MATH-283 (Calculus III) Curriculum

Session 09 - Partial Derivatives

Handout Worksheet
Fall Semester 2026
Session Objectives & Overview

By the end of this session, you will be able to:

  • Compute first-order partial derivatives (fx,fy,fzf_x, f_y, f_zfx​,fy​,fz​) for multivariable functions using algebraic differentiation rules (product, quotient, power, chain rule) and the formal limit definition, treating non-differentiated variables as constant coefficients.
  • Evaluate and geometrically interpret partial derivatives at specified points (x0,y0)(x_0, y_0)(x0​,y0​) or (x0,y0,z0)(x_0, y_0, z_0)(x0​,y0​,z0​) as instantaneous slopes of tangent lines to vertical trace curves (y=y0y = y_0y=y0​ and x=x0x = x_0x=x0​) and directional rates of change.
  • Visually estimate the signs, relative magnitudes, and zero-slope tangencies of partial derivatives from 2D contour maps (level curve diagrams) and tabular sensor grids.

Micro-Lecture

1. The Fundamental Principle of Partial Differentiation

  • Mathematical Foundation: In single-variable calculus, the derivative dfdx\frac{df}{dx}dxdf​ measures the slope of a curve in the xyxyxy-plane. In multivariable calculus, a function z=f(x,y)z = f(x, y)z=f(x,y) defines a curved two-dimensional surface in 3D space R3\mathbb{R}^3R3. Because inputs can vary in infinite directions across the domain plane, we isolate instantaneous rates of change along the coordinate axes using Partial Derivatives. The partial derivative ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ evaluates variation along the xxx-axis while holding yyy strictly constant; conversely, ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ evaluates variation along the yyy-axis while holding xxx strictly constant.
  • Engineering Context: Real physical systems depend on multiple simultaneous inputs: thermodynamic pressure P(V,T)P(V, T)P(V,T) depends on chamber volume and temperature; aircraft lift depends on airspeed and angle of attack. Engineers use partial derivatives to isolate how a system responds to a single variable at a time ("fine-tuning" system controls).

2. Geometric Meaning: Cross-Sectional Trace Tangents

  • Mathematical Foundation: As explored in Geometric Interpretation of Partial Derivatives, slicing the 3D surface z=f(x,y)z = f(x, y)z=f(x,y) with a vertical plane y=y0y = y_0y=y0​ produces a 2D cross-sectional curve C1C_1C1​. The partial derivative fx(x0,y0)f_x(x_0, y_0)fx​(x0​,y0​) is the slope of the tangent line T1T_1T1​ to this curve at (x0,y0,f(x0,y0))(x_0, y_0, f(x_0, y_0))(x0​,y0​,f(x0​,y0​)). Similarly, slicing with x=x0x = x_0x=x0​ produces curve C2C_2C2​, where fy(x0,y0)f_y(x_0, y_0)fy​(x0​,y0​) is the slope of tangent line T2T_2T2​.
  • Engineering Context: Geotechnical engineers evaluate terrain grades along cardinal directions (due east and due north) to design stable building foundations and retaining walls against gravitational shear failure.

3. Visual Estimation from Contour Maps and Sensor Grids

  • Mathematical Foundation: As detailed in Visual Estimation of Partial Derivatives from Contour Maps, partial derivatives can be read directly from level curve contour plots. Taking a step to the right (+x+x+x, holding yyy fixed) across higher contour labels indicates fx>0f_x > 0fx​>0, while crossing into lower labels indicates fx<0f_x < 0fx​<0. If stepping parallel to a coordinate axis is tangent to a contour line, the instantaneous rate of change is zero (fx=0f_x = 0fx​=0 or fy=0f_y = 0fy​=0). Furthermore, closely spaced contour lines represent a steep slope (large derivative magnitude), whereas widely spaced contours indicate gradual, mild slopes.
  • Engineering Context: Environmental engineers inspect topographic contour lines to determine stormwater runoff velocity and pool locations; materials engineers inspect photoelastic strain fringe densities to locate impending micro-fracture sites near geometric notches.

Skill Block 1

Worked Example A: Mixed Rational and Trigonometric Function

Compute ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ for the function:

f(x,y)=x2y+sin⁡(xy)y2+1f(x, y) = \frac{x^2 y + \sin(xy)}{y^2 + 1}f(x,y)=y2+1x2y+sin(xy)​

Worked Solution:
  1. Compute ∂f∂x\frac{\partial f}{\partial x}∂x∂f​: State the Constant Multiple Rule for Partial Derivatives: When differentiating with respect to xxx, the entire denominator (y2+1)(y^2 + 1)(y2+1) depends only on yyy and is treated as a constant scalar factor. Factor it outside the derivative:

    ∂f∂x=1y2+1⋅∂∂x[x2y+sin⁡(xy)]\frac{\partial f}{\partial x} = \frac{1}{y^2 + 1} \cdot \frac{\partial}{\partial x}\left[x^2 y + \sin(xy)\right]∂x∂f​=y2+11​⋅∂x∂​[x2y+sin(xy)]

    • Differentiate x2yx^2 yx2y with respect to xxx (treating yyy as a constant):
      ∂∂x(x2y)=2xy\frac{\partial}{\partial x}(x^2 y) = 2xy∂x∂​(x2y)=2xy
    • Differentiate sin⁡(xy)\sin(xy)sin(xy) with respect to xxx using the Chain Rule:
      ∂∂x[sin⁡(xy)]=cos⁡(xy)⋅∂∂x(xy)=cos⁡(xy)⋅y=ycos⁡(xy)\frac{\partial}{\partial x}[\sin(xy)] = \cos(xy) \cdot \frac{\partial}{\partial x}(xy) = \cos(xy) \cdot y = y\cos(xy)∂x∂​[sin(xy)]=cos(xy)⋅∂x∂​(xy)=cos(xy)⋅y=ycos(xy)
      Combine the terms:
      ∂f∂x=2xy+ycos⁡(xy)y2+1\frac{\partial f}{\partial x} = \frac{2xy + y\cos(xy)}{y^2 + 1}∂x∂f​=y2+12xy+ycos(xy)​
  2. Compute ∂f∂y\frac{\partial f}{\partial y}∂y∂f​: State the Quotient Rule for Partial Derivatives: Because yyy appears in both the numerator and the denominator, apply ∂∂y[uv]=∂u∂yv−u∂v∂yv2\frac{\partial}{\partial y}\left[\frac{u}{v}\right] = \frac{\frac{\partial u}{\partial y} v - u \frac{\partial v}{\partial y}}{v^2}∂y∂​[vu​]=v2∂y∂u​v−u∂y∂v​​ with u=x2y+sin⁡(xy)u = x^2 y + \sin(xy)u=x2y+sin(xy) and v=y2+1v = y^2 + 1v=y2+1.

    • Differentiate numerator uuu with respect to yyy (treating xxx as a constant):
      ∂u∂y=∂∂y(x2y)+∂∂y[sin⁡(xy)]=x2(1)+cos⁡(xy)⋅x=x2+xcos⁡(xy)\frac{\partial u}{\partial y} = \frac{\partial}{\partial y}(x^2 y) + \frac{\partial}{\partial y}[\sin(xy)] = x^2(1) + \cos(xy) \cdot x = x^2 + x\cos(xy)∂y∂u​=∂y∂​(x2y)+∂y∂​[sin(xy)]=x2(1)+cos(xy)⋅x=x2+xcos(xy)
    • Differentiate denominator vvv with respect to yyy:
      ∂v∂y=∂∂y(y2+1)=2y\frac{\partial v}{\partial y} = \frac{\partial}{\partial y}(y^2 + 1) = 2y∂y∂v​=∂y∂​(y2+1)=2y
      Substitute into the Quotient Rule:
      ∂f∂y=(x2+xcos⁡(xy))(y2+1)−(x2y+sin⁡(xy))(2y)(y2+1)2\frac{\partial f}{\partial y} = \frac{(x^2 + x\cos(xy))(y^2 + 1) - (x^2 y + \sin(xy))(2y)}{(y^2 + 1)^2}∂y∂f​=(y2+1)2(x2+xcos(xy))(y2+1)−(x2y+sin(xy))(2y)​

Worked Example B: Three-Variable Function with Logarithmic Composition

Compute ∂g∂x,∂g∂y\frac{\partial g}{\partial x}, \frac{\partial g}{\partial y}∂x∂g​,∂y∂g​, and ∂g∂z\frac{\partial g}{\partial z}∂z∂g​ for the three-variable function:

g(x,y,z)=ln⁡(x2+y2+z2)g(x, y, z) = \ln(x^2 + y^2 + z^2)g(x,y,z)=ln(x2+y2+z2)

Worked Solution:
  1. Compute ∂g∂x\frac{\partial g}{\partial x}∂x∂g​: State the Natural Logarithm Chain Rule:

    ∂∂x[ln⁡(u)]=1u⋅∂u∂x\frac{\partial}{\partial x}[\ln(u)] = \frac{1}{u} \cdot \frac{\partial u}{\partial x}∂x∂​[ln(u)]=u1​⋅∂x∂u​
    where u(x,y,z)=x2+y2+z2u(x, y, z) = x^2 + y^2 + z^2u(x,y,z)=x2+y2+z2.

    • Holding yyy and zzz constant, their derivatives are zero:
      ∂u∂x=∂∂x(x2+y2+z2)=2x+0+0=2x\frac{\partial u}{\partial x} = \frac{\partial}{\partial x}(x^2 + y^2 + z^2) = 2x + 0 + 0 = 2x∂x∂u​=∂x∂​(x2+y2+z2)=2x+0+0=2x
      Combine components:
      ∂g∂x=2xx2+y2+z2\frac{\partial g}{\partial x} = \frac{2x}{x^2 + y^2 + z^2}∂x∂g​=x2+y2+z22x​
  2. Compute ∂g∂y\frac{\partial g}{\partial y}∂y∂g​ and ∂g∂z\frac{\partial g}{\partial z}∂z∂g​ by Symmetry: Notice that the function g(x,y,z)g(x, y, z)g(x,y,z) is algebraically symmetric with respect to all three variables. Holding xxx and zzz constant when differentiating with respect to yyy, and holding xxx and yyy constant when differentiating with respect to zzz, yields:

    ∂g∂y=2yx2+y2+z2\frac{\partial g}{\partial y} = \frac{2y}{x^2 + y^2 + z^2}∂y∂g​=x2+y2+z22y​
    ∂g∂z=2zx2+y2+z2\frac{\partial g}{\partial z} = \frac{2z}{x^2 + y^2 + z^2}∂z∂g​=x2+y2+z22z​

Practice Problem 1: Concept & Reading Check

Open this Skill Block on the Memex to locate the information needed to answer the following:

  • (a) State the core operational rule of partial differentiation when computing ∂f∂x\frac{\partial f}{\partial x}∂x∂f​. How are all other variables treated?
  • (b) In Worked Example A, explain why the Quotient Rule was mandatory when calculating ∂f∂y\frac{\partial f}{\partial y}∂y∂f​, but was unnecessary when calculating ∂f∂x\frac{\partial f}{\partial x}∂x∂f​.
  • (c) In Thermal Protection Tile Heat Flux (Aerospace Engineering), why does conductive heat flux depend directly on the directional spatial gradients ∂T∂x\frac{\partial T}{\partial x}∂x∂T​ and ∂T∂y\frac{\partial T}{\partial y}∂y∂T​?
Solution Key:
  • (a) As defined in Partial Derivatives, the fundamental rule states that to compute ∂f∂x\frac{\partial f}{\partial x}∂x∂f​, you perform ordinary single-variable differentiation with respect to xxx while holding all other variables (y,zy, zy,z) strictly fixed as if they were constant numerical coefficients.
  • (b) In Worked Example A, the denominator is y2+1y^2 + 1y2+1. When differentiating with respect to xxx, this denominator contains zero instances of xxx, making 1y2+1\frac{1}{y^2 + 1}y2+11​ a constant coefficient that factors cleanly out of the derivative. When differentiating with respect to yyy, the variable yyy appears in both the numerator and the denominator, making the Quotient Rule mandatory.
  • (c) In Thermal Protection Tile Heat Flux (Aerospace Engineering), Fourier's Law of Heat Conduction states that heat energy flows spontaneously from high temperature to low temperature at a rate proportional to the spatial temperature gradient: q⃗=−k∇T=−k⟨∂T∂x,∂T∂y⟩\vec{q} = -k \nabla T = -k \langle \frac{\partial T}{\partial x}, \frac{\partial T}{\partial y} \rangleq​=−k∇T=−k⟨∂x∂T​,∂y∂T​⟩. The partial derivatives isolate heat diffusion rates along orthogonal structural axes.
Show your steps and calculations here.

Practice Problem 2

Compute ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ for the radical function:

f(x,y)=x2+y2f(x, y) = \sqrt{x^2 + y^2}f(x,y)=x2+y2​

Solution Key:
  1. Differentiate with respect to xxx: State the Generalized Power Rule:

    ∂f∂x=∂∂x[(x2+y2)1/2]=12(x2+y2)−1/2⋅∂∂x(x2+y2)\frac{\partial f}{\partial x} = \frac{\partial}{\partial x}\left[(x^2 + y^2)^{1/2}\right] = \frac{1}{2}(x^2 + y^2)^{-1/2} \cdot \frac{\partial}{\partial x}(x^2 + y^2)∂x∂f​=∂x∂​[(x2+y2)1/2]=21​(x2+y2)−1/2⋅∂x∂​(x2+y2)
    Holding yyy constant, ∂∂x(x2+y2)=2x+0=2x\frac{\partial}{\partial x}(x^2 + y^2) = 2x + 0 = 2x∂x∂​(x2+y2)=2x+0=2x:
    ∂f∂x=12x2+y2⋅(2x)=xx2+y2\frac{\partial f}{\partial x} = \frac{1}{2\sqrt{x^2 + y^2}} \cdot (2x) = \frac{x}{\sqrt{x^2 + y^2}}∂x∂f​=2x2+y2​1​⋅(2x)=x2+y2​x​

  2. Differentiate with respect to yyy: Holding xxx constant, ∂∂y(x2+y2)=0+2y=2y\frac{\partial}{\partial y}(x^2 + y^2) = 0 + 2y = 2y∂y∂​(x2+y2)=0+2y=2y:

    ∂f∂y=12(x2+y2)−1/2⋅(2y)=yx2+y2\frac{\partial f}{\partial y} = \frac{1}{2}(x^2 + y^2)^{-1/2} \cdot (2y) = \frac{y}{\sqrt{x^2 + y^2}}∂y∂f​=21​(x2+y2)−1/2⋅(2y)=x2+y2​y​

Show your steps and calculations here.

Practice Problem 3

Compute ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ for the exponential function:

f(x,y)=exyf(x, y) = e^{xy}f(x,y)=exy

Solution Key:
  1. Differentiate with respect to xxx: State the Exponential Chain Rule:

    ∂f∂x=exy⋅∂∂x(xy)\frac{\partial f}{\partial x} = e^{xy} \cdot \frac{\partial}{\partial x}(xy)∂x∂f​=exy⋅∂x∂​(xy)
    Holding yyy constant, yyy acts as a constant scalar coefficient on xxx: ∂∂x(xy)=y(1)=y\frac{\partial}{\partial x}(xy) = y(1) = y∂x∂​(xy)=y(1)=y:
    ∂f∂x=yexy\frac{\partial f}{\partial x} = y e^{xy}∂x∂f​=yexy

  2. Differentiate with respect to yyy: Holding xxx constant, xxx acts as a constant scalar coefficient on yyy: ∂∂y(xy)=x(1)=x\frac{\partial}{\partial y}(xy) = x(1) = x∂y∂​(xy)=x(1)=x:

    ∂f∂y=xexy\frac{\partial f}{\partial y} = x e^{xy}∂y∂f​=xexy

Show your steps and calculations here.

Practice Problem 4

Let f(x,y)=x2+3xyf(x, y) = x^2 + 3xyf(x,y)=x2+3xy. Compute ∂f∂x(2,1)\frac{\partial f}{\partial x}(2, 1)∂x∂f​(2,1) using the formal limit definition of a partial derivative:

∂f∂x(2,1)=lim⁡h→0f(2+h,1)−f(2,1)h\frac{\partial f}{\partial x}(2, 1) = \lim_{h \to 0} \frac{f(2+h, 1) - f(2, 1)}{h}∂x∂f​(2,1)=h→0lim​hf(2+h,1)−f(2,1)​

Solution Key:
  1. State the Formal Limit Definition:

    ∂f∂x(a,b)=lim⁡h→0f(a+h,b)−f(a,b)h\frac{\partial f}{\partial x}(a, b) = \lim_{h \to 0} \frac{f(a+h, b) - f(a, b)}{h}∂x∂f​(a,b)=h→0lim​hf(a+h,b)−f(a,b)​
    For (a,b)=(2,1)(a, b) = (2, 1)(a,b)=(2,1), we hold y=1y = 1y=1 constant.

  2. Evaluate the Difference Quotient Terms:

    • At (2,1)(2, 1)(2,1):
      f(2,1)=(2)2+3(2)(1)=4+6=10f(2, 1) = (2)^2 + 3(2)(1) = 4 + 6 = 10f(2,1)=(2)2+3(2)(1)=4+6=10
    • At (2+h,1)(2+h, 1)(2+h,1):
      f(2+h,1)=(2+h)2+3(2+h)(1)=(4+4h+h2)+(6+3h)=10+7h+h2f(2+h, 1) = (2+h)^2 + 3(2+h)(1) = (4 + 4h + h^2) + (6 + 3h) = 10 + 7h + h^2f(2+h,1)=(2+h)2+3(2+h)(1)=(4+4h+h2)+(6+3h)=10+7h+h2
  3. Simplify and Evaluate the Limit:

    f(2+h,1)−f(2,1)h=(10+7h+h2)−10h=7h+h2h=h(7+h)h\frac{f(2+h, 1) - f(2, 1)}{h} = \frac{(10 + 7h + h^2) - 10}{h} = \frac{7h + h^2}{h} = \frac{h(7 + h)}{h}hf(2+h,1)−f(2,1)​=h(10+7h+h2)−10​=h7h+h2​=hh(7+h)​
    For h≠0h \ne 0h=0, cancel hhh:
    lim⁡h→0(7+h)=7+0=7\lim_{h \to 0} (7 + h) = 7 + 0 = 7h→0lim​(7+h)=7+0=7
    (Verification: ∂f∂x=2x+3y  ⟹  fx(2,1)=2(2)+3(1)=4+3=7\frac{\partial f}{\partial x} = 2x + 3y \implies f_x(2, 1) = 2(2) + 3(1) = 4 + 3 = 7∂x∂f​=2x+3y⟹fx​(2,1)=2(2)+3(1)=4+3=7.)

Show your steps and calculations here.

Practice Problem 5

Compute ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ for the mixed product function:

f(x,y)=x2ycos⁡(x+2y)f(x, y) = x^2 y \cos(x + 2y)f(x,y)=x2ycos(x+2y)

Solution Key:
  1. Compute ∂f∂x\frac{\partial f}{\partial x}∂x∂f​: Let u(x,y)=x2yu(x, y) = x^2 yu(x,y)=x2y and v(x,y)=cos⁡(x+2y)v(x, y) = \cos(x + 2y)v(x,y)=cos(x+2y).

    • Holding yyy constant:
      ∂u∂x=2xy\frac{\partial u}{\partial x} = 2xy∂x∂u​=2xy
      ∂v∂x=−sin⁡(x+2y)⋅∂∂x(x+2y)=−sin⁡(x+2y)⋅(1+0)=−sin⁡(x+2y)\frac{\partial v}{\partial x} = -\sin(x + 2y) \cdot \frac{\partial}{\partial x}(x + 2y) = -\sin(x + 2y) \cdot (1 + 0) = -\sin(x + 2y)∂x∂v​=−sin(x+2y)⋅∂x∂​(x+2y)=−sin(x+2y)⋅(1+0)=−sin(x+2y)
    • By the Product Rule:
      ∂f∂x=∂u∂xv+u∂v∂x=(2xy)cos⁡(x+2y)+(x2y)(−sin⁡(x+2y))\frac{\partial f}{\partial x} = \frac{\partial u}{\partial x} v + u \frac{\partial v}{\partial x} = (2xy)\cos(x + 2y) + (x^2 y)(-\sin(x + 2y))∂x∂f​=∂x∂u​v+u∂x∂v​=(2xy)cos(x+2y)+(x2y)(−sin(x+2y))
      ∂f∂x=2xycos⁡(x+2y)−x2ysin⁡(x+2y)\frac{\partial f}{\partial x} = 2xy \cos(x + 2y) - x^2 y \sin(x + 2y)∂x∂f​=2xycos(x+2y)−x2ysin(x+2y)
  2. Compute ∂f∂y\frac{\partial f}{\partial y}∂y∂f​: With u(x,y)=x2yu(x, y) = x^2 yu(x,y)=x2y and v(x,y)=cos⁡(x+2y)v(x, y) = \cos(x + 2y)v(x,y)=cos(x+2y):

    • Holding xxx constant:
      ∂u∂y=x2(1)=x2\frac{\partial u}{\partial y} = x^2(1) = x^2∂y∂u​=x2(1)=x2
      ∂v∂y=−sin⁡(x+2y)⋅∂∂y(x+2y)=−sin⁡(x+2y)⋅2=−2sin⁡(x+2y)\frac{\partial v}{\partial y} = -\sin(x + 2y) \cdot \frac{\partial}{\partial y}(x + 2y) = -\sin(x + 2y) \cdot 2 = -2\sin(x + 2y)∂y∂v​=−sin(x+2y)⋅∂y∂​(x+2y)=−sin(x+2y)⋅2=−2sin(x+2y)
    • By the Product Rule:
      ∂f∂y=(x2)cos⁡(x+2y)+(x2y)(−2sin⁡(x+2y))\frac{\partial f}{\partial y} = (x^2)\cos(x + 2y) + (x^2 y)(-2\sin(x + 2y))∂y∂f​=(x2)cos(x+2y)+(x2y)(−2sin(x+2y))
      ∂f∂y=x2cos⁡(x+2y)−2x2ysin⁡(x+2y)\frac{\partial f}{\partial y} = x^2 \cos(x + 2y) - 2x^2 y \sin(x + 2y)∂y∂f​=x2cos(x+2y)−2x2ysin(x+2y)

Show your steps and calculations here.

Regroup 1

  • Constant Extraction Strategy: When differentiating with respect to xxx, mentally replace every yyy with a constant number (like 555) to confirm whether terms differentiate to zero (additive constants) or factor through (multiplicative constants).
  • Quotient vs Constant Multiplier: If the variable of differentiation does not appear in the denominator, never use the Quotient Rule—simply pull the denominator out as a constant scalar factor.

Skill Block 2

Worked Example A: Evaluating and Interpreting Slopes on a Cubic-Quadratic Surface

For the surface defined by:

f(x,y)=x2y−y3f(x, y) = x^2 y - y^3f(x,y)=x2y−y3

  1. Compute the general partial derivatives ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​.
  2. Evaluate ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ at the point (1,2)(1, 2)(1,2).
  3. Interpret the physical and geometric meaning of these numerical values in terms of surface slopes along vertical cross-sections.
Worked Solution:
  1. Find General Partial Derivatives: State the Constant-Variable Rule:

    • Differentiating with respect to xxx (treating yyy as a constant):
      ∂f∂x=∂∂x(x2y)−∂∂x(y3)=2xy−0=2xy\frac{\partial f}{\partial x} = \frac{\partial}{\partial x}(x^2 y) - \frac{\partial}{\partial x}(y^3) = 2xy - 0 = 2xy∂x∂f​=∂x∂​(x2y)−∂x∂​(y3)=2xy−0=2xy
    • Differentiating with respect to yyy (treating xxx as a constant):
      ∂f∂y=∂∂y(x2y)−∂∂y(y3)=x2(1)−3y2=x2−3y2\frac{\partial f}{\partial y} = \frac{\partial}{\partial y}(x^2 y) - \frac{\partial}{\partial y}(y^3) = x^2(1) - 3y^2 = x^2 - 3y^2∂y∂f​=∂y∂​(x2y)−∂y∂​(y3)=x2(1)−3y2=x2−3y2
  2. Evaluate at (x0,y0)=(1,2)(x_0, y_0) = (1, 2)(x0​,y0​)=(1,2): Substitute x=1x = 1x=1 and y=2y = 2y=2:

    ∂f∂x∣(1,2)=2(1)(2)=4\left.\frac{\partial f}{\partial x}\right|_{(1, 2)} = 2(1)(2) = 4∂x∂f​​(1,2)​=2(1)(2)=4
    ∂f∂y∣(1,2)=(1)2−3(2)2=1−3(4)=1−12=−11\left.\frac{\partial f}{\partial y}\right|_{(1, 2)} = (1)^2 - 3(2)^2 = 1 - 3(4) = 1 - 12 = -11∂y∂f​​(1,2)​=(1)2−3(2)2=1−3(4)=1−12=−11

  3. Geometric Interpretation:

    • xxx-Direction Slope (mx=4m_x = 4mx​=4): Slicing the surface with the vertical plane y=2y = 2y=2 produces the parabolic trace curve z=f(x,2)=2x2−8z = f(x, 2) = 2x^2 - 8z=f(x,2)=2x2−8. The tangent line to this trace at (1,2,−6)(1, 2, -6)(1,2,−6) has slope 444. If an engineer stands at (1,2,−6)(1, 2, -6)(1,2,−6) and walks parallel to the positive xxx-axis, the surface rises at an instantaneous rate of 444 units of height per unit of horizontal distance.
    • yyy-Direction Slope (my=−11m_y = -11my​=−11): Slicing the surface with the vertical plane x=1x = 1x=1 produces the cubic trace curve z=f(1,y)=y−y3z = f(1, y) = y - y^3z=f(1,y)=y−y3. The tangent line to this trace at (1,2,−6)(1, 2, -6)(1,2,−6) has slope −11-11−11. If the engineer walks parallel to the positive yyy-axis, the surface drops steeply at a rate of 111111 units of depth per unit of distance.

Practice Problem 6: Concept & Reading Check

Open this Skill Block on the Memex to locate the information needed to answer the following:

  • (a) Slicing the surface z=f(x,y)z = f(x, y)z=f(x,y) with the vertical plane y=y0y = y_0y=y0​ produces a 2D trace curve. How is ∂f∂x(x0,y0)\frac{\partial f}{\partial x}(x_0, y_0)∂x∂f​(x0​,y0​) related to this curve?
  • (b) In Worked Example A, describe what a walker at (1,2,−6)(1, 2, -6)(1,2,−6) experiences if they step in the +x+x+x direction versus the +y+y+y direction.
  • (c) In Stress Concentration at Bolt Hole (Mechanical & Civil Engineering), why are the spatial derivatives ∂σ∂x\frac{\partial \sigma}{\partial x}∂x∂σ​ and ∂σ∂y\frac{\partial \sigma}{\partial y}∂y∂σ​ negative at (1,1) mm(1, 1)\text{ mm}(1,1) mm?
Solution Key:
  • (a) As detailed in Geometric Interpretation of Partial Derivatives, slicing z=f(x,y)z = f(x, y)z=f(x,y) with the plane y=y0y = y_0y=y0​ produces the cross-sectional trace curve C1:z=f(x,y0)C_1: z = f(x, y_0)C1​:z=f(x,y0​). The partial derivative ∂f∂x(x0,y0)\frac{\partial f}{\partial x}(x_0, y_0)∂x∂f​(x0​,y0​) is precisely the instantaneous slope dzdx\frac{dz}{dx}dxdz​ of the tangent line T1T_1T1​ to C1C_1C1​ at the point P(x0,y0,f(x0,y0))P(x_0, y_0, f(x_0, y_0))P(x0​,y0​,f(x0​,y0​)).
  • (b) In Worked Example A, the partial derivatives at (1,2)(1, 2)(1,2) are fx=4f_x = 4fx​=4 and fy=−11f_y = -11fy​=−11. A person standing at (1,2,−6)(1, 2, -6)(1,2,−6) walking parallel to the positive xxx-axis climbs upward at an incline grade of +4+4+4 (+400%+400\%+400%). Walking parallel to the positive yyy-axis plunges steeply downward at an incline grade of −11-11−11 (−1100%-1100\%−1100%).
  • (c) In Stress Concentration at Bolt Hole (Mechanical & Civil Engineering), the stress distribution is σ(x,y)=400x2+2y2+1\sigma(x, y) = \frac{400}{x^2 + 2y^2 + 1}σ(x,y)=x2+2y2+1400​. Peak stress occurs at the aperture edge (0,0)(0, 0)(0,0). As an inspector moves away from the hole (increasing xxx or yyy), the denominator increases, causing stress to diminish. Negative derivatives indicate decreasing stress concentration away from the defect.
Show your steps and calculations here.

Practice Problem 7

For the rational surface:

f(x,y)=xy+1f(x, y) = \frac{x}{y + 1}f(x,y)=y+1x​

  1. Determine the partial derivatives ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​.
  2. Evaluate ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ at the point (2,1)(2, 1)(2,1).
  3. Interpret these values geometrically in terms of trace curve slopes.
Solution Key:
  1. Find General Partial Derivatives:

    • With respect to xxx:
      ∂f∂x=1y+1⋅∂∂x(x)=1y+1\frac{\partial f}{\partial x} = \frac{1}{y+1} \cdot \frac{\partial}{\partial x}(x) = \frac{1}{y+1}∂x∂f​=y+11​⋅∂x∂​(x)=y+11​
    • With respect to yyy:
      ∂f∂y=x⋅∂∂y[(y+1)−1]=x[−(y+1)−2(1)]=−x(y+1)2\frac{\partial f}{\partial y} = x \cdot \frac{\partial}{\partial y}\left[(y+1)^{-1}\right] = x\left[-(y+1)^{-2}(1)\right] = -\frac{x}{(y+1)^2}∂y∂f​=x⋅∂y∂​[(y+1)−1]=x[−(y+1)−2(1)]=−(y+1)2x​
  2. Evaluate at (2,1)(2, 1)(2,1):

    ∂f∂x∣(2,1)=11+1=12\left.\frac{\partial f}{\partial x}\right|_{(2, 1)} = \frac{1}{1+1} = \frac{1}{2}∂x∂f​​(2,1)​=1+11​=21​
    ∂f∂y∣(2,1)=−2(1+1)2=−24=−12\left.\frac{\partial f}{\partial y}\right|_{(2, 1)} = -\frac{2}{(1+1)^2} = -\frac{2}{4} = -\frac{1}{2}∂y∂f​​(2,1)​=−(1+1)22​=−42​=−21​

  3. Geometric Interpretation:

    • In the vertical plane y=1y = 1y=1, the trace is a straight line z=12xz = \frac{1}{2}xz=21​x. Its slope is a constant +1/2+1/2+1/2 everywhere.
    • In the vertical plane x=2x = 2x=2, the trace is a hyperbola z=2y+1z = \frac{2}{y+1}z=y+12​. At y=1y = 1y=1, the tangent line has slope −1/2-1/2−1/2, meaning the surface decreases at rate 0.50.50.5 in the positive yyy-direction.
Show your steps and calculations here.

Practice Problem 8

For the inverse trigonometric surface:

f(x,y)=arctan⁡(xy)f(x, y) = \arctan(xy)f(x,y)=arctan(xy)

  1. Determine ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​.
  2. Evaluate ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ at the point (0,1)(0, 1)(0,1).
  3. Explain the geometric significance of the value obtained for ∂f∂y(0,1)\frac{\partial f}{\partial y}(0, 1)∂y∂f​(0,1).
Solution Key:
  1. Find General Partial Derivatives: State the Arctangent Derivative Rule:

    ∂f∂x=11+(xy)2⋅∂∂x(xy)=y1+x2y2\frac{\partial f}{\partial x} = \frac{1}{1 + (xy)^2} \cdot \frac{\partial}{\partial x}(xy) = \frac{y}{1 + x^2 y^2}∂x∂f​=1+(xy)21​⋅∂x∂​(xy)=1+x2y2y​
    ∂f∂y=11+(xy)2⋅∂∂y(xy)=x1+x2y2\frac{\partial f}{\partial y} = \frac{1}{1 + (xy)^2} \cdot \frac{\partial}{\partial y}(xy) = \frac{x}{1 + x^2 y^2}∂y∂f​=1+(xy)21​⋅∂y∂​(xy)=1+x2y2x​

  2. Evaluate at (0,1)(0, 1)(0,1):

    ∂f∂x∣(0,1)=11+(0)2(1)2=11=1\left.\frac{\partial f}{\partial x}\right|_{(0, 1)} = \frac{1}{1 + (0)^2(1)^2} = \frac{1}{1} = 1∂x∂f​​(0,1)​=1+(0)2(1)21​=11​=1
    ∂f∂y∣(0,1)=01+(0)2(1)2=01=0\left.\frac{\partial f}{\partial y}\right|_{(0, 1)} = \frac{0}{1 + (0)^2(1)^2} = \frac{0}{1} = 0∂y∂f​​(0,1)​=1+(0)2(1)20​=10​=0

  3. Geometric Significance:

    • Along the plane x=0x = 0x=0 (the yzyzyz-plane), f(0,y)=arctan⁡(0)=0f(0, y) = \arctan(0) = 0f(0,y)=arctan(0)=0 for all yyy. The trace curve is the horizontal line z=0z = 0z=0.
    • Because this trace is perfectly horizontal, its slope ∂f∂y(0,1)\frac{\partial f}{\partial y}(0, 1)∂y∂f​(0,1) is identically zero. The surface is tangent to a horizontal line in the yyy-direction at (0,1,0)(0, 1, 0)(0,1,0).
Show your steps and calculations here.

Practice Problem 9

For the three-variable scalar field:

f(x,y,z)=x2+y2−z2f(x, y, z) = x^2 + y^2 - z^2f(x,y,z)=x2+y2−z2

  1. Determine ∂f∂x,∂f∂y\frac{\partial f}{\partial x}, \frac{\partial f}{\partial y}∂x∂f​,∂y∂f​, and ∂f∂z\frac{\partial f}{\partial z}∂z∂f​.
  2. Evaluate all three partial derivatives at the point (1,−1,2)(1, -1, 2)(1,−1,2).
  3. Interpret these values in terms of directional rates of change within 3D space.
Solution Key:
  1. Find General Partial Derivatives:

    • Treating y,zy, zy,z as constants: ∂f∂x=2x+0−0=2x\frac{\partial f}{\partial x} = 2x + 0 - 0 = 2x∂x∂f​=2x+0−0=2x.
    • Treating x,zx, zx,z as constants: ∂f∂y=0+2y−0=2y\frac{\partial f}{\partial y} = 0 + 2y - 0 = 2y∂y∂f​=0+2y−0=2y.
    • Treating x,yx, yx,y as constants: ∂f∂z=0+0−2z=−2z\frac{\partial f}{\partial z} = 0 + 0 - 2z = -2z∂z∂f​=0+0−2z=−2z.
  2. Evaluate at (1,−1,2)(1, -1, 2)(1,−1,2):

    ∂f∂x∣(1,−1,2)=2(1)=2\left.\frac{\partial f}{\partial x}\right|_{(1, -1, 2)} = 2(1) = 2∂x∂f​​(1,−1,2)​=2(1)=2
    ∂f∂y∣(1,−1,2)=2(−1)=−2\left.\frac{\partial f}{\partial y}\right|_{(1, -1, 2)} = 2(-1) = -2∂y∂f​​(1,−1,2)​=2(−1)=−2
    ∂f∂z∣(1,−1,2)=−2(2)=−4\left.\frac{\partial f}{\partial z}\right|_{(1, -1, 2)} = -2(2) = -4∂z∂f​​(1,−1,2)​=−2(2)=−4

  3. Physical Interpretation in 3D Space: In this 3D scalar field:

    • Stepping parallel to the positive xxx-axis (holding y=−1,z=2y = -1, z = 2y=−1,z=2) increases fff at an instantaneous rate of 222 units per unit distance.
    • Stepping parallel to the positive yyy-axis (holding x=1,z=2x = 1, z = 2x=1,z=2) decreases fff at an instantaneous rate of 222 units per unit distance.
    • Stepping parallel to the positive zzz-axis (holding x=1,y=−1x = 1, y = -1x=1,y=−1) causes fff to decrease rapidly at a rate of 444 units per unit distance.

Show your steps and calculations here.

Regroup 2

  • Trace Plane Visualization: Always remember that fxf_xfx​ lives in the slicing plane y=constanty = \text{constant}y=constant and fyf_yfy​ lives in the slicing plane x=constantx = \text{constant}x=constant.
  • Vector Bridge: The two tangent vectors v⃗1=⟨1,0,fx⟩\vec{v}_1 = \langle 1, 0, f_x \ranglev1​=⟨1,0,fx​⟩ and v⃗2=⟨0,1,fy⟩\vec{v}_2 = \langle 0, 1, f_y \ranglev2​=⟨0,1,fy​⟩ cross to form the normal vector n⃗=⟨fx,fy,−1⟩\vec{n} = \langle f_x, f_y, -1 \ranglen=⟨fx​,fy​,−1⟩, which is the foundation of tangent planes in Session 10.

Skill Block 3

Worked Example A: Visual Estimation on Elliptic Paraboloid Contours

Given the contour plot of f(x,y)=x2+2y2f(x, y) = x^2 + 2y^2f(x,y)=x2+2y2, whose level curves are concentric ellipses x2+2y2=cx^2 + 2y^2 = cx2+2y2=c:

  1. Visually estimate the signs and relative values of ∂f∂x(1,0)\frac{\partial f}{\partial x}(1, 0)∂x∂f​(1,0) and ∂f∂y(1,0)\frac{\partial f}{\partial y}(1, 0)∂y∂f​(1,0) from the contour plot.
  2. Verify your visual estimations by computing the exact analytical partial derivatives at (1,0)(1, 0)(1,0).
Worked Solution:
  1. Visual Geometric Analysis from Contour Map:

    • Locate Point (1,0)(1, 0)(1,0): The point sits on the positive xxx-axis on the ellipse x2+2y2=1x^2 + 2y^2 = 1x2+2y2=1 (c=1c = 1c=1).
    • Analyze ∂f∂x(1,0)\frac{\partial f}{\partial x}(1, 0)∂x∂f​(1,0): Take a small step to the right (in the +x+x+x direction) along the line y=0y = 0y=0. As xxx increases past 111, you cross out of the c=1c = 1c=1 ellipse and enter regions bounded by c=2,4,9c = 2, 4, 9c=2,4,9. Because contour values are increasing, ∂f∂x(1,0)>0\frac{\partial f}{\partial x}(1, 0) > 0∂x∂f​(1,0)>0 (positive slope).
    • Analyze ∂f∂y(1,0)\frac{\partial f}{\partial y}(1, 0)∂y∂f​(1,0): Take a small step straight upward (in the +y+y+y direction) along the line x=1x = 1x=1. The ellipse x2+2y2=1x^2 + 2y^2 = 1x2+2y2=1 has a vertical tangent line at its vertex (1,0)(1, 0)(1,0). Because the vertical line x=1x = 1x=1 is tangent to the contour ellipse at this point, taking an infinitesimal step along yyy remains along the constant height curve. Therefore, ∂f∂y(1,0)=0\frac{\partial f}{\partial y}(1, 0) = 0∂y∂f​(1,0)=0.
  2. Analytical Verification:

    • Differentiate f(x,y)=x2+2y2f(x, y) = x^2 + 2y^2f(x,y)=x2+2y2:
      ∂f∂x=2x  ⟹  ∂f∂x∣(1,0)=2(1)=2>0\frac{\partial f}{\partial x} = 2x \implies \left.\frac{\partial f}{\partial x}\right|_{(1, 0)} = 2(1) = 2 > 0∂x∂f​=2x⟹∂x∂f​​(1,0)​=2(1)=2>0
      ∂f∂y=4y  ⟹  ∂f∂y∣(1,0)=4(0)=0\frac{\partial f}{\partial y} = 4y \implies \left.\frac{\partial f}{\partial y}\right|_{(1, 0)} = 4(0) = 0∂y∂f​=4y⟹∂y∂f​​(1,0)​=4(0)=0
      The analytical calculations confirm the visual observations: ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ is positive (+2+2+2) and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ is exactly zero.

Practice Problem 10: Concept & Reading Check

Open this Skill Block on the Memex to locate the information needed to answer the following:

  • (a) How can you immediately tell whether ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ is positive, negative, or zero directly from a contour plot?
  • (b) Why did ∂f∂y(1,0)\frac{\partial f}{\partial y}(1, 0)∂y∂f​(1,0) equal zero in Worked Example A? How is this related to curve tangency?
  • (c) In Ceramic Engine Component Thermal Strain (Materials & Mechanical Engineering), how does the ratio of contour spacing between the xxx and yyy axes inform engineers about directional stress concentrations?
Solution Key:
  • (a) As established in Visual Estimation of Partial Derivatives from Contour Maps, you apply the Step-and-Observe Rule: start at the point and step to the right along the positive xxx-direction (holding yyy constant). If you cross into contour lines with higher numerical values, ∂f∂x>0\frac{\partial f}{\partial x} > 0∂x∂f​>0. If you cross into lower values, ∂f∂x<0\frac{\partial f}{\partial x} < 0∂x∂f​<0. If your step is tangent to the contour line, ∂f∂x=0\frac{\partial f}{\partial x} = 0∂x∂f​=0.
  • (b) In Worked Example A, the level curves are concentric ellipses centered at the origin. At the point (1,0)(1, 0)(1,0) on the xxx-axis, the vertical line x=1x = 1x=1 is perfectly tangent to the elliptical level curve. Stepping in the yyy-direction moves along the tangent line of the constant-value contour, meaning the instantaneous rate of change is zero.
  • (c) In Ceramic Engine Component Thermal Strain (Materials & Mechanical Engineering), contour lines of strain are spaced at Δx=0.2 mm\Delta x = 0.2\text{ mm}Δx=0.2 mm along the xxx-axis but Δy=2.0 mm\Delta y = 2.0\text{ mm}Δy=2.0 mm along the yyy-axis. Since gradient magnitude is inversely proportional to contour spacing, ∂ϵ∂x\frac{\partial \epsilon}{\partial x}∂x∂ϵ​ is 300 times larger than ∂ϵ∂y\frac{\partial \epsilon}{\partial y}∂y∂ϵ​, indicating severe unconstrained stress concentration across the horizontal axis.
Show your steps and calculations here.

Practice Problem 11

Consider the circular paraboloid f(x,y)=x2+y2f(x, y) = x^2 + y^2f(x,y)=x2+y2.

  1. Describe the geometry of the level curves f(x,y)=cf(x, y) = cf(x,y)=c for c>0c > 0c>0.
  2. At the point (2,0)(2, 0)(2,0), determine the visual signs of ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ and ∂f∂y\frac{\partial f}{\partial y}∂y∂f​.
  3. Verify by computing the exact analytical values of ∂f∂x(2,0)\frac{\partial f}{\partial x}(2, 0)∂x∂f​(2,0) and ∂f∂y(2,0)\frac{\partial f}{\partial y}(2, 0)∂y∂f​(2,0).
Solution Key:
  1. Describe Level Curves: The level curves are x2+y2=cx^2 + y^2 = cx2+y2=c. For each c>0c > 0c>0, this represents a circle centered at (0,0)(0, 0)(0,0) with radius r=cr = \sqrt{c}r=c​. As ccc increases, the circles expand outward.

  2. Visual Estimation at (2,0)(2, 0)(2,0):

    • Point (2,0)(2, 0)(2,0) lies on the circle of radius 222 (c=4c = 4c=4).
    • Stepping right (+x+x+x) along y=0y = 0y=0 moves to larger radii (r>2r > 2r>2), crossing into outer circles where c>4c > 4c>4. Thus, ∂f∂x(2,0)>0\frac{\partial f}{\partial x}(2, 0) > 0∂x∂f​(2,0)>0.
    • Stepping upward (+y+y+y) along x=2x = 2x=2 is tangent to the circle x2+y2=4x^2 + y^2 = 4x2+y2=4 at the rightmost vertex (2,0)(2, 0)(2,0). Thus, ∂f∂y(2,0)=0\frac{\partial f}{\partial y}(2, 0) = 0∂y∂f​(2,0)=0.
  3. Analytical Verification:

    ∂f∂x=2x  ⟹  fx(2,0)=2(2)=4\frac{\partial f}{\partial x} = 2x \implies f_x(2, 0) = 2(2) = 4∂x∂f​=2x⟹fx​(2,0)=2(2)=4
    ∂f∂y=2y  ⟹  fy(2,0)=2(0)=0\frac{\partial f}{\partial y} = 2y \implies f_y(2, 0) = 2(0) = 0∂y∂f​=2y⟹fy​(2,0)=2(0)=0

Show your steps and calculations here.

Practice Problem 12

Use the contour plot of the circular cone f(x,y)=x2+y2f(x, y) = \sqrt{x^2 + y^2}f(x,y)=x2+y2​ to estimate and evaluate ∂f∂y(1,1)\frac{\partial f}{\partial y}(1, 1)∂y∂f​(1,1).

  1. Visually determine the sign of ∂f∂y(1,1)\frac{\partial f}{\partial y}(1, 1)∂y∂f​(1,1) by observing how stepping in the positive yyy-direction moves relative to the level curves.
  2. Compute the exact analytical value of ∂f∂y(1,1)\frac{\partial f}{\partial y}(1, 1)∂y∂f​(1,1) and compare it to the cone's constant radial slope.
Solution Key:
  1. Visual Analysis: The level curves are f(x,y)=x2+y2=c  ⟹  x2+y2=c2f(x, y) = \sqrt{x^2 + y^2} = c \implies x^2 + y^2 = c^2f(x,y)=x2+y2​=c⟹x2+y2=c2, circles of radius ccc.

    • Point (1,1)(1, 1)(1,1) has distance r=12+12=2r = \sqrt{1^2 + 1^2} = \sqrt{2}r=12+12​=2​ from the origin, lying on contour c=2≈1.414c = \sqrt{2} \approx 1.414c=2​≈1.414.
    • Taking a step upward along x=1x = 1x=1 in the positive yyy-direction increases yyy. The distance to the origin becomes 12+y2>2\sqrt{1^2 + y^2} > \sqrt{2}12+y2​>2​, crossing into outer circles with higher ccc values.
    • Therefore, ∂f∂y(1,1)\frac{\partial f}{\partial y}(1, 1)∂y∂f​(1,1) must be positive.
  2. Analytical Computation: State the Radical Chain Rule:

    ∂f∂y=∂∂y[(x2+y2)1/2]=12x2+y2⋅(2y)=yx2+y2\frac{\partial f}{\partial y} = \frac{\partial}{\partial y}\left[(x^2 + y^2)^{1/2}\right] = \frac{1}{2\sqrt{x^2 + y^2}} \cdot (2y) = \frac{y}{\sqrt{x^2 + y^2}}∂y∂f​=∂y∂​[(x2+y2)1/2]=2x2+y2​1​⋅(2y)=x2+y2​y​
    Evaluate at (1,1)(1, 1)(1,1):
    ∂f∂y∣(1,1)=112+12=12=22≈0.707\left.\frac{\partial f}{\partial y}\right|_{(1, 1)} = \frac{1}{\sqrt{1^2 + 1^2}} = \frac{1}{\sqrt{2}} = \frac{\sqrt{2}}{2} \approx 0.707∂y∂f​​(1,1)​=12+12​1​=2​1​=22​​≈0.707
    Because the cone has a constant generator slope of 111 radially, moving purely along the yyy-direction at a 45∘45^\circ45∘ angle yields a slope of 1⋅cos⁡(45∘)=221 \cdot \cos(45^\circ) = \frac{\sqrt{2}}{2}1⋅cos(45∘)=22​​.

Show your steps and calculations here.

Practice Problem 13

Conceptual Contour Analysis: Suppose the level curves of a surface z=f(x,y)z = f(x, y)z=f(x,y) are a family of parallel horizontal straight lines y=cy = cy=c.

  1. Determine the value of ∂f∂x\frac{\partial f}{\partial x}∂x∂f​ at any point (x,y)(x, y)(x,y).
  2. What can you conclude about the behavior of ∂f∂y\frac{\partial f}{\partial y}∂y∂f​? Can f(x,y)f(x, y)f(x,y) be written as a single-variable function?
Solution Key:
  1. Analyze the xxx-Direction: If the level curves are horizontal lines parallel to the xxx-axis, then along any line y=y0y = y_0y=y0​, the function value f(x,y0)f(x, y_0)f(x,y0​) is strictly constant. Moving in the positive or negative xxx-direction never crosses into another contour line. Therefore, there is zero change in function value along xxx:

    ∂f∂x=0everywhere\frac{\partial f}{\partial x} = 0 \quad \text{everywhere}∂x∂f​=0everywhere

  2. Analyze the yyy-Direction: Because the contours vary as you move vertically across the horizontal strips, moving in the yyy-direction crosses from one contour line to another. Therefore, ∂f∂y\frac{\partial f}{\partial y}∂y∂f​ will generally be non-zero (either positive or negative depending on whether height increases or decreases northward). Since ∂f∂x=0\frac{\partial f}{\partial x} = 0∂x∂f​=0, integrating with respect to xxx shows that f(x,y)f(x, y)f(x,y) has no xxx-dependence:

    f(x,y)=g(y)f(x, y) = g(y)f(x,y)=g(y)
    The 3D surface is a cylindrical trough or ridge oriented parallel to the xxx-axis.

Show your steps and calculations here.

Practice Problem 14

A thermal sensor array embedded in a circuit board substrate measures surface temperatures T(x,y)T(x, y)T(x,y) in ∘C^\circ\text{C}∘C at 1 cm1\text{ cm}1 cm spatial grid intervals:

y\xy \backslash xy\x x=0 cmx = 0\text{ cm}x=0 cm x=1 cmx = 1\text{ cm}x=1 cm x=2 cmx = 2\text{ cm}x=2 cm
y=2 cmy = 2\text{ cm}y=2 cm 85∘C85^\circ\text{C}85∘C 92∘C92^\circ\text{C}92∘C 101∘C101^\circ\text{C}101∘C
y=1 cmy = 1\text{ cm}y=1 cm 78∘C78^\circ\text{C}78∘C 84∘C84^\circ\text{C}84∘C 91∘C91^\circ\text{C}91∘C
y=0 cmy = 0\text{ cm}y=0 cm 70∘C70^\circ\text{C}70∘C 75∘C75^\circ\text{C}75∘C 80∘C80^\circ\text{C}80∘C
  1. Estimate ∂T∂x(1,1)\frac{\partial T}{\partial x}(1, 1)∂x∂T​(1,1) using the central difference quotient formula:
    ∂T∂x(1,1)≈T(1+Δx,1)−T(1−Δx,1)2Δx\frac{\partial T}{\partial x}(1, 1) \approx \frac{T(1 + \Delta x, 1) - T(1 - \Delta x, 1)}{2\Delta x}∂x∂T​(1,1)≈2ΔxT(1+Δx,1)−T(1−Δx,1)​
  2. Estimate ∂T∂y(1,1)\frac{\partial T}{\partial y}(1, 1)∂y∂T​(1,1) using the central difference quotient formula:
    ∂T∂y(1,1)≈T(1,1+Δy)−T(1,1−Δy)2Δy\frac{\partial T}{\partial y}(1, 1) \approx \frac{T(1, 1 + \Delta y) - T(1, 1 - \Delta y)}{2\Delta y}∂y∂T​(1,1)≈2ΔyT(1,1+Δy)−T(1,1−Δy)​
  3. State the units of each derivative and interpret which axis exhibits greater thermal gradient across the center sensor.
Solution Key:
  1. Estimate ∂T∂x(1,1)\frac{\partial T}{\partial x}(1, 1)∂x∂T​(1,1) using Central Difference: State the Central Difference Formula along xxx: With Δx=1 cm\Delta x = 1\text{ cm}Δx=1 cm, the neighbor coordinates along the row y=1y = 1y=1 are (0,1)(0, 1)(0,1) and (2,1)(2, 1)(2,1):

    T(0,1)=78∘C,T(2,1)=91∘CT(0, 1) = 78^\circ\text{C}, \quad T(2, 1) = 91^\circ\text{C}T(0,1)=78∘C,T(2,1)=91∘C
    ∂T∂x(1,1)≈T(2,1)−T(0,1)2Δx=91∘C−78∘C2(1 cm)=13∘C2 cm=6.5∘C/cm\frac{\partial T}{\partial x}(1, 1) \approx \frac{T(2, 1) - T(0, 1)}{2\Delta x} = \frac{91^\circ\text{C} - 78^\circ\text{C}}{2(1\text{ cm})} = \frac{13^\circ\text{C}}{2\text{ cm}} = 6.5^\circ\text{C/cm}∂x∂T​(1,1)≈2ΔxT(2,1)−T(0,1)​=2(1 cm)91∘C−78∘C​=2 cm13∘C​=6.5∘C/cm

  2. Estimate ∂T∂y(1,1)\frac{\partial T}{\partial y}(1, 1)∂y∂T​(1,1) using Central Difference: State the Central Difference Formula along yyy: With Δy=1 cm\Delta y = 1\text{ cm}Δy=1 cm, the neighbor coordinates along the column x=1x = 1x=1 are (1,0)(1, 0)(1,0) and (1,2)(1, 2)(1,2):

    T(1,0)=75∘C,T(1,2)=92∘CT(1, 0) = 75^\circ\text{C}, \quad T(1, 2) = 92^\circ\text{C}T(1,0)=75∘C,T(1,2)=92∘C
    ∂T∂y(1,1)≈T(1,2)−T(1,0)2Δy=92∘C−75∘C2(1 cm)=17∘C2 cm=8.5∘C/cm\frac{\partial T}{\partial y}(1, 1) \approx \frac{T(1, 2) - T(1, 0)}{2\Delta y} = \frac{92^\circ\text{C} - 75^\circ\text{C}}{2(1\text{ cm})} = \frac{17^\circ\text{C}}{2\text{ cm}} = 8.5^\circ\text{C/cm}∂y∂T​(1,1)≈2ΔyT(1,2)−T(1,0)​=2(1 cm)92∘C−75∘C​=2 cm17∘C​=8.5∘C/cm

  3. Units and Engineering Interpretation:

    • Units: Degrees Celsius per centimeter (∘C/cm^\circ\text{C/cm}∘C/cm).
    • Interpretation: Temperature rises at an average instantaneous rate of 6.5∘C/cm6.5^\circ\text{C/cm}6.5∘C/cm moving eastward and 8.5∘C/cm8.5^\circ\text{C/cm}8.5∘C/cm moving northward from the central sensor (1,1)(1, 1)(1,1). Because ∂T∂y=8.5>∂T∂x=6.5\frac{\partial T}{\partial y} = 8.5 > \frac{\partial T}{\partial x} = 6.5∂y∂T​=8.5>∂x∂T​=6.5, heat accumulation is more pronounced along the vertical axis, signaling that active heat pipe cooling should prioritize heat extraction along the yyy-direction.

Show your steps and calculations here.

Regroup 3

  • Contour Density Intuition: Tightly spaced contour lines always equal a steep slope (large rate of change); widely spaced contour lines always equal a gentle slope (small rate of change).
  • Central vs Forward Difference: Central difference quotients are preferred in sensor grid processing because truncation errors cancel, providing a second-order accurate approximation O(Δx2)\mathcal{O}(\Delta x^2)O(Δx2).

Synthesis Wrap-up

  • Core Session Takeaways:
    1. A partial derivative isolates variation along a single coordinate axis, holding all other variables constant.
    2. Geometrically, fxf_xfx​ and fyf_yfy​ represent the slopes of tangent lines to vertical trace curves in the slicing planes y=y0y = y_0y=y0​ and x=x0x = x_0x=x0​.
    3. Visually, partial derivatives can be estimated from contour maps by stepping in the coordinate direction and observing whether height increases (>0> 0>0), decreases (<0< 0<0), or remains tangent (=0= 0=0).
  • Looking Ahead to Session 10: In Session 10, we will combine the two tangent vectors ⟨1,0,fx⟩\langle 1, 0, f_x \rangle⟨1,0,fx​⟩ and ⟨0,1,fy⟩\langle 0, 1, f_y \rangle⟨0,1,fy​⟩ to construct the Tangent Plane Equation z−z0=fx(x0,y0)(x−x0)+fy(x0,y0)(y−y0)z - z_0 = f_x(x_0, y_0)(x - x_0) + f_y(x_0, y_0)(y - y_0)z−z0​=fx​(x0​,y0​)(x−x0​)+fy​(x0​,y0​)(y−y0​) and establish linear approximations for multivariable engineering systems.
  • Knewton Alta Homework Scope: Complete adaptive problem sets: Partial Derivatives of a Function and Partial Derivatives of a Function of Three Variables.