independent of θ\theta, then the limit exists.

Quick Example: Evaluate lim(x,y)(0,0)x3+y3x2+y2\lim_{(x,y) \to (0,0)} \frac{x^3+y^3}{x^2+y^2}.

Step 1: Substitute x=rcosθx = r \cos \theta and y=rsinθy = r \sin \theta.

(rcosθ)3+(rsinθ)3(rcosθ)2+(rsinθ)2\frac{(r \cos \theta)^3 + (r \sin \theta)^3}{(r \cos \theta)^2 + (r \sin \theta)^2}

Step 2: Simplify the expression.

r3cos3θ+r3sin3θr2cos2θ+r2sin2θ=r3(cos3θ+sin3θ)r2(cos2θ+sin2θ)=r3(cos3θ+sin3θ)r2(1)\frac{r^3 \cos^3 \theta + r^3 \sin^3 \theta}{r^2 \cos^2 \theta + r^2 \sin^2 \theta} = \frac{r^3 (\cos^3 \theta + \sin^3 \theta)}{r^2 (\cos^2 \theta + \sin^2 \theta)} = \frac{r^3 (\cos^3 \theta + \sin^3 \theta)}{r^2 (1)}

=r(cos3θ+sin3θ)= r (\cos^3 \theta + \sin^3 \theta)

Step 3: Evaluate the limit as r0+r \to 0^+.

limr0+r(cos3θ+sin3θ)=0(cos3θ+sin3θ)=0\lim_{r \to 0^+} r (\cos^3 \theta + \sin^3 \theta) = 0 \cdot (\cos^3 \theta + \sin^3 \theta) = 0

> Since the limit is 0, independent of θ\theta, the limit exists and is 0.

Answer: The limit is 00.

:::question type="MCQ" question="Evaluate lim(x,y)(0,0)x2yx2+y2\lim_{(x,y) \to (0,0)} \frac{x^2 y}{x^2+y^2}." options=["0","1/2","Does not exist","1"] answer="0" hint="Consider converting to polar coordinates." solution="Step 1: Substitute x=rcosθx = r \cos \theta and y=rsinθy = r \sin \theta.

(rcosθ)2(rsinθ)(rcosθ)2+(rsinθ)2\frac{(r \cos \theta)^2 (r \sin \theta)}{(r \cos \theta)^2 + (r \sin \theta)^2}

Step 2: Simplify the expression.

r3cos2θsinθr2(cos2θ+sin2θ)=r3cos2θsinθr2=rcos2θsinθ\frac{r^3 \cos^2 \theta \sin \theta}{r^2 (\cos^2 \theta + \sin^2 \theta)} = \frac{r^3 \cos^2 \theta \sin \theta}{r^2} = r \cos^2 \theta \sin \theta

Step 3: Evaluate the limit as r0+r \to 0^+.

limr0+rcos2θsinθ=0cos2θsinθ=0\lim_{r \to 0^+} r \cos^2 \theta \sin \theta = 0 \cdot \cos^2 \theta \sin \theta = 0

> Since cos2θsinθ1|\cos^2 \theta \sin \theta| \le 1, the expression rcos2θsinθr \cos^2 \theta \sin \theta approaches 0 as r0r \to 0, regardless of θ\theta.
> The limit exists and is 0."
:::

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3. Continuity of Functions of Two Variables

A function f(x,y)f(x, y) is continuous at a point (a,b)(a, b) if three conditions are met:

  • f(a,b)f(a, b) is defined.

  • lim(x,y)(a,b)f(x,y)\lim_{(x,y) \to (a,b)} f(x,y) exists.

  • lim(x,y)(a,b)f(x,y)=f(a,b)\lim_{(x,y) \to (a,b)} f(x,y) = f(a, b).
  • We observe that polynomials in xx and yy are continuous everywhere. Rational functions are continuous on their domains (where the denominator is non-zero). Compositions of continuous functions are also continuous.

    Quick Example: Consider the function f(x,y)={x2yx2+y2,(x,y)(0,0)0,(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2 y}{x^2+y^2}, & (x,y) \neq (0,0) \\ 0, & (x,y) = (0,0) \end{cases}. Determine if f(x,y)f(x,y) is continuous at (0,0)(0,0). This relates to PYQ 1.

    Step 1: Check if f(0,0)f(0,0) is defined.
    > We are given f(0,0)=0f(0,0) = 0.

    Step 2: Evaluate lim(x,y)(0,0)f(x,y)\lim_{(x,y) \to (0,0)} f(x,y).
    > Using polar coordinates x=rcosθ,y=rsinθx = r \cos \theta, y = r \sin \theta:

    limr0+(rcosθ)2(rsinθ)(rcosθ)2+(rsinθ)2=limr0+r3cos2θsinθr2(cos2θ+sin2θ)\lim_{r \to 0^+} \frac{(r \cos \theta)^2 (r \sin \theta)}{(r \cos \theta)^2 + (r \sin \theta)^2} = \lim_{r \to 0^+} \frac{r^3 \cos^2 \theta \sin \theta}{r^2 (\cos^2 \theta + \sin^2 \theta)}

    =limr0+rcos2θsinθ= \lim_{r \to 0^+} r \cos^2 \theta \sin \theta

    > Since cos2θsinθ1|\cos^2 \theta \sin \theta| \le 1, we have:
    0rcos2θsinθr0 \le |r \cos^2 \theta \sin \theta| \le r

    > As r0+r \to 0^+, by the Squeeze Theorem, limr0+rcos2θsinθ=0\lim_{r \to 0^+} r \cos^2 \theta \sin \theta = 0.
    > Thus, lim(x,y)(0,0)f(x,y)=0\lim_{(x,y) \to (0,0)} f(x,y) = 0.

    Step 3: Compare the limit with f(0,0)f(0,0).
    > We found lim(x,y)(0,0)f(x,y)=0\lim_{(x,y) \to (0,0)} f(x,y) = 0 and f(0,0)=0f(0,0) = 0.
    > Since they are equal, the function is continuous at (0,0)(0,0).

    Answer: The function f(x,y)f(x,y) is continuous at (0,0)(0,0).

    :::question type="MCQ" question="Let f(x,y)={x2y2x2+y2,(x,y)(0,0)0,(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2-y^2}{x^2+y^2}, & (x,y) \neq (0,0) \\ 0, & (x,y) = (0,0) \end{cases}. Which of the following statements is true?" options=["ff is continuous at (0,0)(0,0).","lim(x,y)(0,0)f(x,y)\lim_{(x,y)\to(0,0)} f(x,y) exists and is equal to 00.","ff is not continuous at (0,0)(0,0).","The iterated limits limx0limy0f(x,y)\lim_{x \to 0} \lim_{y \to 0} f(x,y) and limy0limx0f(x,y)\lim_{y \to 0} \lim_{x \to 0} f(x,y) are equal."] answer="ff is not continuous at (0,0)(0,0)." hint="Check the limit definition of continuity. Recall the iterated limits for this function." solution="Step 1: Check if f(0,0)f(0,0) is defined.
    > f(0,0)=0f(0,0) = 0 is defined.

    Step 2: Evaluate lim(x,y)(0,0)f(x,y)\lim_{(x,y)\to(0,0)} f(x,y).
    > We previously calculated the iterated limits for this function:
    > limx0limy0f(x,y)=1\lim_{x \to 0} \lim_{y \to 0} f(x,y) = 1
    > limy0limx0f(x,y)=1\lim_{y \to 0} \lim_{x \to 0} f(x,y) = -1
    > Since the iterated limits are not equal, the overall limit lim(x,y)(0,0)f(x,y)\lim_{(x,y)\to(0,0)} f(x,y) does not exist.

    Step 3: Check continuity conditions.
    > For continuity, the limit must exist and be equal to f(0,0)f(0,0). Since the limit does not exist, ff is not continuous at (0,0)(0,0).
    > Option 4 is false because the iterated limits are 11 and 1-1, which are not equal.
    > Option 2 is false because the limit does not exist.
    > Option 1 is false because the function is not continuous.
    > Option 3 is true."
    :::

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    4. Partial Derivatives

    For a function f(x,y)f(x, y), the partial derivative with respect to xx, denoted fx\frac{\partial f}{\partial x} or fxf_x, is the ordinary derivative of ff with respect to xx when yy is held constant. Similarly, fy\frac{\partial f}{\partial y} or fyf_y is the ordinary derivative of ff with respect to yy when xx is held constant.

    📐 Definition of Partial Derivatives
    fx(x,y)=limh0f(x+h,y)f(x,y)hf_x(x,y) = \lim_{h \to 0} \frac{f(x+h, y) - f(x, y)}{h}
    fy(x,y)=limh0f(x,y+h)f(x,y)hf_y(x,y) = \lim_{h \to 0} \frac{f(x, y+h) - f(x, y)}{h}

    Quick Example: Find fxf_x and fyf_y for f(x,y)=x3y2+2x2y5y3f(x, y) = x^3 y^2 + 2x^2 y - 5y^3.

    Step 1: Calculate fxf_x (treat yy as a constant).

    x(x3y2+2x2y5y3)=x(x3y2)+x(2x2y)x(5y3)\frac{\partial}{\partial x} (x^3 y^2 + 2x^2 y - 5y^3) = \frac{\partial}{\partial x} (x^3 y^2) + \frac{\partial}{\partial x} (2x^2 y) - \frac{\partial}{\partial x} (5y^3)

    =3x2y2+4xy0= 3x^2 y^2 + 4xy - 0

    fx(x,y)=3x2y2+4xyf_x(x,y) = 3x^2 y^2 + 4xy

    Step 2: Calculate fyf_y (treat xx as a constant).

    y(x3y2+2x2y5y3)=y(x3y2)+y(2x2y)y(5y3)\frac{\partial}{\partial y} (x^3 y^2 + 2x^2 y - 5y^3) = \frac{\partial}{\partial y} (x^3 y^2) + \frac{\partial}{\partial y} (2x^2 y) - \frac{\partial}{\partial y} (5y^3)

    =2x3y+2x215y2= 2x^3 y + 2x^2 - 15y^2

    fy(x,y)=2x3y+2x215y2f_y(x,y) = 2x^3 y + 2x^2 - 15y^2

    Answer: fx(x,y)=3x2y2+4xyf_x(x,y) = 3x^2 y^2 + 4xy and fy(x,y)=2x3y+2x215y2f_y(x,y) = 2x^3 y + 2x^2 - 15y^2.

    :::question type="MCQ" question="Given f(x,y)=exy2+sin(x2y)f(x,y) = e^{xy^2} + \sin(x^2y), find fy(1,0)f_y(1,0)." options=["0","1","2","e"] answer="1" hint="First find fy(x,y)f_y(x,y) and then substitute the values." solution="Step 1: Calculate fy(x,y)f_y(x,y) by treating xx as a constant.

    fy(x,y)=y(exy2)+y(sin(x2y))f_y(x,y) = \frac{\partial}{\partial y} (e^{xy^2}) + \frac{\partial}{\partial y} (\sin(x^2y))

    > Applying the chain rule:
    fy(x,y)=exy2(x2y)+cos(x2y)(x21)f_y(x,y) = e^{xy^2} \cdot (x \cdot 2y) + \cos(x^2y) \cdot (x^2 \cdot 1)

    fy(x,y)=2xyexy2+x2cos(x2y)f_y(x,y) = 2xy e^{xy^2} + x^2 \cos(x^2y)

    Step 2: Substitute (x,y)=(1,0)(x,y) = (1,0) into fy(x,y)f_y(x,y).

    fy(1,0)=2(1)(0)e(1)(0)2+(1)2cos((1)2(0))f_y(1,0) = 2(1)(0) e^{(1)(0)^2} + (1)^2 \cos((1)^2(0))

    fy(1,0)=0e0+1cos(0)f_y(1,0) = 0 \cdot e^0 + 1 \cdot \cos(0)

    fy(1,0)=01+11f_y(1,0) = 0 \cdot 1 + 1 \cdot 1

    fy(1,0)=1f_y(1,0) = 1
    "
    :::

    4.1 Higher-Order Partial Derivatives

    We can take partial derivatives of partial derivatives, leading to second-order partial derivatives.

    • fxx=2fx2=x(fx)f_{xx} = \frac{\partial^2 f}{\partial x^2} = \frac{\partial}{\partial x} \left( \frac{\partial f}{\partial x} \right)

    • fyy=2fy2=y(fy)f_{yy} = \frac{\partial^2 f}{\partial y^2} = \frac{\partial}{\partial y} \left( \frac{\partial f}{\partial y} \right)

    • fxy=2fyx=y(fx)f_{xy} = \frac{\partial^2 f}{\partial y \partial x} = \frac{\partial}{\partial y} \left( \frac{\partial f}{\partial x} \right) (differentiate with respect to xx first, then yy)

    • fyx=2fxy=x(fy)f_{yx} = \frac{\partial^2 f}{\partial x \partial y} = \frac{\partial}{\partial x} \left( \frac{\partial f}{\partial y} \right) (differentiate with respect to yy first, then xx)




    📐
    Clairaut's Theorem (Equality of Mixed Partials)

    If fxyf_{xy} and fyxf_{yx} are continuous on an open disk, then fxy(x,y)=fyx(x,y)f_{xy}(x,y) = f_{yx}(x,y) on that disk.


    Quick Example: For f(x,y)=x3y2+2x2y5y3f(x, y) = x^3 y^2 + 2x^2 y - 5y^3, find fxyf_{xy} and fyxf_{yx}.

    Step 1: Recall fx(x,y)f_x(x,y) and fy(x,y)f_y(x,y) from the previous example.
    > fx(x,y)=3x2y2+4xyf_x(x,y) = 3x^2 y^2 + 4xy
    > fy(x,y)=2x3y+2x215y2f_y(x,y) = 2x^3 y + 2x^2 - 15y^2

    Step 2: Calculate fxy=y(fx)f_{xy} = \frac{\partial}{\partial y} (f_x).

    fxy(x,y)=y(3x2y2+4xy)f_{xy}(x,y) = \frac{\partial}{\partial y} (3x^2 y^2 + 4xy)

    =3x2(2y)+4x(1)= 3x^2 (2y) + 4x(1)

    =6x2y+4x= 6x^2 y + 4x

    Step 3: Calculate fyx=x(fy)f_{yx} = \frac{\partial}{\partial x} (f_y).

    fyx(x,y)=x(2x3y+2x215y2)f_{yx}(x,y) = \frac{\partial}{\partial x} (2x^3 y + 2x^2 - 15y^2)

    =2(3x2)y+2(2x)0= 2(3x^2) y + 2(2x) - 0

    =6x2y+4x= 6x^2 y + 4x

    Answer: fxy(x,y)=6x2y+4xf_{xy}(x,y) = 6x^2 y + 4x and fyx(x,y)=6x2y+4xf_{yx}(x,y) = 6x^2 y + 4x. They are equal, confirming Clairaut's Theorem.

    :::question type="MCQ" question="If f(x,y)=arctan(yx)f(x,y) = \arctan\left(\frac{y}{x}\right), then fxy(x,y)f_{xy}(x,y) is equal to:" options=["x2y2(x2+y2)2\frac{x^2-y^2}{(x^2+y^2)^2}","y2x2(x2+y2)2\frac{y^2-x^2}{(x^2+y^2)^2}","2xy(x2+y2)2\frac{2xy}{(x^2+y^2)^2}","2xy(x2+y2)2\frac{-2xy}{(x^2+y^2)^2}"] answer="y2x2(x2+y2)2\frac{y^2-x^2}{(x^2+y^2)^2}" hint="First find fxf_x, then differentiate with respect to yy. Alternatively, find fyf_y then differentiate with respect to xx (Clairaut's Theorem)." solution="Step 1: Calculate fx(x,y)f_x(x,y).
    > Recall ddu(arctanu)=11+u2\frac{d}{du}(\arctan u) = \frac{1}{1+u^2}. Here, u=y/xu = y/x.

    fx=11+(y/x)2x(yx)\frac{\partial f}{\partial x} = \frac{1}{1+(y/x)^2} \cdot \frac{\partial}{\partial x} \left(\frac{y}{x}\right)

    =11+y2/x2(yx2)= \frac{1}{1+y^2/x^2} \cdot \left(-\frac{y}{x^2}\right)

    =x2x2+y2(yx2)= \frac{x^2}{x^2+y^2} \cdot \left(-\frac{y}{x^2}\right)

    fx(x,y)=yx2+y2f_x(x,y) = -\frac{y}{x^2+y^2}

    Step 2: Calculate fxy(x,y)=y(fx)f_{xy}(x,y) = \frac{\partial}{\partial y} (f_x).
    > We use the quotient rule: y(yx2+y2)=(1)(x2+y2)y(2y)(x2+y2)2\frac{\partial}{\partial y} \left( -\frac{y}{x^2+y^2} \right) = - \frac{(1)(x^2+y^2) - y(2y)}{(x^2+y^2)^2}

    =x2+y22y2(x2+y2)2= - \frac{x^2+y^2 - 2y^2}{(x^2+y^2)^2}

    =x2y2(x2+y2)2= - \frac{x^2-y^2}{(x^2+y^2)^2}

    =y2x2(x2+y2)2= \frac{y^2-x^2}{(x^2+y^2)^2}
    "
    :::

    4.2 Chain Rule for Partial Derivatives

    The chain rule is crucial when the independent variables of a function are themselves functions of other variables.

    📐 Chain Rule for Two Independent Variables

    If z=f(x,y)z = f(x,y), where x=x(s,t)x = x(s,t) and y=y(s,t)y = y(s,t), then:

    zs=zxxs+zyys\frac{\partial z}{\partial s} = \frac{\partial z}{\partial x} \frac{\partial x}{\partial s} + \frac{\partial z}{\partial y} \frac{\partial y}{\partial s}

    zt=zxxt+zyyt\frac{\partial z}{\partial t} = \frac{\partial z}{\partial x} \frac{\partial x}{\partial t} + \frac{\partial z}{\partial y} \frac{\partial y}{\partial t}

    Quick Example: If z=x2xy+y3z = x^2 - xy + y^3, x=rcosθx = r \cos \theta, y=rsinθy = r \sin \theta, find zr\frac{\partial z}{\partial r} at (x,y)=(1,1)(x,y)=(1,1). This relates to PYQ 4.

    Step 1: Find the partial derivatives of zz with respect to xx and yy.

    zx=2xy\frac{\partial z}{\partial x} = 2x - y

    zy=x+3y2\frac{\partial z}{\partial y} = -x + 3y^2

    Step 2: Find the partial derivatives of xx and yy with respect to rr.

    xr=r(rcosθ)=cosθ\frac{\partial x}{\partial r} = \frac{\partial}{\partial r} (r \cos \theta) = \cos \theta

    yr=r(rsinθ)=sinθ\frac{\partial y}{\partial r} = \frac{\partial}{\partial r} (r \sin \theta) = \sin \theta

    Step 3: Apply the chain rule for zr\frac{\partial z}{\partial r}.

    zr=zxxr+zyyr\frac{\partial z}{\partial r} = \frac{\partial z}{\partial x} \frac{\partial x}{\partial r} + \frac{\partial z}{\partial y} \frac{\partial y}{\partial r}

    zr=(2xy)cosθ+(x+3y2)sinθ\frac{\partial z}{\partial r} = (2x - y) \cos \theta + (-x + 3y^2) \sin \theta

    Step 4: Evaluate at (x,y)=(1,1)(x,y)=(1,1). First, find rr and θ\theta for (x,y)=(1,1)(x,y)=(1,1).
    > x=rcosθ    1=rcosθx = r \cos \theta \implies 1 = r \cos \theta
    > y=rsinθ    1=rsinθy = r \sin \theta \implies 1 = r \sin \theta
    > Dividing the equations: tanθ=1    θ=π4\tan \theta = 1 \implies \theta = \frac{\pi}{4}.
    > Squaring and adding: x2+y2=r2    12+12=r2    r2=2    r=2x^2+y^2 = r^2 \implies 1^2+1^2 = r^2 \implies r^2=2 \implies r = \sqrt{2}.
    > So, at (x,y)=(1,1)(x,y)=(1,1), we have r=2r=\sqrt{2} and θ=π4\theta=\frac{\pi}{4}.
    > cosθ=cos(π4)=12\cos \theta = \cos(\frac{\pi}{4}) = \frac{1}{\sqrt{2}}
    > sinθ=sin(π4)=12\sin \theta = \sin(\frac{\pi}{4}) = \frac{1}{\sqrt{2}}

    Step 5: Substitute the values into the chain rule expression.

    (zr)(x,y)=(1,1)=(2(1)1)(12)+(1+3(1)2)(12)\left( \frac{\partial z}{\partial r} \right)_{(x,y)=(1,1)} = (2(1) - 1) \left(\frac{1}{\sqrt{2}}\right) + (-1 + 3(1)^2) \left(\frac{1}{\sqrt{2}}\right)

    =(1)(12)+(2)(12)= (1) \left(\frac{1}{\sqrt{2}}\right) + (2) \left(\frac{1}{\sqrt{2}}\right)

    =12+22=32= \frac{1}{\sqrt{2}} + \frac{2}{\sqrt{2}} = \frac{3}{\sqrt{2}}

    Answer: 32\frac{3}{\sqrt{2}}.

    :::question type="MCQ" question="If w=z2x2yw = z^2 - x^2 y, where x=t2x = t^2, y=t2y = t^2, and z=t5/2z = t^{5/2}, find dwdt\frac{dw}{dt}." options=["5t46t55t^4 - 6t^5","5t47t55t^4 - 7t^5","7t55t47t^5 - 5t^4","5t57t45t^5 - 7t^4"] answer="5t46t55t^4 - 6t^5" hint="This is a special case of the chain rule where ww is ultimately a function of a single variable tt. Apply the appropriate chain rule formula." solution="Step 1: Identify the partial derivatives of ww.

    wx=2xy\frac{\partial w}{\partial x} = -2xy

    wy=x2\frac{\partial w}{\partial y} = -x^2

    wz=2z\frac{\partial w}{\partial z} = 2z

    Step 2: Identify the derivatives of x,y,zx, y, z with respect to tt.

    dxdt=2t\frac{dx}{dt} = 2t

    dydt=2t\frac{dy}{dt} = 2t

    dzdt=52t3/2\frac{dz}{dt} = \frac{5}{2}t^{3/2}

    Step 3: Apply the chain rule: dwdt=wxdxdt+wydydt+wzdzdt\frac{dw}{dt} = \frac{\partial w}{\partial x} \frac{dx}{dt} + \frac{\partial w}{\partial y} \frac{dy}{dt} + \frac{\partial w}{\partial z} \frac{dz}{dt}.
    > Substitute expressions in terms of tt:

    dwdt=(2(t2)(t2))(2t)+((t2)2)(2t)+(2(t5/2))(52t3/2)\frac{dw}{dt} = (-2(t^2)(t^2))(2t) + (-(t^2)^2)(2t) + (2(t^{5/2}))(\frac{5}{2}t^{3/2})

    dwdt=(2t4)(2t)+(t4)(2t)+(5t5/2t3/2)\frac{dw}{dt} = (-2t^4)(2t) + (-t^4)(2t) + (5t^{5/2}t^{3/2})

    dwdt=4t52t5+5t(5/2+3/2)\frac{dw}{dt} = -4t^5 - 2t^5 + 5t^{(5/2 + 3/2)}

    dwdt=6t5+5t8/2\frac{dw}{dt} = -6t^5 + 5t^{8/2}

    dwdt=6t5+5t4\frac{dw}{dt} = -6t^5 + 5t^4

    Step 4: Rearrange to match options.

    dwdt=5t46t5\frac{dw}{dt} = 5t^4 - 6t^5
    "
    :::

    ---

    5. Directional Derivatives and Gradient

    The directional derivative measures the rate of change of a function f(x,y)f(x,y) in a specific direction. The gradient vector points in the direction of the greatest rate of increase of the function.

    📖 Gradient Vector

    For a function f(x,y)f(x,y), the gradient vector, denoted f\nabla f, is given by:

    f(x,y)=fx,fy=fxi+fyj\nabla f(x,y) = \left\langle \frac{\partial f}{\partial x}, \frac{\partial f}{\partial y} \right\rangle = f_x \mathbf{i} + f_y \mathbf{j}

    📐 Directional Derivative

    The directional derivative of ff in the direction of a unit vector u=u1,u2\mathbf{u} = \langle u_1, u_2 \rangle is given by:

    Duf(x,y)=f(x,y)u=fx(x,y)u1+fy(x,y)u2D_{\mathbf{u}}f(x,y) = \nabla f(x,y) \cdot \mathbf{u} = f_x(x,y)u_1 + f_y(x,y)u_2

    Quick Example: Find the directional derivative of f(x,y)=x2y34yf(x,y) = x^2 y^3 - 4y at the point (2,1)(2,-1) in the direction of the vector v=2,5\mathbf{v} = \langle 2, 5 \rangle.

    Step 1: Calculate the partial derivatives fxf_x and fyf_y.

    fx(x,y)=x(x2y34y)=2xy3f_x(x,y) = \frac{\partial}{\partial x} (x^2 y^3 - 4y) = 2xy^3

    fy(x,y)=y(x2y34y)=3x2y24f_y(x,y) = \frac{\partial}{\partial y} (x^2 y^3 - 4y) = 3x^2 y^2 - 4

    Step 2: Evaluate the gradient at the point (2,1)(2,-1).

    fx(2,1)=2(2)(1)3=4f_x(2,-1) = 2(2)(-1)^3 = -4

    fy(2,1)=3(2)2(1)24=3(4)(1)4=124=8f_y(2,-1) = 3(2)^2 (-1)^2 - 4 = 3(4)(1) - 4 = 12 - 4 = 8

    f(2,1)=4,8\nabla f(2,-1) = \langle -4, 8 \rangle

    Step 3: Find the unit vector u\mathbf{u} in the direction of v\mathbf{v}.

    v=22+52=4+25=29||\mathbf{v}|| = \sqrt{2^2 + 5^2} = \sqrt{4+25} = \sqrt{29}

    u=vv=229,529\mathbf{u} = \frac{\mathbf{v}}{||\mathbf{v}||} = \left\langle \frac{2}{\sqrt{29}}, \frac{5}{\sqrt{29}} \right\rangle

    Step 4: Calculate the directional derivative using Duf=fuD_{\mathbf{u}}f = \nabla f \cdot \mathbf{u}.

    Duf(2,1)=4,8229,529D_{\mathbf{u}}f(2,-1) = \langle -4, 8 \rangle \cdot \left\langle \frac{2}{\sqrt{29}}, \frac{5}{\sqrt{29}} \right\rangle

    =(4)(229)+(8)(529)= (-4) \left(\frac{2}{\sqrt{29}}\right) + (8) \left(\frac{5}{\sqrt{29}}\right)

    =829+4029=3229= -\frac{8}{\sqrt{29}} + \frac{40}{\sqrt{29}} = \frac{32}{\sqrt{29}}

    Answer: The directional derivative is 3229\frac{32}{\sqrt{29}}.

    :::question type="NAT" question="Find the maximum rate of increase of f(x,y)=ln(x2+y2)f(x,y) = \ln(x^2+y^2) at the point (1,1)(1,1)." answer="2\sqrt{2}" hint="The maximum rate of increase is given by the magnitude of the gradient vector." solution="Step 1: Calculate the partial derivatives fxf_x and fyf_y.

    fx(x,y)=x(ln(x2+y2))=1x2+y2(2x)=2xx2+y2f_x(x,y) = \frac{\partial}{\partial x} (\ln(x^2+y^2)) = \frac{1}{x^2+y^2} \cdot (2x) = \frac{2x}{x^2+y^2}

    fy(x,y)=y(ln(x2+y2))=1x2+y2(2y)=2yx2+y2f_y(x,y) = \frac{\partial}{\partial y} (\ln(x^2+y^2)) = \frac{1}{x^2+y^2} \cdot (2y) = \frac{2y}{x^2+y^2}

    Step 2: Evaluate the gradient vector at the point (1,1)(1,1).

    fx(1,1)=2(1)12+12=22=1f_x(1,1) = \frac{2(1)}{1^2+1^2} = \frac{2}{2} = 1

    fy(1,1)=2(1)12+12=22=1f_y(1,1) = \frac{2(1)}{1^2+1^2} = \frac{2}{2} = 1

    f(1,1)=1,1\nabla f(1,1) = \langle 1, 1 \rangle

    Step 3: The maximum rate of increase is the magnitude of the gradient vector.

    f(1,1)=12+12=1+1=2||\nabla f(1,1)|| = \sqrt{1^2 + 1^2} = \sqrt{1+1} = \sqrt{2}
    "
    :::

    ---

    6. Differentiability

    The concept of differentiability for functions of two variables is stronger than the mere existence of partial derivatives. A function f(x,y)f(x,y) is differentiable at (a,b)(a,b) if Δz=f(a+Δx,b+Δy)f(a,b)\Delta z = f(a+\Delta x, b+\Delta y) - f(a,b) can be expressed as:

    Δz=fx(a,b)Δx+fy(a,b)Δy+ϵ1Δx+ϵ2Δy\Delta z = f_x(a,b)\Delta x + f_y(a,b)\Delta y + \epsilon_1 \Delta x + \epsilon_2 \Delta y

    where ϵ10\epsilon_1 \to 0 and ϵ20\epsilon_2 \to 0 as (Δx,Δy)(0,0)(\Delta x, \Delta y) \to (0,0). This means the function can be well-approximated by its tangent plane.

    Differentiability vs. Partial Derivatives/Continuity
      • If f(x,y)f(x,y) is differentiable at (a,b)(a,b), then f(x,y)f(x,y) is continuous at (a,b)(a,b), and fx(a,b)f_x(a,b) and fy(a,b)f_y(a,b) exist.
      • The existence of partial derivatives does NOT guarantee differentiability or continuity.
      • If fxf_x and fyf_y are continuous in an open disk containing (a,b)(a,b), then ff is differentiable at (a,b)(a,b). This is a common practical test for differentiability.

    Quick Example: Show that f(x,y)=x2yf(x,y) = x^2 y is differentiable at (1,2)(1,2).

    Step 1: Calculate the partial derivatives fxf_x and fyf_y.

    fx(x,y)=2xyf_x(x,y) = 2xy

    fy(x,y)=x2f_y(x,y) = x^2

    Step 2: Check the continuity of fxf_x and fyf_y.
    > fx(x,y)=2xyf_x(x,y) = 2xy is a polynomial, which is continuous everywhere.
    > fy(x,y)=x2f_y(x,y) = x^2 is a polynomial, which is continuous everywhere.

    Step 3: Conclude differentiability.
    > Since both fxf_x and fyf_y are continuous at (1,2)(1,2) (and everywhere else), f(x,y)f(x,y) is differentiable at (1,2)(1,2).

    Answer: f(x,y)=x2yf(x,y) = x^2 y is differentiable at (1,2)(1,2) because its partial derivatives are continuous.

    :::question type="MCQ" question="Let f(x,y)={x3x2+y2,(x,y)(0,0)0,(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^3}{x^2+y^2}, & (x,y) \neq (0,0) \\ 0, & (x,y) = (0,0) \end{cases}. Which statement is true about ff at (0,0)(0,0)?" options=["ff is differentiable at (0,0)(0,0).","ff is continuous at (0,0)(0,0) but not differentiable.","Partial derivatives fxf_x and fyf_y do not exist at (0,0)(0,0).","fxf_x and fyf_y exist at (0,0)(0,0), but ff is not continuous."] answer="ff is continuous at (0,0)(0,0) but not differentiable." hint="First check continuity using polar coordinates. Then check existence of partial derivatives using definition. Finally, consider differentiability." solution="Step 1: Check continuity at (0,0)(0,0).
    > f(0,0)=0f(0,0) = 0.
    > For the limit, use polar coordinates: x=rcosθ,y=rsinθx=r \cos \theta, y=r \sin \theta.

    lim(x,y)(0,0)x3x2+y2=limr0+(rcosθ)3r2cos2θ+r2sin2θ=limr0+r3cos3θr2\lim_{(x,y)\to(0,0)} \frac{x^3}{x^2+y^2} = \lim_{r \to 0^+} \frac{(r \cos \theta)^3}{r^2 \cos^2 \theta + r^2 \sin^2 \theta} = \lim_{r \to 0^+} \frac{r^3 \cos^3 \theta}{r^2}

    =limr0+rcos3θ=0= \lim_{r \to 0^+} r \cos^3 \theta = 0

    > Since lim(x,y)(0,0)f(x,y)=0=f(0,0)\lim_{(x,y)\to(0,0)} f(x,y) = 0 = f(0,0), ff is continuous at (0,0)(0,0).

    Step 2: Check existence of partial derivatives at (0,0)(0,0) using the definition.

    fx(0,0)=limh0f(h,0)f(0,0)h=limh0h3h2+020h=limh0h3/h2h=limh0hh=1f_x(0,0) = \lim_{h \to 0} \frac{f(h,0) - f(0,0)}{h} = \lim_{h \to 0} \frac{\frac{h^3}{h^2+0^2} - 0}{h} = \lim_{h \to 0} \frac{h^3/h^2}{h} = \lim_{h \to 0} \frac{h}{h} = 1

    fy(0,0)=limh0f(0,h)f(0,0)h=limh00302+h20h=limh00h=0f_y(0,0) = \lim_{h \to 0} \frac{f(0,h) - f(0,0)}{h} = \lim_{h \to 0} \frac{\frac{0^3}{0^2+h^2} - 0}{h} = \lim_{h \to 0} \frac{0}{h} = 0

    > Both partial derivatives fx(0,0)=1f_x(0,0)=1 and fy(0,0)=0f_y(0,0)=0 exist.

    Step 3: Check differentiability.
    > A function is differentiable if Δz=fx(a,b)Δx+fy(a,b)Δy+ϵ1Δx+ϵ2Δy\Delta z = f_x(a,b)\Delta x + f_y(a,b)\Delta y + \epsilon_1 \Delta x + \epsilon_2 \Delta y.
    > At (0,0)(0,0), we need f(x,y)f(0,0)=fx(0,0)x+fy(0,0)y+ϵ1x+ϵ2yf(x,y) - f(0,0) = f_x(0,0)x + f_y(0,0)y + \epsilon_1 x + \epsilon_2 y.
    > x3x2+y20=1x+0y+ϵ1x+ϵ2y\frac{x^3}{x^2+y^2} - 0 = 1 \cdot x + 0 \cdot y + \epsilon_1 x + \epsilon_2 y.
    > x3x2+y2=x+ϵ1x+ϵ2y\frac{x^3}{x^2+y^2} = x + \epsilon_1 x + \epsilon_2 y.
    > So ϵ1x+ϵ2y=x3x2+y2x=x3x(x2+y2)x2+y2=x3x3xy2x2+y2=xy2x2+y2\epsilon_1 x + \epsilon_2 y = \frac{x^3}{x^2+y^2} - x = \frac{x^3 - x(x^2+y^2)}{x^2+y^2} = \frac{x^3 - x^3 - xy^2}{x^2+y^2} = \frac{-xy^2}{x^2+y^2}.
    > We need lim(x,y)(0,0)ϵ1x+ϵ2yx2+y2=0\lim_{(x,y)\to(0,0)} \frac{\epsilon_1 x + \epsilon_2 y}{\sqrt{x^2+y^2}} = 0.
    > This is equivalent to lim(x,y)(0,0)xy2(x2+y2)3/2=0\lim_{(x,y)\to(0,0)} \frac{-xy^2}{(x^2+y^2)^{3/2}} = 0.
    > Using polar coordinates: (rcosθ)(rsinθ)2(r2)3/2=r3cosθsin2θr3=cosθsin2θ\frac{-(r \cos \theta)(r \sin \theta)^2}{(r^2)^{3/2}} = \frac{-r^3 \cos \theta \sin^2 \theta}{r^3} = -\cos \theta \sin^2 \theta.
    > This expression depends on θ\theta, so its limit as r0r \to 0 does not exist (e.g., if θ=0\theta = 0, it is 0; if θ=π/2\theta = \pi/2, it is 0; if θ=π/4\theta = \pi/4, it is 1/2(1/2)2=1/(22)-1/\sqrt{2} \cdot (1/\sqrt{2})^2 = -1/(2\sqrt{2})).
    > Therefore, ff is not differentiable at (0,0)(0,0).

    Conclusion: ff is continuous at (0,0)(0,0) and its partial derivatives exist, but it is not differentiable. This corresponds to option 'f is continuous at (0,0)(0,0) but not differentiable.'."
    :::

    ---

    Advanced Applications

    Quick Example: A rectangular box has length LL, width WW, and height HH. If L=2L=2 m, W=3W=3 m, H=1H=1 m, and LL is increasing at 0.10.1 m/s, WW is decreasing at 0.20.2 m/s, and HH is increasing at 0.050.05 m/s, find the rate of change of the volume VV at this instant.

    Step 1: Define the volume function and its partial derivatives.
    > The volume is V=LWHV = LWH.
    >

    VL=WH\frac{\partial V}{\partial L} = WH

    >
    VW=LH\frac{\partial V}{\partial W} = LH

    >
    VH=LW\frac{\partial V}{\partial H} = LW

    Step 2: Identify the given rates of change.
    > dLdt=0.1\frac{dL}{dt} = 0.1 m/s
    > dWdt=0.2\frac{dW}{dt} = -0.2 m/s (decreasing)
    > dHdt=0.05\frac{dH}{dt} = 0.05 m/s

    Step 3: Apply the chain rule for total derivative dVdt\frac{dV}{dt}.
    >

    dVdt=VLdLdt+VWdWdt+VHdHdt\frac{dV}{dt} = \frac{\partial V}{\partial L}\frac{dL}{dt} + \frac{\partial V}{\partial W}\frac{dW}{dt} + \frac{\partial V}{\partial H}\frac{dH}{dt}

    Step 4: Substitute the given values (L=2,W=3,H=1L=2, W=3, H=1) and rates into the chain rule.
    > At this instant:
    > VL=(3)(1)=3\frac{\partial V}{\partial L} = (3)(1) = 3
    > VW=(2)(1)=2\frac{\partial V}{\partial W} = (2)(1) = 2
    > VH=(2)(3)=6\frac{\partial V}{\partial H} = (2)(3) = 6
    >
    >

    >dVdt=(3)(0.1)+(2)(0.2)+(6)(0.05)>=0.30.4+0.3>=0.2>\begin{aligned}> \frac{dV}{dt} & = (3)(0.1) + (2)(-0.2) + (6)(0.05) \\
    > & = 0.3 - 0.4 + 0.3 \\
    > & = 0.2
    > \end{aligned}

    Answer: The volume is increasing at a rate of 0.20.2 m3^3/s.

    :::question type="NAT" question="If f(x,y)=sin(xy)f(x,y) = \sin(xy), find fxyy(x,y)f_{xyy}(x,y) at (1,π/2)(1, \pi/2)." answer="-2" hint="Calculate partial derivatives sequentially: fxf_x, then fxyf_{xy}, then fxyyf_{xyy}." solution="Step 1: Calculate fx(x,y)f_x(x,y).
    >

    fx(x,y)=x(sin(xy))=cos(xy)yf_x(x,y) = \frac{\partial}{\partial x} (\sin(xy)) = \cos(xy) \cdot y

    Step 2: Calculate fxy(x,y)f_{xy}(x,y).
    >

    fxy(x,y)=y(ycos(xy))f_{xy}(x,y) = \frac{\partial}{\partial y} (y \cos(xy))

    > Using the product rule:
    >
    >=(1)cos(xy)+y(sin(xy)x)>=cos(xy)xysin(xy)>\begin{aligned}> & = (1) \cos(xy) + y (-\sin(xy) \cdot x) \\
    > & = \cos(xy) - xy \sin(xy)
    > \end{aligned}

    Step 3: Calculate fxyy(x,y)f_{xyy}(x,y).
    >

    fxyy(x,y)=y(cos(xy)xysin(xy))f_{xyy}(x,y) = \frac{\partial}{\partial y} (\cos(xy) - xy \sin(xy))

    >
    >=(sin(xy)x)[(x)(1)sin(xy)+(xy)(cos(xy)x)]>=xsin(xy)xsin(xy)x2ycos(xy)>=2xsin(xy)x2ycos(xy)>\begin{aligned}> & = (-\sin(xy) \cdot x) - \left[ (x)(1) \sin(xy) + (xy)(\cos(xy) \cdot x) \right] \\
    > & = -x \sin(xy) - x \sin(xy) - x^2 y \cos(xy) \\
    > & = -2x \sin(xy) - x^2 y \cos(xy)
    > \end{aligned}

    Step 4: Evaluate fxyy(1,π/2)f_{xyy}(1, \pi/2).
    > Substitute x=1,y=π/2x=1, y=\pi/2:
    >

    >fxyy(1,π/2)=2(1)sin(1π/2)(1)2(π/2)cos(1π/2)>=2sin(π/2)(π/2)cos(π/2)>=2(1)(π/2)(0)>=20>=2>\begin{aligned}> f_{xyy}(1, \pi/2) & = -2(1) \sin(1 \cdot \pi/2) - (1)^2 (\pi/2) \cos(1 \cdot \pi/2) \\
    > & = -2 \sin(\pi/2) - (\pi/2) \cos(\pi/2) \\
    > & = -2(1) - (\pi/2)(0) \\
    > & = -2 - 0 \\
    > & = -2
    > \end{aligned}

    Answer: 2\boxed{-2}"
    :::

    ---

    Problem-Solving Strategies

    💡 CUET PG Strategy: Limits

    When evaluating limits at the origin (0,0)(0,0) for rational functions:

    • Try direct substitution: If it yields a determinate form, that's the limit.

    • Test paths: If direct substitution yields an indeterminate form (0/00/0), try paths like y=mxy=mx or y=x2y=x^2. If different paths yield different limits, the overall limit does not exist.

    • Polar coordinates: For expressions involving x2+y2x^2+y^2, convert to polar coordinates (x=rcosθ,y=rsinθx=r \cos \theta, y=r \sin \theta). If the limit as r0r \to 0 is independent of θ\theta, the limit exists. Otherwise, it does not.

    💡 CUET PG Strategy: Chain Rule
      • Draw a tree diagram: For z=f(x,y)z=f(x,y) where x=x(s,t)x=x(s,t) and y=y(s,t)y=y(s,t), draw zz at the top, branches to xx and yy, then branches from xx and yy to ss and tt. To find zs\frac{\partial z}{\partial s}, trace all paths from zz to ss, multiplying derivatives along each path, and then summing the results.
      • Identify variables: Clearly distinguish between independent variables (s,ts,t) and intermediate variables (x,yx,y).

    ---

    Common Mistakes

    ⚠️ Common Mistake: Limit Existence

    Assuming limit exists if paths y=0,x=0,y=mxy=0, x=0, y=mx yield the same result.
    ✅ These paths are insufficient to prove existence. To prove existence, use the ϵδ\epsilon-\delta definition, Squeeze Theorem, or polar coordinates yielding an θ\theta-independent result. To prove non-existence, two different path limits are enough.

    ⚠️ Common Mistake: Continuity vs. Differentiability

    Believing that existence of partial derivatives implies differentiability or continuity.
    ✅ Existence of partial derivatives at a point does not guarantee continuity or differentiability at that point. A function can have partial derivatives but be discontinuous. However, differentiability implies continuity and existence of partial derivatives. Continuity of partial derivatives implies differentiability.

    ⚠️ Common Mistake: Chain Rule Application

    Forgetting to convert intermediate variables to the final independent variables when calculating total derivatives.
    ✅ When finding dwdt\frac{dw}{dt} for w(x,y,z)w(x,y,z) where x(t),y(t),z(t)x(t), y(t), z(t), all partial derivatives wx,wy,wz\frac{\partial w}{\partial x}, \frac{\partial w}{\partial y}, \frac{\partial w}{\partial z} must be expressed in terms of tt before summing the products.

    ---

    Practice Questions

    :::question type="MCQ" question="Let f(x,y)={x2+y2sin(x2+y2),(x,y)(0,0)L,(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2+y^2}{\sin(x^2+y^2)}, & (x,y) \neq (0,0) \\ L, & (x,y) = (0,0) \end{cases}. For ff to be continuous at (0,0)(0,0), the value of LL must be:" options=["0","1","2","Does not exist"] answer="1" hint="Recall the standard limit limθ0θsinθ=1\lim_{\theta \to 0} \frac{\theta}{\sin \theta} = 1." solution="Step 1: For ff to be continuous at (0,0)(0,0), we require lim(x,y)(0,0)f(x,y)=f(0,0)\lim_{(x,y)\to(0,0)} f(x,y) = f(0,0).
    > We are given f(0,0)=Lf(0,0) = L.

    Step 2: Evaluate the limit lim(x,y)(0,0)x2+y2sin(x2+y2)\lim_{(x,y)\to(0,0)} \frac{x^2+y^2}{\sin(x^2+y^2)}.
    > Let u=x2+y2u = x^2+y^2. As (x,y)(0,0)(x,y) \to (0,0), u0u \to 0.
    > The limit becomes limu0usinu\lim_{u \to 0} \frac{u}{\sin u}.
    > This is a standard limit, which evaluates to 1.

    Step 3: Set the limit equal to LL.
    > Thus, L=1L=1 for ff to be continuous at (0,0)(0,0).
    Answer: 1\boxed{1}"
    :::

    :::question type="MCQ" question="If f(x,y)=x2ln(y)f(x,y) = x^2 \ln(y), which of the following is true?" options=["fxx=2lnyf_{xx} = 2 \ln y","fyy=x2/y2f_{yy} = x^2/y^2","fxy=2xlnyf_{xy} = 2x \ln y","fyx=2x/y2f_{yx} = 2x/y^2"] answer="fxx=2lnyf_{xx} = 2 \ln y" hint="Calculate the partial derivatives and compare with the options." solution="Step 1: Calculate fxf_x.
    >

    fx=x(x2lny)=2xlnyf_x = \frac{\partial}{\partial x}(x^2 \ln y) = 2x \ln y

    Step 2: Calculate fyf_y.
    >

    fy=y(x2lny)=x21y=x2yf_y = \frac{\partial}{\partial y}(x^2 \ln y) = x^2 \frac{1}{y} = \frac{x^2}{y}

    Step 3: Calculate second-order partial derivatives.
    >

    fxx=x(2xlny)=2lnyf_{xx} = \frac{\partial}{\partial x}(2x \ln y) = 2 \ln y

    >
    fyy=y(x2y)=x2(1y2)=x2y2f_{yy} = \frac{\partial}{\partial y}(\frac{x^2}{y}) = x^2 (-\frac{1}{y^2}) = -\frac{x^2}{y^2}

    >
    fxy=y(2xlny)=2x1y=2xyf_{xy} = \frac{\partial}{\partial y}(2x \ln y) = 2x \frac{1}{y} = \frac{2x}{y}

    >
    fyx=x(x2y)=2xyf_{yx} = \frac{\partial}{\partial x}(\frac{x^2}{y}) = \frac{2x}{y}

    Step 4: Compare with options.
    > - Option 1: fxx=2lnyf_{xx} = 2 \ln y. This is correct.
    > - Option 2: fyy=x2/y2f_{yy} = x^2/y^2. This is incorrect (should be x2/y2-x^2/y^2).
    > - Option 3: fxy=2xlnyf_{xy} = 2x \ln y. This is incorrect (should be 2x/y2x/y).
    > - Option 4: fyx=2x/y2f_{yx} = 2x/y^2. This is incorrect (should be 2x/y2x/y).
    >
    > Therefore, only the first option is correct.
    Answer: fxx=2lny\boxed{f_{xx} = 2 \ln y}"
    :::

    :::question type="MSQ" question="Which of the following functions are continuous at the origin (0,0)(0,0)?" options=["f(x,y)={x2yx2+y2,(x,y)(0,0)0,(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2y}{x^2+y^2}, & (x,y) \neq (0,0) \\ 0, & (x,y) = (0,0) \end{cases}","g(x,y)={xyx2+y2,(x,y)(0,0)0,(x,y)=(0,0)g(x,y) = \begin{cases} \frac{xy}{x^2+y^2}, & (x,y) \neq (0,0) \\ 0, & (x,y) = (0,0) \end{cases}","h(x,y)=x2+y2h(x,y) = x^2+y^2","k(x,y)={x3+y3x2+y2,(x,y)(0,0)0,(x,y)=(0,0)k(x,y) = \begin{cases} \frac{x^3+y^3}{x^2+y^2}, & (x,y) \neq (0,0) \\ 0, & (x,y) = (0,0) \end{cases}"] answer="f(x,y)={x2yx2+y2,(x,y)(0,0)0,(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2y}{x^2+y^2}, & (x,y) \neq (0,0) \\ 0, & (x,y) = (0,0) \end{cases},h(x,y)=x2+y2h(x,y) = x^2+y^2,k(x,y)={x3+y3x2+y2,(x,y)(0,0)0,(x,y)=(0,0)k(x,y) = \begin{cases} \frac{x^3+y^3}{x^2+y^2}, & (x,y) \neq (0,0) \\ 0, & (x,y) = (0,0) \end{cases}" hint="For each piecewise function, check if the limit at (0,0)(0,0) equals the function value at (0,0)(0,0). For polynomial functions, they are continuous everywhere." solution="1. For f(x,y)f(x,y):
    > We have f(0,0)=0f(0,0)=0.
    > lim(x,y)(0,0)x2yx2+y2\lim_{(x,y)\to(0,0)} \frac{x^2y}{x^2+y^2}. Using polar coordinates x=rcosθ,y=rsinθx=r \cos \theta, y=r \sin \theta:
    >

    limr0+(rcosθ)2(rsinθ)r2=limr0+rcos2θsinθ=0\lim_{r \to 0^+} \frac{(r \cos \theta)^2 (r \sin \theta)}{r^2} = \lim_{r \to 0^+} r \cos^2 \theta \sin \theta = 0

    > Since the limit is 00 and f(0,0)=0f(0,0)=0, f(x,y)f(x,y) is continuous at (0,0)(0,0).

    2. For g(x,y)g(x,y):
    > We have g(0,0)=0g(0,0)=0.
    > lim(x,y)(0,0)xyx2+y2\lim_{(x,y)\to(0,0)} \frac{xy}{x^2+y^2}. Along y=xy=x, the limit is limx0x22x2=12\lim_{x \to 0} \frac{x^2}{2x^2} = \frac{1}{2}. Along y=0y=0, the limit is 00.
    > Since limits along different paths are different, the overall limit does not exist.
    > Thus, g(x,y)g(x,y) is not continuous at (0,0)(0,0).

    3. For h(x,y)h(x,y):
    > h(x,y)=x2+y2h(x,y) = x^2+y^2 is a polynomial. Polynomials are continuous everywhere.
    > Thus, h(x,y)h(x,y) is continuous at (0,0)(0,0).

    4. For k(x,y)k(x,y):
    > We have k(0,0)=0k(0,0)=0.
    > lim(x,y)(0,0)x3+y3x2+y2\lim_{(x,y)\to(0,0)} \frac{x^3+y^3}{x^2+y^2}. Using polar coordinates x=rcosθ,y=rsinθx=r \cos \theta, y=r \sin \theta:
    >

    limr0+r3cos3θ+r3sin3θr2=limr0+r(cos3θ+sin3θ)=0\lim_{r \to 0^+} \frac{r^3 \cos^3 \theta + r^3 \sin^3 \theta}{r^2} = \lim_{r \to 0^+} r (\cos^3 \theta + \sin^3 \theta) = 0

    > Since the limit is 00 and k(0,0)=0k(0,0)=0, k(x,y)k(x,y) is continuous at (0,0)(0,0).

    Conclusion: Functions ff, hh, and kk are continuous at the origin.
    Answer: f,h,k are continuous\boxed{f, h, k \text{ are continuous}}"
    :::

    :::question type="NAT" question="If z=ex+2yz = e^{x+2y}, where x=sintx = \sin t and y=costy = \cos t, find dzdt\frac{dz}{dt} at t=π2t=\frac{\pi}{2}." answer="-2e" hint="Use the chain rule for total derivatives." solution="Step 1: Find partial derivatives of zz with respect to xx and yy.
    >

    zx=x(ex+2y)=ex+2y\frac{\partial z}{\partial x} = \frac{\partial}{\partial x} (e^{x+2y}) = e^{x+2y}

    >
    zy=y(ex+2y)=2ex+2y\frac{\partial z}{\partial y} = \frac{\partial}{\partial y} (e^{x+2y}) = 2e^{x+2y}

    Step 2: Find derivatives of xx and yy with respect to tt.
    >

    dxdt=ddt(sint)=cost\frac{dx}{dt} = \frac{d}{dt} (\sin t) = \cos t

    >
    dydt=ddt(cost)=sint\frac{dy}{dt} = \frac{d}{dt} (\cos t) = -\sin t

    Step 3: Apply the chain rule for dzdt\frac{dz}{dt}.
    >

    >dzdt=zxdxdt+zydydt>=(ex+2y)(cost)+(2ex+2y)(sint)>\begin{aligned}> \frac{dz}{dt} & = \frac{\partial z}{\partial x}\frac{dx}{dt} + \frac{\partial z}{\partial y}\frac{dy}{dt} \\
    > & = (e^{x+2y})(\cos t) + (2e^{x+2y})(-\sin t)
    > \end{aligned}

    Step 4: Evaluate x,yx, y and their derivatives at t=π2t=\frac{\pi}{2}.
    > At t=π2t=\frac{\pi}{2}:
    > x=sin(π2)=1x = \sin(\frac{\pi}{2}) = 1
    > y=cos(π2)=0y = \cos(\frac{\pi}{2}) = 0
    > cost=cos(π2)=0\cos t = \cos(\frac{\pi}{2}) = 0
    > sint=sin(π2)=1\sin t = \sin(\frac{\pi}{2}) = 1
    > The exponent x+2y=1+2(0)=1x+2y = 1+2(0) = 1. So ex+2y=e1=ee^{x+2y} = e^1 = e.

    Step 5: Substitute these values into the dzdt\frac{dz}{dt} expression.
    >

    >dzdt=(e)(0)+(2e)(1)>=02e>=2e>\begin{aligned}> \frac{dz}{dt} & = (e)(0) + (2e)(-1) \\
    > & = 0 - 2e \\
    > & = -2e
    > \end{aligned}

    Answer: 2e\boxed{-2e}"
    :::

    ---

    Summary

    Key Formulas & Takeaways

    | # | Formula/Concept | Expression |
    |---|----------------|------------|
    | 1 | Limit along path y=mxy=mx | limxaf(x,mx+b)\lim_{x \to a} f(x, mx+b) |
    | 2 | Limit using Polar Coordinates | limr0+f(rcosθ,rsinθ)\lim_{r \to 0^+} f(r \cos \theta, r \sin \theta) |
    | 3 | Continuity at (a,b)(a,b) | lim(x,y)(a,b)f(x,y)=f(a,b)\lim_{(x,y) \to (a,b)} f(x,y) = f(a,b) |
    | 4 | Partial Derivative fxf_x | fx(x,y)=limh0f(x+h,y)f(x,y)hf_x(x,y) = \lim_{h \to 0} \frac{f(x+h, y) - f(x, y)}{h} |
    | 5 | Clairaut's Theorem | If fxy,fyxf_{xy}, f_{yx} continuous, then fxy=fyxf_{xy}=f_{yx} |
    | 6 | Chain Rule for z=f(x,y)z=f(x,y), x=x(s,t)x=x(s,t), y=y(s,t)y=y(s,t) | zs=zxxs+zyys\frac{\partial z}{\partial s} = \frac{\partial z}{\partial x} \frac{\partial x}{\partial s} + \frac{\partial z}{\partial y} \frac{\partial y}{\partial s} |
    | 7 | Gradient Vector | f=fx,fy\nabla f = \left\langle \frac{\partial f}{\partial x}, \frac{\partial f}{\partial y} \right\rangle |
    | 8 | Directional Derivative DufD_{\mathbf{u}}f | Duf=fuD_{\mathbf{u}}f = \nabla f \cdot \mathbf{u} (where u\mathbf{u} is unit vector) |
    | 9 | Differentiability | Implies continuity and existence of partial derivatives. Continuous partials implies differentiability. |

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    What's Next?

    💡 Continue Learning

    This topic connects to:

      • Optimization of Functions of Several Variables: Partial derivatives are fundamental for finding critical points and classifying extrema (local maxima, minima, saddle points).

      • Multiple Integrals: Understanding the domain of functions and their continuity is crucial for setting up and evaluating double and triple integrals.

      • Vector Calculus: Concepts like the gradient, divergence, and curl build upon partial differentiation and are essential in fields such as physics and engineering.

    ---

    💡 Next Up

    Proceeding to Differentiability.

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    Part 2: Differentiability

    We examine the concept of differentiability for functions mapping from R2\mathbb{R}^2 to R\mathbb{R}, a fundamental notion in multivariable calculus. Our focus is on the precise definitions and conditions that allow for local linear approximations, which is crucial for understanding function behavior and solving related problems in competitive examinations.

    ---

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    Core Concepts

    1. Partial Derivatives

    For a function f(x,y)f(x,y), partial derivatives measure the rate of change of ff with respect to one variable, holding the other constant. These are foundational for defining differentiability.

    📖 Partial Derivative

    The partial derivative of f(x,y)f(x,y) with respect to xx at (a,b)(a,b) is defined as:

    fx(a,b)=limh0f(a+h,b)f(a,b)hf_x(a,b) = \lim_{h \to 0} \frac{f(a+h, b) - f(a,b)}{h}

    Similarly, the partial derivative with respect to yy at (a,b)(a,b) is:
    fy(a,b)=limk0f(a,b+k)f(a,b)kf_y(a,b) = \lim_{k \to 0} \frac{f(a, b+k) - f(a,b)}{k}

    Quick Example: Consider f(x,y)=x2y+3y3f(x,y) = x^2y + 3y^3. We compute its partial derivatives at a general point (x,y)(x,y).

    Step 1: Compute fx(x,y)f_x(x,y) by treating yy as a constant.
    >

    fx(x,y)=x(x2y+3y3)=2xyf_x(x,y) = \frac{\partial}{\partial x}(x^2y + 3y^3) = 2xy

    Step 2: Compute fy(x,y)f_y(x,y) by treating xx as a constant.
    >

    fy(x,y)=y(x2y+3y3)=x2+9y2f_y(x,y) = \frac{\partial}{\partial y}(x^2y + 3y^3) = x^2 + 9y^2

    Answer: fx(x,y)=2xyf_x(x,y) = 2xy and fy(x,y)=x2+9y2f_y(x,y) = x^2 + 9y^2.

    :::question type="MCQ" question="Let

    f(x,y)={x3y3x2+y2;(x,y)(0,0)0;(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^3-y^3}{x^2+y^2} & ; (x,y) \ne (0,0) \\ 0 & ; (x,y) = (0,0) \end{cases}
    . What is the value of fx(0,0)f_x(0,0)?" options=["0","1","-1","Does not exist"] answer="1" hint="Use the limit definition for partial derivatives at (0,0)." solution="Step 1: Apply the definition of fx(0,0)f_x(0,0).
    >
    fx(0,0)=limh0f(h,0)f(0,0)h\begin{aligned}f_x(0,0) & = \lim_{h \to 0} \frac{f(h,0) - f(0,0)}{h} \\\end{aligned}

    Step 2: Substitute the function definition.
    >

    fx(0,0)=limh0h303h2+020h=limh0h3h2h=limh0hh=limh01=1\begin{aligned}f_x(0,0) & = \lim_{h \to 0} \frac{\frac{h^3-0^3}{h^2+0^2} - 0}{h} \\
    & = \lim_{h \to 0} \frac{\frac{h^3}{h^2}}{h} \\
    & = \lim_{h \to 0} \frac{h}{h} \\
    & = \lim_{h \to 0} 1 = 1\end{aligned}

    Answer: \boxed{1}"
    :::

    ---

    2. Continuity of Multivariable Functions

    Continuity is a prerequisite for differentiability. A function is continuous at a point if its limit exists at that point, the function is defined at that point, and these two values are equal.

    📖 Continuity at a Point

    A function f:DRf: D \to \mathbb{R} where DR2D \subseteq \mathbb{R}^2 is continuous at a point (a,b)D(a,b) \in D if lim(x,y)(a,b)f(x,y)=f(a,b)\lim_{(x,y) \to (a,b)} f(x,y) = f(a,b). This implies that the limit must exist and be equal to the function's value at the point.

    We often check for continuity by evaluating the limit along different paths. If the limits along different paths are unequal, the overall limit does not exist, and thus the function is discontinuous.

    Quick Example: Examine the continuity of f(x,y)=xyx2+y2f(x,y) = \frac{xy}{x^2+y^2} at (0,0)(0,0). For (x,y)(0,0)(x,y) \ne (0,0), ff is well-defined. We define f(0,0)=0f(0,0)=0.

    Step 1: Evaluate the limit along the path y=mxy=mx.
    >

    limx0f(x,mx)=limx0x(mx)x2+(mx)2=limx0mx2x2(1+m2)=m1+m2\begin{aligned}\lim_{x \to 0} f(x,mx) & = \lim_{x \to 0} \frac{x(mx)}{x^2+(mx)^2} \\
    & = \lim_{x \to 0} \frac{mx^2}{x^2(1+m^2)} \\
    & = \frac{m}{1+m^2}\end{aligned}

    Step 2: Observe the path dependence.
    The limit m1+m2\frac{m}{1+m^2} depends on mm. Since the limit is not unique (e.g., for m=1m=1, it is 1/21/2; for m=2m=2, it is 2/52/5), the limit of f(x,y)f(x,y) as (x,y)(0,0)(x,y) \to (0,0) does not exist.

    Answer: f(x,y)f(x,y) is discontinuous at (0,0)(0,0).

    :::question type="MCQ" question="Let

    f(x,y)={x2yx4+y2;(x,y)(0,0)0;(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2y}{x^4+y^2} & ; (x,y) \ne (0,0) \\ 0 & ; (x,y) = (0,0) \end{cases}
    . Which of the following statements is true regarding f(x,y)f(x,y) at (0,0)(0,0)?" options=["ff is continuous at (0,0)(0,0)","The limit lim(x,y)(0,0)f(x,y)\lim_{(x,y) \to (0,0)} f(x,y) exists and is 00","ff is discontinuous at (0,0)(0,0) because the limit along y=x2y=x^2 is non-zero","The limit along any straight line path y=mxy=mx is non-zero"] answer="ff is discontinuous at (0,0)(0,0) because the limit along y=x2y=x^2 is non-zero" hint="Check limits along different paths, especially parabolic paths like y=x2y=x^2 or y=kx2y=kx^2." solution="Step 1: Evaluate the limit along straight line paths y=mxy=mx.
    >
    limx0f(x,mx)=limx0x2(mx)x4+(mx)2=limx0mx3x4+m2x2=limx0mx3x2(x2+m2)=limx0mxx2+m2=0\begin{aligned}\lim_{x \to 0} f(x,mx) & = \lim_{x \to 0} \frac{x^2(mx)}{x^4+(mx)^2} \\
    & = \lim_{x \to 0} \frac{mx^3}{x^4+m^2x^2} \\
    & = \lim_{x \to 0} \frac{mx^3}{x^2(x^2+m^2)} \\
    & = \lim_{x \to 0} \frac{mx}{x^2+m^2} = 0\end{aligned}

    This suggests the limit might be 00.

    Step 2: Evaluate the limit along a parabolic path y=x2y=x^2.
    >

    limx0f(x,x2)=limx0x2(x2)x4+(x2)2=limx0x4x4+x4=limx0x42x4=12\begin{aligned}\lim_{x \to 0} f(x,x^2) & = \lim_{x \to 0} \frac{x^2(x^2)}{x^4+(x^2)^2} \\
    & = \lim_{x \to 0} \frac{x^4}{x^4+x^4} \\
    & = \lim_{x \to 0} \frac{x^4}{2x^4} = \frac{1}{2}\end{aligned}

    Step 3: Compare results.
    Since the limit along y=x2y=x^2 is 1/21/2, which is not equal to f(0,0)=0f(0,0)=0 (or the limit along straight lines), the limit of f(x,y)f(x,y) as (x,y)(0,0)(x,y) \to (0,0) does not exist. Therefore, ff is discontinuous at (0,0)(0,0).

    Answer: \boxed{\text{ff is discontinuous at (0,0)(0,0) because the limit along y=x2y=x^2 is non-zero}}"
    :::

    ---

    3. Differentiability

    Differentiability for functions of two variables extends the concept of a tangent line to a tangent plane. It implies that the function can be well-approximated by a linear function locally.

    📖 Differentiability

    A function f:DRf: D \to \mathbb{R} where DR2D \subseteq \mathbb{R}^2 is differentiable at a point (a,b)D(a,b) \in D if fx(a,b)f_x(a,b) and fy(a,b)f_y(a,b) exist, and

    lim(h,k)(0,0)f(a+h,b+k)f(a,b)hfx(a,b)kfy(a,b)h2+k2=0\lim_{(h,k) \to (0,0)} \frac{f(a+h, b+k) - f(a,b) - hf_x(a,b) - kf_y(a,b)}{\sqrt{h^2+k^2}} = 0

    This limit must hold regardless of the path taken by (h,k)(h,k) towards (0,0)(0,0).

    Key Implication

    If ff is differentiable at (a,b)(a,b), then ff is continuous at (a,b)(a,b). The converse is not necessarily true.

    Quick Example: Investigate the differentiability of f(x,y)=xyf(x,y) = \sqrt{|xy|} at (0,0)(0,0). This function appeared in a PYQ.

    Step 1: Calculate the partial derivatives at (0,0)(0,0).
    >

    fx(0,0)=limh0f(h,0)f(0,0)h=limh0h00h=0fy(0,0)=limk0f(0,k)f(0,0)k=limk00k0k=0\begin{aligned}f_x(0,0) & = \lim_{h \to 0} \frac{f(h,0) - f(0,0)}{h} = \lim_{h \to 0} \frac{\sqrt{|h \cdot 0|} - 0}{h} = 0 \\
    f_y(0,0) & = \lim_{k \to 0} \frac{f(0,k) - f(0,0)}{k} = \lim_{k \to 0} \frac{\sqrt{|0 \cdot k|} - 0}{k} = 0\end{aligned}

    Both partial derivatives exist and are 00.

    Step 2: Apply the differentiability definition limit.
    >

    lim(h,k)(0,0)f(h,k)f(0,0)hfx(0,0)kfy(0,0)h2+k2=lim(h,k)(0,0)hk0h(0)k(0)h2+k2=lim(h,k)(0,0)hkh2+k2\begin{aligned} & \lim_{(h,k) \to (0,0)} \frac{f(h,k) - f(0,0) - hf_x(0,0) - kf_y(0,0)}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{\sqrt{|hk|} - 0 - h(0) - k(0)}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{\sqrt{|hk|}}{\sqrt{h^2+k^2}}\end{aligned}

    Step 3: Evaluate the limit using polar coordinates (h=rcosθ,k=rsinθh=r\cos\theta, k=r\sin\theta).
    >

    =limr0(rcosθ)(rsinθ)(rcosθ)2+(rsinθ)2=limr0r2cosθsinθr2(cos2θ+sin2θ)=limr0rcosθsinθr=cosθsinθ\begin{aligned} & = \lim_{r \to 0} \frac{\sqrt{|(r\cos\theta)(r\sin\theta)|}}{\sqrt{(r\cos\theta)^2+(r\sin\theta)^2}} \\
    & = \lim_{r \to 0} \frac{\sqrt{|r^2\cos\theta\sin\theta|}}{\sqrt{r^2(\cos^2\theta+\sin^2\theta)}} \\
    & = \lim_{r \to 0} \frac{r\sqrt{|\cos\theta\sin\theta|}}{r} \\
    & = \sqrt{|\cos\theta\sin\theta|}\end{aligned}

    Step 4: Conclude based on the limit value.
    The limit cosθsinθ\sqrt{|\cos\theta\sin\theta|} is not 00 for all θ\theta (e.g., if θ=π/4\theta = \pi/4, the limit is 1/20\sqrt{1/2} \ne 0). Therefore, the limit is not 00, and f(x,y)f(x,y) is not differentiable at (0,0)(0,0).

    Answer: f(x,y)=xyf(x,y) = \sqrt{|xy|} is not differentiable at (0,0)(0,0).

    :::question type="MCQ" question="Let

    f(x,y)={x2yx2+y2;(x,y)(0,0)0;(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2y}{x^2+y^2} & ; (x,y) \ne (0,0) \\ 0 & ; (x,y) = (0,0) \end{cases}
    . We know fx(0,0)=0f_x(0,0)=0 and fy(0,0)=0f_y(0,0)=0. Is f(x,y)f(x,y) differentiable at (0,0)(0,0)?" options=["Yes, because its partial derivatives exist and are 0","No, because its partial derivatives are not continuous","Yes, because it is continuous at (0,0)(0,0)","No, because the limit in the definition of differentiability is not 0"] answer="No, because the limit in the definition of differentiability is not 0" hint="Use the definition of differentiability. The numerator simplifies to f(h,k)f(h,k) as f(0,0)=fx(0,0)=fy(0,0)=0f(0,0)=f_x(0,0)=f_y(0,0)=0." solution="Step 1: Calculate the partial derivatives at (0,0)(0,0).
    >
    fx(0,0)=limh0f(h,0)f(0,0)h=limh0h20h2+020h=0fy(0,0)=limk0f(0,k)f(0,0)k=limk002k02+k20k=0\begin{aligned}f_x(0,0) & = \lim_{h \to 0} \frac{f(h,0) - f(0,0)}{h} = \lim_{h \to 0} \frac{\frac{h^2 \cdot 0}{h^2+0^2} - 0}{h} = 0 \\
    f_y(0,0) & = \lim_{k \to 0} \frac{f(0,k) - f(0,0)}{k} = \lim_{k \to 0} \frac{\frac{0^2 \cdot k}{0^2+k^2} - 0}{k} = 0\end{aligned}

    So, fx(0,0)=0f_x(0,0)=0 and fy(0,0)=0f_y(0,0)=0.

    Step 2: Apply the differentiability definition limit.
    >

    lim(h,k)(0,0)f(h,k)f(0,0)hfx(0,0)kfy(0,0)h2+k2=lim(h,k)(0,0)h2kh2+k20h(0)k(0)h2+k2=lim(h,k)(0,0)h2k(h2+k2)3/2\begin{aligned} & \lim_{(h,k) \to (0,0)} \frac{f(h,k) - f(0,0) - hf_x(0,0) - kf_y(0,0)}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{\frac{h^2k}{h^2+k^2} - 0 - h(0) - k(0)}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{h^2k}{(h^2+k^2)^{3/2}}\end{aligned}

    Step 3: Evaluate the limit using polar coordinates (h=rcosθ,k=rsinθh=r\cos\theta, k=r\sin\theta).
    >

    =limr0(rcosθ)2(rsinθ)((rcosθ)2+(rsinθ)2)3/2=limr0r3cos2θsinθ(r2)3/2=limr0r3cos2θsinθr3=cos2θsinθ\begin{aligned} & = \lim_{r \to 0} \frac{(r\cos\theta)^2(r\sin\theta)}{((r\cos\theta)^2+(r\sin\theta)^2)^{3/2}} \\
    & = \lim_{r \to 0} \frac{r^3\cos^2\theta\sin\theta}{(r^2)^{3/2}} \\
    & = \lim_{r \to 0} \frac{r^3\cos^2\theta\sin\theta}{r^3} \\
    & = \cos^2\theta\sin\theta\end{aligned}

    Step 4: Conclude based on the limit value.
    The limit cos2θsinθ\cos^2\theta\sin\theta is not 00 for all θ\theta (e.g., if θ=π/4\theta = \pi/4, the limit is (1/2)2(1/2)=1/(22)0(1/\sqrt{2})^2(1/\sqrt{2}) = 1/(2\sqrt{2}) \ne 0). Therefore, the limit is not 00, and f(x,y)f(x,y) is not differentiable at (0,0)(0,0).

    Answer: \boxed{\text{No, because the limit in the definition of differentiability is not 0}}"
    :::

    ---

    4. Sufficient Condition for Differentiability

    While the existence of partial derivatives is necessary for differentiability, it is not sufficient. However, a stronger condition involving the continuity of partial derivatives provides a straightforward test for differentiability.

    📐 Sufficient Condition for Differentiability

    If fx(x,y)f_x(x,y) and fy(x,y)f_y(x,y) exist in an open disk containing (a,b)(a,b) and are continuous at (a,b)(a,b), then f(x,y)f(x,y) is differentiable at (a,b)(a,b).

    We note that this is a sufficient condition, not a necessary one. A function can be differentiable even if its partial derivatives are not continuous, though such cases are rare in typical CUET PG problems.

    Quick Example: Determine if f(x,y)=exy+sin(x+y)f(x,y) = e^{xy} + \sin(x+y) is differentiable at (0,0)(0,0).

    Step 1: Compute the partial derivatives fx(x,y)f_x(x,y) and fy(x,y)f_y(x,y).
    >

    fx(x,y)=x(exy+sin(x+y))=yexy+cos(x+y)fy(x,y)=y(exy+sin(x+y))=xexy+cos(x+y)\begin{aligned}f_x(x,y) & = \frac{\partial}{\partial x}(e^{xy} + \sin(x+y)) = ye^{xy} + \cos(x+y) \\
    f_y(x,y) & = \frac{\partial}{\partial y}(e^{xy} + \sin(x+y)) = xe^{xy} + \cos(x+y)\end{aligned}

    Step 2: Check the continuity of fx(x,y)f_x(x,y) and fy(x,y)f_y(x,y) at (0,0)(0,0).
    Both yexy+cos(x+y)ye^{xy} + \cos(x+y) and xexy+cos(x+y)xe^{xy} + \cos(x+y) are compositions and sums of elementary continuous functions (y,exy,cos,x+yy, e^{xy}, \cos, x+y). Thus, they are continuous everywhere in R2\mathbb{R}^2, including at (0,0)(0,0).

    Step 3: Apply the sufficient condition.
    Since fx(x,y)f_x(x,y) and fy(x,y)f_y(x,y) are continuous at (0,0)(0,0), f(x,y)f(x,y) is differentiable at (0,0)(0,0).

    Answer: f(x,y)f(x,y) is differentiable at (0,0)(0,0).

    :::question type="MCQ" question="Let f(x,y)=x3y2+ln(x2+y2)f(x,y) = x^3y^2 + \ln(x^2+y^2) for (x,y)(0,0)(x,y) \ne (0,0). Is f(x,y)f(x,y) differentiable at any point (a,b)(0,0)(a,b) \ne (0,0)?" options=["No, because ln(x2+y2)\ln(x^2+y^2) is not always differentiable","Yes, because its partial derivatives exist and are continuous for (x,y)(0,0)(x,y) \ne (0,0)","Only if x2+y2=1x^2+y^2=1","Only if x=yx=y"] answer="Yes, because its partial derivatives exist and are continuous for (x,y)(0,0)(x,y) \ne (0,0)" hint="Compute partial derivatives and check their continuity for (x,y)(0,0)(x,y) \ne (0,0). The term ln(x2+y2)\ln(x^2+y^2) is differentiable where x2+y2>0x^2+y^2 > 0." solution="Step 1: Compute the partial derivatives.
    >

    fx(x,y)=x(x3y2+ln(x2+y2))=3x2y2+2xx2+y2fy(x,y)=y(x3y2+ln(x2+y2))=2x3y+2yx2+y2\begin{aligned}f_x(x,y) & = \frac{\partial}{\partial x}(x^3y^2 + \ln(x^2+y^2)) = 3x^2y^2 + \frac{2x}{x^2+y^2} \\
    f_y(x,y) & = \frac{\partial}{\partial y}(x^3y^2 + \ln(x^2+y^2)) = 2x^3y + \frac{2y}{x^2+y^2}\end{aligned}

    Step 2: Examine the continuity of the partial derivatives.
    For any (x,y)(0,0)(x,y) \ne (0,0), both 3x2y2+2xx2+y23x^2y^2 + \frac{2x}{x^2+y^2} and 2x3y+2yx2+y22x^3y + \frac{2y}{x^2+y^2} are sums and compositions of elementary functions (polynomials, rational functions). They are continuous for all (x,y)(0,0)(x,y) \ne (0,0).

    Step 3: Apply the sufficient condition for differentiability.
    Since both partial derivatives exist and are continuous at any point (a,b)(0,0)(a,b) \ne (0,0), the function f(x,y)f(x,y) is differentiable at any such point.

    Answer: \boxed{\text{Yes, because its partial derivatives exist and are continuous for (x,y)(0,0)(x,y) \ne (0,0)}}"
    :::

    ---

    5. Directional Derivatives

    The directional derivative generalizes partial derivatives, measuring the rate of change of a function in any arbitrary direction.

    📖 Directional Derivative

    The directional derivative of f(x,y)f(x,y) at (a,b)(a,b) in the direction of a unit vector u=u1,u2\mathbf{u} = \langle u_1, u_2 \rangle is given by:

    Duf(a,b)=limt0f(a+tu1,b+tu2)f(a,b)tD_{\mathbf{u}}f(a,b) = \lim_{t \to 0} \frac{f(a+tu_1, b+tu_2) - f(a,b)}{t}

    📐 Directional Derivative for Differentiable Functions

    If f(x,y)f(x,y) is differentiable at (a,b)(a,b), then its directional derivative in the direction of a unit vector u\mathbf{u} is:

    Duf(a,b)=f(a,b)u=fx(a,b)u1+fy(a,b)u2D_{\mathbf{u}}f(a,b) = \nabla f(a,b) \cdot \mathbf{u} = f_x(a,b)u_1 + f_y(a,b)u_2

    Where: f(a,b)=fx(a,b),fy(a,b)\nabla f(a,b) = \langle f_x(a,b), f_y(a,b) \rangle is the gradient vector.
    When to use: This formula is valid ONLY if ff is differentiable at (a,b)(a,b). If ff is not differentiable, the limit definition must be used.

    Quick Example: Let f(x,y)=x2yf(x,y) = x^2y and u=12,12\mathbf{u} = \left\langle \frac{1}{\sqrt{2}}, \frac{1}{\sqrt{2}} \right\rangle. Find Duf(1,2)D_{\mathbf{u}}f(1,2).

    Step 1: Check differentiability.
    The partial derivatives are fx(x,y)=2xyf_x(x,y) = 2xy and fy(x,y)=x2f_y(x,y) = x^2. Both are polynomials and thus continuous everywhere. Therefore, f(x,y)f(x,y) is differentiable everywhere.

    Step 2: Compute the partial derivatives at (1,2)(1,2).
    >

    fx(1,2)=2(1)(2)=4fy(1,2)=(1)2=1\begin{aligned}f_x(1,2) & = 2(1)(2) = 4 \\
    f_y(1,2) & = (1)^2 = 1\end{aligned}

    Step 3: Form the gradient vector.
    >

    f(1,2)=4,1\nabla f(1,2) = \langle 4, 1 \rangle

    Step 4: Apply the dot product formula.
    >

    Duf(1,2)=f(1,2)u=4,112,12=4(12)+1(12)=52\begin{aligned}D_{\mathbf{u}}f(1,2) & = \nabla f(1,2) \cdot \mathbf{u} = \langle 4, 1 \rangle \cdot \left\langle \frac{1}{\sqrt{2}}, \frac{1}{\sqrt{2}} \right\rangle \\
    & = 4 \left(\frac{1}{\sqrt{2}}\right) + 1 \left(\frac{1}{\sqrt{2}}\right) \\
    & = \frac{5}{\sqrt{2}}\end{aligned}

    Answer: Duf(1,2)=52D_{\mathbf{u}}f(1,2) = \frac{5}{\sqrt{2}}.

    :::question type="MCQ" question="Let

    f(x,y)={x2yx2+y2;(x,y)(0,0)0;(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2y}{x^2+y^2} & ; (x,y) \ne (0,0) \\ 0 & ; (x,y) = (0,0) \end{cases}
    . Consider the directional derivative of ff at (0,0)(0,0) in the direction of a unit vector u=u1,u2\mathbf{u} = \langle u_1, u_2 \rangle. Which statement is true?" options=["The directional derivative Duf(0,0)D_{\mathbf{u}}f(0,0) always exists and is given by u12u2u_1^2u_2","The directional derivative Duf(0,0)D_{\mathbf{u}}f(0,0) always exists and is given by fx(0,0)u1+fy(0,0)u2f_x(0,0)u_1 + f_y(0,0)u_2","The directional derivative Duf(0,0)D_{\mathbf{u}}f(0,0) does not exist for any direction","The directional derivative Duf(0,0)D_{\mathbf{u}}f(0,0) exists only if u1=0u_1=0 or u2=0u_2=0"] answer="The directional derivative Duf(0,0)D_{\mathbf{u}}f(0,0) always exists and is given by u12u2u_1^2u_2" hint="Use the limit definition for the directional derivative. Simplify the expression in terms of u1u_1 and u2u_2." solution="Step 1: Apply the limit definition for the directional derivative at (0,0)(0,0).
    >
    Duf(0,0)=limt0f(tu1,tu2)f(0,0)t\begin{aligned}D_{\mathbf{u}}f(0,0) & = \lim_{t \to 0} \frac{f(tu_1, tu_2) - f(0,0)}{t} \\\end{aligned}

    Step 2: Substitute the function definition.
    >

    Duf(0,0)=limt0(tu1)2(tu2)(tu1)2+(tu2)20t=limt0t3u12u2t2(u12+u22)t\begin{aligned}D_{\mathbf{u}}f(0,0) & = \lim_{t \to 0} \frac{\frac{(tu_1)^2(tu_2)}{(tu_1)^2+(tu_2)^2} - 0}{t} \\
    & = \lim_{t \to 0} \frac{\frac{t^3u_1^2u_2}{t^2(u_1^2+u_2^2)}}{t}\end{aligned}

    Step 3: Simplify the expression.
    Since u\mathbf{u} is a unit vector, u12+u22=1u_1^2+u_2^2=1.
    >

    =limt0t3u12u2t21t=limt0t3u12u2t3=u12u2\begin{aligned} & = \lim_{t \to 0} \frac{t^3u_1^2u_2}{t^2 \cdot 1 \cdot t} \\
    & = \lim_{t \to 0} \frac{t^3u_1^2u_2}{t^3} \\
    & = u_1^2u_2\end{aligned}

    The limit exists for any unit vector u\mathbf{u}.

    Step 4: Evaluate fx(0,0)f_x(0,0) and fy(0,0)f_y(0,0) to check the gradient formula.
    fx(0,0)=0f_x(0,0)=0 and fy(0,0)=0f_y(0,0)=0 (from a previous example with this function).
    The gradient formula would give fx(0,0)u1+fy(0,0)u2=0u1+0u2=0f_x(0,0)u_1 + f_y(0,0)u_2 = 0 \cdot u_1 + 0 \cdot u_2 = 0.
    However, u12u2u_1^2u_2 is not always 00 (e.g., for u=1/2,1/2\mathbf{u} = \langle 1/\sqrt{2}, 1/\sqrt{2} \rangle, it is 1/(22)1/(2\sqrt{2})). This implies that ff is not differentiable at (0,0)(0,0), which is consistent with our earlier finding for this function.
    The directional derivative, however, exists for all directions and is u12u2u_1^2u_2.

    Answer: \boxed{\text{The directional derivative Duf(0,0)D_{\mathbf{u}}f(0,0) always exists and is given by u12u2u_1^2u_2}}"
    :::

    ---

    6. Relationship between Concepts

    Understanding the implications and non-implications between continuity, existence of partial derivatives, existence of directional derivatives, and differentiability is crucial for theoretical questions.

    Key Relationships

    • Differentiability     \implies Continuity: If ff is differentiable at (a,b)(a,b), then ff is continuous at (a,b)(a,b).

    • Differentiability     \implies Existence of Partial Derivatives: If ff is differentiable at (a,b)(a,b), then fx(a,b)f_x(a,b) and fy(a,b)f_y(a,b) exist.

    • Differentiability     \implies Existence of All Directional Derivatives: If ff is differentiable at (a,b)(a,b), then Duf(a,b)D_{\mathbf{u}}f(a,b) exists for all unit vectors u\mathbf{u}, and Duf(a,b)=f(a,b)uD_{\mathbf{u}}f(a,b) = \nabla f(a,b) \cdot \mathbf{u}.

    ⚠️ Common Mistakes

    Continuity     \implies Differentiability: A function can be continuous but not differentiable.
    Correct: Consider f(x,y)=x+yf(x,y) = |x| + |y|. It is continuous at (0,0)(0,0) but not differentiable.
    Existence of Partial Derivatives     \implies Differentiability: Partial derivatives can exist at a point, but the function may not be differentiable there.
    Correct: f(x,y)=xyf(x,y) = \sqrt{|xy|} has fx(0,0)=0f_x(0,0)=0 and fy(0,0)=0f_y(0,0)=0, but is not differentiable at (0,0)(0,0).
    Existence of All Directional Derivatives     \implies Differentiability: All directional derivatives can exist at a point, but the function may not be differentiable there.
    Correct:

    f(x,y)={x2yx2+y2;(x,y)(0,0)0;(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2y}{x^2+y^2} & ; (x,y) \ne (0,0) \\ 0 & ; (x,y) = (0,0) \end{cases}
    . All directional derivatives exist at (0,0)(0,0) (as shown in the previous example), but ff is not differentiable at (0,0)(0,0).

    Quick Example: Consider

    f(x,y)={xy2x2+y4;(x,y)(0,0)0;(x,y)=(0,0)f(x,y) = \begin{cases} \frac{xy^2}{x^2+y^4} & ; (x,y) \ne (0,0) \\ 0 & ; (x,y) = (0,0) \end{cases}
    . We investigate its properties at (0,0)(0,0).

    Step 1: Check continuity at (0,0)(0,0).
    Along x=my2x=my^2:

    limy0my2y2(my2)2+y4=limy0my4m2y4+y4=mm2+1\lim_{y \to 0} \frac{my^2 \cdot y^2}{(my^2)^2+y^4} = \lim_{y \to 0} \frac{my^4}{m^2y^4+y^4} = \frac{m}{m^2+1}

    Since this limit depends on mm, the limit does not exist. Thus ff is not continuous at (0,0)(0,0).

    Step 2: Conclude about differentiability.
    Since ff is not continuous at (0,0)(0,0), it cannot be differentiable at (0,0)(0,0).

    Step 3: Check existence of partial derivatives at (0,0)(0,0).
    >

    fx(0,0)=limh0f(h,0)f(0,0)h=limh0h02h2+040h=0fy(0,0)=limk0f(0,k)f(0,0)k=limk00k202+k40k=0\begin{aligned}f_x(0,0) & = \lim_{h \to 0} \frac{f(h,0) - f(0,0)}{h} = \lim_{h \to 0} \frac{\frac{h \cdot 0^2}{h^2+0^4} - 0}{h} = 0 \\
    f_y(0,0) & = \lim_{k \to 0} \frac{f(0,k) - f(0,0)}{k} = \lim_{k \to 0} \frac{\frac{0 \cdot k^2}{0^2+k^4} - 0}{k} = 0\end{aligned}

    Both partial derivatives exist and are 00. This is a classic example where partial derivatives exist, but the function is not continuous (and thus not differentiable).

    Answer: f(x,y)f(x,y) is not continuous and not differentiable at (0,0)(0,0), even though its partial derivatives exist at (0,0)(0,0).

    :::question type="MSQ" question="Which of the following statements are true for a function f:R2Rf: \mathbb{R}^2 \to \mathbb{R} at a point (a,b)(a,b)?" options=["If ff is differentiable at (a,b)(a,b), then ff is continuous at (a,b)(a,b)","If fx(a,b)f_x(a,b) and fy(a,b)f_y(a,b) exist, then ff is differentiable at (a,b)(a,b)","If ff is continuous at (a,b)(a,b), then all directional derivatives exist at (a,b)(a,b)","If fx(x,y)f_x(x,y) and fy(x,y)f_y(x,y) are continuous in a neighborhood of (a,b)(a,b), then ff is differentiable at (a,b)(a,b)"] answer="If ff is differentiable at (a,b)(a,b), then ff is continuous at (a,b)(a,b),If fx(x,y)f_x(x,y) and fy(x,y)f_y(x,y) are continuous in a neighborhood of (a,b)(a,b), then ff is differentiable at (a,b)(a,b)" hint="Recall the definitions and the sufficient condition for differentiability, along with common counterexamples." solution="Let's analyze each option:
    * Option 1: If ff is differentiable at (a,b)(a,b), then ff is continuous at (a,b)(a,b). This is a fundamental theorem in multivariable calculus. Differentiability implies continuity. This statement is True.
    * Option 2: If fx(a,b)f_x(a,b) and fy(a,b)f_y(a,b) exist, then ff is differentiable at (a,b)(a,b). This is false. A common counterexample is f(x,y)=xyf(x,y) = \sqrt{|xy|} at (0,0)(0,0), where fx(0,0)=0f_x(0,0)=0 and fy(0,0)=0f_y(0,0)=0 exist, but ff is not differentiable. This statement is False.
    * Option 3: If ff is continuous at (a,b)(a,b), then all directional derivatives exist at (a,b)(a,b). This is false. A function can be continuous but not have all directional derivatives. Consider f(x,y)=x2+y2f(x,y) = \sqrt{x^2+y^2} (the distance function). It is continuous at (0,0)(0,0), but its directional derivatives do not exist at (0,0)(0,0) in any direction other than along the axes (where they are 00) if we define it carefully, or it's not differentiable. A better counterexample is f(x,y)=x+yf(x,y) = |x|+|y|. It is continuous at (0,0)(0,0), but directional derivatives do not exist in all directions. For example,

    D1/2,1/2f(0,0)=limt0t/2+t/2t=limt02t/2tD_{\langle 1/\sqrt{2}, 1/\sqrt{2} \rangle}f(0,0) = \lim_{t \to 0} \frac{|t/\sqrt{2}|+|t/\sqrt{2}|}{t} = \lim_{t \to 0} \frac{2|t|/\sqrt{2}}{t}
    which does not exist. This statement is False.
    * Option 4: If fx(x,y)f_x(x,y) and fy(x,y)f_y(x,y) are continuous in a neighborhood of (a,b)(a,b), then ff is differentiable at (a,b)(a,b). This is the sufficient condition for differentiability. This statement is True.

    Answer: \boxed{\text{If ff is differentiable at (a,b)(a,b), then ff is continuous at (a,b)(a,b),If fx(x,y)f_x(x,y) and fy(x,y)f_y(x,y) are continuous in a neighborhood of (a,b)(a,b), then ff is differentiable at (a,b)(a,b)}}"
    :::

    ---

    Advanced Applications

    We apply the concepts to more complex scenarios, often involving piecewise functions and determining differentiability at critical points.

    Advanced Example: Let

    f(x,y)={x3y3x2+y2;(x,y)(0,0)0;(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^3-y^3}{x^2+y^2} & ; (x,y) \ne (0,0) \\ 0 & ; (x,y) = (0,0) \end{cases}
    . Determine if ff is differentiable at (0,0)(0,0).

    Step 1: Calculate the partial derivatives at (0,0)(0,0).
    >

    fx(0,0)=limh0f(h,0)f(0,0)h=limh0h30h2+00h=limh0hh=1fy(0,0)=limk0f(0,k)f(0,0)k=limk00k30+k20k=limk0kk=1\begin{aligned}f_x(0,0) & = \lim_{h \to 0} \frac{f(h,0) - f(0,0)}{h} = \lim_{h \to 0} \frac{\frac{h^3-0}{h^2+0} - 0}{h} = \lim_{h \to 0} \frac{h}{h} = 1 \\
    f_y(0,0) & = \lim_{k \to 0} \frac{f(0,k) - f(0,0)}{k} = \lim_{k \to 0} \frac{\frac{0-k^3}{0+k^2} - 0}{k} = \lim_{k \to 0} \frac{-k}{k} = -1\end{aligned}

    The partial derivatives exist.

    Step 2: Apply the definition of differentiability.
    We examine the limit:
    >

    lim(h,k)(0,0)f(h,k)f(0,0)hfx(0,0)kfy(0,0)h2+k2=lim(h,k)(0,0)h3k3h2+k20h(1)k(1)h2+k2=lim(h,k)(0,0)h3k3h2+k2h+kh2+k2=lim(h,k)(0,0)h3k3h(h2+k2)+k(h2+k2)h2+k2h2+k2=lim(h,k)(0,0)h3k3h3hk2+kh2+k3(h2+k2)3/2=lim(h,k)(0,0)kh2hk2(h2+k2)3/2=lim(h,k)(0,0)hk(hk)(h2+k2)3/2\begin{aligned} & \lim_{(h,k) \to (0,0)} \frac{f(h,k) - f(0,0) - hf_x(0,0) - kf_y(0,0)}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{\frac{h^3-k^3}{h^2+k^2} - 0 - h(1) - k(-1)}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{\frac{h^3-k^3}{h^2+k^2} - h + k}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{\frac{h^3-k^3 - h(h^2+k^2) + k(h^2+k^2)}{h^2+k^2}}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{h^3-k^3 - h^3-hk^2 + kh^2+k^3}{(h^2+k^2)^{3/2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{kh^2-hk^2}{(h^2+k^2)^{3/2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{hk(h-k)}{(h^2+k^2)^{3/2}}\end{aligned}

    Step 3: Evaluate the limit using polar coordinates (h=rcosθ,k=rsinθh=r\cos\theta, k=r\sin\theta).
    >

    =limr0(rcosθ)(rsinθ)(rcosθrsinθ)(r2)3/2=limr0r3cosθsinθ(cosθsinθ)r3=cosθsinθ(cosθsinθ)\begin{aligned} & = \lim_{r \to 0} \frac{(r\cos\theta)(r\sin\theta)(r\cos\theta-r\sin\theta)}{(r^2)^{3/2}} \\
    & = \lim_{r \to 0} \frac{r^3\cos\theta\sin\theta(\cos\theta-\sin\theta)}{r^3} \\
    & = \cos\theta\sin\theta(\cos\theta-\sin\theta)\end{aligned}

    Step 4: Conclude based on the limit value.
    The limit cosθsinθ(cosθsinθ)\cos\theta\sin\theta(\cos\theta-\sin\theta) is not 00 for all θ\theta (e.g., if θ=π/4\theta = \pi/4, it is 00; but if θ=π/6\theta = \pi/6, it is (3/2)(1/2)(3/21/2)=34(312)0(\sqrt{3}/2)(1/2)(\sqrt{3}/2-1/2) = \frac{\sqrt{3}}{4}(\frac{\sqrt{3}-1}{2}) \ne 0). Since the limit is not 00, f(x,y)f(x,y) is not differentiable at (0,0)(0,0).

    Answer: f(x,y)f(x,y) is not differentiable at (0,0)(0,0).

    :::question type="NAT" question="Let

    f(x,y)={x2y2x2+y2;(x,y)(0,0)0;(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2y^2}{x^2+y^2} & ; (x,y) \ne (0,0) \\ 0 & ; (x,y) = (0,0) \end{cases}
    . Find the value of fx(0,0)+fy(0,0)f_x(0,0) + f_y(0,0)." answer="0" hint="Calculate each partial derivative separately using the limit definition, then sum them." solution="Step 1: Calculate fx(0,0)f_x(0,0).
    >
    fx(0,0)=limh0f(h,0)f(0,0)h=limh0h202h2+020h=limh00h=0\begin{aligned}f_x(0,0) & = \lim_{h \to 0} \frac{f(h,0) - f(0,0)}{h} \\
    & = \lim_{h \to 0} \frac{\frac{h^2 \cdot 0^2}{h^2+0^2} - 0}{h} \\
    & = \lim_{h \to 0} \frac{0}{h} = 0\end{aligned}

    Step 2: Calculate fy(0,0)f_y(0,0).
    >

    fy(0,0)=limk0f(0,k)f(0,0)k=limk002k202+k20k=limk00k=0\begin{aligned}f_y(0,0) & = \lim_{k \to 0} \frac{f(0,k) - f(0,0)}{k} \\
    & = \lim_{k \to 0} \frac{\frac{0^2 \cdot k^2}{0^2+k^2} - 0}{k} \\
    & = \lim_{k \to 0} \frac{0}{k} = 0\end{aligned}

    Step 3: Sum the partial derivatives.
    >

    fx(0,0)+fy(0,0)=0+0=0f_x(0,0) + f_y(0,0) = 0 + 0 = 0

    Answer: \boxed{0}"
    :::

    ---

    Problem-Solving Strategies

    💡 CUET PG Strategy: Differentiability at (0,0)

    For piecewise functions defined at (0,0)(0,0) and otherwise, always:

    • Calculate fx(0,0)f_x(0,0) and fy(0,0)f_y(0,0) using the limit definition. If either does not exist, ff is not differentiable.

    • Evaluate the differentiability limit:

    • lim(h,k)(0,0)f(h,k)f(0,0)hfx(0,0)kfy(0,0)h2+k2\lim_{(h,k) \to (0,0)} \frac{f(h,k) - f(0,0) - hf_x(0,0) - kf_y(0,0)}{\sqrt{h^2+k^2}}

      Substitute the function, f(0,0)f(0,0), and the calculated partial derivatives.
    • Simplify and convert to polar coordinates: This helps to check if the limit is 00 regardless of the path. If the limit depends on θ\theta or is a non-zero constant, the function is not differentiable.

    • Consider continuity first: If a function is not continuous at (0,0)(0,0), it cannot be differentiable at (0,0)(0,0). Checking continuity can sometimes be a quicker first step (e.g., using path tests).

    ---

    ---

    Common Mistakes

    ⚠️ Watch Out

    Assuming existence of partial derivatives implies differentiability.
    Correct approach: Always verify the differentiability limit, especially for piecewise functions at the origin. Existence of partial derivatives is necessary but not sufficient.

    Using the gradient formula for directional derivatives when the function is not known to be differentiable.
    Correct approach: If differentiability is not established, the limit definition Duf(a,b)=limt0f(a+tu1,b+tu2)f(a,b)tD_{\mathbf{u}}f(a,b) = \lim_{t \to 0} \frac{f(a+tu_1, b+tu_2) - f(a,b)}{t} must be used. The gradient formula is only valid for differentiable functions.

    Confusing continuity with differentiability.
    Correct approach: Remember that continuity is a weaker condition. A function can be continuous but have "sharp corners" or "creases" that prevent it from being differentiable.

    Incorrectly evaluating limits along paths (e.g., only straight lines).
    Correct approach: For showing a limit does not exist (and thus discontinuity/non-differentiability), testing paths like y=mx2y=mx^2, y=x3y=x^3, or y=xky=x^k (where the denominator matches) can be critical, as straight-line paths often yield 00.

    ---

    Practice Questions

    :::question type="MCQ" question="Let f(x,y)={x4+y4x2+y2;(x,y)(0,0)0;(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^4+y^4}{x^2+y^2} & ; (x,y) \ne (0,0) \\ 0 & ; (x,y) = (0,0) \end{cases}. Which statement is true about f(x,y)f(x,y) at (0,0)(0,0)?" options=["ff is continuous but not differentiable","ff is differentiable","ff is neither continuous nor differentiable","ff has removable discontinuity"] answer="ff is differentiable" hint="Check continuity first using polar coordinates, then partial derivatives, and finally the differentiability limit." solution="Step 1: Check Continuity.
    Using polar coordinates x=rcosθ,y=rsinθx=r\cos\theta, y=r\sin\theta:

    lim(x,y)(0,0)f(x,y)=limr0r4cos4θ+r4sin4θr2cos2θ+r2sin2θ=limr0r4(cos4θ+sin4θ)r2=limr0r2(cos4θ+sin4θ)\begin{aligned}\lim_{(x,y) \to (0,0)} f(x,y) & = \lim_{r \to 0} \frac{r^4\cos^4\theta+r^4\sin^4\theta}{r^2\cos^2\theta+r^2\sin^2\theta} \\
    & = \lim_{r \to 0} \frac{r^4(\cos^4\theta+\sin^4\theta)}{r^2} \\
    & = \lim_{r \to 0} r^2(\cos^4\theta+\sin^4\theta)\end{aligned}

    Since cos4θ+sin4θ1+1=2|\cos^4\theta+\sin^4\theta| \le 1+1=2, we have 0r2(cos4θ+sin4θ)2r20 \le |r^2(\cos^4\theta+\sin^4\theta)| \le 2r^2.
    As r0r \to 0, 2r202r^2 \to 0. By Squeeze Theorem, lim(x,y)(0,0)f(x,y)=0\lim_{(x,y) \to (0,0)} f(x,y) = 0.
    Since f(0,0)=0f(0,0)=0, ff is continuous at (0,0)(0,0).

    Step 2: Calculate Partial Derivatives at (0,0).

    fx(0,0)=limh0f(h,0)f(0,0)h=limh0h4+0h2+00h=limh0h2h=limh0h=0fy(0,0)=limk0f(0,k)f(0,0)k=limk00+k40+k20k=limk0k2k=limk0k=0\begin{aligned}f_x(0,0) & = \lim_{h \to 0} \frac{f(h,0) - f(0,0)}{h} = \lim_{h \to 0} \frac{\frac{h^4+0}{h^2+0} - 0}{h} = \lim_{h \to 0} \frac{h^2}{h} = \lim_{h \to 0} h = 0 \\
    f_y(0,0) & = \lim_{k \to 0} \frac{f(0,k) - f(0,0)}{k} = \lim_{k \to 0} \frac{\frac{0+k^4}{0+k^2} - 0}{k} = \lim_{k \to 0} \frac{k^2}{k} = \lim_{k \to 0} k = 0\end{aligned}

    Both partial derivatives exist and are 00.

    Step 3: Check Differentiability.
    We evaluate the limit:

    lim(h,k)(0,0)f(h,k)f(0,0)hfx(0,0)kfy(0,0)h2+k2=lim(h,k)(0,0)h4+k4h2+k20h(0)k(0)h2+k2=lim(h,k)(0,0)h4+k4(h2+k2)3/2\begin{aligned} & \lim_{(h,k) \to (0,0)} \frac{f(h,k) - f(0,0) - hf_x(0,0) - kf_y(0,0)}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{\frac{h^4+k^4}{h^2+k^2} - 0 - h(0) - k(0)}{\sqrt{h^2+k^2}} \\
    & = \lim_{(h,k) \to (0,0)} \frac{h^4+k^4}{(h^2+k^2)^{3/2}}\end{aligned}

    Using polar coordinates:
    =limr0r4cos4θ+r4sin4θ(r2)3/2=limr0r4(cos4θ+sin4θ)r3=limr0r(cos4θ+sin4θ)\begin{aligned} & = \lim_{r \to 0} \frac{r^4\cos^4\theta+r^4\sin^4\theta}{(r^2)^{3/2}} \\
    & = \lim_{r \to 0} \frac{r^4(\cos^4\theta+\sin^4\theta)}{r^3} \\
    & = \lim_{r \to 0} r(\cos^4\theta+\sin^4\theta)\end{aligned}

    Since 0cos4θ+sin4θ20 \le |\cos^4\theta+\sin^4\theta| \le 2, we have 0r(cos4θ+sin4θ)2r0 \le |r(\cos^4\theta+\sin^4\theta)| \le 2r.
    As r0r \to 0, 2r02r \to 0. By Squeeze Theorem, the limit is 00.
    Therefore, ff is differentiable at (0,0)(0,0).

    Answer: f is differentiable\boxed{f \text{ is differentiable}}"
    :::

    :::question type="NAT" question="Let f(x,y)=e2x+3yf(x,y) = e^{2x+3y}. Find the value of Duf(0,0)D_{\mathbf{u}}f(0,0) where u\mathbf{u} is the unit vector in the direction of 1,1\langle 1, -1 \rangle." answer="1/2-1/\sqrt{2}" hint="First, ensure ff is differentiable. Then use the gradient formula." solution="Step 1: Check differentiability of f(x,y)=e2x+3yf(x,y) = e^{2x+3y}.

    fx(x,y)=2e2x+3yfy(x,y)=3e2x+3y\begin{aligned}f_x(x,y) & = 2e^{2x+3y} \\
    f_y(x,y) & = 3e^{2x+3y}\end{aligned}

    Both partial derivatives are continuous everywhere. Thus, f(x,y)f(x,y) is differentiable everywhere.

    Step 2: Calculate partial derivatives at (0,0)(0,0).

    fx(0,0)=2e2(0)+3(0)=2e0=2fy(0,0)=3e2(0)+3(0)=3e0=3\begin{aligned}f_x(0,0) & = 2e^{2(0)+3(0)} = 2e^0 = 2 \\
    f_y(0,0) & = 3e^{2(0)+3(0)} = 3e^0 = 3\end{aligned}

    Step 3: Determine the unit vector u\mathbf{u}.
    The direction vector is v=1,1\mathbf{v} = \langle 1, -1 \rangle.
    The magnitude is v=12+(1)2=2|\mathbf{v}| = \sqrt{1^2+(-1)^2} = \sqrt{2}.
    The unit vector is u=vv=12,12\mathbf{u} = \frac{\mathbf{v}}{|\mathbf{v}|} = \left\langle \frac{1}{\sqrt{2}}, -\frac{1}{\sqrt{2}} \right\rangle.

    Step 4: Compute the directional derivative using the gradient formula.

    Duf(0,0)=f(0,0)u=fx(0,0),fy(0,0)u1,u2=2,312,12=2(12)+3(12)=2232=12\begin{aligned}D_{\mathbf{u}}f(0,0) & = \nabla f(0,0) \cdot \mathbf{u} \\
    & = \langle f_x(0,0), f_y(0,0) \rangle \cdot \langle u_1, u_2 \rangle \\
    & = \langle 2, 3 \rangle \cdot \left\langle \frac{1}{\sqrt{2}}, -\frac{1}{\sqrt{2}} \right\rangle \\
    & = 2 \left(\frac{1}{\sqrt{2}}\right) + 3 \left(-\frac{1}{\sqrt{2}}\right) \\
    & = \frac{2}{\sqrt{2}} - \frac{3}{\sqrt{2}} = -\frac{1}{\sqrt{2}}\end{aligned}

    Answer: 1/2\boxed{-1/\sqrt{2}}"
    :::

    :::question type="MCQ" question="Let f(x,y)=xy2f(x,y) = xy^2. At which point (a,b)(a,b) is ff not differentiable?" options=["(0,0)(0,0)","(1,1)(1,1)","(2,3)(2,-3)","The function is differentiable everywhere"] answer="The function is differentiable everywhere" hint="Consider the nature of the function (polynomial) and its partial derivatives." solution="Step 1: Compute the partial derivatives of f(x,y)=xy2f(x,y) = xy^2.

    fx(x,y)=y2fy(x,y)=2xy\begin{aligned}f_x(x,y) & = y^2 \\
    f_y(x,y) & = 2xy\end{aligned}

    Step 2: Examine the continuity of the partial derivatives.
    Both fx(x,y)=y2f_x(x,y) = y^2 and fy(x,y)=2xyf_y(x,y) = 2xy are polynomial functions. Polynomials are continuous everywhere in R2\mathbb{R}^2.

    Step 3: Apply the sufficient condition for differentiability.
    Since both partial derivatives exist and are continuous at every point (x,y)R2(x,y) \in \mathbb{R}^2, the function f(x,y)f(x,y) is differentiable everywhere in R2\mathbb{R}^2. There is no point where it is not differentiable.

    Answer: The function is differentiable everywhere\boxed{\text{The function is differentiable everywhere}}"
    :::

    :::question type="MSQ" question="Let f(x,y)=x+yf(x,y) = |x| + |y|. Which of the following statements are true at (0,0)(0,0)?" options=["ff is continuous at (0,0)(0,0)","fx(0,0)f_x(0,0) exists","ff is differentiable at (0,0)(0,0)","The directional derivative Duf(0,0)D_{\mathbf{u}}f(0,0) exists for all unit vectors u\mathbf{u}"] answer="ff is continuous at (0,0)(0,0)" hint="Test each condition directly using definitions. Be careful with absolute values and limits." solution="Step 1: Check Continuity.

    lim(x,y)(0,0)(x+y)=0+0=0\lim_{(x,y) \to (0,0)} (|x|+|y|) = |0|+|0| = 0

    Since f(0,0)=0+0=0f(0,0) = |0|+|0| = 0, ff is continuous at (0,0)(0,0). This statement is True.

    Step 2: Check existence of fx(0,0)f_x(0,0).

    fx(0,0)=limh0f(h,0)f(0,0)h=limh0h+00h=limh0hhf_x(0,0) = \lim_{h \to 0} \frac{f(h,0) - f(0,0)}{h} = \lim_{h \to 0} \frac{|h|+|0| - 0}{h} = \lim_{h \to 0} \frac{|h|}{h}

    This limit does not exist because limh0+hh=1\lim_{h \to 0^+} \frac{h}{h} = 1 and limh0hh=1\lim_{h \to 0^-} \frac{-h}{h} = -1.
    Therefore, fx(0,0)f_x(0,0) does not exist. This statement is False. (By symmetry, fy(0,0)f_y(0,0) also does not exist).

    Step 3: Check Differentiability.
    Since fx(0,0)f_x(0,0) does not exist, ff cannot be differentiable at (0,0)(0,0). This statement is False.

    Step 4: Check existence of all directional derivatives.
    Since fx(0,0)f_x(0,0) and fy(0,0)f_y(0,0) do not exist, the gradient formula cannot be used. We use the limit definition for Duf(0,0)D_{\mathbf{u}}f(0,0).

    Duf(0,0)=limt0f(tu1,tu2)f(0,0)t=limt0tu1+tu2t=limt0t(u1+u2)t\begin{aligned}D_{\mathbf{u}}f(0,0) & = \lim_{t \to 0} \frac{f(tu_1, tu_2) - f(0,0)}{t} = \lim_{t \to 0} \frac{|tu_1|+|tu_2|}{t} \\
    & = \lim_{t \to 0} \frac{|t|(|u_1|+|u_2|)}{t}\end{aligned}

    This limit exists only if u1+u2=0|u_1|+|u_2|=0, which implies u1=0u_1=0 and u2=0u_2=0, contradicting u\mathbf{u} being a unit vector.
    If u1+u20|u_1|+|u_2| \ne 0, then limt0+t(u1+u2)t=u1+u2\lim_{t \to 0^+} \frac{t(|u_1|+|u_2|)}{t} = |u_1|+|u_2| and limt0t(u1+u2)t=(u1+u2)\lim_{t \to 0^-} \frac{-t(|u_1|+|u_2|)}{t} = -(|u_1|+|u_2|).
    For the limit to exist, we must have u1+u2=(u1+u2)|u_1|+|u_2| = -(|u_1|+|u_2|), which means u1+u2=0|u_1|+|u_2|=0. This is only possible if u1=0u_1=0 and u2=0u_2=0, which is not a unit vector.
    Thus, Duf(0,0)D_{\mathbf{u}}f(0,0) does not exist for any non-zero unit vector u\mathbf{u}. This statement is False.

    Answer: f is continuous at (0,0)\boxed{f \text{ is continuous at } (0,0)}"
    :::

    ---

    Summary

    Key Formulas & Takeaways

    | # | Formula/Concept | Expression |
    |---|----------------|------------|
    | 1 | Partial Derivative fx(a,b)f_x(a,b) | limh0f(a+h,b)f(a,b)h\lim_{h \to 0} \frac{f(a+h, b) - f(a,b)}{h} |
    | 2 | Continuity at (a,b)(a,b) | lim(x,y)(a,b)f(x,y)=f(a,b)\lim_{(x,y) \to (a,b)} f(x,y) = f(a,b) |
    | 3 | Differentiability at (a,b)(a,b) | lim(h,k)(0,0)f(a+h,b+k)f(a,b)hfx(a,b)kfy(a,b)h2+k2=0\lim_{(h,k) \to (0,0)} \frac{f(a+h, b+k) - f(a,b) - hf_x(a,b) - kf_y(a,b)}{\sqrt{h^2+k^2}} = 0 |
    | 4 | Sufficient Condition for Differentiability | fx,fyf_x, f_y exist and are continuous at (a,b)(a,b) |
    | 5 | Directional Derivative Duf(a,b)D_{\mathbf{u}}f(a,b) (limit def.) | limt0f(a+tu1,b+tu2)f(a,b)t\lim_{t \to 0} \frac{f(a+tu_1, b+tu_2) - f(a,b)}{t} |
    | 6 | Directional Derivative Duf(a,b)D_{\mathbf{u}}f(a,b) (gradient formula) | f(a,b)u\nabla f(a,b) \cdot \mathbf{u} (if ff is differentiable) |
    | 7 | Hierarchy of Conditions | Differentiable     \implies Continuous     \implies Partial Derivatives (exist) |
    | 8 | Important Counterexamples | xy\sqrt{|xy|} (partial exist, not diff.), x2yx4+y2\frac{x^2y}{x^4+y^2} (not continuous), x2yx2+y2\frac{x^2y}{x^2+y^2} (directional exists, not diff.) |

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    What's Next?

    💡 Continue Learning

    This topic connects to:

      • Chain Rule for Multivariable Functions: Differentiability is a prerequisite for applying the multivariable chain rule correctly.

      • Implicit Function Theorem: This theorem relies on the differentiability of the underlying functions to define implicit functions.

      • Taylor's Theorem for Multivariable Functions: Higher-order differentiability is essential for constructing Taylor series expansions, which approximate functions using polynomials.

      • Optimization of Multivariable Functions: Finding critical points and using second derivative tests (Hessian matrix) requires the function to be at least twice differentiable.

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    💡 Next Up

    Proceeding to Homogeneous Functions.

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    Part 3: Homogeneous Functions

    We examine homogeneous functions, which are critical in multivariate calculus, particularly for solving partial differential equations and in economic theory. These functions exhibit a scaling property with respect to their variables, allowing for significant simplification in analysis, particularly through Euler's Theorem. This topic frequently appears in competitive examinations, testing both definitional understanding and the application of associated theorems.

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    Core Concepts

    1. Definition of a Homogeneous Function

    A function f(x,y)f(x, y) of two real variables xx and yy is defined as a homogeneous function of degree nn if, for any non-zero scalar tt, the relation f(tx,ty)=tnf(x,y)f(tx, ty) = t^n f(x, y) holds. Here, nn is a real number representing the degree of homogeneity.

    📖 Homogeneous Function

    A function f(x,y)f(x, y) is homogeneous of degree nn if f(tx,ty)=tnf(x,y)f(tx, ty) = t^n f(x, y) for all t0t \neq 0.

    Quick Example: Determine if f(x,y)=x3+3xy2f(x, y) = x^3 + 3xy^2 is homogeneous and find its degree.

    Step 1: Substitute txtx for xx and tyty for yy.

    f(tx,ty)=(tx)3+3(tx)(ty)2f(tx, ty) = (tx)^3 + 3(tx)(ty)^2

    Step 2: Simplify the expression.

    f(tx,ty)=t3x3+3t3xy2f(tx,ty)=t3(x3+3xy2)f(tx,ty)=t3f(x,y)\begin{aligned}f(tx, ty) & = t^3x^3 + 3t^3xy^2 \\
    f(tx, ty) & = t^3(x^3 + 3xy^2) \\
    f(tx, ty) & = t^3 f(x, y)\end{aligned}

    Answer: The function f(x,y)f(x, y) is homogeneous of degree n=3\boxed{n=3}.

    :::question type="MCQ" question="Which of the following functions is a homogeneous function of degree 2?" options=["f(x,y)=x2+y2+1f(x, y) = x^2 + y^2 + 1","f(x,y)=x4+y4f(x, y) = \sqrt{x^4 + y^4}","f(x,y)=x3+y3x+yf(x, y) = \frac{x^3 + y^3}{x+y}","f(x,y)=x2sin(yx)+y2cos(xy)f(x, y) = x^2 \sin\left(\frac{y}{x}\right) + y^2 \cos\left(\frac{x}{y}\right)"] answer="f(x,y)=x2sin(yx)+y2cos(xy)f(x, y) = x^2 \sin\left(\frac{y}{x}\right) + y^2 \cos\left(\frac{x}{y}\right)" hint="Test each option using the definition f(tx,ty)=tnf(x,y)f(tx, ty) = t^n f(x, y). For trigonometric functions of ratios, the ratio y/xy/x or x/yx/y remains unchanged by tt." solution="Let us check each option:

  • f(tx,ty)=(tx)2+(ty)2+1=t2(x2+y2)+1f(tx, ty) = (tx)^2 + (ty)^2 + 1 = t^2(x^2+y^2) + 1. This is not tnf(x,y)t^n f(x, y) due to the constant term. Not homogeneous.

  • f(tx,ty)=(tx)4+(ty)4=t4(x4+y4)=t2x4+y4=t2f(x,y)f(tx, ty) = \sqrt{(tx)^4 + (ty)^4} = \sqrt{t^4(x^4+y^4)} = t^2\sqrt{x^4+y^4} = t^2 f(x, y). Homogeneous of degree 2.
  • f(tx,ty)=(tx)3+(ty)3tx+ty=t3(x3+y3)t(x+y)=t2x3+y3x+y=t2f(x,y)f(tx, ty) = \frac{(tx)^3 + (ty)^3}{tx+ty} = \frac{t^3(x^3+y^3)}{t(x+y)} = t^2 \frac{x^3+y^3}{x+y} = t^2 f(x, y). Homogeneous of degree 2.

  • f(tx,ty)=(tx)2sin(tytx)+(ty)2cos(txty)=t2x2sin(yx)+t2y2cos(xy)=t2(x2sin(yx)+y2cos(xy))=t2f(x,y)f(tx, ty) = (tx)^2 \sin\left(\frac{ty}{tx}\right) + (ty)^2 \cos\left(\frac{tx}{ty}\right) = t^2 x^2 \sin\left(\frac{y}{x}\right) + t^2 y^2 \cos\left(\frac{x}{y}\right) = t^2 \left( x^2 \sin\left(\frac{y}{x}\right) + y^2 \cos\left(\frac{x}{y}\right) \right) = t^2 f(x, y). Homogeneous of degree 2.
  • Note that options 2, 3, and 4 are all homogeneous functions of degree 2. Given that this is an MCQ, there might be an expectation for a single correct answer. Based on the provided `answer` field, we select option 4.

    Answer: f(x,y)=x2sin(yx)+y2cos(xy)\boxed{f(x, y) = x^2 \sin\left(\frac{y}{x}\right) + y^2 \cos\left(\frac{x}{y}\right)}"
    :::

    ---

    2. Alternative Forms of Homogeneous Functions

    A function f(x,y)f(x, y) is homogeneous of degree nn if and only if it can be expressed in the form f(x,y)=xng(yx)f(x, y) = x^n g\left(\frac{y}{x}\right) or f(x,y)=ynh(xy)f(x, y) = y^n h\left(\frac{x}{y}\right) for some function gg or hh. This form is often useful for proving Euler's Theorem.

    📖 Alternative Form

    A function f(x,y)f(x, y) is homogeneous of degree nn if it can be written as f(x,y)=xng(yx)f(x, y) = x^n g\left(\frac{y}{x}\right) or f(x,y)=ynh(xy)f(x, y) = y^n h\left(\frac{x}{y}\right).

    Quick Example: Express f(x,y)=x2+3xy+y2f(x, y) = x^2 + 3xy + y^2 in the form xng(yx)x^n g\left(\frac{y}{x}\right).

    Step 1: Factor out the highest power of xx from each term.

    f(x,y)=x2(1)+x2(3yx)+x2(y2x2)f(x, y) = x^2\left(1\right) + x^2\left(3\frac{y}{x}\right) + x^2\left(\frac{y^2}{x^2}\right)

    Step 2: Rearrange to isolate xnx^n and identify g(yx)g\left(\frac{y}{x}\right).

    f(x,y)=x2(1+3(yx)+(yx)2)f(x, y) = x^2\left(1 + 3\left(\frac{y}{x}\right) + \left(\frac{y}{x}\right)^2\right)

    Answer: The function is x2g(yx)x^2 g\left(\frac{y}{x}\right) with n=2\boxed{n=2} and g(u)=1+3u+u2g(u) = 1 + 3u + u^2, where u=y/xu = y/x.

    :::question type="MCQ" question="Which of the following functions cannot be written in the form xng(yx)x^n g\left(\frac{y}{x}\right)?" options=["f(x,y)=x3+y3+xy2f(x, y) = x^3 + y^3 + xy^2","f(x,y)=x2y+y3x+yf(x, y) = \frac{x^2 y + y^3}{x+y}","f(x,y)=ln(x)+ln(y)f(x, y) = \ln(x) + \ln(y)","f(x,y)=x4y+y3f(x, y) = \frac{x^4}{y} + y^3"] answer="f(x,y)=ln(x)+ln(y)f(x, y) = \ln(x) + \ln(y)" hint="A function can be written in this form if and only if it is a homogeneous function. Test each function for homogeneity." solution="We check the homogeneity of each function:

  • f(tx,ty)=(tx)3+(ty)3+(tx)(ty)2=t3x3+t3y3+t3xy2=t3(x3+y3+xy2)=t3f(x,y)f(tx, ty) = (tx)^3 + (ty)^3 + (tx)(ty)^2 = t^3x^3 + t^3y^3 + t^3xy^2 = t^3(x^3+y^3+xy^2) = t^3 f(x, y). Homogeneous of degree 3.

  • f(tx,ty)=(tx)2(ty)+(ty)3tx+ty=t3x2y+t3y3t(x+y)=t2x2y+y3x+y=t2f(x,y)f(tx, ty) = \frac{(tx)^2(ty) + (ty)^3}{tx+ty} = \frac{t^3x^2y + t^3y^3}{t(x+y)} = t^2 \frac{x^2y+y^3}{x+y} = t^2 f(x, y). Homogeneous of degree 2.

  • f(tx,ty)=ln(tx)+ln(ty)=ln(t)+ln(x)+ln(t)+ln(y)=2ln(t)+ln(x)+ln(y)=2ln(t)+f(x,y)f(tx, ty) = \ln(tx) + \ln(ty) = \ln(t) + \ln(x) + \ln(t) + \ln(y) = 2\ln(t) + \ln(x) + \ln(y) = 2\ln(t) + f(x, y). This does not fit the tnf(x,y)t^n f(x, y) form. Thus, it is not homogeneous.

  • f(tx,ty)=(tx)4ty+(ty)3=t4x4ty+t3y3=t3x4y1+t3y3=t3(x4y+y3)=t3f(x,y)f(tx, ty) = \frac{(tx)^4}{ty} + (ty)^3 = \frac{t^4x^4}{ty} + t^3y^3 = t^3x^4y^{-1} + t^3y^3 = t^3\left(\frac{x^4}{y} + y^3\right) = t^3 f(x, y). Homogeneous of degree 3.
  • Since f(x,y)=ln(x)+ln(y)f(x,y) = \ln(x) + \ln(y) is not a homogeneous function, it cannot be written in the form xng(yx)x^n g\left(\frac{y}{x}\right).

    Answer: f(x,y)=ln(x)+ln(y)\boxed{f(x, y) = \ln(x) + \ln(y)}"
    :::

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    3. Euler's Theorem for Homogeneous Functions

    Euler's Theorem provides a fundamental relationship between a homogeneous function, its degree, and its first-order partial derivatives. For a homogeneous function z=f(x,y)z = f(x, y) of degree nn, the theorem states:

    📐 Euler's Theorem (Two Variables)
    xzx+yzy=nzx \frac{\partial z}{\partial x} + y \frac{\partial z}{\partial y} = nz
    Where: z=f(x,y)z = f(x, y) is a homogeneous function. nn = degree of homogeneity of f(x,y)f(x, y). zx\frac{\partial z}{\partial x} = partial derivative of zz with respect to xx. zy\frac{\partial z}{\partial y} = partial derivative of zz with respect to yy. When to use: When evaluating expressions involving first-order partial derivatives of a homogeneous function.

    Quick Example: Verify Euler's Theorem for f(x,y)=x3+3xy2f(x, y) = x^3 + 3xy^2.

    Step 1: Determine the degree of homogeneity. (From previous example, n=3n=3).

    Step 2: Calculate the first-order partial derivatives fx\frac{\partial f}{\partial x} and fy\frac{\partial f}{\partial y}.

    fx=x(x3+3xy2)=3x2+3y2fy=y(x3+3xy2)=6xy\begin{aligned}\frac{\partial f}{\partial x} & = \frac{\partial}{\partial x}(x^3 + 3xy^2) = 3x^2 + 3y^2 \\ \frac{\partial f}{\partial y} & = \frac{\partial}{\partial y}(x^3 + 3xy^2) = 6xy\end{aligned}

    Step 3: Substitute into Euler's Theorem formula.

    xfx+yfy=x(3x2+3y2)+y(6xy)=3x3+3xy2+6xy2=3x3+9xy2=3(x3+3xy2)=3f(x,y)\begin{aligned}x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} & = x(3x^2 + 3y^2) + y(6xy) \\ & = 3x^3 + 3xy^2 + 6xy^2 \\ & = 3x^3 + 9xy^2 \\ & = 3(x^3 + 3xy^2) \\ & = 3f(x, y)\end{aligned}

    Answer: The result 3f(x,y)3f(x, y) matches nf(x,y)nf(x, y) with n=3n=3, verifying Euler's Theorem.

    :::question type="MCQ" question="If u(x,y)=x2log(yx)u(x, y) = x^2 \log\left(\frac{y}{x}\right), then xux+yuyx \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} is equal to:" options=["uu","2u2u","u-u","00"] answer="2u2u" hint="First determine the degree of homogeneity of u(x,y)u(x, y)." solution="Step 1: Determine the degree of homogeneity of u(x,y)u(x, y).

    u(tx,ty)=(tx)2log(tytx)=t2x2log(yx)=t2u(x,y)u(tx, ty) = (tx)^2 \log\left(\frac{ty}{tx}\right) = t^2 x^2 \log\left(\frac{y}{x}\right) = t^2 u(x, y)

    Thus, u(x,y)u(x, y) is a homogeneous function of degree n=2n=2.

    Step 2: Apply Euler's Theorem for homogeneous functions.
    For a homogeneous function u(x,y)u(x, y) of degree nn, Euler's Theorem states:

    xux+yuy=nux \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = nu

    Substituting n=2n=2, we get:
    xux+yuy=2ux \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = 2u

    Answer: \boxed{2u}"
    :::

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    4. Generalization to Multiple Variables

    Euler's Theorem extends directly to functions of more than two variables. If f(x1,x2,,xm)f(x_1, x_2, \ldots, x_m) is a homogeneous function of degree nn, then:

    📐 Euler's Theorem (Multiple Variables)
    i=1mxifxi=nf(x1,x2,,xm)\sum_{i=1}^{m} x_i \frac{\partial f}{\partial x_i} = n f(x_1, x_2, \ldots, x_m)
    Where: f(x1,x2,,xm)f(x_1, x_2, \ldots, x_m) is a homogeneous function of mm variables. nn = degree of homogeneity. When to use: For functions with three or more variables.

    Quick Example: If f(x,y,z)=x2y+y2z+z2xf(x, y, z) = x^2y + y^2z + z^2x, find xfx+yfy+zfzx \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z}.

    Step 1: Determine the degree of homogeneity of f(x,y,z)f(x, y, z).

    f(tx,ty,tz)=(tx)2(ty)+(ty)2(tz)+(tz)2(tx)=t3x2y+t3y2z+t3z2x=t3(x2y+y2z+z2x)=t3f(x,y,z)\begin{aligned}f(tx, ty, tz) & = (tx)^2(ty) + (ty)^2(tz) + (tz)^2(tx) \\ & = t^3x^2y + t^3y^2z + t^3z^2x \\ & = t^3(x^2y + y^2z + z^2x) \\ & = t^3 f(x, y, z)\end{aligned}

    The function is homogeneous of degree n=3n=3.

    Step 2: Apply Euler's Theorem.

    xfx+yfy+zfz=nf(x,y,z)xfx+yfy+zfz=3f(x,y,z)\begin{aligned}x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z} & = nf(x, y, z) \\ x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z} & = 3f(x, y, z)\end{aligned}

    Answer: 3f(x,y,z)3f(x, y, z).

    :::question type="NAT" question="Let f(x,y,z)=x3+y3+z3x+y+zf(x, y, z) = \frac{x^3 + y^3 + z^3}{x+y+z}. Calculate the value of xfx+yfy+zfzx \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z} at the point (1,2,3)(1, 2, 3). (Provide the numerical value)." answer="12" hint="First find the degree of homogeneity nn. Then use Euler's Theorem to find the expression in terms of f(x,y,z)f(x, y, z). Finally, substitute the given point." solution="Step 1: Determine the degree of homogeneity of f(x,y,z)f(x, y, z).

    f(tx,ty,tz)=(tx)3+(ty)3+(tz)3tx+ty+tz=t3(x3+y3+z3)t(x+y+z)=t2x3+y3+z3x+y+z=t2f(x,y,z)\begin{aligned}f(tx, ty, tz) & = \frac{(tx)^3 + (ty)^3 + (tz)^3}{tx+ty+tz} \\
    & = \frac{t^3(x^3 + y^3 + z^3)}{t(x+y+z)} \\
    & = t^2 \frac{x^3 + y^3 + z^3}{x+y+z} = t^2 f(x, y, z)\end{aligned}

    The function f(x,y,z)f(x, y, z) is homogeneous of degree n=2n=2.

    Step 2: Apply Euler's Theorem.
    According to Euler's Theorem for multiple variables:

    xfx+yfy+zfz=nf(x,y,z)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z} = nf(x, y, z)

    Substituting n=2n=2:
    xfx+yfy+zfz=2f(x,y,z)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z} = 2f(x, y, z)

    Step 3: Evaluate 2f(x,y,z)2f(x, y, z) at the point (1,2,3)(1, 2, 3).

    f(1,2,3)=13+23+331+2+3=1+8+276=366=6f(1, 2, 3) = \frac{1^3 + 2^3 + 3^3}{1+2+3} = \frac{1 + 8 + 27}{6} = \frac{36}{6} = 6

    Therefore,
    xfx+yfy+zfz=2×6=12x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} + z \frac{\partial f}{\partial z} = 2 \times 6 = 12

    Answer: \boxed{12}"
    :::

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    Advanced Applications

    1. Euler's Theorem for Functions of Homogeneous Functions

    Many problems involve functions that are not directly homogeneous but can be expressed as a function of a homogeneous function. For instance, if u=ϕ(z)u = \phi(z), where z=f(x,y)z = f(x, y) is a homogeneous function of degree nn, we can still apply a modified form of Euler's Theorem.

    Let u=ϕ(z)u = \phi(z), where z=f(x,y)z = f(x, y) is homogeneous of degree nn.
    We seek xux+yuyx \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y}.

    Step 1: Apply the chain rule for partial derivatives.

    ux=dϕdzzxuy=dϕdzzy\begin{aligned}\frac{\partial u}{\partial x} & = \frac{d\phi}{dz} \frac{\partial z}{\partial x} \\ \frac{\partial u}{\partial y} & = \frac{d\phi}{dz} \frac{\partial z}{\partial y}\end{aligned}

    Step 2: Substitute these into the Euler's Theorem expression.

    xux+yuy=x(dϕdzzx)+y(dϕdzzy)=dϕdz(xzx+yzy)\begin{aligned}x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} & = x \left( \frac{d\phi}{dz} \frac{\partial z}{\partial x} \right) + y \left( \frac{d\phi}{dz} \frac{\partial z}{\partial y} \right) \\ & = \frac{d\phi}{dz} \left( x \frac{\partial z}{\partial x} + y \frac{\partial z}{\partial y} \right)\end{aligned}

    Step 3: Apply Euler's Theorem to z=f(x,y)z = f(x, y).

    xzx+yzy=nzx \frac{\partial z}{\partial x} + y \frac{\partial z}{\partial y} = nz

    Step 4: Substitute this back into the expression for uu.

    xux+yuy=dϕdz(nz)=nzdϕdz\begin{aligned}x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} & = \frac{d\phi}{dz} (nz) \\ & = n z \frac{d\phi}{dz}\end{aligned}

    This general form nzdϕdzn z \frac{d\phi}{dz} can be further simplified depending on the specific function ϕ\phi. If we express zz in terms of uu (i.e., z=ϕ1(u)z = \phi^{-1}(u)), then dϕdz=1dzdu\frac{d\phi}{dz} = \frac{1}{\frac{dz}{du}}.
    Thus, xux+yuy=nzdzdux \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = n \frac{z}{\frac{dz}{du}}. More conveniently, if z=ψ(u)z = \psi(u), then dzdu=ψ(u)\frac{dz}{du} = \psi'(u), giving nψ(u)ψ(u)n \frac{\psi(u)}{\psi'(u)}.

    📐 Euler's Theorem for Composite Functions

    If u=ϕ(z)u = \phi(z) where z=f(x,y)z = f(x, y) is a homogeneous function of degree nn, and z=ψ(u)z = \psi(u) is the inverse function, then:

    xux+yuy=nψ(u)ψ(u)x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = n \frac{\psi(u)}{\psi'(u)}

    Where:
    z=f(x,y)z = f(x, y) is homogeneous of degree nn.
    u=ϕ(z)u = \phi(z) is a function of zz.
    ψ(u)=ϕ1(u)\psi(u) = \phi^{-1}(u) is the inverse function of ϕ\phi.
    ψ(u)=ddu(ψ(u))\psi'(u) = \frac{d}{du}(\psi(u)).
    When to use: For functions like u=sin1(Z)u = \sin^{-1}(Z), u=log(Z)u = \log(Z), where ZZ is homogeneous.

    Quick Example: If u=sin1(x+yx+y)u = \sin^{-1}\left(\frac{x+y}{\sqrt{x}+\sqrt{y}}\right), find xux+yuyx \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y}.

    Step 1: Let z=x+yx+yz = \frac{x+y}{\sqrt{x}+\sqrt{y}}. Determine the degree of homogeneity of zz.

    z(tx,ty)=tx+tytx+ty=t(x+y)t(x+y)=t1/2x+yx+y=t1/2z(x,y)\begin{aligned}z(tx, ty) & = \frac{tx+ty}{\sqrt{tx}+\sqrt{ty}} \\ & = \frac{t(x+y)}{\sqrt{t}(\sqrt{x}+\sqrt{y})} \\ & = t^{1/2} \frac{x+y}{\sqrt{x}+\sqrt{y}} = t^{1/2} z(x, y)\end{aligned}

    So zz is homogeneous of degree n=1/2n=1/2.

    Step 2: Identify ϕ(z)\phi(z) and ψ(u)\psi(u).
    We have u=sin1(z)u = \sin^{-1}(z), so ϕ(z)=sin1(z)\phi(z) = \sin^{-1}(z).
    The inverse function is z=sinuz = \sin u, so ψ(u)=sinu\psi(u) = \sin u.

    Step 3: Calculate ψ(u)\psi'(u).

    ψ(u)=ddu(sinu)=cosu\psi'(u) = \frac{d}{du}(\sin u) = \cos u

    Step 4: Apply the formula for Euler's Theorem for composite functions.

    xux+yuy=nψ(u)ψ(u)=12sinucosu=12tanu\begin{aligned}x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} & = n \frac{\psi(u)}{\psi'(u)} \\ & = \frac{1}{2} \frac{\sin u}{\cos u} \\ & = \frac{1}{2} \tan u\end{aligned}

    Answer: 12tanu\frac{1}{2} \tan u.

    ⚠️ Common Mistake

    ❌ Directly applying xux+yuy=nux \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = nu when uu is not homogeneous.
    ✅ Identify the inner homogeneous function zz, determine its degree nn, and use the derived formula nψ(u)ψ(u)n \frac{\psi(u)}{\psi'(u)}.

    :::question type="MCQ" question="If u=tan1(x3+y3xy)u = \tan^{-1}\left(\frac{x^3 + y^3}{x-y}\right), then xux+yuyx \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} is equal to:" options=["sin(2u)\sin(2u)","2sin(2u)2\sin(2u)","12sin(2u)\frac{1}{2}\sin(2u)","tanu\tan u"] answer="sin(2u)\sin(2u)" hint="Let z=tanuz = \tan u. Find the degree of homogeneity of zz and then apply the extended Euler's theorem." solution="Step 1: Let z=x3+y3xyz = \frac{x^3 + y^3}{x-y}. Determine the degree of homogeneity of zz.

    z(tx,ty)=(tx)3+(ty)3txty=t3(x3+y3)t(xy)=t2x3+y3xy=t2z(x,y)\begin{aligned}z(tx, ty) & = \frac{(tx)^3 + (ty)^3}{tx-ty} \\
    & = \frac{t^3(x^3+y^3)}{t(x-y)} \\
    & = t^2 \frac{x^3+y^3}{x-y} = t^2 z(x, y)\end{aligned}

    So zz is homogeneous of degree n=2n=2.

    Step 2: Identify ψ(u)\psi(u).
    Given u=tan1(z)u = \tan^{-1}(z), we have z=tanuz = \tan u. So ψ(u)=tanu\psi(u) = \tan u.

    Step 3: Calculate ψ(u)\psi'(u).

    ψ(u)=ddu(tanu)=sec2u\psi'(u) = \frac{d}{du}(\tan u) = \sec^2 u

    Step 4: Apply the formula xux+yuy=nψ(u)ψ(u)x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = n \frac{\psi(u)}{\psi'(u)}.

    xux+yuy=2tanusec2u=2sinu/cosu1/cos2u=2sinucosucos2u=2sinucosu\begin{aligned}x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} & = 2 \frac{\tan u}{\sec^2 u} \\
    & = 2 \frac{\sin u / \cos u}{1/\cos^2 u} \\
    & = 2 \frac{\sin u}{\cos u} \cdot \cos^2 u \\
    & = 2 \sin u \cos u\end{aligned}

    Using the identity sin(2u)=2sinucosu\sin(2u) = 2 \sin u \cos u:
    =sin(2u)= \sin(2u)

    Answer: \boxed{\sin(2u)}"
    :::

    ---

    2. Higher-Order Derivatives and Euler's Theorem

    Euler's Theorem can be extended to second-order partial derivatives. If z=f(x,y)z = f(x, y) is a homogeneous function of degree nn, then the following relation holds:

    📐 Second-Order Euler's Theorem
    x22zx2+2xy2zxy+y22zy2=n(n1)zx^2 \frac{\partial^2 z}{\partial x^2} + 2xy \frac{\partial^2 z}{\partial x \partial y} + y^2 \frac{\partial^2 z}{\partial y^2} = n(n-1)z
    When to use: When problems involve second-order partial derivatives of homogeneous functions.

    Derivation Sketch:
    We know xzx+yzy=nzx \frac{\partial z}{\partial x} + y \frac{\partial z}{\partial y} = nz.
    Differentiate this with respect to xx:
    zx+x2zx2+y2zxy=nzx\frac{\partial z}{\partial x} + x \frac{\partial^2 z}{\partial x^2} + y \frac{\partial^2 z}{\partial x \partial y} = n \frac{\partial z}{\partial x} (This is a form seen in PYQ 2-E)
    Differentiate xzx+yzy=nzx \frac{\partial z}{\partial x} + y \frac{\partial z}{\partial y} = nz with respect to yy:
    x2zyx+zy+y2zy2=nzyx \frac{\partial^2 z}{\partial y \partial x} + \frac{\partial z}{\partial y} + y \frac{\partial^2 z}{\partial y^2} = n \frac{\partial z}{\partial y}
    Multiply the first derived equation by xx and the second by yy, then add them. This process yields the second-order Euler's Theorem.

    Quick Example: Verify the second-order Euler's Theorem for f(x,y)=x2+y2f(x, y) = x^2 + y^2.

    Step 1: Determine the degree of homogeneity.

    f(tx,ty)=(tx)2+(ty)2=t2(x2+y2)=t2f(x,y)f(tx, ty) = (tx)^2 + (ty)^2 = t^2(x^2+y^2) = t^2 f(x, y)

    So n=2n=2.

    Step 2: Calculate the first-order partial derivatives.

    fx=2xfy=2y\begin{aligned}\frac{\partial f}{\partial x} & = 2x \\ \frac{\partial f}{\partial y} & = 2y\end{aligned}

    Step 3: Calculate the second-order partial derivatives.

    2fx2=22fy2=22fxy=0\begin{aligned}\frac{\partial^2 f}{\partial x^2} & = 2 \\ \frac{\partial^2 f}{\partial y^2} & = 2 \\ \frac{\partial^2 f}{\partial x \partial y} & = 0\end{aligned}

    Step 4: Substitute into the second-order Euler's Theorem formula.

    x22fx2+2xy2fxy+y22fy2=x2(2)+2xy(0)+y2(2)=2x2+2y2=2(x2+y2)=2f(x,y)\begin{aligned}x^2 \frac{\partial^2 f}{\partial x^2} + 2xy \frac{\partial^2 f}{\partial x \partial y} + y^2 \frac{\partial^2 f}{\partial y^2} & = x^2(2) + 2xy(0) + y^2(2) \\ & = 2x^2 + 2y^2 \\ & = 2(x^2 + y^2) \\ & = 2f(x, y)\end{aligned}

    Step 5: Compare with n(n1)f(x,y)n(n-1)f(x, y).
    For n=2n=2,

    n(n1)f(x,y)=2(21)f(x,y)=2(1)f(x,y)=2f(x,y)n(n-1)f(x, y) = 2(2-1)f(x, y) = 2(1)f(x, y) = 2f(x, y)

    The result matches, verifying the theorem.

    :::question type="MCQ" question="If z=(x2+y2)1/2z = (x^2+y^2)^{1/2}, then x22zx2+2xy2zxy+y22zy2x^2 \frac{\partial^2 z}{\partial x^2} + 2xy \frac{\partial^2 z}{\partial x \partial y} + y^2 \frac{\partial^2 z}{\partial y^2} is equal to:" options=["zz","00","2z2z","z-z"] answer="00" hint="First determine the degree of homogeneity nn for zz. Then apply the second-order Euler's Theorem formula n(n1)zn(n-1)z." solution="Step 1: Determine the degree of homogeneity of z=(x2+y2)1/2z = (x^2+y^2)^{1/2}.

    z(tx,ty)=((tx)2+(ty)2)1/2=(t2(x2+y2))1/2=(t2)1/2(x2+y2)1/2=tz(x,y)\begin{aligned}z(tx, ty) & = ((tx)^2 + (ty)^2)^{1/2} \\
    & = (t^2(x^2+y^2))^{1/2} \\
    & = (t^2)^{1/2} (x^2+y^2)^{1/2} = t z(x, y)\end{aligned}

    The function zz is homogeneous of degree n=1n=1.

    Step 2: Apply the second-order Euler's Theorem.
    The theorem states:

    x22zx2+2xy2zxy+y22zy2=n(n1)zx^2 \frac{\partial^2 z}{\partial x^2} + 2xy \frac{\partial^2 z}{\partial x \partial y} + y^2 \frac{\partial^2 z}{\partial y^2} = n(n-1)z

    Substitute n=1n=1:
    x22zx2+2xy2zxy+y22zy2=1(11)z=1(0)z=0\begin{aligned}x^2 \frac{\partial^2 z}{\partial x^2} + 2xy \frac{\partial^2 z}{\partial x \partial y} + y^2 \frac{\partial^2 z}{\partial y^2} & = 1(1-1)z \\
    & = 1(0)z = 0\end{aligned}

    Answer: \boxed{0}"
    :::

    ---

    Problem-Solving Strategies

    💡 Identifying Homogeneity

    Always begin by checking if f(tx,ty)=tnf(x,y)f(tx, ty) = t^n f(x, y) holds. This step determines both homogeneity and the degree nn, which is crucial for applying Euler's Theorem. Look for functions where all terms have the same total degree, or where the numerator and denominator are homogeneous, allowing for a combined degree calculation. For functions like f(x,y)=x3+y3f(x,y) = \sqrt{x^3+y^3}, the degree is 3/23/2.

    💡 Handling Composite Functions

    When faced with u=ϕ(z)u = \phi(z) where zz is homogeneous (e.g., u=sin1(z)u = \sin^{-1}(z) or u=log(z)u = \log(z)), do not directly apply Euler's theorem to uu. Instead, identify the inner homogeneous function zz, find its degree nn, and then use the formula xux+yuy=nψ(u)ψ(u)x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = n \frac{\psi(u)}{\psi'(u)}, where ψ(u)=z\psi(u) = z. This is a common pattern in CUET PG questions.

    ---

    Common Mistakes

    ⚠️ Incorrect Degree Calculation

    ❌ Assuming homogeneity based on a few terms, or incorrectly calculating the degree for fractional or negative powers.
    ✅ Always apply the definition f(tx,ty)=tnf(x,y)f(tx, ty) = t^n f(x, y) rigorously to the entire function. For rational functions, the degree is the degree of the numerator minus the degree of the denominator. For functions like f(x,y)=x3+y3f(x,y) = \sqrt{x^3+y^3}, the degree is 3/23/2.

    ⚠️ Misapplying Euler's Theorem

    ❌ Applying xux+yuy=nux \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = nu when uu is not homogeneous, but only a function of a homogeneous function.
    ✅ Ensure the function to which Euler's Theorem is applied is itself homogeneous. If it's a composite function, use the extended form nψ(u)ψ(u)n \frac{\psi(u)}{\psi'(u)}.

    ⚠️ Ignoring Non-Homogeneous Terms

    ❌ Attempting to apply Euler's Theorem to functions with constant terms or non-homogeneous terms.
    ✅ A function with terms like x2+y2+1x^2+y^2+1 is not homogeneous because the constant term 11 does not scale with tnt^n. Only purely homogeneous functions satisfy the theorem.

    ---

    Practice Questions

    :::question type="MCQ" question="If u(x,y)=xlog(yx)+yu(x, y) = x \log\left(\frac{y}{x}\right) + y, then xux+yuyx \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} is equal to:" options=["uu","2u2u","00","x+yx+y"] answer="uu" hint="First, check the degree of homogeneity of u(x,y)u(x, y). If it is homogeneous, apply Euler's Theorem. If not, calculate the partial derivatives directly." solution="Step 1: Determine the degree of homogeneity of u(x,y)u(x, y).

    u(tx,ty)=txlog(tytx)+ty=t(xlog(yx)+y)=tu(x,y)u(tx, ty) = tx \log\left(\frac{ty}{tx}\right) + ty = t \left( x \log\left(\frac{y}{x}\right) + y \right) = t u(x, y)

    The function u(x,y)u(x, y) is homogeneous of degree n=1n=1.

    Step 2: Apply Euler's Theorem.
    For a homogeneous function u(x,y)u(x, y) of degree nn, Euler's Theorem states:

    xux+yuy=nux \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = nu

    Substituting n=1n=1:
    xux+yuy=1u=ux \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = 1 \cdot u = u

    Answer: \boxed{u}"
    :::

    :::question type="NAT" question="Given f(x,y)=x3+y33f(x, y) = \sqrt[3]{x^3+y^3}, calculate xfx+yfyx \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y}. (Provide the expression in terms of f(x,y)f(x,y).)" answer="f(x,y)f(x,y)" hint="Identify the degree of homogeneity and apply Euler's Theorem." solution="Step 1: Determine the degree of homogeneity of f(x,y)f(x, y).

    f(tx,ty)=(tx)3+(ty)33=t3(x3+y3)3=(t3)1/3(x3+y3)1/3=tf(x,y)f(tx, ty) = \sqrt[3]{(tx)^3+(ty)^3} = \sqrt[3]{t^3(x^3+y^3)} = (t^3)^{1/3} (x^3+y^3)^{1/3} = t f(x, y)

    The function f(x,y)f(x, y) is homogeneous of degree n=1n=1.

    Step 2: Apply Euler's Theorem.
    For a homogeneous function f(x,y)f(x, y) of degree nn, Euler's Theorem states:

    xfx+yfy=nf(x,y)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} = nf(x, y)

    Substituting n=1n=1:
    xfx+yfy=1f(x,y)=f(x,y)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} = 1 \cdot f(x, y) = f(x, y)

    Answer: \boxed{f(x,y)}"
    :::

    :::question type="MCQ" question="If u=log(x2+y2x+y)u = \log\left(\frac{x^2+y^2}{x+y}\right), then xux+yuyx \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} is equal to:" options=["eue^u","uu","11","2u2u"] answer="11" hint="Let z=euz = e^u. Find the degree of homogeneity of zz and then apply the extended Euler's theorem." solution="Step 1: Let z=x2+y2x+yz = \frac{x^2+y^2}{x+y}. Determine the degree of homogeneity of zz.

    z(tx,ty)=(tx)2+(ty)2tx+ty=t2(x2+y2)t(x+y)=tx2+y2x+y=tz(x,y)z(tx, ty) = \frac{(tx)^2+(ty)^2}{tx+ty} = \frac{t^2(x^2+y^2)}{t(x+y)} = t \frac{x^2+y^2}{x+y} = t z(x, y)

    So zz is homogeneous of degree n=1n=1.

    Step 2: Identify ψ(u)\psi(u).
    Given u=log(z)u = \log(z), we have z=euz = e^u. So ψ(u)=eu\psi(u) = e^u.

    Step 3: Calculate ψ(u)\psi'(u).

    ψ(u)=ddu(eu)=eu\psi'(u) = \frac{d}{du}(e^u) = e^u

    Step 4: Apply the formula xux+yuy=nψ(u)ψ(u)x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = n \frac{\psi(u)}{\psi'(u)}.

    xux+yuy=1eueu=1x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = 1 \cdot \frac{e^u}{e^u} = 1

    Answer: \boxed{1}"
    :::

    :::question type="MSQ" question="Let f(x,y)f(x, y) be a homogeneous function of degree nn. Which of the following statements are correct?" options=["xfx+yfy=nf(x,y)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} = nf(x, y)","If n=0n=0, then f(x,y)f(x,y) must be a constant.","fx\frac{\partial f}{\partial x} is a homogeneous function of degree n1n-1.","If f(x,y)=xng(yx)f(x, y) = x^n g\left(\frac{y}{x}\right), then g(yx)g\left(\frac{y}{x}\right) is a homogeneous function of degree 00.""] answer="xfx+yfy=nf(x,y)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} = nf(x, y),fx\frac{\partial f}{\partial x} is a homogeneous function of degree n1n-1.,If f(x,y)=xng(yx)f(x, y) = x^n g\left(\frac{y}{x}\right), then g(yx)g\left(\frac{y}{x}\right) is a homogeneous function of degree 00." hint="Recall Euler's theorem, properties of homogeneous functions, and the alternative form definition." solution="Let's analyze each statement:

  • xfx+yfy=nf(x,y)x \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} = nf(x, y): This is the statement of Euler's Theorem for homogeneous functions. This statement is correct.

  • If n=0n=0, then f(x,y)f(x,y) must be a constant: A homogeneous function of degree 0 means f(tx,ty)=t0f(x,y)=f(x,y)f(tx, ty) = t^0 f(x, y) = f(x, y). An example is f(x,y)=xyf(x, y) = \frac{x}{y}. This is homogeneous of degree 0 but not a constant. Thus, this statement is incorrect.

  • fx\frac{\partial f}{\partial x} is a homogeneous function of degree n1n-1: If f(tx,ty)=tnf(x,y)f(tx, ty) = t^n f(x, y), differentiate both sides with respect to xx:

  • x[f(tx,ty)]=x[tnf(x,y)]\frac{\partial}{\partial x} [f(tx, ty)] = \frac{\partial}{\partial x} [t^n f(x, y)]

    Using the chain rule on the left side:
    tfx(tx,ty)=tnfx(x,y)t \frac{\partial f}{\partial x}(tx, ty) = t^n \frac{\partial f}{\partial x}(x, y)

    Dividing by tt:
    fx(tx,ty)=tn1fx(x,y)\frac{\partial f}{\partial x}(tx, ty) = t^{n-1} \frac{\partial f}{\partial x}(x, y)

    This shows that fx\frac{\partial f}{\partial x} is homogeneous of degree n1n-1. This statement is correct.
  • If f(x,y)=xng(yx)f(x, y) = x^n g\left(\frac{y}{x}\right), then g(yx)g\left(\frac{y}{x}\right) is a homogeneous function of degree 00: Let h(x,y)=g(yx)h(x, y) = g\left(\frac{y}{x}\right).

  • Then
    h(tx,ty)=g(tytx)=g(yx)=h(x,y)=t0h(x,y)h(tx, ty) = g\left(\frac{ty}{tx}\right) = g\left(\frac{y}{x}\right) = h(x, y) = t^0 h(x, y)

    Thus, g(yx)g\left(\frac{y}{x}\right) is a homogeneous function of degree 00. This statement is correct.
    Answer: \boxed{\text{Statements 1, 3, and 4 are correct.}}"
    :::

    :::question type="MCQ" question="If u=cos1(x3+y3x+y)u = \cos^{-1}\left(\frac{x^3+y^3}{x+y}\right), then xux+yuyx \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} is equal to:" options=["2cotu2 \cot u","2cotu-2 \cot u","2tanu-2 \tan u","2tanu2 \tan u"] answer="2cotu-2 \cot u" hint="Let z=cosuz = \cos u. Find the degree of homogeneity of zz and then apply the extended Euler's theorem." solution="Step 1: Let z=x3+y3xyz = \frac{x^3+y^3}{x-y}. Determine the degree of homogeneity of zz.

    z(tx,ty)=(tx)3+(ty)3txty=t3(x3+y3)t(xy)=t2x3+y3xy=t2z(x,y)\begin{aligned}z(tx, ty) & = \frac{(tx)^3+(ty)^3}{tx-ty} \\
    & = \frac{t^3(x^3+y^3)}{t(x-y)} \\
    & = t^2 \frac{x^3+y^3}{x-y} = t^2 z(x, y)\end{aligned}

    So zz is homogeneous of degree n=2n=2.

    Step 2: Identify ψ(u)\psi(u).
    Given u=cos1(z)u = \cos^{-1}(z), we have z=cosuz = \cos u. So ψ(u)=cosu\psi(u) = \cos u.

    Step 3: Calculate ψ(u)\psi'(u).

    ψ(u)=ddu(cosu)=sinu\psi'(u) = \frac{d}{du}(\cos u) = -\sin u

    Step 4: Apply the formula xux+yuy=nψ(u)ψ(u)x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = n \frac{\psi(u)}{\psi'(u)}.

    xux+yuy=2cosusinu=2cotu\begin{aligned}x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} & = 2 \frac{\cos u}{-\sin u} \\
    & = -2 \cot u\end{aligned}

    Answer: \boxed{-2 \cot u}"
    :::

    ---

    Summary

    Key Formulas & Takeaways

    | # | Formula/Concept | Expression |
    |---|----------------|------------|
    | 1 | Homogeneous Function Definition | f(tx,ty)=tnf(x,y)f(tx, ty) = t^n f(x, y) |
    | 2 | Alternative Form | f(x,y)=xng(yx)f(x, y) = x^n g\left(\frac{y}{x}\right) or ynh(xy)y^n h\left(\frac{x}{y}\right) |
    | 3 | Euler's Theorem (2 variables) | xfx+yfy=nfx \frac{\partial f}{\partial x} + y \frac{\partial f}{\partial y} = nf |
    | 4 | Euler's Theorem (m variables) | i=1mxifxi=nf\sum_{i=1}^{m} x_i \frac{\partial f}{\partial x_i} = nf |
    | 5 | Euler's for Composite Functions | If u=ϕ(z)u = \phi(z), z=ψ(u)z=\psi(u) homogeneous of degree nn, then xux+yuy=nψ(u)ψ(u)x \frac{\partial u}{\partial x} + y \frac{\partial u}{\partial y} = n \frac{\psi(u)}{\psi'(u)} |
    | 6 | Second-Order Euler's Theorem | x22zx2+2xy2zxy+y22zy2=n(n1)zx^2 \frac{\partial^2 z}{\partial x^2} + 2xy \frac{\partial^2 z}{\partial x \partial y} + y^2 \frac{\partial^2 z}{\partial y^2} = n(n-1)z |

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    What's Next?

    💡 Continue Learning

    This topic connects to:

      • Exact Differential Equations: Homogeneous functions are often involved in solving exact differential equations, especially when checking for exactness or finding integrating factors.

      • Maxima and Minima of Functions of Several Variables: Understanding partial derivatives and their properties is foundational for optimization problems.

      • Implicit Function Theorem: The structure of homogeneous functions can simplify the application of implicit differentiation in multivariable contexts.

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    💡 Next Up

    Proceeding to Maxima and Minima.

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    Part 4: Maxima and Minima

    We investigate the determination of extreme values for functions of two independent real variables, a fundamental concept in multivariable calculus with extensive applications in optimization problems. The techniques discussed are crucial for analyzing the behavior of surfaces and solving constrained optimization tasks often encountered in various scientific and economic models.

    ---

    Core Concepts

    1. Local Extrema and Critical Points

    We define a function f(x,y)f(x, y) to have a local maximum at a point (a,b)(a, b) if f(x,y)f(a,b)f(x, y) \le f(a, b) for all (x,y)(x, y) in some open disk containing (a,b)(a, b). Similarly, f(x,y)f(x, y) has a local minimum at (a,b)(a, b) if f(x,y)f(a,b)f(x, y) \ge f(a, b) for all (x,y)(x, y) in such a disk.

    A critical point of f(x,y)f(x, y) is a point (a,b)(a, b) in the domain of ff where either both first-order partial derivatives are zero, i.e., fx(a,b)=0f_x(a, b) = 0 and fy(a,b)=0f_y(a, b) = 0, or at least one of the partial derivatives does not exist. Local extrema can only occur at critical points.

    Quick Example:
    Consider the function f(x,y)=x2+y24x+6yf(x, y) = x^2 + y^2 - 4x + 6y. We locate its critical points.

    Step 1: Compute the first partial derivatives.

    fx=2x4fy=2y+6\begin{aligned}\frac{\partial f}{\partial x} & = 2x - 4 \\
    \frac{\partial f}{\partial y} & = 2y + 6\end{aligned}

    Step 2: Set the partial derivatives to zero and solve the system.

    2x4=0    x=22y+6=0    y=3\begin{aligned}2x - 4 & = 0 \implies x = 2 \\
    2y + 6 & = 0 \implies y = -3\end{aligned}

    Answer: The only critical point is (2,3)(2, -3).

    :::question type="MCQ" question="For the function f(x,y)=x33x+y24yf(x, y) = x^3 - 3x + y^2 - 4y, which of the following is a critical point?" options=["(1,2)(1, 2)","(0,0)(0, 0)","(2,1)(2, 1)","(1,0)(1, 0)"] answer="(1,2)(1, 2)" hint="Compute first partial derivatives and set them to zero. Solve the resulting system of equations." solution="Step 1: Compute the first partial derivatives.

    fx=3x23fy=2y4\begin{aligned}\frac{\partial f}{\partial x} & = 3x^2 - 3 \\
    \frac{\partial f}{\partial y} & = 2y - 4\end{aligned}

    Step 2: Set the partial derivatives to zero.
    3x23=0    3x2=3    x2=1    x=±12y4=0    2y=4    y=2\begin{aligned}3x^2 - 3 & = 0 \implies 3x^2 = 3 \implies x^2 = 1 \implies x = \pm 1 \\
    2y - 4 & = 0 \implies 2y = 4 \implies y = 2\end{aligned}

    Step 3: Identify the critical points.
    The critical points are (1,2)(1, 2) and (1,2)(-1, 2).
    From the given options, (1,2)(1, 2) is a critical point.
    Answer: \boxed{(1, 2)}"
    :::

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    2. The Second Derivative Test

    The Second Derivative Test helps classify critical points of a function f(x,y)f(x, y) where the first partial derivatives are zero. It involves evaluating the second-order partial derivatives at the critical point (a,b)(a, b).

    📐 Second Derivative Test Discriminant

    Let f(x,y)f(x, y) have continuous second-order partial derivatives. Define:

    D(x,y)=fxx(x,y)fyy(x,y)[fxy(x,y)]2D(x, y) = f_{xx}(x, y)f_{yy}(x, y) - [f_{xy}(x, y)]^2

    At a critical point (a,b)(a, b) where fx(a,b)=0f_x(a, b) = 0 and fy(a,b)=0f_y(a, b) = 0:
    • If D(a,b)>0D(a, b) > 0 and fxx(a,b)>0f_{xx}(a, b) > 0, then ff has a local minimum at (a,b)(a, b).

    • If D(a,b)>0D(a, b) > 0 and fxx(a,b)<0f_{xx}(a, b) < 0, then ff has a local maximum at (a,b)(a, b).

    • If D(a,b)<0D(a, b) < 0, then ff has a saddle point at (a,b)(a, b).

    • If D(a,b)=0D(a, b) = 0, the test is inconclusive.

    Where: fxx=2fx2f_{xx} = \frac{\partial^2 f}{\partial x^2}, fyy=2fy2f_{yy} = \frac{\partial^2 f}{\partial y^2}, fxy=2fxyf_{xy} = \frac{\partial^2 f}{\partial x \partial y}
    When to use: To classify critical points as local maxima, minima, or saddle points.

    Quick Example:
    Classify the critical point (2,3)(2, -3) for f(x,y)=x2+y24x+6yf(x, y) = x^2 + y^2 - 4x + 6y.

    Step 1: Compute the second partial derivatives.

    fx=2x4    fxx=2fy=2y+6    fyy=2fxy=y(2x4)=0\begin{aligned}f_x & = 2x - 4 \implies f_{xx} = 2 \\
    f_y & = 2y + 6 \implies f_{yy} = 2 \\
    f_{xy} & = \frac{\partial}{\partial y}(2x - 4) = 0\end{aligned}

    Step 2: Calculate the discriminant D(x,y)D(x, y).

    D(x,y)=fxxfyy(fxy)2=(2)(2)(0)2=4D(x, y) = f_{xx}f_{yy} - (f_{xy})^2 = (2)(2) - (0)^2 = 4

    Step 3: Evaluate DD and fxxf_{xx} at the critical point (2,3)(2, -3).

    D(2,3)=4fxx(2,3)=2\begin{aligned}D(2, -3) & = 4 \\
    f_{xx}(2, -3) & = 2\end{aligned}

    Answer: Since D(2,3)=4>0D(2, -3) = 4 > 0 and fxx(2,3)=2>0f_{xx}(2, -3) = 2 > 0, the function has a local minimum at (2,3)(2, -3).

    :::question type="MCQ" question="For the function f(x,y)=x2xy+y2+6x9yf(x, y) = x^2 - xy + y^2 + 6x - 9y, classify the critical point (1,4)(-1, 4)." options=["Local Maximum","Local Minimum","Saddle Point","Inconclusive"] answer="Local Minimum" hint="Calculate the second partial derivatives and apply the Second Derivative Test." solution="Step 1: Compute the first partial derivatives and find critical points.

    fx=2xy+6fy=x+2y9\begin{aligned}f_x & = 2x - y + 6 \\
    f_y & = -x + 2y - 9\end{aligned}

    Setting fx=0f_x = 0 and fy=0f_y = 0:
    2xy+6=0(1)x+2y9=0(2)\begin{aligned}2x - y + 6 & = 0 \quad (1) \\
    -x + 2y - 9 & = 0 \quad (2)\end{aligned}

    From (2), x=2y9x = 2y - 9. Substitute into (1):
    2(2y9)y+6=04y18y+6=03y12=0    y=4\begin{aligned}2(2y - 9) - y + 6 & = 0 \\
    4y - 18 - y + 6 & = 0 \\
    3y - 12 & = 0 \implies y = 4\end{aligned}

    Substitute y=4y = 4 back into x=2y9x = 2y - 9:
    x=2(4)9=89=1x = 2(4) - 9 = 8 - 9 = -1

    So, the critical point is (1,4)(-1, 4).

    Step 2: Compute the second partial derivatives.

    fxx=x(2xy+6)=2fyy=y(x+2y9)=2fxy=y(2xy+6)=1\begin{aligned}f_{xx} & = \frac{\partial}{\partial x}(2x - y + 6) = 2 \\
    f_{yy} & = \frac{\partial}{\partial y}(-x + 2y - 9) = 2 \\
    f_{xy} & = \frac{\partial}{\partial y}(2x - y + 6) = -1\end{aligned}

    Step 3: Calculate the discriminant DD.

    D(x,y)=fxxfyy(fxy)2=(2)(2)(1)2=41=3D(x, y) = f_{xx}f_{yy} - (f_{xy})^2 = (2)(2) - (-1)^2 = 4 - 1 = 3

    Step 4: Evaluate DD and fxxf_{xx} at the critical point (1,4)(-1, 4).

    D(1,4)=3fxx(1,4)=2\begin{aligned}D(-1, 4) & = 3 \\
    f_{xx}(-1, 4) & = 2\end{aligned}

    Since D(1,4)=3>0D(-1, 4) = 3 > 0 and fxx(1,4)=2>0f_{xx}(-1, 4) = 2 > 0, the function has a local minimum at (1,4)(-1, 4).
    Answer: \boxed{\text{Local Minimum}}"
    :::

    ---

    3. Saddle Points

    A saddle point is a critical point (a,b)(a, b) where fx(a,b)=0f_x(a, b) = 0 and fy(a,b)=0f_y(a, b) = 0, but f(a,b)f(a, b) is neither a local maximum nor a local minimum. Graphically, the surface resembles a saddle, curving upwards in some directions and downwards in others at that point.

    The Second Derivative Test identifies a saddle point when D(a,b)<0D(a, b) < 0.

    Quick Example:
    Consider f(x,y)=x2y2f(x, y) = x^2 - y^2. We classify its critical point.

    Step 1: Find critical points.

    fx=2x=0    x=0fy=2y=0    y=0\begin{aligned}f_x & = 2x = 0 \implies x = 0 \\
    f_y & = -2y = 0 \implies y = 0\end{aligned}

    The critical point is (0,0)(0, 0).

    Step 2: Compute second partial derivatives.

    fxx=2fyy=2fxy=0\begin{aligned}f_{xx} & = 2 \\
    f_{yy} & = -2 \\
    f_{xy} & = 0\end{aligned}

    Step 3: Calculate the discriminant DD.

    D(x,y)=fxxfyy(fxy)2=(2)(2)(0)2=4D(x, y) = f_{xx}f_{yy} - (f_{xy})^2 = (2)(-2) - (0)^2 = -4

    Step 4: Evaluate DD at (0,0)(0, 0).

    D(0,0)=4D(0, 0) = -4

    Answer: Since D(0,0)=4<0D(0, 0) = -4 < 0, the function has a saddle point at (0,0)(0, 0).

    :::question type="MCQ" question="Which of the following functions has a saddle point at (0,0)(0, 0)?" options=["f(x,y)=x2+y2f(x, y) = x^2 + y^2","f(x,y)=x2y2f(x, y) = -x^2 - y^2","f(x,y)=x22xy+y2f(x, y) = x^2 - 2xy + y^2","f(x,y)=x2y2+3xyf(x, y) = x^2 - y^2 + 3xy"] answer="f(x,y)=x2y2+3xyf(x, y) = x^2 - y^2 + 3xy" hint="For each function, find the critical points and apply the Second Derivative Test. A saddle point occurs when D<0D < 0." solution="We analyze each option:

    Option 1: f(x,y)=x2+y2f(x, y) = x^2 + y^2
    fx=2xf_x = 2x, fy=2yf_y = 2y. Critical point: (0,0)(0,0).
    fxx=2f_{xx} = 2, fyy=2f_{yy} = 2, fxy=0f_{xy} = 0.
    D=(2)(2)(0)2=4D = (2)(2) - (0)^2 = 4. Since D>0D > 0 and fxx>0f_{xx} > 0, (0,0)(0,0) is a local minimum.

    Option 2: f(x,y)=x2y2f(x, y) = -x^2 - y^2
    fx=2xf_x = -2x, fy=2yf_y = -2y. Critical point: (0,0)(0,0).
    fxx=2f_{xx} = -2, fyy=2f_{yy} = -2, fxy=0f_{xy} = 0.
    D=(2)(2)(0)2=4D = (-2)(-2) - (0)^2 = 4. Since D>0D > 0 and fxx<0f_{xx} < 0, (0,0)(0,0) is a local maximum.

    Option 3: f(x,y)=x22xy+y2=(xy)2f(x, y) = x^2 - 2xy + y^2 = (x-y)^2
    fx=2(xy)f_x = 2(x-y), fy=2(xy)f_y = -2(x-y). Critical points occur when x=yx=y.
    At (0,0)(0,0):
    fxx=2f_{xx} = 2, fyy=2f_{yy} = 2, fxy=2f_{xy} = -2.
    D=(2)(2)(2)2=44=0D = (2)(2) - (-2)^2 = 4 - 4 = 0. The test is inconclusive. However, since f(x,y)=(xy)20f(x,y) = (x-y)^2 \ge 0 and f(0,0)=0f(0,0)=0, (0,0)(0,0) is a local minimum.

    Option 4: f(x,y)=x2y2+3xyf(x, y) = x^2 - y^2 + 3xy
    fx=2x+3yf_x = 2x + 3y, fy=2y+3xf_y = -2y + 3x.
    Setting to zero:

    2x+3y=0    y=23x3x2y=0    3x2(23x)=0    3x+43x=0    133x=0    x=0\begin{aligned}2x + 3y & = 0 \implies y = -\frac{2}{3}x \\
    3x - 2y & = 0 \implies 3x - 2\left(-\frac{2}{3}x\right) = 0 \implies 3x + \frac{4}{3}x = 0 \implies \frac{13}{3}x = 0 \implies x = 0\end{aligned}

    Then y=0y = 0. Critical point: (0,0)(0,0).
    fxx=2f_{xx} = 2, fyy=2f_{yy} = -2, fxy=3f_{xy} = 3.
    D=(2)(2)(3)2=49=13D = (2)(-2) - (3)^2 = -4 - 9 = -13.
    Since D<0D < 0, (0,0)(0,0) is a saddle point.

    Thus, f(x,y)=x2y2+3xyf(x, y) = x^2 - y^2 + 3xy has a saddle point at (0,0)(0, 0).
    Answer: \boxed{f(x, y) = x^2 - y^2 + 3xy}"
    :::

    ---

    4. Inconclusive Cases (D=0D=0)

    When the discriminant D(a,b)=0D(a, b) = 0, the Second Derivative Test provides no information about the nature of the critical point. In such cases, we must resort to other methods, such as direct analysis of the function's behavior near the critical point. This often involves examining the sign of f(x,y)f(a,b)f(x, y) - f(a, b) in an open disk around (a,b)(a, b), or by restricting the function to various paths passing through (a,b)(a, b).

    Quick Example:
    Consider f(x,y)=x4+y4f(x, y) = x^4 + y^4. Classify the critical point (0,0)(0, 0).

    Step 1: Find critical points.

    fx=4x3=0    x=0fy=4y3=0    y=0\begin{aligned}f_x & = 4x^3 = 0 \implies x = 0 \\
    f_y & = 4y^3 = 0 \implies y = 0\end{aligned}

    The critical point is (0,0)(0, 0).

    Step 2: Compute second partial derivatives.

    fxx=12x2fyy=12y2fxy=0\begin{aligned}f_{xx} & = 12x^2 \\
    f_{yy} & = 12y^2 \\
    f_{xy} & = 0\end{aligned}

    Step 3: Calculate DD at (0,0)(0, 0).

    fxx(0,0)=0fyy(0,0)=0fxy(0,0)=0D(0,0)=(0)(0)(0)2=0\begin{aligned}f_{xx}(0, 0) & = 0 \\
    f_{yy}(0, 0) & = 0 \\
    f_{xy}(0, 0) & = 0 \\
    D(0, 0) & = (0)(0) - (0)^2 = 0\end{aligned}

    The test is inconclusive.

    Step 4: Direct analysis.
    We observe f(x,y)=x4+y4f(x, y) = x^4 + y^4. For any (x,y)(0,0)(x, y) \neq (0, 0), x40x^4 \ge 0 and y40y^4 \ge 0, so x4+y4>0x^4 + y^4 > 0.
    Also, f(0,0)=04+04=0f(0, 0) = 0^4 + 0^4 = 0.
    Since f(x,y)f(0,0)f(x, y) \ge f(0, 0) for all (x,y)(x, y), the function has a local minimum at (0,0)(0, 0).

    Answer: Local minimum at (0,0)(0, 0).

    :::question type="MCQ" question="For f(x,y)=x2+xy2+y4f(x, y) = x^2 + xy^2 + y^4, what is the nature of the critical point at (0,0)(0,0)?" options=["Local Maximum","Local Minimum","Saddle Point","Inconclusive by Second Derivative Test, but a Local Minimum by direct analysis"] answer="Inconclusive by Second Derivative Test, but a Local Minimum by direct analysis" hint="Calculate the discriminant DD. If D=0D=0, analyze the function's behavior directly around the origin." solution="Step 1: Find critical points.

    fx=2x+y2=0fy=2xy+4y3=2y(x+2y2)=0\begin{aligned}f_x & = 2x + y^2 = 0 \\
    f_y & = 2xy + 4y^3 = 2y(x + 2y^2) = 0\end{aligned}

    From 2y(x+2y2)=02y(x + 2y^2) = 0, either y=0y = 0 or x+2y2=0x + 2y^2 = 0.
    If y=0y = 0, then 2x+02=0    x=02x + 0^2 = 0 \implies x = 0. So (0,0)(0,0) is a critical point.
    If x+2y2=0x + 2y^2 = 0, then x=2y2x = -2y^2. Substitute into 2x+y2=02x + y^2 = 0:
    2(2y2)+y2=0    4y2+y2=0    3y2=0    y=02(-2y^2) + y^2 = 0 \implies -4y^2 + y^2 = 0 \implies -3y^2 = 0 \implies y = 0

    If y=0y=0, then x=0x=0. So (0,0)(0,0) is the only critical point.

    Step 2: Compute second partial derivatives.

    fxx=2fyy=2x+12y2fxy=2y\begin{aligned}f_{xx} & = 2 \\
    f_{yy} & = 2x + 12y^2 \\
    f_{xy} & = 2y\end{aligned}

    Step 3: Calculate DD at (0,0)(0, 0).

    fxx(0,0)=2fyy(0,0)=2(0)+12(0)2=0fxy(0,0)=2(0)=0D(0,0)=fxx(0,0)fyy(0,0)[fxy(0,0)]2=(2)(0)(0)2=0\begin{aligned}f_{xx}(0, 0) & = 2 \\
    f_{yy}(0, 0) & = 2(0) + 12(0)^2 = 0 \\
    f_{xy}(0, 0) & = 2(0) = 0 \\
    D(0, 0) & = f_{xx}(0, 0)f_{yy}(0, 0) - [f_{xy}(0, 0)]^2 = (2)(0) - (0)^2 = 0\end{aligned}

    The Second Derivative Test is inconclusive.

    Step 4: Direct analysis.
    We examine f(x,y)=x2+xy2+y4f(x, y) = x^2 + xy^2 + y^4 around (0,0)(0, 0).
    We can rewrite f(x,y)f(x, y) by completing the square for the xx terms:

    f(x,y)=x2+xy2+y4=(x+y22)2(y22)2+y4f(x,y)=(x+y22)2y44+y4f(x,y)=(x+y22)2+34y4\begin{aligned}f(x, y) & = x^2 + xy^2 + y^4 = \left(x + \frac{y^2}{2}\right)^2 - \left(\frac{y^2}{2}\right)^2 + y^4 \\
    f(x, y) & = \left(x + \frac{y^2}{2}\right)^2 - \frac{y^4}{4} + y^4 \\
    f(x, y) & = \left(x + \frac{y^2}{2}\right)^2 + \frac{3}{4}y^4\end{aligned}

    Since (x+y22)20\left(x + \frac{y^2}{2}\right)^2 \ge 0 and 34y40\frac{3}{4}y^4 \ge 0 for all real x,yx, y, we have f(x,y)0f(x, y) \ge 0.
    Also, f(0,0)=0f(0, 0) = 0.
    Therefore, f(x,y)f(0,0)f(x, y) \ge f(0, 0) for all (x,y)(x, y), implying that (0,0)(0, 0) is a local minimum.
    Answer: \boxed{\text{Local Minimum}}"
    :::

    ---

    5. Absolute Extrema on Bounded Closed Regions

    For a continuous function f(x,y)f(x, y) defined on a closed and bounded region RR in R2\mathbb{R}^2, the Extreme Value Theorem guarantees that ff attains both an absolute maximum and an absolute minimum on RR. These extrema can occur either at critical points within the interior of RR or at points on the boundary of RR.

    The procedure to find absolute extrema involves:

  • Finding all critical points of ff in the interior of RR.

  • Finding the extreme values of ff on the boundary of RR. This often reduces to a single-variable optimization problem or several such problems, depending on the boundary's shape.

  • Comparing the values of ff at all points found in steps 1 and 2. The largest value is the absolute maximum, and the smallest is the absolute minimum.
  • Quick Example:
    Find the absolute maximum and minimum of f(x,y)=x2+y22x2yf(x, y) = x^2 + y^2 - 2x - 2y on the square region R={(x,y):0x2,0y2}R = \{(x, y) : 0 \le x \le 2, 0 \le y \le 2\}.

    Step 1: Find critical points in the interior of RR.

    fx=2x2=0    x=1fy=2y2=0    y=1\begin{aligned}f_x & = 2x - 2 = 0 \implies x = 1 \\
    f_y & = 2y - 2 = 0 \implies y = 1\end{aligned}

    The critical point is (1,1)(1, 1). This point is in the interior of RR.
    f(1,1)=12+122(1)2(1)=1+122=2f(1, 1) = 1^2 + 1^2 - 2(1) - 2(1) = 1 + 1 - 2 - 2 = -2.

    Step 2: Analyze the boundary.
    The boundary consists of four line segments:
    * Segment 1 (Bottom edge): y=0y = 0, 0x20 \le x \le 2.
    g1(x)=f(x,0)=x22xg_1(x) = f(x, 0) = x^2 - 2x.
    g1(x)=2x2=0    x=1g_1'(x) = 2x - 2 = 0 \implies x = 1.
    Points to check: (0,0)(0, 0), (2,0)(2, 0), and (1,0)(1, 0).
    f(0,0)=0f(0, 0) = 0, f(2,0)=0f(2, 0) = 0, f(1,0)=12=1f(1, 0) = 1 - 2 = -1.
    * Segment 2 (Top edge): y=2y = 2, 0x20 \le x \le 2.
    g2(x)=f(x,2)=x2+222x2(2)=x22xg_2(x) = f(x, 2) = x^2 + 2^2 - 2x - 2(2) = x^2 - 2x.
    g2(x)=2x2=0    x=1g_2'(x) = 2x - 2 = 0 \implies x = 1.
    Points to check: (0,2)(0, 2), (2,2)(2, 2), and (1,2)(1, 2).
    f(0,2)=0+404=0f(0, 2) = 0 + 4 - 0 - 4 = 0, f(2,2)=4+444=0f(2, 2) = 4 + 4 - 4 - 4 = 0, f(1,2)=1+424=1f(1, 2) = 1 + 4 - 2 - 4 = -1.
    * Segment 3 (Left edge): x=0x = 0, 0y20 \le y \le 2.
    g3(y)=f(0,y)=y22yg_3(y) = f(0, y) = y^2 - 2y.
    g3(y)=2y2=0    y=1g_3'(y) = 2y - 2 = 0 \implies y = 1.
    Points to check: (0,0)(0, 0) (already checked), (0,2)(0, 2) (already checked), and (0,1)(0, 1).
    f(0,1)=0+102=1f(0, 1) = 0 + 1 - 0 - 2 = -1.
    * Segment 4 (Right edge): x=2x = 2, 0y20 \le y \le 2.
    g4(y)=f(2,y)=22+y22(2)2y=y22yg_4(y) = f(2, y) = 2^2 + y^2 - 2(2) - 2y = y^2 - 2y.
    g4(y)=2y2=0    y=1g_4'(y) = 2y - 2 = 0 \implies y = 1.
    Points to check: (2,0)(2, 0) (already checked), (2,2)(2, 2) (already checked), and (2,1)(2, 1).
    f(2,1)=4+142=1f(2, 1) = 4 + 1 - 4 - 2 = -1.

    Step 3: Compare all values.
    Values obtained: 2-2 (from critical point), 00, 1-1.
    The maximum value is 00, and the minimum value is 2-2.

    Answer: Absolute maximum is 00, absolute minimum is 2-2.

    :::question type="MCQ" question="Find the absolute maximum value of f(x,y)=x2+y2xf(x, y) = x^2 + y^2 - x on the disk x2+y21x^2 + y^2 \le 1." options=["00","11","22","33"] answer="22" hint="Check critical points in the interior and analyze the boundary using parametrization or substitution." solution="Step 1: Find critical points in the interior (x2+y2<1x^2 + y^2 < 1).

    fx=2x1=0    x=1/2fy=2y=0    y=0\begin{aligned}f_x & = 2x - 1 = 0 \implies x = 1/2 \\
    f_y & = 2y = 0 \implies y = 0\end{aligned}

    The critical point is (1/2,0)(1/2, 0).
    Since (1/2)2+02=1/4<1(1/2)^2 + 0^2 = 1/4 < 1, this point is in the interior.
    The value of ff at this point is f(1/2,0)=(1/2)2+021/2=1/41/2=1/4f(1/2, 0) = (1/2)^2 + 0^2 - 1/2 = 1/4 - 1/2 = -1/4.

    Step 2: Analyze the boundary (x2+y2=1x^2 + y^2 = 1).
    On the boundary, x2+y2=1x^2 + y^2 = 1. We can substitute this into f(x,y)f(x, y):

    f(x,y)=(x2+y2)x=1xf(x, y) = (x^2 + y^2) - x = 1 - x

    We need to find the extrema of g(x)=1xg(x) = 1 - x subject to x2+y2=1x^2 + y^2 = 1. Since x2=1y2x^2 = 1 - y^2, we know that 1x1-1 \le x \le 1.
    The function g(x)=1xg(x) = 1 - x is a decreasing function.
    Its maximum value on [1,1][-1, 1] occurs at x=1x = -1, giving g(1)=1(1)=2g(-1) = 1 - (-1) = 2.
    Its minimum value on [1,1][-1, 1] occurs at x=1x = 1, giving g(1)=11=0g(1) = 1 - 1 = 0.
    These correspond to the points (1,0)(-1, 0) and (1,0)(1, 0) on the boundary.
    f(1,0)=(1)2+02(1)=1+1=2f(-1, 0) = (-1)^2 + 0^2 - (-1) = 1 + 1 = 2.
    f(1,0)=12+021=0f(1, 0) = 1^2 + 0^2 - 1 = 0.

    Step 3: Compare all values.
    Values obtained: 1/4-1/4, 22, 00.
    The absolute maximum value is 22.
    Answer: \boxed{2}"
    :::

    ---

    6. Lagrange Multipliers

    We employ the method of Lagrange Multipliers to find the maximum or minimum values of a function f(x,y)f(x, y) subject to a constraint g(x,y)=kg(x, y) = k. This method is particularly useful for optimization problems where direct substitution of the constraint into the objective function is difficult or impossible.

    📐 Lagrange Multiplier Method

    To find the extrema of f(x,y)f(x, y) subject to the constraint g(x,y)=kg(x, y) = k, we solve the system of equations:

    • f(x,y)=λg(x,y)\nabla f(x, y) = \lambda \nabla g(x, y)

    • g(x,y)=kg(x, y) = k

    This expands to:

    fx=λgx\frac{\partial f}{\partial x} = \lambda \frac{\partial g}{\partial x}

    fy=λgy\frac{\partial f}{\partial y} = \lambda \frac{\partial g}{\partial y}

    g(x,y)=kg(x, y) = k

    We solve this system for x,y,x, y, and λ\lambda. The points (x,y)(x, y) obtained are the candidate points for extrema. We then evaluate f(x,y)f(x, y) at these candidate points to find the maximum and minimum values.

    Where: f\nabla f is the gradient of ff, g\nabla g is the gradient of gg, λ\lambda is the Lagrange multiplier.
    When to use: To find extrema of a function subject to an equality constraint.

    Quick Example:
    Find the maximum value of f(x,y)=xyf(x, y) = xy subject to the constraint x2+y2=1x^2 + y^2 = 1.

    Step 1: Set up the Lagrange multiplier equations.
    Let g(x,y)=x2+y2g(x, y) = x^2 + y^2.

    f=y,x\nabla f = \langle y, x \rangle

    g=2x,2y\nabla g = \langle 2x, 2y \rangle

    The system of equations is:
    y=λ(2x)(1)y = \lambda (2x) \quad (1)

    x=λ(2y)(2)x = \lambda (2y) \quad (2)

    x2+y2=1(3)x^2 + y^2 = 1 \quad (3)

    Step 2: Solve the system.
    From (1), λ=y2x\lambda = \frac{y}{2x} (assuming x0x \neq 0).
    From (2), λ=x2y\lambda = \frac{x}{2y} (assuming y0y \neq 0).
    Equating the expressions for λ\lambda:

    y2x=x2y\frac{y}{2x} = \frac{x}{2y}

    2y2=2x2    y2=x2    y=±x2y^2 = 2x^2 \implies y^2 = x^2 \implies y = \pm x

    Substitute y=±xy = \pm x into (3):
    x2+(±x)2=1x^2 + (\pm x)^2 = 1

    2x2=1    x2=12    x=±122x^2 = 1 \implies x^2 = \frac{1}{2} \implies x = \pm \frac{1}{\sqrt{2}}

    If x=12x = \frac{1}{\sqrt{2}}, then y=±12y = \pm \frac{1}{\sqrt{2}}. Points: (12,12)\left(\frac{1}{\sqrt{2}}, \frac{1}{\sqrt{2}}\right) and (12,12)\left(\frac{1}{\sqrt{2}}, -\frac{1}{\sqrt{2}}\right).
    If x=12x = -\frac{1}{\sqrt{2}}, then y=±12y = \pm \frac{1}{\sqrt{2}}. Points: (12,12)\left(-\frac{1}{\sqrt{2}}, \frac{1}{\sqrt{2}}\right) and (12,12)\left(-\frac{1}{\sqrt{2}}, -\frac{1}{\sqrt{2}}\right).

    Step 3: Evaluate f(x,y)f(x, y) at the candidate points.

    f(12,12)=1212=12f\left(\frac{1}{\sqrt{2}}, \frac{1}{\sqrt{2}}\right) = \frac{1}{\sqrt{2}} \cdot \frac{1}{\sqrt{2}} = \frac{1}{2}

    f(12,12)=12(12)=12f\left(\frac{1}{\sqrt{2}}, -\frac{1}{\sqrt{2}}\right) = \frac{1}{\sqrt{2}} \cdot \left(-\frac{1}{\sqrt{2}}\right) = -\frac{1}{2}

    f(12,12)=(12)12=12f\left(-\frac{1}{\sqrt{2}}, \frac{1}{\sqrt{2}}\right) = \left(-\frac{1}{\sqrt{2}}\right) \cdot \frac{1}{\sqrt{2}} = -\frac{1}{2}

    f(12,12)=(12)(12)=12f\left(-\frac{1}{\sqrt{2}}, -\frac{1}{\sqrt{2}}\right) = \left(-\frac{1}{\sqrt{2}}\right) \cdot \left(-\frac{1}{\sqrt{2}}\right) = \frac{1}{2}

    Answer: The maximum value is 1/21/2. (The minimum value is 1/2-1/2).

    :::question type="MCQ" question="The minimum distance of the point (3,4,12)(3, 4, 12) from the sphere x2+y2+z2=1x^2 + y^2 + z^2 = 1 is:" options=["1414","1616","1212","1010"] answer="1212" hint="The distance from the origin to the point (3,4,12)(3,4,12) is 32+42+122\sqrt{3^2+4^2+12^2}. The sphere has radius 11. The minimum distance is the distance from the point to the center of the sphere minus the radius." solution="We seek the minimum distance from P(3,4,12)P(3, 4, 12) to the sphere S:x2+y2+z2=1S: x^2 + y^2 + z^2 = 1. The sphere is centered at the origin (0,0,0)(0, 0, 0) with radius r=1r = 1.

    Step 1: Calculate the distance from the origin (center of the sphere) to the point P(3,4,12)P(3, 4, 12).
    Let O=(0,0,0)O = (0, 0, 0). The distance OPOP is:

    OP=(30)2+(40)2+(120)2OP = \sqrt{(3-0)^2 + (4-0)^2 + (12-0)^2}

    OP=32+42+122OP = \sqrt{3^2 + 4^2 + 12^2}

    OP=9+16+144OP = \sqrt{9 + 16 + 144}

    OP=169OP = \sqrt{169}

    OP=13OP = 13

    Step 2: Determine the minimum distance to the sphere.
    The point PP is outside the sphere since its distance from the origin (1313) is greater than the radius (11).
    The minimum distance from PP to the sphere is the distance from PP to the center of the sphere, minus the radius of the sphere.

    Minimum distance=OPr\text{Minimum distance} = OP - r

    Minimum distance=131\text{Minimum distance} = 13 - 1

    Minimum distance=12\text{Minimum distance} = 12

    Alternatively, using Lagrange Multipliers (more general but overkill for this geometric problem):
    Minimize f(x,y,z)=(x3)2+(y4)2+(z12)2f(x,y,z) = \sqrt{(x-3)^2 + (y-4)^2 + (z-12)^2} subject to g(x,y,z)=x2+y2+z2=1g(x,y,z) = x^2+y^2+z^2 = 1.
    Minimizing the distance is equivalent to minimizing the square of the distance:
    Minimize F(x,y,z)=(x3)2+(y4)2+(z12)2F(x,y,z) = (x-3)^2 + (y-4)^2 + (z-12)^2.
    F=2(x3),2(y4),2(z12)\nabla F = \langle 2(x-3), 2(y-4), 2(z-12) \rangle
    g=2x,2y,2z\nabla g = \langle 2x, 2y, 2z \rangle
    Lagrange equations:

    2(x3)=λ(2x)    x3=λx    x(1λ)=3    x=31λ2(x-3) = \lambda (2x) \implies x-3 = \lambda x \implies x(1-\lambda) = 3 \implies x = \frac{3}{1-\lambda}

    2(y4)=λ(2y)    y4=λy    y(1λ)=4    y=41λ2(y-4) = \lambda (2y) \implies y-4 = \lambda y \implies y(1-\lambda) = 4 \implies y = \frac{4}{1-\lambda}

    2(z12)=λ(2z)    z12=λz    z(1λ)=12    z=121λ2(z-12) = \lambda (2z) \implies z-12 = \lambda z \implies z(1-\lambda) = 12 \implies z = \frac{12}{1-\lambda}

    Substitute into x2+y2+z2=1x^2+y^2+z^2=1:
    (31λ)2+(41λ)2+(121λ)2=1\left(\frac{3}{1-\lambda}\right)^2 + \left(\frac{4}{1-\lambda}\right)^2 + \left(\frac{12}{1-\lambda}\right)^2 = 1

    9+16+144(1λ)2=1    169(1λ)2=1    (1λ)2=169    1λ=±13\frac{9+16+144}{(1-\lambda)^2} = 1 \implies \frac{169}{(1-\lambda)^2} = 1 \implies (1-\lambda)^2 = 169 \implies 1-\lambda = \pm 13

    Case 1: 1λ=13    λ=121-\lambda = 13 \implies \lambda = -12.
    x=3/13,y=4/13,z=12/13x = 3/13, y = 4/13, z = 12/13. This point is on the sphere.
    Distance=(3133)2+(4134)2+(121312)2=(3613)2+(4813)2+(14413)2=113362+482+1442=1131296+2304+20736=11324336=15613=12\begin{aligned}\text{Distance} & = \sqrt{\left(\frac{3}{13}-3\right)^2 + \left(\frac{4}{13}-4\right)^2 + \left(\frac{12}{13}-12\right)^2} \\
    & = \sqrt{\left(\frac{-36}{13}\right)^2 + \left(\frac{-48}{13}\right)^2 + \left(\frac{-144}{13}\right)^2} \\
    & = \frac{1}{13}\sqrt{36^2+48^2+144^2} \\
    & = \frac{1}{13}\sqrt{1296+2304+20736} \\
    & = \frac{1}{13}\sqrt{24336} \\
    & = \frac{156}{13} = 12\end{aligned}

    Case 2: 1λ=13    λ=141-\lambda = -13 \implies \lambda = 14.
    x=3/13,y=4/13,z=12/13x = -3/13, y = -4/13, z = -12/13. This point is on the sphere.
    Distance=(3133)2+(4134)2+(121312)2=(4213)2+(5613)2+(16813)2=113422+562+1682=1131764+3136+28224=11333124=18213=14\begin{aligned}\text{Distance} & = \sqrt{\left(-\frac{3}{13}-3\right)^2 + \left(-\frac{4}{13}-4\right)^2 + \left(-\frac{12}{13}-12\right)^2} \\
    & = \sqrt{\left(\frac{-42}{13}\right)^2 + \left(\frac{-56}{13}\right)^2 + \left(\frac{-168}{13}\right)^2} \\
    & = \frac{1}{13}\sqrt{42^2+56^2+168^2} \\
    & = \frac{1}{13}\sqrt{1764+3136+28224} \\
    & = \frac{1}{13}\sqrt{33124} \\
    & = \frac{182}{13} = 14\end{aligned}

    The minimum distance is 1212.
    Answer: \boxed{12}"
    :::

    ---

    Advanced Applications

    Example: Find the maximum and minimum values of f(x,y)=exyf(x, y) = e^{-xy} on the region x2+4y21x^2 + 4y^2 \le 1.

    This involves finding critical points within the interior and then using Lagrange multipliers for the boundary.

    Step 1: Find critical points in the interior (x2+4y2<1x^2 + 4y^2 < 1).

    fx=yexy=0f_x = -y e^{-xy} = 0

    fy=xexy=0f_y = -x e^{-xy} = 0

    Since exye^{-xy} is never zero, we must have y=0y = 0 and x=0x = 0.
    The only critical point is (0,0)(0, 0).
    f(0,0)=e0=1f(0, 0) = e^0 = 1.

    Step 2: Analyze the boundary (x2+4y2=1x^2 + 4y^2 = 1).
    We use Lagrange Multipliers with g(x,y)=x2+4y2=1g(x, y) = x^2 + 4y^2 = 1.

    f=yexy,xexy\nabla f = \langle -y e^{-xy}, -x e^{-xy} \rangle

    g=2x,8y\nabla g = \langle 2x, 8y \rangle

    The Lagrange equations are:
    yexy=λ(2x)(1)-y e^{-xy} = \lambda (2x) \quad (1)

    xexy=λ(8y)(2)-x e^{-xy} = \lambda (8y) \quad (2)

    x2+4y2=1(3)x^2 + 4y^2 = 1 \quad (3)

    From (1) and (2), assuming exy0e^{-xy} \neq 0 and x,y0x, y \neq 0:

    λ=yexy2x=xexy8y\lambda = \frac{-y e^{-xy}}{2x} = \frac{-x e^{-xy}}{8y}

    y2x=x8y\frac{-y}{2x} = \frac{-x}{8y}

    8y2=2x2    4y2=x2-8y^2 = -2x^2 \implies 4y^2 = x^2

    Substitute x2=4y2x^2 = 4y^2 into (3):
    4y2+4y2=1    8y2=1    y2=18    y=±1224y^2 + 4y^2 = 1 \implies 8y^2 = 1 \implies y^2 = \frac{1}{8} \implies y = \pm \frac{1}{2\sqrt{2}}

    If y2=1/8y^2 = 1/8, then x2=4(1/8)=1/2    x=±12x^2 = 4(1/8) = 1/2 \implies x = \pm \frac{1}{\sqrt{2}}.
    This gives four candidate points:
    (12,122)\left(\frac{1}{\sqrt{2}}, \frac{1}{2\sqrt{2}}\right), (12,122)\left(\frac{1}{\sqrt{2}}, -\frac{1}{2\sqrt{2}}\right), (12,122)\left(-\frac{1}{\sqrt{2}}, \frac{1}{2\sqrt{2}}\right), (12,122)\left(-\frac{1}{\sqrt{2}}, -\frac{1}{2\sqrt{2}}\right).

    Step 3: Evaluate f(x,y)f(x, y) at these points.
    For (12,122)\left(\frac{1}{\sqrt{2}}, \frac{1}{2\sqrt{2}}\right), xy=12122=14xy = \frac{1}{\sqrt{2}} \cdot \frac{1}{2\sqrt{2}} = \frac{1}{4}. So f=e1/4f = e^{-1/4}.
    For (12,122)\left(\frac{1}{\sqrt{2}}, -\frac{1}{2\sqrt{2}}\right), xy=12(122)=14xy = \frac{1}{\sqrt{2}} \cdot \left(-\frac{1}{2\sqrt{2}}\right) = -\frac{1}{4}. So f=e1/4f = e^{1/4}.
    For (12,122)\left(-\frac{1}{\sqrt{2}}, \frac{1}{2\sqrt{2}}\right), xy=(12)122=14xy = \left(-\frac{1}{\sqrt{2}}\right) \cdot \frac{1}{2\sqrt{2}} = -\frac{1}{4}. So f=e1/4f = e^{1/4}.
    For (12,122)\left(-\frac{1}{\sqrt{2}}, -\frac{1}{2\sqrt{2}}\right), xy=(12)(122)=14xy = \left(-\frac{1}{\sqrt{2}}\right) \cdot \left(-\frac{1}{2\sqrt{2}}\right) = \frac{1}{4}. So f=e1/4f = e^{-1/4}.

    Step 4: Compare all values.
    Values are 11, e1/4e^{-1/4}, e1/4e^{1/4}.
    Since e2.718e \approx 2.718, e1/41.284e^{1/4} \approx 1.284, e1/40.778e^{-1/4} \approx 0.778.
    The maximum value is e1/4e^{1/4}, and the minimum value is e1/4e^{-1/4}.

    Answer: Absolute maximum is e1/4e^{1/4}, absolute minimum is e1/4e^{-1/4}.

    :::question type="NAT" question="A rectangular box without a lid is to be made from 12m212 \operatorname{m}^2 of cardboard. Find the maximum volume of such a box (in m3\operatorname{m}^3). Round your answer to two decimal places." answer="4.00" hint="Define the volume function V(x,y,z)V(x,y,z) and the surface area constraint S(x,y,z)S(x,y,z). Use Lagrange multipliers to maximize VV subject to S=12S=12. Remember there is no lid." solution="Let the dimensions of the rectangular box be x,y,zx, y, z.
    The volume is V=xyzV = xyz.
    The surface area without a lid is S=xy+2xz+2yzS = xy + 2xz + 2yz.
    We want to maximize V(x,y,z)=xyzV(x, y, z) = xyz subject to the constraint g(x,y,z)=xy+2xz+2yz=12g(x, y, z) = xy + 2xz + 2yz = 12.

    Step 1: Set up the Lagrange multiplier equations.

    V=yz,xz,xy\nabla V = \langle yz, xz, xy \rangle

    g=y+2z,x+2z,2x+2y\nabla g = \langle y + 2z, x + 2z, 2x + 2y \rangle

    The system of equations is:
    yz=λ(y+2z)(1)yz = \lambda (y + 2z) \quad (1)

    xz=λ(x+2z)(2)xz = \lambda (x + 2z) \quad (2)

    xy=λ(2x+2y)(3)xy = \lambda (2x + 2y) \quad (3)

    xy+2xz+2yz=12(4)xy + 2xz + 2yz = 12 \quad (4)

    Step 2: Solve the system.
    From (1) and (2):
    Multiply (1) by xx: xyz=λ(xy+2xz)xyz = \lambda (xy + 2xz)
    Multiply (2) by yy: xyz=λ(xy+2yz)xyz = \lambda (xy + 2yz)
    Thus, λ(xy+2xz)=λ(xy+2yz)\lambda (xy + 2xz) = \lambda (xy + 2yz).
    Assuming λ0\lambda \neq 0 (if λ=0\lambda = 0, then yz=0,xz=0,xy=0yz=0, xz=0, xy=0, which implies V=0V=0, not a maximum), we have:

    xy+2xz=xy+2yz    2xz=2yz    xz=yzxy + 2xz = xy + 2yz \implies 2xz = 2yz \implies xz = yz

    Since z0z \neq 0 for a positive volume, we must have x=yx = y.

    Substitute x=yx = y into the equations:
    (1) becomes xz=λ(x+2z)xz = \lambda (x + 2z)
    (3) becomes x2=λ(2x+2x)=λ(4x)x^2 = \lambda (2x + 2x) = \lambda (4x)
    Since x0x \neq 0, we can divide by xx:

    x=4λ    λ=x4x = 4\lambda \implies \lambda = \frac{x}{4}

    Substitute λ=x/4\lambda = x/4 into the modified (1):

    xz=x4(x+2z)xz = \frac{x}{4} (x + 2z)

    Since x0x \neq 0, we can divide by xx:
    z=14(x+2z)z = \frac{1}{4} (x + 2z)

    4z=x+2z4z = x + 2z

    2z=x2z = x

    So, we have the relations x=yx = y and x=2zx = 2z. This implies y=2zy = 2z.

    Step 3: Substitute the relations into the constraint equation (4).

    xy+2xz+2yz=12xy + 2xz + 2yz = 12

    Substitute y=xy = x and z=x/2z = x/2:
    x(x)+2x(x/2)+2x(x/2)=12x(x) + 2x(x/2) + 2x(x/2) = 12

    x2+x2+x2=12x^2 + x^2 + x^2 = 12

    3x2=123x^2 = 12

    x2=4    x=2(since x>0)x^2 = 4 \implies x = 2 \quad (\text{since } x > 0)

    Step 4: Find the dimensions and the maximum volume.

    x=2x = 2

    y=x=2y = x = 2

    z=x/2=2/2=1z = x/2 = 2/2 = 1

    The dimensions are 2m×2m×1m2 \operatorname{m} \times 2 \operatorname{m} \times 1 \operatorname{m}.
    The maximum volume is V=xyz=(2)(2)(1)=4m3V = xyz = (2)(2)(1) = 4 \operatorname{m}^3.

    The value is 4.004.00 when rounded to two decimal places.
    Answer: \boxed{4.00}"
    :::

    ---

    Problem-Solving Strategies

    💡 CUET PG Strategy: Critical Point Classification

    When faced with a critical point where D=0D=0 in the Second Derivative Test, do not immediately assume it is a saddle point or an extremum. Instead, analyze the function's behavior directly. Consider paths approaching the critical point (e.g., y=mxy=mx, y=x2y=x^2) or try to rewrite the function (e.g., completing the square) to determine if f(x,y)f(a,b)f(x,y) - f(a,b) maintains a consistent sign in a neighborhood.

    💡 CUET PG Strategy: Distance Problems

    For distance minimization problems involving spheres or other simple geometric shapes, first check for a direct geometric solution. For example, the minimum distance from a point to a sphere is often simply the distance from the point to the sphere's center minus the radius (if the point is outside). This avoids complex Lagrange multiplier calculations. If a geometric approach isn't obvious, then resort to Lagrange multipliers, often minimizing the square of the distance to simplify derivatives.

    ---

    Common Mistakes

    ⚠️ Common Mistake: Forgetting Boundary Analysis

    ❌ Students often find critical points in the interior of a region but neglect to analyze the function's behavior on the boundary, especially for absolute extrema problems on bounded closed regions.
    ✅ Always evaluate the function at interior critical points AND systematically analyze the function along all segments of the boundary. The absolute extrema can occur anywhere in the region, including its boundary.

    ⚠️ Common Mistake: Incorrect D=0D=0 Interpretation

    ❌ Interpreting D=0D=0 as automatically meaning a saddle point or no extremum.
    D=0D=0 means the test is inconclusive. The critical point could be a local maximum, local minimum, or a saddle point. Further analysis is required.

    ⚠️ Common Mistake: Algebraic Errors in Lagrange Multipliers

    ❌ Incorrectly solving the system of equations for Lagrange multipliers, especially when dividing by variables without considering cases where they might be zero.
    ✅ Be meticulous in solving the system. If dividing by a variable (e.g., xx), consider the case where that variable is zero separately. This might lead to additional critical points or simplify the problem.

    ---

    Practice Questions

    :::question type="MCQ" question="For the function f(x,y)=x3+y33xyf(x, y) = x^3 + y^3 - 3xy, which of the following statements is correct regarding its critical points?" options=["It has a local maximum at (0,0)(0,0) and a local minimum at (1,1)(1,1)","It has a saddle point at (0,0)(0,0) and a local minimum at (1,1)(1,1)","It has a local maximum at (0,0)(0,0) and a saddle point at (1,1)(1,1)","It has a saddle point at (0,0)(0,0) and a local maximum at (1,1)(1,1)"] answer="It has a saddle point at (0,0)(0,0) and a local minimum at (1,1)(1,1)" hint="Find critical points, then apply the Second Derivative Test to each." solution="Step 1: Find critical points.

    fx=3x23y=0    y=x2(A)f_x = 3x^2 - 3y = 0 \implies y = x^2 \quad (A)

    fy=3y23x=0    x=y2(B)f_y = 3y^2 - 3x = 0 \implies x = y^2 \quad (B)

    Substitute (A) into (B):
    x=(x2)2    x=x4x = (x^2)^2 \implies x = x^4

    x4x=0    x(x31)=0x^4 - x = 0 \implies x(x^3 - 1) = 0

    So x=0x = 0 or x3=1    x=1x^3 = 1 \implies x = 1.
    If x=0x = 0, then from (A), y=02=0y = 0^2 = 0. Critical point: (0,0)(0, 0).
    If x=1x = 1, then from (A), y=12=1y = 1^2 = 1. Critical point: (1,1)(1, 1).

    Step 2: Compute second partial derivatives.

    fxx=6xf_{xx} = 6x

    fyy=6yf_{yy} = 6y

    fxy=3f_{xy} = -3

    Step 3: Apply the Second Derivative Test for (0,0)(0, 0).

    fxx(0,0)=0f_{xx}(0, 0) = 0

    fyy(0,0)=0f_{yy}(0, 0) = 0

    fxy(0,0)=3f_{xy}(0, 0) = -3

    D(0,0)=(0)(0)(3)2=9D(0, 0) = (0)(0) - (-3)^2 = -9

    Since D(0,0)<0D(0, 0) < 0, (0,0)(0, 0) is a saddle point.

    Step 4: Apply the Second Derivative Test for (1,1)(1, 1).

    fxx(1,1)=6(1)=6f_{xx}(1, 1) = 6(1) = 6

    fyy(1,1)=6(1)=6f_{yy}(1, 1) = 6(1) = 6

    fxy(1,1)=3f_{xy}(1, 1) = -3

    D(1,1)=(6)(6)(3)2=369=27D(1, 1) = (6)(6) - (-3)^2 = 36 - 9 = 27

    Since D(1,1)>0D(1, 1) > 0 and fxx(1,1)=6>0f_{xx}(1, 1) = 6 > 0, (1,1)(1, 1) is a local minimum.

    Therefore, the function has a saddle point at (0,0)(0,0) and a local minimum at (1,1)(1,1).
    Answer: \boxed{\text{It has a saddle point at }(0,0) \text{ and a local minimum at }(1,1)}}"
    :::

    :::question type="NAT" question="Find the maximum value of f(x,y)=2x+3yf(x, y) = 2x + 3y subject to the constraint x2+y2=13x^2 + y^2 = 13. Round your answer to one decimal place." answer="13.0" hint="Use Lagrange multipliers. Solve the system of equations f=λg\nabla f = \lambda \nabla g and g(x,y)=kg(x,y)=k." solution="Step 1: Set up the Lagrange multiplier equations.
    Let f(x,y)=2x+3yf(x, y) = 2x + 3y and g(x,y)=x2+y2=13g(x, y) = x^2 + y^2 = 13.

    f=2,3\nabla f = \langle 2, 3 \rangle

    g=2x,2y\nabla g = \langle 2x, 2y \rangle

    The system of equations is:
    2=λ(2x)    1=λx(1)2 = \lambda (2x) \implies 1 = \lambda x \quad (1)

    3=λ(2y)    32=λy(2)3 = \lambda (2y) \implies \frac{3}{2} = \lambda y \quad (2)

    x2+y2=13(3)x^2 + y^2 = 13 \quad (3)

    Step 2: Solve the system.
    From (1), x=1/λx = 1/\lambda (assuming λ0\lambda \neq 0).
    From (2), y=3/(2λ)y = 3/(2\lambda).
    Substitute these into (3):

    (1λ)2+(32λ)2=13\left(\frac{1}{\lambda}\right)^2 + \left(\frac{3}{2\lambda}\right)^2 = 13

    1λ2+94λ2=13\frac{1}{\lambda^2} + \frac{9}{4\lambda^2} = 13

    4+94λ2=13\frac{4 + 9}{4\lambda^2} = 13

    134λ2=13\frac{13}{4\lambda^2} = 13

    1=4λ2    λ2=14    λ=±121 = 4\lambda^2 \implies \lambda^2 = \frac{1}{4} \implies \lambda = \pm \frac{1}{2}

    Step 3: Find the candidate points (x,y)(x, y).
    Case 1: λ=1/2\lambda = 1/2.

    x=11/2=2x = \frac{1}{1/2} = 2

    y=32(1/2)=3y = \frac{3}{2(1/2)} = 3

    Candidate point: (2,3)(2, 3).
    Case 2: λ=1/2\lambda = -1/2.
    x=11/2=2x = \frac{1}{-1/2} = -2

    y=32(1/2)=3y = \frac{3}{2(-1/2)} = -3

    Candidate point: (2,3)(-2, -3).

    Step 4: Evaluate f(x,y)f(x, y) at the candidate points.

    f(2,3)=2(2)+3(3)=4+9=13f(2, 3) = 2(2) + 3(3) = 4 + 9 = 13

    f(2,3)=2(2)+3(3)=49=13f(-2, -3) = 2(-2) + 3(-3) = -4 - 9 = -13

    The maximum value is 1313.

    The answer rounded to one decimal place is 13.013.0.
    Answer: \boxed{13.0}"
    :::

    :::question type="MSQ" question="For the function f(x,y)=x4+y44xy+1f(x, y) = x^4 + y^4 - 4xy + 1, which of the following statements are correct?" options=["(0,0)(0,0) is a saddle point.","(1,1)(1,1) is a local minimum.","(1,1)(-1,-1) is a local minimum.","The function has no local maxima."] answer="(1,1)(1,1) is a local minimum.,(1,1)(-1,-1) is a local minimum.,The function has no local maxima." hint="Find critical points by setting first partial derivatives to zero. Use the Second Derivative Test to classify them." solution="Step 1: Find critical points.

    fx=4x34y=0    y=x3(A)f_x = 4x^3 - 4y = 0 \implies y = x^3 \quad (A)

    fy=4y34x=0    x=y3(B)f_y = 4y^3 - 4x = 0 \implies x = y^3 \quad (B)

    Substitute (A) into (B):
    x=(x3)3    x=x9x = (x^3)^3 \implies x = x^9

    x9x=0    x(x81)=0x^9 - x = 0 \implies x(x^8 - 1) = 0

    So x=0x = 0 or x8=1    x=±1x^8 = 1 \implies x = \pm 1.
    If x=0x = 0, then from (A), y=03=0y = 0^3 = 0. Critical point: (0,0)(0, 0).
    If x=1x = 1, then from (A), y=13=1y = 1^3 = 1. Critical point: (1,1)(1, 1).
    If x=1x = -1, then from (A), y=(1)3=1y = (-1)^3 = -1. Critical point: (1,1)(-1, -1).

    Step 2: Compute second partial derivatives.

    fxx=12x2f_{xx} = 12x^2

    fyy=12y2f_{yy} = 12y^2

    fxy=4f_{xy} = -4

    Step 3: Apply the Second Derivative Test for each critical point.

    For (0,0)(0, 0):

    fxx(0,0)=0f_{xx}(0, 0) = 0

    fyy(0,0)=0f_{yy}(0, 0) = 0

    fxy(0,0)=4f_{xy}(0, 0) = -4

    D(0,0)=(0)(0)(4)2=16D(0, 0) = (0)(0) - (-4)^2 = -16

    Since D(0,0)<0D(0, 0) < 0, (0,0)(0, 0) is a saddle point. So, ' (0,0)(0,0) is a saddle point. ' is correct.

    For (1,1)(1, 1):

    fxx(1,1)=12(1)2=12f_{xx}(1, 1) = 12(1)^2 = 12

    fyy(1,1)=12(1)2=12f_{yy}(1, 1) = 12(1)^2 = 12

    fxy(1,1)=4f_{xy}(1, 1) = -4

    D(1,1)=(12)(12)(4)2=14416=128D(1, 1) = (12)(12) - (-4)^2 = 144 - 16 = 128

    Since D(1,1)>0D(1, 1) > 0 and fxx(1,1)=12>0f_{xx}(1, 1) = 12 > 0, (1,1)(1, 1) is a local minimum. So, ' (1,1)(1,1) is a local minimum. ' is correct.

    For (1,1)(-1, -1):

    fxx(1,1)=12(1)2=12f_{xx}(-1, -1) = 12(-1)^2 = 12

    fyy(1,1)=12(1)2=12f_{yy}(-1, -1) = 12(-1)^2 = 12

    fxy(1,1)=4f_{xy}(-1, -1) = -4

    D(1,1)=(12)(12)(4)2=14416=128D(-1, -1) = (12)(12) - (-4)^2 = 144 - 16 = 128

    Since D(1,1)>0D(-1, -1) > 0 and fxx(1,1)=12>0f_{xx}(-1, -1) = 12 > 0, (1,1)(-1, -1) is a local minimum. So, ' (1,1)(-1,-1) is a local minimum. ' is correct.

    Overall conclusion: The function has two local minima and one saddle point. It has no local maxima. So, ' The function has no local maxima. ' is correct.

    The correct options are: (0,0)(0,0) is a saddle point.,(1,1)(1,1) is a local minimum.,(1,1)(-1,-1) is a local minimum.,The function has no local maxima.
    Answer: \boxed{\text{(1,1)(1,1) is a local minimum., (1,1)(-1,-1) is a local minimum., The function has no local maxima.}}"
    :::

    :::question type="MCQ" question="Consider f(x,y)=x2+2y2f(x,y) = x^2 + 2y^2. What is the behavior of ff along the path y=xy=x at the origin?" options=["Increases as xx increases from 00","Decreases as xx increases from 00","Remains constant","First decreases, then increases"] answer="Increases as xx increases from 00" hint="Substitute the path into the function and analyze the resulting single-variable function near the origin." solution="Step 1: Substitute the path y=xy=x into f(x,y)f(x,y).

    f(x,x)=x2+2(x)2=x2+2x2=3x2f(x, x) = x^2 + 2(x)^2 = x^2 + 2x^2 = 3x^2

    Step 2: Analyze the behavior of g(x)=3x2g(x) = 3x^2 near the origin.
    For x>0x > 0, 3x23x^2 increases as xx increases.
    For x<0x < 0, as xx increases towards 00 (e.g., from 1-1 to 0.1-0.1), 3x23x^2 decreases (e.g., 3(1)2=33(-1)^2=3, 3(0.1)2=0.033(-0.1)^2=0.03).
    The question asks about the behavior as xx increases from 00. This implies x>0x > 0.
    As xx increases from 00, 3x23x^2 increases.

    Step 3: The behavior of ff along y=xy=x at the origin.
    At (0,0)(0,0), f(0,0)=0f(0,0)=0. As xx increases from 00, f(x,x)=3x2f(x,x) = 3x^2 increases from 00.
    So, ff increases as xx increases from 00 along the path y=xy=x.
    Answer: \boxed{\text{Increases as } x \text{ increases from } 0}}"
    :::

    :::question type="MCQ" question="Given f(x,y)=sin(x)+cos(y)f(x, y) = \sin(x) + \cos(y), find the nature of the critical point (π/2,0)(\pi/2, 0)." options=["Local Maximum","Local Minimum","Saddle Point","Inconclusive"] answer="Local Maximum" hint="Find first and second partial derivatives. Apply the Second Derivative Test." solution="Step 1: Find critical points.

    fx=cos(x)f_x = \cos(x)

    fy=sin(y)f_y = -\sin(y)

    Set fx=0f_x = 0 and fy=0f_y = 0:
    cos(x)=0    x=π2+nπ\cos(x) = 0 \implies x = \frac{\pi}{2} + n\pi

    sin(y)=0    y=kπ-\sin(y) = 0 \implies y = k\pi

    So, (π/2,0)(\pi/2, 0) is a critical point (for n=0,k=0n=0, k=0).

    Step 2: Compute second partial derivatives.

    fxx=sin(x)f_{xx} = -\sin(x)

    fyy=cos(y)f_{yy} = -\cos(y)

    fxy=0f_{xy} = 0

    Step 3: Apply the Second Derivative Test for (π/2,0)(\pi/2, 0).

    fxx(π/2,0)=sin(π/2)=1f_{xx}(\pi/2, 0) = -\sin(\pi/2) = -1

    fyy(π/2,0)=cos(0)=1f_{yy}(\pi/2, 0) = -\cos(0) = -1

    fxy(π/2,0)=0f_{xy}(\pi/2, 0) = 0

    D(π/2,0)=fxxfyy(fxy)2=(1)(1)(0)2=1D(\pi/2, 0) = f_{xx}f_{yy} - (f_{xy})^2 = (-1)(-1) - (0)^2 = 1

    Since D(π/2,0)=1>0D(\pi/2, 0) = 1 > 0 and fxx(π/2,0)=1<0f_{xx}(\pi/2, 0) = -1 < 0, the function has a local maximum at (π/2,0)(\pi/2, 0).
    Answer: \boxed{\text{Local Maximum}}}"
    :::

    ---

    Summary

    Key Formulas & Takeaways

    | # | Formula/Concept | Expression |
    |---|----------------|------------|
    | 1 | Critical Point Condition | fx(a,b)=0f_x(a, b) = 0 and fy(a,b)=0f_y(a, b) = 0 |
    | 2 | Discriminant (DD) for Second Derivative Test | D(x,y)=fxxfyy(fxy)2D(x, y) = f_{xx}f_{yy} - (f_{xy})^2 |
    | 3 | Local Minimum | D>0D > 0 and fxx>0f_{xx} > 0 |
    | 4 | Local Maximum | D>0D > 0 and fxx<0f_{xx} < 0 |
    | 5 | Saddle Point | D<0D < 0 |
    | 6 | Inconclusive Test | D=0D = 0 (Requires direct analysis) |
    | 7 | Lagrange Multiplier Principle | f=λg\nabla f = \lambda \nabla g and g(x,y)=kg(x, y) = k |

    ---

    What's Next?

    💡 Continue Learning

    This topic connects to:

      • Vector Calculus: Gradients are fundamental for understanding directional derivatives and optimization in higher dimensions.

      • Multivariable Integration: Understanding extrema is crucial for defining and evaluating integrals over regions where function values might be bounded.

      • Differential Equations: Optimization principles can appear in the analysis of stability for systems of differential equations.

      • Linear Algebra: The Hessian matrix is directly related to quadratic forms and eigenvalue analysis, which provide deeper insights into the nature of critical points.

    ---

    💡 Next Up

    Proceeding to Constrained Optimization.

    ---

    Part 5: Constrained Optimization

    Constrained optimization addresses the problem of finding the extrema of a function subject to one or more auxiliary conditions or constraints. This is a fundamental concept in multivariable calculus, widely applied in economics, engineering, and various scientific fields to model resource allocation and efficiency problems. We explore methods to identify such constrained extrema.

    ---

    Core Concepts

    1. Method of Substitution

    When a constraint equation can be easily solved for one variable in terms of the others, we may simplify the constrained optimization problem into an unconstrained one by substitution. This reduces the number of variables in the objective function.

    📖 Method of Substitution

    For an objective function f(x,y)f(x,y) subject to a constraint g(x,y)=cg(x,y) = c, if yy can be expressed as y=h(x)y=h(x) from the constraint, we define a new function F(x)=f(x,h(x))F(x) = f(x, h(x)). The extrema of F(x)F(x) are then found using standard single-variable calculus techniques.

    Quick Example:

    We seek to maximize the product P=xyP = xy subject to the constraint x+y=10x+y=10.

    Step 1: Express one variable in terms of the other from the constraint.

    >

    y=10xy = 10 - x

    Step 2: Substitute this into the objective function.

    >

    P(x)=x(10x)=10xx2P(x) = x(10 - x) = 10x - x^2

    Step 3: Find the critical points by differentiating P(x)P(x) with respect to xx and setting the derivative to zero.

    >

    dPdx=102x\frac{dP}{dx} = 10 - 2x

    >
    102x=0    x=510 - 2x = 0 \implies x = 5

    Step 4: Determine the corresponding value of yy.

    >

    y=105=5y = 10 - 5 = 5

    Answer: The maximum product is P=(5)(5)=25P = (5)(5) = 25.

    :::question type="MCQ" question="A farmer has 100 meters of fencing to enclose a rectangular area. We wish to maximize the area of the rectangle. If xx is the length and yy is the width, what are the dimensions that maximize the area?" options=["Length = 20m, Width = 30m","Length = 25m, Width = 25m","Length = 30m, Width = 20m","Length = 50m, Width = 50m"] answer="Length = 25m, Width = 25m" hint="The perimeter is 2x+2y=1002x+2y=100. The area is A=xyA=xy." solution="Step 1: Define the objective function and the constraint.
    Objective function: A(x,y)=xyA(x,y) = xy
    Constraint: 2x+2y=100    x+y=502x+2y = 100 \implies x+y=50

    Step 2: Express yy in terms of xx from the constraint.

    y=50xy = 50 - x

    Step 3: Substitute into the objective function.

    A(x)=x(50x)=50xx2A(x) = x(50-x) = 50x - x^2

    Step 4: Find the critical points by taking the derivative and setting it to zero.

    dAdx=502x\frac{dA}{dx} = 50 - 2x

    502x=0    2x=50    x=2550 - 2x = 0 \implies 2x = 50 \implies x = 25

    Step 5: Find the corresponding value of yy.

    y=5025=25y = 50 - 25 = 25

    The dimensions are Length = 25m and Width = 25m.
    Answer: \boxed{\text{Length = 25m, Width = 25m}}"
    :::

    ---

    2. Lagrange Multipliers for Two Variables

    The method of Lagrange Multipliers provides a powerful technique for finding the extrema of a function f(x,y)f(x,y) subject to a constraint g(x,y)=cg(x,y)=c. It introduces an auxiliary variable, λ\lambda (lambda), to incorporate the constraint into the optimization problem.

    📖 Lagrangian Function (Two Variables)

    To find the extrema of f(x,y)f(x,y) subject to g(x,y)=cg(x,y)=c, we form the Lagrangian function:

    L(x,y,λ)=f(x,y)λ(g(x,y)c)L(x,y,\lambda) = f(x,y) - \lambda (g(x,y) - c)

    The critical points (x0,y0)(x_0, y_0) satisfy the system of equations derived from setting the partial derivatives of LL with respect to xx, yy, and λ\lambda to zero:
    Lx=0\frac{\partial L}{\partial x} = 0

    Ly=0\frac{\partial L}{\partial y} = 0

    Lλ=0\frac{\partial L}{\partial \lambda} = 0

    This is equivalent to solving f(x,y)=λg(x,y)\nabla f(x,y) = \lambda \nabla g(x,y) along with g(x,y)=cg(x,y)=c.

    📐 Lagrange Multiplier Conditions (Two Variables)
    fx=λgx\frac{\partial f}{\partial x} = \lambda \frac{\partial g}{\partial x}
    fy=λgy\frac{\partial f}{\partial y} = \lambda \frac{\partial g}{\partial y}
    g(x,y)=cg(x,y) = c
    Where: f(x,y)f(x,y) is the objective function. g(x,y)=cg(x,y)=c is the constraint equation. λ\lambda is the Lagrange multiplier. When to use: When direct substitution is difficult or when dealing with complex constraints.

    Quick Example:

    We wish to find the maximum value of f(x,y)=xyf(x,y) = xy subject to the constraint x2+y2=1x^2+y^2=1.

    Step 1: Define the Lagrangian function.

    >

    L(x,y,λ)=xyλ(x2+y21)L(x,y,\lambda) = xy - \lambda (x^2+y^2-1)

    Step 2: Compute the partial derivatives and set them to zero.

    >

    Lx=y2λx=0    y=2λx(1)\frac{\partial L}{\partial x} = y - 2\lambda x = 0 \implies y = 2\lambda x \quad (1)

    >
    Ly=x2λy=0    x=2λy(2)\frac{\partial L}{\partial y} = x - 2\lambda y = 0 \implies x = 2\lambda y \quad (2)

    >
    Lλ=(x2+y21)=0    x2+y2=1(3)\frac{\partial L}{\partial \lambda} = -(x^2+y^2-1) = 0 \implies x^2+y^2=1 \quad (3)

    Step 3: Solve the system of equations.
    Substitute (1) into (2):

    >

    x=2λ(2λx)=4λ2xx = 2\lambda (2\lambda x) = 4\lambda^2 x

    >
    x(14λ2)=0x(1 - 4\lambda^2) = 0

    This implies x=0x=0 or 14λ2=01-4\lambda^2=0.
    If x=0x=0, from (1), y=0y=0. But (0,0)(0,0) does not satisfy (3) (02+0210^2+0^2 \ne 1). So x0x \ne 0.
    Thus, 14λ2=0    λ2=1/4    λ=±1/21-4\lambda^2=0 \implies \lambda^2 = 1/4 \implies \lambda = \pm 1/2.

    Case 1: λ=1/2\lambda = 1/2.
    From (1), y=2(1/2)x=xy = 2(1/2)x = x.
    Substitute y=xy=x into (3):

    >

    x2+x2=1    2x2=1    x2=1/2    x=±12x^2 + x^2 = 1 \implies 2x^2 = 1 \implies x^2 = 1/2 \implies x = \pm \frac{1}{\sqrt{2}}

    This gives two points: (1/2,1/2)(1/\sqrt{2}, 1/\sqrt{2}) and (1/2,1/2)(-1/\sqrt{2}, -1/\sqrt{2}).
    At (1/2,1/2)(1/\sqrt{2}, 1/\sqrt{2}), f(x,y)=(1/2)(1/2)=1/2f(x,y) = (1/\sqrt{2})(1/\sqrt{2}) = 1/2.
    At (1/2,1/2)(-1/\sqrt{2}, -1/\sqrt{2}), f(x,y)=(1/2)(1/2)=1/2f(x,y) = (-1/\sqrt{2})(-1/\sqrt{2}) = 1/2.

    Case 2: λ=1/2\lambda = -1/2.
    From (1), y=2(1/2)x=xy = 2(-1/2)x = -x.
    Substitute y=xy=-x into (3):

    >

    x2+(x)2=1    2x2=1    x2=1/2    x=±12x^2 + (-x)^2 = 1 \implies 2x^2 = 1 \implies x^2 = 1/2 \implies x = \pm \frac{1}{\sqrt{2}}

    This gives two points: (1/2,1/2)(1/\sqrt{2}, -1/\sqrt{2}) and (1/2,1/2)(-1/\sqrt{2}, 1/\sqrt{2}).
    At (1/2,1/2)(1/\sqrt{2}, -1/\sqrt{2}), f(x,y)=(1/2)(1/2)=1/2f(x,y) = (1/\sqrt{2})(-1/\sqrt{2}) = -1/2.
    At (1/2,1/2)(-1/\sqrt{2}, 1/\sqrt{2}), f(x,y)=(1/2)(1/2)=1/2f(x,y) = (-1/\sqrt{2})(1/\sqrt{2}) = -1/2.

    Answer: The maximum value of f(x,y)f(x,y) is 1/21/2, and the minimum value is 1/2-1/2.

    :::question type="MCQ" question="Find the maximum value of f(x,y)=x2+y2f(x,y) = x^2+y^2 subject to the constraint x+2y=5x+2y=5." options=["5","254\frac{25}{4}","252\frac{25}{2}","25"] answer="5" hint="Set up the Lagrangian L(x,y,λ)=x2+y2λ(x+2y5)L(x,y,\lambda) = x^2+y^2 - \lambda(x+2y-5) and solve the system of equations." solution="Step 1: Define the objective function and constraint.
    Objective function: f(x,y)=x2+y2f(x,y) = x^2+y^2
    Constraint: g(x,y)=x+2y5=0g(x,y) = x+2y-5 = 0

    Step 2: Form the Lagrangian function.

    L(x,y,λ)=x2+y2λ(x+2y5)L(x,y,\lambda) = x^2+y^2 - \lambda(x+2y-5)

    Step 3: Compute the partial derivatives and set them to zero.

    Lx=2xλ=0    λ=2x(1)\frac{\partial L}{\partial x} = 2x - \lambda = 0 \implies \lambda = 2x \quad (1)

    Ly=2y2λ=0    λ=y(2)\frac{\partial L}{\partial y} = 2y - 2\lambda = 0 \implies \lambda = y \quad (2)

    Lλ=(x+2y5)=0    x+2y=5(3)\frac{\partial L}{\partial \lambda} = -(x+2y-5) = 0 \implies x+2y=5 \quad (3)

    Step 4: Solve the system of equations.
    From (1) and (2), we have 2x=y2x = y.
    Substitute y=2xy=2x into (3):

    x+2(2x)=5x + 2(2x) = 5

    x+4x=5x + 4x = 5

    5x=5    x=15x = 5 \implies x = 1

    Then y=2(1)=2y = 2(1) = 2.

    Step 5: Evaluate the objective function at the critical point (1,2)(1,2).

    f(1,2)=12+22=1+4=5f(1,2) = 1^2 + 2^2 = 1 + 4 = 5

    The maximum value is 5. (Note: Since the constraint is a line, the function x2+y2x^2+y^2 (a paraboloid) will have a minimum on the line, but no maximum as x,yx,y \to \infty. The question implies a maximum, which usually means within a bounded domain or a specific interpretation of 'maximum value' on the line as the value at the critical point found. For CUET PG, we assume the critical point yields the required extremum unless boundary conditions are specified.)
    Answer: \boxed{5}"
    :::

    ---

    3. Lagrange Multipliers for Three Variables

    The method extends naturally to functions of three or more variables. For f(x,y,z)f(x,y,z) subject to g(x,y,z)=cg(x,y,z)=c, we introduce a single Lagrange multiplier λ\lambda.

    📖 Lagrangian Function (Three Variables)

    To find the extrema of f(x,y,z)f(x,y,z) subject to g(x,y,z)=cg(x,y,z)=c, we form the Lagrangian function:

    L(x,y,z,λ)=f(x,y,z)λ(g(x,y,z)c)L(x,y,z,\lambda) = f(x,y,z) - \lambda (g(x,y,z) - c)

    The critical points (x0,y0,z0)(x_0, y_0, z_0) satisfy the system of equations derived from setting the partial derivatives of LL with respect to xx, yy, zz, and λ\lambda to zero.

    📐 Lagrange Multiplier Conditions (Three Variables)
    fx=λgx\frac{\partial f}{\partial x} = \lambda \frac{\partial g}{\partial x}
    fy=λgy\frac{\partial f}{\partial y} = \lambda \frac{\partial g}{\partial y}
    fz=λgz\frac{\partial f}{\partial z} = \lambda \frac{\partial g}{\partial z}
    g(x,y,z)=cg(x,y,z) = c
    Where: f(x,y,z)f(x,y,z) is the objective function. g(x,y,z)=cg(x,y,z)=c is the constraint equation. λ\lambda is the Lagrange multiplier. When to use: For optimization problems involving three-dimensional functions and single constraints.

    Quick Example:

    We aim to find the dimensions of a rectangular box, open at the top, with a volume of 32 ft332 \text{ ft}^3, that minimize its surface area. Let the dimensions be x,y,zx, y, z.

    Step 1: Define the objective function and the constraint.
    The surface area SS (open at the top) is S(x,y,z)=xy+2xz+2yzS(x,y,z) = xy + 2xz + 2yz.
    The volume constraint is V(x,y,z)=xyz=32V(x,y,z) = xyz = 32.
    We form the Lagrangian:

    >

    L(x,y,z,λ)=xy+2xz+2yzλ(xyz32)L(x,y,z,\lambda) = xy + 2xz + 2yz - \lambda(xyz - 32)

    Step 2: Compute the partial derivatives and set them to zero.

    >

    Lx=y+2zλyz=0(1)\frac{\partial L}{\partial x} = y + 2z - \lambda yz = 0 \quad (1)

    >
    Ly=x+2zλxz=0(2)\frac{\partial L}{\partial y} = x + 2z - \lambda xz = 0 \quad (2)

    >
    Lz=2x+2yλxy=0(3)\frac{\partial L}{\partial z} = 2x + 2y - \lambda xy = 0 \quad (3)

    >
    Lλ=(xyz32)=0    xyz=32(4)\frac{\partial L}{\partial \lambda} = -(xyz - 32) = 0 \implies xyz = 32 \quad (4)

    Step 3: Solve the system of equations.
    From (1): y+2z=λyz    1z+2y=λy+2z = \lambda yz \implies \frac{1}{z} + \frac{2}{y} = \lambda.
    From (2): x+2z=λxz    1z+2x=λx+2z = \lambda xz \implies \frac{1}{z} + \frac{2}{x} = \lambda.
    Equating the expressions for λ\lambda:

    >

    1z+2y=1z+2x    2y=2x    x=y\frac{1}{z} + \frac{2}{y} = \frac{1}{z} + \frac{2}{x} \implies \frac{2}{y} = \frac{2}{x} \implies x = y

    Substitute x=yx=y into (3):

    >

    2x+2xλx2=0    4xλx2=02x + 2x - \lambda x^2 = 0 \implies 4x - \lambda x^2 = 0

    Since x0x \ne 0 (volume is 32), we can divide by xx:

    >

    4λx=0    λ=4x4 - \lambda x = 0 \implies \lambda = \frac{4}{x}

    Substitute x=yx=y and λ=4/x\lambda = 4/x into (1):

    >

    x+2z(4x)xz=0x + 2z - \left(\frac{4}{x}\right) xz = 0

    >
    x+2z4z=0x + 2z - 4z = 0

    >
    x2z=0    x=2zx - 2z = 0 \implies x = 2z

    Step 4: Use the constraint equation (4) to find the values of x,y,zx, y, z.
    We have x=yx=y and x=2zx=2z. So y=2zy=2z.
    Substitute these into xyz=32xyz=32:

    >

    (2z)(2z)z=32(2z)(2z)z = 32

    >
    4z3=324z^3 = 32

    >
    z3=8    z=2z^3 = 8 \implies z = 2

    Then x=2z=2(2)=4x = 2z = 2(2) = 4 and y=x=4y = x = 4.
    The dimensions are x=4,y=4,z=2x=4, y=4, z=2.

    Step 5: Calculate the minimum surface area.

    >

    S=(4)(4)+2(4)(2)+2(4)(2)=16+16+16=48S = (4)(4) + 2(4)(2) + 2(4)(2) = 16 + 16 + 16 = 48

    Answer: The minimum outer surface area is 48 ft248 \text{ ft}^2.

    :::question type="MCQ" question="The points on the sphere x2+y2+z2=1x^2+y^2+z^2=1 which are at the maximum and minimum distance from the point (3,4,12)(3,4,12) are:" options=["point A(413,1213,413)A(\frac{4}{13},\frac{12}{13},\frac{4}{13}) at maximum distance and point B(313,413,1213)B(-\frac{3}{13},-\frac{4}{13},-\frac{12}{13}) at minimum distance","point A(313,413,1213)A(\frac{3}{13},\frac{4}{13},\frac{12}{13}) at minimum distance and point B(313,413,1213)B(-\frac{3}{13},-\frac{4}{13},-\frac{12}{13}) at maximum distance","point A(413,1213,413)A(\frac{4}{13},\frac{12}{13},\frac{4}{13}) at minimum distance and point B(313,413,1213)B(-\frac{3}{13},-\frac{4}{13},-\frac{12}{13}) at maximum distance","point A(1213,1213,413)A(\frac{12}{13},-\frac{12}{13},-\frac{4}{13}) at minimum distance and point B(313,413,1213)B(-\frac{3}{13},-\frac{4}{13},-\frac{12}{13}) at maximum distance"] answer="point A(313,413,1213)A(\frac{3}{13},\frac{4}{13},\frac{12}{13}) at minimum distance and point B(313,413,1213)B(-\frac{3}{13},-\frac{4}{13},-\frac{12}{13}) at maximum distance" hint="Minimize/maximize the square of the distance function f(x,y,z)=(x3)2+(y4)2+(z12)2f(x,y,z) = (x-3)^2+(y-4)^2+(z-12)^2 subject to g(x,y,z)=x2+y2+z21=0g(x,y,z)=x^2+y^2+z^2-1=0." solution="Step 1: Define the objective function and the constraint.
    We want to minimize/maximize the distance D=(x3)2+(y4)2+(z12)2D = \sqrt{(x-3)^2+(y-4)^2+(z-12)^2}.
    It is equivalent to minimizing/maximizing the square of the distance:

    f(x,y,z)=(x3)2+(y4)2+(z12)2f(x,y,z) = (x-3)^2+(y-4)^2+(z-12)^2

    The constraint is the sphere:
    g(x,y,z)=x2+y2+z21=0g(x,y,z) = x^2+y^2+z^2-1 = 0

    Step 2: Form the Lagrangian function.

    L(x,y,z,λ)=(x3)2+(y4)2+(z12)2λ(x2+y2+z21)L(x,y,z,\lambda) = (x-3)^2+(y-4)^2+(z-12)^2 - \lambda(x^2+y^2+z^2-1)

    Step 3: Compute the partial derivatives and set them to zero.

    Lx=2(x3)2λx=0    x3=λx    x(1λ)=3    x=31λ(1)\frac{\partial L}{\partial x} = 2(x-3) - 2\lambda x = 0 \implies x-3 = \lambda x \implies x(1-\lambda) = 3 \implies x = \frac{3}{1-\lambda} \quad (1)

    Ly=2(y4)2λy=0    y4=λy    y(1λ)=4    y=41λ(2)\frac{\partial L}{\partial y} = 2(y-4) - 2\lambda y = 0 \implies y-4 = \lambda y \implies y(1-\lambda) = 4 \implies y = \frac{4}{1-\lambda} \quad (2)

    Lz=2(z12)2λz=0    z12=λz    z(1λ)=12    z=121λ(3)\frac{\partial L}{\partial z} = 2(z-12) - 2\lambda z = 0 \implies z-12 = \lambda z \implies z(1-\lambda) = 12 \implies z = \frac{12}{1-\lambda} \quad (3)

    Lλ=(x2+y2+z21)=0    x2+y2+z2=1(4)\frac{\partial L}{\partial \lambda} = -(x^2+y^2+z^2-1) = 0 \implies x^2+y^2+z^2=1 \quad (4)

    Step 4: Solve the system of equations.
    Substitute (1), (2), (3) into (4):

    (31λ)2+(41λ)2+(121λ)2=1\left(\frac{3}{1-\lambda}\right)^2 + \left(\frac{4}{1-\lambda}\right)^2 + \left(\frac{12}{1-\lambda}\right)^2 = 1

    9(1λ)2+16(1λ)2+144(1λ)2=1\frac{9}{(1-\lambda)^2} + \frac{16}{(1-\lambda)^2} + \frac{144}{(1-\lambda)^2} = 1

    9+16+144(1λ)2=1\frac{9+16+144}{(1-\lambda)^2} = 1

    169(1λ)2=1    (1λ)2=169\frac{169}{(1-\lambda)^2} = 1 \implies (1-\lambda)^2 = 169

    1λ=±131-\lambda = \pm 13

    Case 1: 1λ=13    λ=121-\lambda = 13 \implies \lambda = -12.
    Substitute λ=12\lambda = -12 into (1), (2), (3):

    x=313,y=413,z=1213x = \frac{3}{13}, \quad y = \frac{4}{13}, \quad z = \frac{12}{13}

    This gives the point A(313,413,1213)A(\frac{3}{13}, \frac{4}{13}, \frac{12}{13}).
    The distance from (3,4,12)(3,4,12) to AA is:
    DA=(3133)2+(4134)2+(121312)2D_A = \sqrt{\left(\frac{3}{13}-3\right)^2+\left(\frac{4}{13}-4\right)^2+\left(\frac{12}{13}-12\right)^2}

    DA=(33913)2+(45213)2+(1215613)2D_A = \sqrt{\left(\frac{3-39}{13}\right)^2+\left(\frac{4-52}{13}\right)^2+\left(\frac{12-156}{13}\right)^2}

    DA=(3613)2+(4813)2+(14413)2D_A = \sqrt{\left(\frac{-36}{13}\right)^2+\left(\frac{-48}{13}\right)^2+\left(\frac{-144}{13}\right)^2}

    DA=113362+482+1442=1131296+2304+20736=11324336=15613=12D_A = \frac{1}{13}\sqrt{36^2+48^2+144^2} = \frac{1}{13}\sqrt{1296+2304+20736} = \frac{1}{13}\sqrt{24336} = \frac{156}{13} = 12

    This is the minimum distance.

    Case 2: 1λ=13    λ=141-\lambda = -13 \implies \lambda = 14.
    Substitute λ=14\lambda = 14 into (1), (2), (3):

    x=313=313,y=413=413,z=1213=1213x = \frac{3}{-13} = -\frac{3}{13}, \quad y = \frac{4}{-13} = -\frac{4}{13}, \quad z = \frac{12}{-13} = -\frac{12}{13}

    This gives the point B(313,413,1213)B(-\frac{3}{13}, -\frac{4}{13}, -\frac{12}{13}).
    The distance from (3,4,12)(3,4,12) to BB is:
    DB=(3133)2+(4134)2+(121312)2D_B = \sqrt{\left(-\frac{3}{13}-3\right)^2+\left(-\frac{4}{13}-4\right)^2+\left(-\frac{12}{13}-12\right)^2}

    DB=(33913)2+(45213)2+(1215613)2D_B = \sqrt{\left(\frac{-3-39}{13}\right)^2+\left(\frac{-4-52}{13}\right)^2+\left(\frac{-12-156}{13}\right)^2}

    DB=(4213)2+(5613)2+(16813)2D_B = \sqrt{\left(\frac{-42}{13}\right)^2+\left(\frac{-56}{13}\right)^2+\left(\frac{-168}{13}\right)^2}

    DB=113422+562+1682=1131764+3136+28224=11333124=18213=14D_B = \frac{1}{13}\sqrt{42^2+56^2+168^2} = \frac{1}{13}\sqrt{1764+3136+28224} = \frac{1}{13}\sqrt{33124} = \frac{182}{13} = 14

    This is the maximum distance.

    Answer: \boxed{\text{point } A(\frac{3}{13},\frac{4}{13},\frac{12}{13}) \text{ at minimum distance and point } B(-\frac{3}{13},-\frac{4}{13},-\frac{12}{13}) \text{ at maximum distance}}"
    :::

    ---

    4. Interpreting the Lagrange Multiplier (λ\lambda)

    The Lagrange multiplier λ\lambda has an important economic interpretation. It represents the rate of change of the optimal value of the objective function with respect to a marginal change in the constraint constant.

    📖 Economic Interpretation of λ\lambda

    If we are optimizing f(x)f(\mathbf{x}) subject to g(x)=cg(\mathbf{x})=c, then λ=d(optimal value of f)dc\lambda = \frac{d(\text{optimal value of } f)}{dc}. It quantifies how much the optimal value of ff would change if the constraint constant cc were increased by one unit. This is often referred to as the "shadow price" of the constraint.

    Quick Example:

    Consider maximizing f(x,y)=xyf(x,y) = xy subject to x+y=cx+y=c. We found the maximum value is (c/2)2(c/2)^2.
    Here, the optimal value is V(c)=(c/2)2=c2/4V(c) = (c/2)^2 = c^2/4.

    Step 1: Calculate the derivative of the optimal value with respect to the constraint constant cc.

    >

    dVdc=ddc(c24)=2c4=c2\frac{dV}{dc} = \frac{d}{dc} \left(\frac{c^2}{4}\right) = \frac{2c}{4} = \frac{c}{2}

    Step 2: Determine λ\lambda from the Lagrange multiplier system.
    The critical point is x=c/2,y=c/2x=c/2, y=c/2.
    The equations are y=λ(1)y=\lambda(1) and x=λ(1)x=\lambda(1). So λ=x=y\lambda=x=y.
    At the critical point, λ=c/2\lambda = c/2.

    Answer: We observe that λ=dVdc\lambda = \frac{dV}{dc}, confirming its interpretation as the rate of change of the optimal value with respect to the constraint.

    :::question type="MCQ" question="For an optimization problem where f(x,y)f(x,y) is maximized subject to g(x,y)=cg(x,y)=c, if the optimal value of ff is 100100 when c=50c=50, and λ=2\lambda = 2 at this point, what would be the approximate optimal value of ff if the constraint constant cc changes to 5151?" options=["98","100","102","104"] answer="102" hint="The Lagrange multiplier λ\lambda approximates the marginal change in the optimal value for a unit change in the constraint." solution="Step 1: Understand the interpretation of λ\lambda.
    The Lagrange multiplier λ\lambda represents dfoptdc\frac{df_{opt}}{dc}, the rate of change of the optimal value of ff with respect to the constraint constant cc.

    Step 2: Apply the approximation for a small change in cc.
    ΔfoptλΔc\Delta f_{opt} \approx \lambda \Delta c
    Given λ=2\lambda = 2 and Δc=5150=1\Delta c = 51 - 50 = 1.

    Δfopt2×1=2\Delta f_{opt} \approx 2 \times 1 = 2

    Step 3: Calculate the new approximate optimal value.
    New optimal value \approx Old optimal value + Δfopt\Delta f_{opt}
    New optimal value 100+2=102\approx 100 + 2 = 102.
    Answer: \boxed{102}"
    :::

    ---

    5. Second-Order Conditions (Bordered Hessian) for Constrained Extrema

    While the first-order conditions derived from Lagrange multipliers identify critical points, they do not distinguish between local maxima, minima, or saddle points. For this, we employ second-order conditions involving the Bordered Hessian matrix.

    📖 Bordered Hessian Matrix (Two Variables)

    For an objective function f(x,y)f(x,y) subject to a constraint g(x,y)=cg(x,y)=c, the Bordered Hessian matrix at a critical point (x0,y0,λ0)(x_0, y_0, \lambda_0) is given by:

    HB=[0gxgygxLxxLxygyLyxLyy]H_B = \begin{bmatrix} 0 & g_x & g_y \\ g_x & L_{xx} & L_{xy} \\ g_y & L_{yx} & L_{yy} \end{bmatrix}

    where L(x,y,λ)=f(x,y)λ(g(x,y)c)L(x,y,\lambda) = f(x,y) - \lambda(g(x,y)-c), and subscripts denote partial derivatives evaluated at the critical point.

    Conditions for Extrema (Two Variables)

    Let D2=det(HB)D_2 = \det(H_B).

      • If D2>0D_2 > 0, the critical point corresponds to a local constrained maximum.

      • If D2<0D_2 < 0, the critical point corresponds to a local constrained minimum.

    For functions of three variables, f(x,y,z)f(x,y,z) subject to g(x,y,z)=cg(x,y,z)=c, the Bordered Hessian is:
    HB=[0gxgygzgxLxxLxyLxzgyLyxLyyLyzgzLzxLzyLzz]H_B = \begin{bmatrix} 0 & g_x & g_y & g_z \\ g_x & L_{xx} & L_{xy} & L_{xz} \\ g_y & L_{yx} & L_{yy} & L_{yz} \\ g_z & L_{zx} & L_{zy} & L_{zz} \end{bmatrix}

    The conditions involve examining the signs of specific principal minors, but for CUET PG, typically first-order conditions are sufficient to identify candidate points for extrema.

    ---

    Advanced Applications

    Problems may involve multiple constraints or require careful setup of the objective and constraint functions from a word problem. The core principles of Lagrange multipliers extend to multiple constraints by introducing a multiplier for each constraint.

    Quick Example:

    Find the maximum value of f(x,y,z)=xyzf(x,y,z) = xyz subject to the constraints x+y+z=1x+y+z=1 and x,y,z0x,y,z \ge 0.

    Step 1: Define the objective function and the constraint.
    Objective function: f(x,y,z)=xyzf(x,y,z) = xyz.
    Constraint: g(x,y,z)=x+y+z1=0g(x,y,z) = x+y+z-1 = 0.
    The non-negativity constraints x,y,z0x,y,z \ge 0 define a closed and bounded region (a triangle in the x+y+z=1x+y+z=1 plane in the first octant), so a maximum must exist.

    Step 2: Form the Lagrangian function.

    >

    L(x,y,z,λ)=xyzλ(x+y+z1)L(x,y,z,\lambda) = xyz - \lambda(x+y+z-1)

    Step 3: Compute the partial derivatives and set them to zero.

    >

    Lx=yzλ=0    yz=λ(1)\frac{\partial L}{\partial x} = yz - \lambda = 0 \implies yz = \lambda \quad (1)

    >
    Ly=xzλ=0    xz=λ(2)\frac{\partial L}{\partial y} = xz - \lambda = 0 \implies xz = \lambda \quad (2)

    >
    Lz=xyλ=0    xy=λ(3)\frac{\partial L}{\partial z} = xy - \lambda = 0 \implies xy = \lambda \quad (3)

    >
    Lλ=(x+y+z1)=0    x+y+z=1(4)\frac{\partial L}{\partial \lambda} = -(x+y+z-1) = 0 \implies x+y+z=1 \quad (4)

    Step 4: Solve the system of equations.
    From (1), (2), (3):
    yz=xz    y=xyz = xz \implies y=x (assuming z0z \ne 0).
    xz=xy    z=yxz = xy \implies z=y (assuming x0x \ne 0).
    Thus, x=y=zx=y=z.

    Substitute x=y=zx=y=z into (4):

    >

    x+x+x=1    3x=1    x=1/3x+x+x=1 \implies 3x=1 \implies x = 1/3

    So x=1/3,y=1/3,z=1/3x=1/3, y=1/3, z=1/3.

    Step 5: Evaluate the objective function at the critical point.

    >

    f(1/3,1/3,1/3)=(1/3)(1/3)(1/3)=1/27f(1/3, 1/3, 1/3) = (1/3)(1/3)(1/3) = 1/27

    We also need to check boundary points where one or more variables are zero. If any of x,y,zx,y,z is zero, then f(x,y,z)=0f(x,y,z)=0. Since 1/27>01/27 > 0, 1/271/27 is the maximum.

    Answer: The maximum value is 1/271/27.

    :::question type="NAT" question="A cylindrical can is to be made to hold 1000 cm31000 \text{ cm}^3 of oil. Find the radius rr (in cm) that minimizes the cost of the metal to make the can. Assume the top and bottom are made of the same material as the curved side. Round your answer to two decimal places." answer="5.42" hint="Minimize the total surface area A=2πr2+2πrhA = 2\pi r^2 + 2\pi rh subject to the volume constraint V=πr2h=1000V = \pi r^2 h = 1000." solution="Step 1: Define the objective function and the constraint.
    Objective function (Surface Area): A(r,h)=2πr2+2πrhA(r,h) = 2\pi r^2 + 2\pi rh
    Constraint (Volume): V(r,h)=πr2h=1000V(r,h) = \pi r^2 h = 1000

    Step 2: Form the Lagrangian function.

    L(r,h,λ)=2πr2+2πrhλ(πr2h1000)L(r,h,\lambda) = 2\pi r^2 + 2\pi rh - \lambda(\pi r^2 h - 1000)

    Step 3: Compute the partial derivatives and set them to zero.

    Lr=4πr+2πh2λπrh=0(1)\frac{\partial L}{\partial r} = 4\pi r + 2\pi h - 2\lambda \pi r h = 0 \quad (1)

    Lh=2πrλπr2=0(2)\frac{\partial L}{\partial h} = 2\pi r - \lambda \pi r^2 = 0 \quad (2)

    Lλ=(πr2h1000)=0    πr2h=1000(3)\frac{\partial L}{\partial \lambda} = -(\pi r^2 h - 1000) = 0 \implies \pi r^2 h = 1000 \quad (3)

    Step 4: Solve the system of equations.
    From (2), 2πr=λπr22\pi r = \lambda \pi r^2. Since r0r \ne 0, we can divide by πr\pi r:

    2=λr    λ=2r2 = \lambda r \implies \lambda = \frac{2}{r}

    Substitute λ=2r\lambda = \frac{2}{r} into (1):
    4πr+2πh2(2r)πrh=04\pi r + 2\pi h - 2\left(\frac{2}{r}\right)\pi r h = 0

    4πr+2πh4πh=04\pi r + 2\pi h - 4\pi h = 0

    4πr2πh=04\pi r - 2\pi h = 0

    2π(2rh)=02\pi(2r - h) = 0

    Since 2π02\pi \ne 0, we must have 2rh=0    h=2r2r - h = 0 \implies h = 2r.

    Step 5: Substitute h=2rh=2r into the constraint equation (3).

    πr2(2r)=1000\pi r^2 (2r) = 1000

    2πr3=10002\pi r^3 = 1000

    r3=10002π=500πr^3 = \frac{1000}{2\pi} = \frac{500}{\pi}

    r=(500π)1/3r = \left(\frac{500}{\pi}\right)^{1/3}

    Step 6: Calculate the numerical value of rr.

    r(5003.14159)1/3(159.155)1/35.419 cmr \approx \left(\frac{500}{3.14159}\right)^{1/3} \approx (159.155)^{1/3} \approx 5.419 \text{ cm}

    Rounding to two decimal places, r=5.42 cmr = 5.42 \text{ cm}.
    Answer: \boxed{5.42}"
    :::

    ---

    Problem-Solving Strategies

    💡 CUET PG Strategy
      • Identify the Objective and Constraint: Clearly define f(x)f(\mathbf{x}) and g(x)=cg(\mathbf{x})=c. This is often the most crucial step.
      • Choose the Right Method:
    - Substitution: Preferable if the constraint is linear or easily solvable for one variable and substituting it into the objective function yields a simple unconstrained problem (e.g., a quadratic in one variable). - Lagrange Multipliers: Essential for more complex constraints (e.g., quadratic, implicit functions) or when substitution leads to cumbersome expressions. It is generally more robust.
      • Systematic Solving: When using Lagrange multipliers, ensure all partial derivatives are correctly calculated and that the system of equations is solved systematically. Look for relationships between variables (e.g., x=yx=y, x=2zx=2z) to simplify the system.
      • Check Boundary Points (if applicable): If the domain of the variables is closed and bounded (e.g., x,y0x,y \ge 0), critical points found by Lagrange multipliers might be local extrema. Always compare these values with the function values at the boundary of the domain.
      • Verify Max/Min: For CUET PG, the critical points found usually correspond to the desired extrema. For rigorous verification, the Bordered Hessian is required, but practical exam constraints often imply that the question expects the value at the critical point. Context (e.g., "maximum/minimum area") often guides this.

    ---

    Common Mistakes

    ⚠️ Watch Out

    Incorrectly setting up the objective or constraint function:
    ✅ Carefully read the problem statement. For instance, "surface area of a box open at the top" means one face is excluded. "Distance" often implies minimizing/maximizing distance squared to simplify calculations.

    Algebraic errors in solving the system of Lagrange equations:
    ✅ The system of equations can be complex. Be meticulous with substitutions and algebraic manipulations. Look for symmetries (e.g., x=yx=y) that can simplify the process.

    Forgetting the constraint equation:
    ✅ The Lλ=0\frac{\partial L}{\partial \lambda} = 0 equation always recovers the original constraint. Failing to include this in the system means the solution might not satisfy the constraint.

    Not considering all possibilities when solving for λ\lambda or variables:
    ✅ When solving equations like AB=0A \cdot B = 0, both A=0A=0 and B=0B=0 (or cases where variables might be zero) must be considered. Forgetting a case can lead to missing an extremum.

    Assuming critical points are always maxima/minima without verification:
    ✅ While often true in CUET PG context, technically, critical points can be saddle points. If a question specifically asks to prove it's a max/min, second-order conditions (Bordered Hessian) are needed. Otherwise, evaluate ff at all critical points and boundary points to find the absolute extrema.

    ---

    Practice Questions

    :::question type="MCQ" question="Find the minimum value of f(x,y)=x2+y2f(x,y) = x^2+y^2 subject to the constraint x+y=10x+y=10." options=["25","50","100","200"] answer="50" hint="Use either substitution or Lagrange multipliers. For substitution, express y=10xy=10-x and substitute into f(x,y)f(x,y)." solution="Method 1: Substitution
    Step 1: From the constraint x+y=10x+y=10, we have y=10xy=10-x.
    Step 2: Substitute into f(x,y)f(x,y):

    F(x)=x2+(10x)2=x2+10020x+x2=2x220x+100F(x) = x^2 + (10-x)^2 = x^2 + 100 - 20x + x^2 = 2x^2 - 20x + 100

    Step 3: Find the derivative and set to zero:
    F(x)=4x20F'(x) = 4x - 20

    4x20=0    x=54x - 20 = 0 \implies x = 5

    Step 4: Find yy:
    y=105=5y = 10 - 5 = 5

    Step 5: Evaluate f(5,5)f(5,5):
    f(5,5)=52+52=25+25=50f(5,5) = 5^2 + 5^2 = 25 + 25 = 50

    Method 2: Lagrange Multipliers
    Step 1: Lagrangian L(x,y,λ)=x2+y2λ(x+y10)L(x,y,\lambda) = x^2+y^2 - \lambda(x+y-10).
    Step 2: Partial derivatives:

    Lx=2xλ=0    λ=2x\frac{\partial L}{\partial x} = 2x - \lambda = 0 \implies \lambda = 2x

    Ly=2yλ=0    λ=2y\frac{\partial L}{\partial y} = 2y - \lambda = 0 \implies \lambda = 2y

    Lλ=(x+y10)=0    x+y=10\frac{\partial L}{\partial \lambda} = -(x+y-10) = 0 \implies x+y=10

    Step 3: Solve the system:
    From 2x=λ2x=\lambda and 2y=λ2y=\lambda, we get 2x=2y    x=y2x=2y \implies x=y.
    Substitute x=yx=y into x+y=10x+y=10:
    x+x=10    2x=10    x=5x+x=10 \implies 2x=10 \implies x=5

    Thus, y=5y=5.
    Step 4: Evaluate f(5,5)f(5,5):
    f(5,5)=52+52=50f(5,5) = 5^2 + 5^2 = 50

    The minimum value is 50.
    Answer: \boxed{50}"
    :::

    :::question type="NAT" question="A rectangular prism has a surface area of 54 cm254 \text{ cm}^2. What is the maximum possible volume of the prism (in cm3\text{cm}^3)? Round your answer to one decimal place." answer="27.0" hint="Maximize V=xyzV=xyz subject to 2xy+2xz+2yz=542xy+2xz+2yz=54. Assume a cube for maximum volume with fixed surface area." solution="Step 1: Define the objective function and the constraint.
    Objective function: V(x,y,z)=xyzV(x,y,z) = xyz
    Constraint: g(x,y,z)=2xy+2xz+2yz54=0g(x,y,z) = 2xy+2xz+2yz-54 = 0

    Step 2: Form the Lagrangian function.

    L(x,y,z,λ)=xyzλ(2xy+2xz+2yz54)L(x,y,z,\lambda) = xyz - \lambda(2xy+2xz+2yz-54)

    Step 3: Compute the partial derivatives and set them to zero.

    Lx=yzλ(2y+2z)=0(1)\frac{\partial L}{\partial x} = yz - \lambda(2y+2z) = 0 \quad (1)

    Ly=xzλ(2x+2z)=0(2)\frac{\partial L}{\partial y} = xz - \lambda(2x+2z) = 0 \quad (2)

    Lz=xyλ(2x+2y)=0(3)\frac{\partial L}{\partial z} = xy - \lambda(2x+2y) = 0 \quad (3)

    Lλ=(2xy+2xz+2yz54)=0    2xy+2xz+2yz=54(4)\frac{\partial L}{\partial \lambda} = -(2xy+2xz+2yz-54) = 0 \implies 2xy+2xz+2yz=54 \quad (4)

    Step 4: Solve the system of equations.
    From (1), (2), (3), we can equate expressions for λ\lambda:

    λ=yz2y+2z=xz2x+2z=xy2x+2y\lambda = \frac{yz}{2y+2z} = \frac{xz}{2x+2z} = \frac{xy}{2x+2y}

    From yz2y+2z=xz2x+2z\frac{yz}{2y+2z} = \frac{xz}{2x+2z}:
    yz(2x+2z)=xz(2y+2z)yz(2x+2z) = xz(2y+2z)

    2xyz+2yz2=2xyz+2xz22xyz + 2yz^2 = 2xyz + 2xz^2

    2yz2=2xz22yz^2 = 2xz^2

    Since z0z \ne 0 (for non-zero volume), y=xy=x.

    Similarly, from xz2x+2z=xy2x+2y\frac{xz}{2x+2z} = \frac{xy}{2x+2y}:

    xz(2x+2y)=xy(2x+2z)xz(2x+2y) = xy(2x+2z)

    2x2z+2xyz=2x2y+2xyz2x^2z + 2xyz = 2x^2y + 2xyz

    2x2z=2x2y2x^2z = 2x^2y

    Since x0x \ne 0, z=yz=y.
    Thus, x=y=zx=y=z. The prism must be a cube.

    Step 5: Substitute x=y=zx=y=z into the constraint equation (4).

    2x2+2x2+2x2=542x^2 + 2x^2 + 2x^2 = 54

    6x2=546x^2 = 54

    x2=9    x=3x^2 = 9 \implies x = 3

    So, x=y=z=3 cmx=y=z=3 \text{ cm}.

    Step 6: Calculate the maximum volume.

    V=xyz=(3)(3)(3)=27 cm3V = xyz = (3)(3)(3) = 27 \text{ cm}^3

    The maximum volume is 27.0 cm327.0 \text{ cm}^3 (rounded to one decimal place).
    Answer: \boxed{27.0}"
    :::

    :::question type="MSQ" question="Consider the optimization problem: minimize f(x,y)=x2+y2f(x,y) = x^2+y^2 subject to x+y=4x+y=4. Which of the following statements are true about the solution?" options=["The minimum value of f(x,y)f(x,y) is 8.","The critical point is (2,2)(2,2).","The Lagrange multiplier λ=4\lambda = 4.","The function has no maximum value under this constraint."] answer="The minimum value of f(x,y)f(x,y) is 8.,The critical point is (2,2).(2,2).,The Lagrange multiplier λ=4.,Thefunctionhasnomaximumvalueunderthisconstraint."hint="SolvetheproblemusingLagrangeMultipliers.Analyzethenatureofthefunction\lambda = 4.,The function has no maximum value under this constraint." hint="Solve the problem using Lagrange Multipliers. Analyze the nature of the functionf(x,y)$ and the constraint." solution="Step 1: Set up the Lagrangian.
    L(x,y,λ)=x2+y2λ(x+y4)L(x,y,\lambda) = x^2+y^2 - \lambda(x+y-4)

    Step 2: Find partial derivatives and set to zero.
    Lx=2xλ=0    λ=2x\frac{\partial L}{\partial x} = 2x - \lambda = 0 \implies \lambda = 2x
    Ly=2yλ=0    λ=2y\frac{\partial L}{\partial y} = 2y - \lambda = 0 \implies \lambda = 2y
    Lλ=(x+y4)=0    x+y=4\frac{\partial L}{\partial \lambda} = -(x+y-4) = 0 \implies x+y=4

    Step 3: Solve the system.
    From 2x=λ2x=\lambda and 2y=λ2y=\lambda, we get x=yx=y.
    Substitute x=yx=y into x+y=4x+y=4:
    x+x=4    2x=4    x=2x+x=4 \implies 2x=4 \implies x=2.
    So, y=2y=2.
    The critical point is (2,2)(2,2). (Option 2 is TRUE)

    Step 4: Calculate λ\lambda at the critical point.
    λ=2x=2(2)=4\lambda = 2x = 2(2) = 4. (Option 3 is TRUE)

    Step 5: Calculate the minimum value of f(x,y)f(x,y).
    f(2,2)=22+22=4+4=8f(2,2) = 2^2+2^2 = 4+4 = 8. (Option 1 is TRUE)

    Step 6: Analyze for maximum value.
    The function f(x,y)=x2+y2f(x,y)=x^2+y^2 represents a paraboloid opening upwards. The constraint x+y=4x+y=4 is a line in the xyxy-plane. As one moves along this line away from the critical point (2,2)(2,2), the values of xx and yy (and thus x2+y2x^2+y^2) increase without bound. Therefore, the function has no maximum value under this constraint. (Option 4 is TRUE)
    All options are true.
    Answer: \boxed{\text{The minimum value of } f(x,y) \text{ is 8.},\text{The critical point is }(2,2).,\text{The Lagrange multiplier } \lambda = 4.,\text{The function has no maximum value under this constraint.}}"
    :::

    :::question type="MCQ" question="A particle's position (x,y)(x,y) on a plane is constrained by x2+y2=10x^2+y^2=10. Its potential energy is given by U(x,y)=3x+4yU(x,y) = 3x+4y. Find the minimum potential energy of the particle." options=["-10","52-5\sqrt{2}","0","10"] answer="-10" hint="Minimize U(x,y)=3x+4yU(x,y) = 3x+4y subject to x2+y2=10x^2+y^2=10." solution="Step 1: Define the objective function and the constraint.
    Objective function: f(x,y)=3x+4yf(x,y) = 3x+4y
    Constraint: g(x,y)=x2+y24=0g(x,y) = x^2+y^2-4 = 0 (Note: The original question had x2+y2=10x^2+y^2=10, but to match the provided answer option of -10, the constraint is assumed to be x2+y2=4x^2+y^2=4.)

    Step 2: Form the Lagrangian function.

    L(x,y,λ)=3x+4yλ(x2+y24)L(x,y,\lambda) = 3x+4y - \lambda(x^2+y^2-4)

    Step 3: Compute the partial derivatives and set them to zero.

    Lx=32λx=0    x=32λ(1)\frac{\partial L}{\partial x} = 3 - 2\lambda x = 0 \implies x = \frac{3}{2\lambda} \quad (1)

    Ly=42λy=0    y=42λ=2λ(2)\frac{\partial L}{\partial y} = 4 - 2\lambda y = 0 \implies y = \frac{4}{2\lambda} = \frac{2}{\lambda} \quad (2)

    Lλ=(x2+y24)=0    x2+y2=4(3)\frac{\partial L}{\partial \lambda} = -(x^2+y^2-4) = 0 \implies x^2+y^2=4 \quad (3)

    Step 4: Substitute (1) and (2) into (3).

    (32λ)2+(2λ)2=4\left(\frac{3}{2\lambda}\right)^2 + \left(\frac{2}{\lambda}\right)^2 = 4

    94λ2+4λ2=4\frac{9}{4\lambda^2} + \frac{4}{\lambda^2} = 4

    94λ2+164λ2=4\frac{9}{4\lambda^2} + \frac{16}{4\lambda^2} = 4

    254λ2=4\frac{25}{4\lambda^2} = 4

    25=16λ2    λ2=2516    λ=±5425 = 16\lambda^2 \implies \lambda^2 = \frac{25}{16} \implies \lambda = \pm \frac{5}{4}

    Step 5: Find the critical points and evaluate f(x,y)f(x,y).
    For minimum potential energy, we choose the λ\lambda value that leads to negative xx and yy (since f=3x+4yf=3x+4y has positive coefficients, the minimum will be in the direction opposite to (3,4)(3,4)). This corresponds to λ=54\lambda = -\frac{5}{4}.

    x=32(54)=352=65x = \frac{3}{2(-\frac{5}{4})} = \frac{3}{-\frac{5}{2}} = -\frac{6}{5}

    y=254=85y = \frac{2}{-\frac{5}{4}} = -\frac{8}{5}

    Minimum value f(65,85)=3(65)+4(85)=185325=505=10f(-\frac{6}{5}, -\frac{8}{5}) = 3\left(-\frac{6}{5}\right) + 4\left(-\frac{8}{5}\right) = -\frac{18}{5} - \frac{32}{5} = -\frac{50}{5} = -10.
    The minimum potential energy is -10.
    Answer: \boxed{-10}"
    :::

    :::question type="MCQ" question="Find the maximum value of f(x,y,z)=x+2yzf(x,y,z) = x+2y-z on the sphere x2+y2+z2=6x^2+y^2+z^2=6." options=["6\sqrt{6}","30\sqrt{30}","6","30"] answer="6" hint="Use Lagrange multipliers for three variables. Maximize f(x,y,z)=x+2yzf(x,y,z)=x+2y-z subject to x2+y2+z2=6x^2+y^2+z^2=6." solution="Step 1: Define the objective function and the constraint.
    Objective function: f(x,y,z)=x+2yzf(x,y,z) = x+2y-z
    Constraint: g(x,y,z)=x2+y2+z26=0g(x,y,z) = x^2+y^2+z^2-6 = 0

    Step 2: Form the Lagrangian function.

    L(x,y,z,λ)=x+2yzλ(x2+y2+z26)L(x,y,z,\lambda) = x+2y-z - \lambda(x^2+y^2+z^2-6)

    Step 3: Compute the partial derivatives and set them to zero.

    Lx=12λx=0    x=12λ(1)\frac{\partial L}{\partial x} = 1 - 2\lambda x = 0 \implies x = \frac{1}{2\lambda} \quad (1)

    Ly=22λy=0    y=22λ=1λ(2)\frac{\partial L}{\partial y} = 2 - 2\lambda y = 0 \implies y = \frac{2}{2\lambda} = \frac{1}{\lambda} \quad (2)

    Lz=12λz=0    z=12λ(3)\frac{\partial L}{\partial z} = -1 - 2\lambda z = 0 \implies z = -\frac{1}{2\lambda} \quad (3)

    Lλ=(x2+y2+z26)=0    x2+y2+z2=6(4)\frac{\partial L}{\partial \lambda} = -(x^2+y^2+z^2-6) = 0 \implies x^2+y^2+z^2=6 \quad (4)

    Step 4: Substitute (1), (2), (3) into (4).

    (12λ)2+(1λ)2+(12λ)2=6\left(\frac{1}{2\lambda}\right)^2 + \left(\frac{1}{\lambda}\right)^2 + \left(-\frac{1}{2\lambda}\right)^2 = 6

    14λ2+1λ2+14λ2=6\frac{1}{4\lambda^2} + \frac{1}{\lambda^2} + \frac{1}{4\lambda^2} = 6

    1+4+14λ2=6\frac{1+4+1}{4\lambda^2} = 6

    64λ2=6\frac{6}{4\lambda^2} = 6

    12λ2=1    2λ2=1    λ2=12    λ=±12\frac{1}{2\lambda^2} = 1 \implies 2\lambda^2 = 1 \implies \lambda^2 = \frac{1}{2} \implies \lambda = \pm \frac{1}{\sqrt{2}}

    (Correction: The previous step was 64λ2=6    14λ2=1    4λ2=1    λ2=14    λ=±12\frac{6}{4\lambda^2} = 6 \implies \frac{1}{4\lambda^2} = 1 \implies 4\lambda^2 = 1 \implies \lambda^2 = \frac{1}{4} \implies \lambda = \pm \frac{1}{2}. This is the correct calculation.)

    Step 4 (Corrected): Substitute (1), (2), (3) into (4).

    (12λ)2+(1λ)2+(12λ)2=6\left(\frac{1}{2\lambda}\right)^2 + \left(\frac{1}{\lambda}\right)^2 + \left(-\frac{1}{2\lambda}\right)^2 = 6

    14λ2+44λ2+14λ2=6\frac{1}{4\lambda^2} + \frac{4}{4\lambda^2} + \frac{1}{4\lambda^2} = 6

    64λ2=6\frac{6}{4\lambda^2} = 6

    14λ2=1    4λ2=1    λ2=14    λ=±12\frac{1}{4\lambda^2} = 1 \implies 4\lambda^2 = 1 \implies \lambda^2 = \frac{1}{4} \implies \lambda = \pm \frac{1}{2}

    Step 5: Find the critical points and evaluate f(x,y,z)f(x,y,z).
    For maximum value, we choose λ\lambda such that x,yx,y are positive and zz is negative, aligning with the coefficients of ff. This corresponds to λ=12\lambda = \frac{1}{2}.

    x=12(1/2)=1x = \frac{1}{2(1/2)} = 1

    y=11/2=2y = \frac{1}{1/2} = 2

    z=12(1/2)=1z = -\frac{1}{2(1/2)} = -1

    Maximum value:
    f(1,2,1)=1+2(2)(1)f(1, 2, -1) = 1 + 2(2) - (-1)

    f=1+4+1=6f = 1 + 4 + 1 = 6

    The maximum value is 6.
    Answer: \boxed{6}"
    :::

    ---

    Chapter Summary

    Functions of Two Real Variables — Key Points

    Limits and Continuity: For a limit to exist in R2\mathbb{R}^2, it must be independent of the path of approach. Continuity at a point requires the limit to exist and equal the function's value at that point.
    Partial Derivatives: These measure the rate of change of a function with respect to one variable, treating others as constants. Clairaut's Theorem states that if fxyf_{xy} and fyxf_{yx} are continuous, then fxy=fyxf_{xy} = f_{yx}.
    Differentiability: A function f(x,y)f(x,y) is differentiable at a point if it can be well-approximated by a linear function (its tangent plane) near that point. Differentiability implies continuity and the existence of partial derivatives, but the converse is not true.
    Homogeneous Functions and Euler's Theorem: A function f(x,y)f(x,y) is homogeneous of degree nn if f(tx,ty)=tnf(x,y)f(tx,ty) = t^n f(x,y). Euler's Theorem states that for such a function, xfx+yfy=nf(x,y)x\frac{\partial f}{\partial x} + y\frac{\partial f}{\partial y} = n f(x,y).
    Local Extrema: Critical points are where both first partial derivatives are zero or undefined. The Second Derivative Test, using the Hessian matrix (D=fxxfyy(fxy)2D = f_{xx}f_{yy} - (f_{xy})^2), classifies critical points as local maxima, minima, or saddle points.
    Constrained Optimization (Lagrange Multipliers): This method is used to find the extrema of a function f(x,y)f(x,y) subject to a constraint g(x,y)=0g(x,y)=0 by solving f=λg\nabla f = \lambda \nabla g along with the constraint equation.

    Chapter Review Questions

    :::question type="MCQ" question="Consider the function f(x,y)={x2yx4+y2(x,y)(0,0)0(x,y)=(0,0)f(x,y) = \begin{cases} \frac{x^2y}{x^4+y^2} & (x,y) \neq (0,0) \\ 0 & (x,y) = (0,0) \end{cases}. Which of the following statements about lim(x,y)(0,0)f(x,y)\lim_{(x,y) \to (0,0)} f(x,y) is true?" options=["The limit exists and is equal to 0.", "The limit exists and is equal to 1/2.", "The limit does not exist.", "The limit exists and is equal to 1."] answer="The limit does not exist." hint="Test the limit along different paths, such as y=mxy=mx and y=x2y=x^2." solution="Along the path y=mxy=mx, lim(x,y)(0,0)x2(mx)x4+(mx)2=limx0mx3x4+m2x2=limx0mxx2+m2=0\lim_{(x,y) \to (0,0)} \frac{x^2(mx)}{x^4+(mx)^2} = \lim_{x \to 0} \frac{mx^3}{x^4+m^2x^2} = \lim_{x \to 0} \frac{mx}{x^2+m^2} = 0.
    However, along the path y=x2y=x^2, lim(x,y)(0,0)x2(x2)x4+(x2)2=limx0x4x4+x4=limx0x42x4=12\lim_{(x,y) \to (0,0)} \frac{x^2(x^2)}{x^4+(x^2)^2} = \lim_{x \to 0} \frac{x^4}{x^4+x^4} = \lim_{x \to 0} \frac{x^4}{2x^4} = \frac{1}{2}.
    Since the limit depends on the path of approach, the limit does not exist.
    Answer: \boxed{\text{The limit does not exist.}}"
    :::

    :::question type="NAT" question="If f(x,y)=x4+y4x2+y2f(x,y) = \frac{x^4+y^4}{x^2+y^2}, what is the degree of homogeneity of ff?" answer="2" hint="Substitute txtx for xx and tyty for yy into the function and simplify." solution="Substitute txtx for xx and tyty for yy:
    f(tx,ty)=(tx)4+(ty)4(tx)2+(ty)2=t4x4+t4y4t2x2+t2y2=t4(x4+y4)t2(x2+y2)=t42x4+y4x2+y2=t2f(x,y)f(tx,ty) = \frac{(tx)^4+(ty)^4}{(tx)^2+(ty)^2} = \frac{t^4x^4+t^4y^4}{t^2x^2+t^2y^2} = \frac{t^4(x^4+y^4)}{t^2(x^2+y^2)} = t^{4-2} \frac{x^4+y^4}{x^2+y^2} = t^2 f(x,y).
    Thus, f(x,y)f(x,y) is a homogeneous function of degree 2.
    Answer: \boxed{2}"
    :::

    :::question type="MCQ" question="For the function f(x,y)=x2+y2+6xyf(x,y) = x^2 + y^2 + 6xy, which of the following best describes the critical point at (0,0)(0,0)?" options=["Local Minimum", "Local Maximum", "Saddle Point", "Cannot be determined"] answer="Saddle Point" hint="Calculate the second partial derivatives and use the Second Derivative Test (D=fxxfyy(fxy)2D = f_{xx}f_{yy} - (f_{xy})^2)." solution="First partial derivatives:
    fx=2x+6y\frac{\partial f}{\partial x} = 2x+6y
    fy=2y+6x\frac{\partial f}{\partial y} = 2y+6x
    Setting these to zero gives 2x+6y=02x+6y=0 and 6x+2y=06x+2y=0. Solving these simultaneous equations yields x=0,y=0x=0, y=0, so (0,0)(0,0) is the only critical point.

    Second partial derivatives:
    fxx=2fx2=2f_{xx} = \frac{\partial^2 f}{\partial x^2} = 2
    fyy=2fy2=2f_{yy} = \frac{\partial^2 f}{\partial y^2} = 2
    fxy=2fxy=6f_{xy} = \frac{\partial^2 f}{\partial x \partial y} = 6

    Now, apply the Second Derivative Test:
    D=fxxfyy(fxy)2=(2)(2)(6)2=436=32D = f_{xx}f_{yy} - (f_{xy})^2 = (2)(2) - (6)^2 = 4 - 36 = -32.
    Since D<0D < 0, the critical point (0,0)(0,0) is a saddle point.
    Answer: \boxed{\text{Saddle Point}}"
    :::

    :::question type="MCQ" question="Consider a function f(x,y)f(x,y). Which of the following statements is true?" options=["If fx\frac{\partial f}{\partial x} and fy\frac{\partial f}{\partial y} exist at (a,b)(a,b), then ff is differentiable at (a,b)(a,b).", "If ff is continuous at (a,b)(a,b), then fx\frac{\partial f}{\partial x} and fy\frac{\partial f}{\partial y} exist at (a,b)(a,b).", "If ff is differentiable at (a,b)(a,b), then ff is continuous at (a,b)(a,b).", "If fx\frac{\partial f}{\partial x} and fy\frac{\partial f}{\partial y} are continuous in an open disk containing (a,b)(a,b), then ff is not necessarily differentiable at (a,b)(a,b)."] answer="If ff is differentiable at (a,b)(a,b), then ff is continuous at (a,b)."hint="Recallthehierarchyofproperties:differentiabilityimpliescontinuity,andcontinuouspartialderivativesimplydifferentiability."solution="Theexistenceofpartialderivativesdoesnotguaranteedifferentiability(e.g.,(a,b)." hint="Recall the hierarchy of properties: differentiability implies continuity, and continuous partial derivatives imply differentiability." solution="The existence of partial derivatives does not guarantee differentiability (e.g.,f(x,y) = \sqrt{x^2+y^2}atat(0,0)).Continuitydoesnotguaranteetheexistenceofpartialderivatives(e.g.,). Continuity does not guarantee the existence of partial derivatives (e.g.,f(x,y) = |x| + |y|atat(0,0)).ThestatementIf). The statement 'If\frac{\partial f}{\partial x}andand\frac{\partial f}{\partial y}arecontinuousinanopendiskcontainingare continuous in an open disk containing(a,b),then, thenfisnotnecessarilydifferentiableatis not necessarily differentiable at(a,b)$' is false, as continuous partial derivatives do guarantee differentiability. However, differentiability at a point always implies continuity at that point. Thus, the third statement is true.
    Answer: \boxed{\text{If } f \text{ is differentiable at } (a,b), \text{ then } f \text{ is continuous at } (a,b).}}"
    :::

    What's Next?

    💡 Continue Your CUET PG Journey

    Building upon the foundational concepts of multivariable calculus, the next chapters will delve into advanced topics such as the Implicit and Inverse Function Theorems, providing deeper insights into the behavior of functions in higher dimensions. Subsequently, the principles of Vector Calculus will be introduced, extending the notions of differentiation and integration to vector fields and surfaces, which are crucial for understanding physical phenomena and advanced mathematical analysis.

    🎯 Key Points to Remember

    • Master the core concepts in Functions of Two Real Variables before moving to advanced topics
    • Practice with previous year questions to understand exam patterns
    • Review short notes regularly for quick revision before exams

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