MATH-283 (Calculus III) Curriculum

Session 10 - Tangent Planes and Linear Approximations

Handout Worksheet
Fall Semester 2026
Session Objectives & Overview

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

  • Construct vector, point-normal (a(xβˆ’x0)+b(yβˆ’y0)+c(zβˆ’z0)=0a(x-x_0) + b(y-y_0) + c(z-z_0) = 0a(xβˆ’x0​)+b(yβˆ’y0​)+c(zβˆ’z0​)=0), and general (ax+by+cz=dax+by+cz=dax+by+cz=d) equations of flat planes in 3D space from a point and normal vector or three non-collinear points using cross products.
  • Formulate equations of tangent planes to smooth surfaces z=f(x,y)z = f(x, y)z=f(x,y) at given base points (x0,y0,z0)(x_0, y_0, z_0)(x0​,y0​,z0​) by evaluating first-order partial derivatives and constructing upward- or downward-pointing surface normal vectors nβƒ—=⟨fx,fy,βˆ’1⟩\vec{n} = \langle f_x, f_y, -1 \ranglen=⟨fx​,fy​,βˆ’1⟩.
  • Construct linearizations L(x,y)=f(x0,y0)+fx(x0,y0)(xβˆ’x0)+fy(x0,y0)(yβˆ’y0)L(x, y) = f(x_0, y_0) + f_x(x_0, y_0)(x - x_0) + f_y(x_0, y_0)(y - y_0)L(x,y)=f(x0​,y0​)+fx​(x0​,y0​)(xβˆ’x0​)+fy​(x0​,y0​)(yβˆ’y0​) to approximate multivariable function values near a base point, and compute total differentials dz=fxdx+fydydz = f_x dx + f_y dydz=fx​dx+fy​dy to estimate physical propagation of measurement uncertainties and tolerances.

Micro-Lecture

1. Defining Flat Planes in Three-Dimensional Space

  • Mathematical Foundation: In single-variable calculus, defining a line in 2D space requires a known point and a directional slope. In three-dimensional space R3\mathbb{R}^3R3, defining a flat surfaceβ€”a planeβ€”requires a known base point P0(x0,y0,z0)P_0(x_0, y_0, z_0)P0​(x0​,y0​,z0​) and a direction that is completely perpendicular to the entire surface: the normal vector nβƒ—=⟨a,b,c⟩=ai^+bj^+ck^\vec{n} = \langle a, b, c \rangle = a\hat{i} + b\hat{j} + c\hat{k}n=⟨a,b,c⟩=ai^+bj^​+ck^. Any displacement vector rβƒ—βˆ’rβƒ—0\vec{r} - \vec{r}_0rβˆ’r0​ connecting P0P_0P0​ to an arbitrary point P(x,y,z)P(x, y, z)P(x,y,z) on the plane must be orthogonal to nβƒ—\vec{n}n. Applying the dot product orthogonality condition gives the point-normal equation a(xβˆ’x0)+b(yβˆ’y0)+c(zβˆ’z0)=0a(x - x_0) + b(y - y_0) + c(z - z_0) = 0a(xβˆ’x0​)+b(yβˆ’y0​)+c(zβˆ’z0​)=0, which simplifies to the general linear equation ax+by+cz=dax + by + cz = dax+by+cz=d, as explored in Equations of Planes in 3D.
  • Engineering Context: Robotic trajectory-planning systems and Building Information Modeling (BIM) software use planar equations to establish virtual safety barriers, collision envelopes, and structural floor slab elevations.

2. Tangent Planes to Curved Multivariable Surfaces

  • Mathematical Foundation: In single-variable calculus, the derivative fβ€²(x0)f'(x_0)fβ€²(x0​) gives the slope of the tangent line to the curve y=f(x)y = f(x)y=f(x). In multivariable calculus, a function z=f(x,y)z = f(x, y)z=f(x,y) defines a curved 2D surface living in R3\mathbb{R}^3R3. As established in Tangent Planes, slicing the surface with coordinate planes yields vertical trace curves whose tangent slopes are given by the partial derivatives fx(x0,y0)f_x(x_0, y_0)fx​(x0​,y0​) and fy(x0,y0)f_y(x_0, y_0)fy​(x0​,y0​). Taking the cross product of these trace tangent vectors produces the surface normal vector nβƒ—=⟨fx(x0,y0),fy(x0,y0),βˆ’1⟩\vec{n} = \langle f_x(x_0, y_0), f_y(x_0, y_0), -1 \ranglen=⟨fx​(x0​,y0​),fy​(x0​,y0​),βˆ’1⟩. The unique plane containing all directional tangent lines is the tangent plane: z=z0+fx(x0,y0)(xβˆ’x0)+fy(x0,y0)(yβˆ’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​)(xβˆ’x0​)+fy​(x0​,y0​)(yβˆ’y0​).
  • Engineering Context: Aerospace aerodynamicists extract surface normal vectors from tangent planes on curved fuselage nose cones and wings to compute local angles of attack, shock wave incidence, and dynamic pressure distributions.

3. Linear Approximations and Total Differentials

  • Mathematical Foundation: Because smooth differentiable surfaces appear locally flat when viewed under high magnification, the tangent plane serves as the optimal linear model for the surface near the point of tangency. As detailed in Linear Approximations, the linearization function L(x,y)=f(x0,y0)+fx(x0,y0)Ξ”x+fy(x0,y0)Ξ”yL(x, y) = f(x_0, y_0) + f_x(x_0, y_0)\Delta x + f_y(x_0, y_0)\Delta yL(x,y)=f(x0​,y0​)+fx​(x0​,y0​)Ξ”x+fy​(x0​,y0​)Ξ”y replaces complex non-linear functions with rapid linear arithmetic. Furthermore, as shown in Differentials and Error Propagation, the total differential dz=fxdx+fydydz = f_x dx + f_y dydz=fx​dx+fy​dy quantifies how small uncertainties in independent input measurements propagate into the overall output calculation.
  • Engineering Context: Embedded microcontrollers in autonomous quadcopters use real-time linear approximations to adjust propulsion thrust during wind gusts without overburdening CPU resources, while manufacturing quality engineers use total differentials to set dimensional tolerances on machined components.

Skill Block 1

Worked Example A: Plane Equation with a Zero Normal Component

Find the equation of the plane that passes through the point P(2,5,6)P(2, 5, 6)P(2,5,6) and has normal vector nβƒ—=⟨0,2,6⟩=2j^+6k^\vec{n} = \langle 0, 2, 6 \rangle = 2\hat{j} + 6\hat{k}n=⟨0,2,6⟩=2j^​+6k^. Express the final answer in simplest general form.

Worked Solution:
  1. Identify Given Components and State Governing Formula: State the Point-Normal Form of a Plane (defined in Equations of Planes in 3D):

    a(xβˆ’x0)+b(yβˆ’y0)+c(zβˆ’z0)=0a(x - x_0) + b(y - y_0) + c(z - z_0) = 0a(xβˆ’x0​)+b(yβˆ’y0​)+c(zβˆ’z0​)=0

    • Normal vector components: a=0,b=2,c=6a = 0, b = 2, c = 6a=0,b=2,c=6.
    • Known point coordinates: x0=2,y0=5,z0=6x_0 = 2, y_0 = 5, z_0 = 6x0​=2,y0​=5,z0​=6.
  2. Substitute Components into Point-Normal Form:

    0(xβˆ’2)+2(yβˆ’5)+6(zβˆ’6)=00(x - 2) + 2(y - 5) + 6(z - 6) = 00(xβˆ’2)+2(yβˆ’5)+6(zβˆ’6)=0

  3. Expand and Collect Constant Terms:

    0+2yβˆ’10+6zβˆ’36=00 + 2y - 10 + 6z - 36 = 00+2yβˆ’10+6zβˆ’36=0
    2y+6zβˆ’46=02y + 6z - 46 = 02y+6zβˆ’46=0
    2y+6z=462y + 6z = 462y+6z=46

  4. Reduce to Simplest Integer Coefficients: Divide the entire equation by the common factor of 222:

    y+3z=23y + 3z = 23y+3z=23

    • Geometric Insight: Because the coefficient of xxx is zero (a=0a = 0a=0), the variable xxx does not appear in the equation. The normal vector nβƒ—=⟨0,2,6⟩\vec{n} = \langle 0, 2, 6 \ranglen=⟨0,2,6⟩ is perpendicular to the xxx-axis (nβƒ—β‹…i^=0\vec{n} \cdot \hat{i} = 0nβ‹…i^=0), meaning the physical plane is completely parallel to the xxx-axis.

Practice Problem 1: Concept & Reading Check

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

  • (a) In the geometric derivation of the plane equation, why must the dot product nβƒ—β‹…(rβƒ—βˆ’rβƒ—0)\vec{n} \cdot (\vec{r} - \vec{r}_0)nβ‹…(rβˆ’r0​) equal zero for every point P(x,y,z)P(x, y, z)P(x,y,z) on the plane?
  • (b) In Worked Example A, explain why the variable xxx does not appear in the simplified equation y+3z=23y + 3z = 23y+3z=23. What does this indicate about the plane's spatial orientation relative to the xxx-axis?
  • (c) In Robotic Safety Zone Boundary (Robotics & Computer Engineering), how does the automated trajectory controller use the planar scalar equation xβˆ’2y+2zβˆ’9=0x - 2y + 2z - 9 = 0xβˆ’2y+2zβˆ’9=0 to prevent robotic arm collisions with the conveyor belt?
Solution Key:
  • (a) As established in Equations of Planes in 3D, let P0(x0,y0,z0)P_0(x_0, y_0, z_0)P0​(x0​,y0​,z0​) be a fixed base point on the plane and P(x,y,z)P(x, y, z)P(x,y,z) be any arbitrary point on the plane. The displacement vector connecting them is P0Pβƒ—=rβƒ—βˆ’rβƒ—0=⟨xβˆ’x0,yβˆ’y0,zβˆ’z0⟩\vec{P_0P} = \vec{r} - \vec{r}_0 = \langle x - x_0, y - y_0, z - z_0 \rangleP0​P​=rβˆ’r0​=⟨xβˆ’x0​,yβˆ’y0​,zβˆ’z0β€‹βŸ©. Because this displacement vector lies entirely within the flat plane surface, it must be orthogonal to the plane's perpendicular normal vector nβƒ—\vec{n}n. By the fundamental definition of the dot product, two non-zero vectors are perpendicular if and only if their dot product vanishes: nβƒ—β‹…(rβƒ—βˆ’rβƒ—0)=0\vec{n} \cdot (\vec{r} - \vec{r}_0) = 0nβ‹…(rβˆ’r0​)=0.
  • (b) In Worked Example A, the given normal vector is nβƒ—=⟨0,2,6⟩\vec{n} = \langle 0, 2, 6 \ranglen=⟨0,2,6⟩. The component along the xxx-axis is a=0a = 0a=0. When expanding the point-normal form, 0(xβˆ’2)=00(x - 2) = 00(xβˆ’2)=0, eliminating xxx from the equation entirely. Geometrically, this means the normal vector has zero tilt along the xxx-direction (nβƒ—β‹…i^=0\vec{n} \cdot \hat{i} = 0nβ‹…i^=0), which forces the plane itself to run infinitely parallel to the xxx-axis.
  • (c) In Robotic Safety Zone Boundary (Robotics & Computer Engineering), the conveyor belt surface is defined by f(x,y,z)=xβˆ’2y+2zβˆ’9=0f(x, y, z) = x - 2y + 2z - 9 = 0f(x,y,z)=xβˆ’2y+2zβˆ’9=0. The robot's trajectory-tracking firmware computes the signed orthogonal distance from its moving tool tip T(xt,yt,zt)T(x_t, y_t, z_t)T(xt​,yt​,zt​) to the boundary plane. When f(xt,yt,zt)>0f(x_t, y_t, z_t) > 0f(xt​,yt​,zt​)>0, the tool is safely in the operational envelope; if f(xt,yt,zt)≀ϡf(x_t, y_t, z_t) \le \epsilonf(xt​,yt​,zt​)≀ϡ, the tool has reached the safety margin, triggering emergency braking before physical impact occurs.
Show your steps and calculations here.

Practice Problem 2

A plane in 3D space has normal vector nβƒ—=⟨12,βˆ’4,7⟩=12i^βˆ’4j^+7k^\vec{n} = \langle 12, -4, 7 \rangle = 12\hat{i} - 4\hat{j} + 7\hat{k}n=⟨12,βˆ’4,7⟩=12i^βˆ’4j^​+7k^ originating from the anchor point P(0,7,4)P(0, 7, 4)P(0,7,4).

  1. Write the equation of the plane in point-normal form.
  2. Simplify the equation into standard general linear form (ax+by+cz=dax + by + cz = dax+by+cz=d).
Solution Key:
  1. Formulate Point-Normal Form: State the Point-Normal Equation of a Plane:

    a(xβˆ’x0)+b(yβˆ’y0)+c(zβˆ’z0)=0a(x - x_0) + b(y - y_0) + c(z - z_0) = 0a(xβˆ’x0​)+b(yβˆ’y0​)+c(zβˆ’z0​)=0
    Substitute normal vector components a=12,b=βˆ’4,c=7a = 12, b = -4, c = 7a=12,b=βˆ’4,c=7 and anchor coordinates x0=0,y0=7,z0=4x_0 = 0, y_0 = 7, z_0 = 4x0​=0,y0​=7,z0​=4:
    12(xβˆ’0)βˆ’4(yβˆ’7)+7(zβˆ’4)=012(x - 0) - 4(y - 7) + 7(z - 4) = 012(xβˆ’0)βˆ’4(yβˆ’7)+7(zβˆ’4)=0

  2. Simplify to General Form: Expand the products:

    12xβˆ’4y+28+7zβˆ’28=012x - 4y + 28 + 7z - 28 = 012xβˆ’4y+28+7zβˆ’28=0
    Notice that the constant terms cancel identically (28βˆ’28=028 - 28 = 028βˆ’28=0):
    12xβˆ’4y+7z=012x - 4y + 7z = 012xβˆ’4y+7z=0
    Geometric Observation: Because d=0d = 0d=0, the plane passes directly through the Cartesian origin (0,0,0)(0, 0, 0)(0,0,0).

Show your steps and calculations here.

Practice Problem 3

Find the equation of the plane that contains the three non-collinear points A(1,2,βˆ’1)A(1, 2, -1)A(1,2,βˆ’1), B(3,βˆ’1,2)B(3, -1, 2)B(3,βˆ’1,2), and C(0,1,1)C(0, 1, 1)C(0,1,1). Express your final equation in standard general form with positive leading integer coefficients.

Solution Key:
  1. Construct Two In-Plane Displacement Vectors: State the Displacement Vector Formula:

    uβƒ—=ABβƒ—=⟨xBβˆ’xA,yBβˆ’yA,zBβˆ’zA⟩=⟨3βˆ’1,βˆ’1βˆ’2,2βˆ’(βˆ’1)⟩=⟨2,βˆ’3,3⟩\vec{u} = \vec{AB} = \langle x_B - x_A, y_B - y_A, z_B - z_A \rangle = \langle 3 - 1, -1 - 2, 2 - (-1) \rangle = \langle 2, -3, 3 \rangleu=AB=⟨xBβ€‹βˆ’xA​,yBβ€‹βˆ’yA​,zBβ€‹βˆ’zAβ€‹βŸ©=⟨3βˆ’1,βˆ’1βˆ’2,2βˆ’(βˆ’1)⟩=⟨2,βˆ’3,3⟩
    vβƒ—=ACβƒ—=⟨xCβˆ’xA,yCβˆ’yA,zCβˆ’zA⟩=⟨0βˆ’1,1βˆ’2,1βˆ’(βˆ’1)⟩=βŸ¨βˆ’1,βˆ’1,2⟩\vec{v} = \vec{AC} = \langle x_C - x_A, y_C - y_A, z_C - z_A \rangle = \langle 0 - 1, 1 - 2, 1 - (-1) \rangle = \langle -1, -1, 2 \ranglev=AC=⟨xCβ€‹βˆ’xA​,yCβ€‹βˆ’yA​,zCβ€‹βˆ’zAβ€‹βŸ©=⟨0βˆ’1,1βˆ’2,1βˆ’(βˆ’1)⟩=βŸ¨βˆ’1,βˆ’1,2⟩

  2. Compute the Normal Vector via Cross Product: State the Cross Product Determinant Formula:

    nβƒ—=uβƒ—Γ—vβƒ—=∣i^j^k^2βˆ’33βˆ’1βˆ’12∣\vec{n} = \vec{u} \times \vec{v} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & -3 & 3 \\ -1 & -1 & 2 \end{vmatrix}n=uΓ—v=​i^2βˆ’1​j^β€‹βˆ’3βˆ’1​k^32​​
    nβƒ—=i^[(βˆ’3)(2)βˆ’(3)(βˆ’1)]βˆ’j^[(2)(2)βˆ’(3)(βˆ’1)]+k^[(2)(βˆ’1)βˆ’(βˆ’3)(βˆ’1)]\vec{n} = \hat{i}[(-3)(2) - (3)(-1)] - \hat{j}[(2)(2) - (3)(-1)] + \hat{k}[(2)(-1) - (-3)(-1)]n=i^[(βˆ’3)(2)βˆ’(3)(βˆ’1)]βˆ’j^​[(2)(2)βˆ’(3)(βˆ’1)]+k^[(2)(βˆ’1)βˆ’(βˆ’3)(βˆ’1)]
    nβƒ—=i^[βˆ’6+3]βˆ’j^[4+3]+k^[βˆ’2βˆ’3]=βˆ’3i^βˆ’7j^βˆ’5k^=βŸ¨βˆ’3,βˆ’7,βˆ’5⟩\vec{n} = \hat{i}[-6 + 3] - \hat{j}[4 + 3] + \hat{k}[-2 - 3] = -3\hat{i} - 7\hat{j} - 5\hat{k} = \langle -3, -7, -5 \ranglen=i^[βˆ’6+3]βˆ’j^​[4+3]+k^[βˆ’2βˆ’3]=βˆ’3i^βˆ’7j^β€‹βˆ’5k^=βŸ¨βˆ’3,βˆ’7,βˆ’5⟩
    Multiplying by βˆ’1-1βˆ’1 gives the equivalent outward normal vector: nβƒ—=⟨3,7,5⟩\vec{n} = \langle 3, 7, 5 \ranglen=⟨3,7,5⟩.

  3. Substitute into Point-Normal Form Using Point C(0,1,1)C(0, 1, 1)C(0,1,1):

    3(xβˆ’0)+7(yβˆ’1)+5(zβˆ’1)=03(x - 0) + 7(y - 1) + 5(z - 1) = 03(xβˆ’0)+7(yβˆ’1)+5(zβˆ’1)=0
    3x+7yβˆ’7+5zβˆ’5=03x + 7y - 7 + 5z - 5 = 03x+7yβˆ’7+5zβˆ’5=0
    3x+7y+5z=123x + 7y + 5z = 123x+7y+5z=12

  4. Verify Coordinates of Points AAA and BBB:

    • Point A(1,2,βˆ’1)A(1, 2, -1)A(1,2,βˆ’1): 3(1)+7(2)+5(βˆ’1)=3+14βˆ’5=123(1) + 7(2) + 5(-1) = 3 + 14 - 5 = 123(1)+7(2)+5(βˆ’1)=3+14βˆ’5=12. (Verified)
    • Point B(3,βˆ’1,2)B(3, -1, 2)B(3,βˆ’1,2): 3(3)+7(βˆ’1)+5(2)=9βˆ’7+10=123(3) + 7(-1) + 5(2) = 9 - 7 + 10 = 123(3)+7(βˆ’1)+5(2)=9βˆ’7+10=12. (Verified)
Show your steps and calculations here.

Practice Problem 4

Find the standard equation of the plane that passes through the point P(βˆ’2,3,1)P(-2, 3, 1)P(βˆ’2,3,1) and is parallel to the plane 4xβˆ’2y+5z=194x - 2y + 5z = 194xβˆ’2y+5z=19.

Solution Key:
  1. Extract the Normal Vector: State the Linear Coefficient Rule for Normal Vectors: For any plane written in general form ax+by+cz=dax + by + cz = dax+by+cz=d, the normal vector is nβƒ—=⟨a,b,c⟩\vec{n} = \langle a, b, c \ranglen=⟨a,b,c⟩. From the given reference plane 4xβˆ’2y+5z=194x - 2y + 5z = 194xβˆ’2y+5z=19, the normal vector is:

    nβƒ—=⟨4,βˆ’2,5⟩=4i^βˆ’2j^+5k^\vec{n} = \langle 4, -2, 5 \rangle = 4\hat{i} - 2\hat{j} + 5\hat{k}n=⟨4,βˆ’2,5⟩=4i^βˆ’2j^​+5k^

  2. Apply the Parallelism Principle: Two planes are parallel if and only if they share the same normal vector direction. Therefore, the required plane has normal vector nβƒ—=⟨4,βˆ’2,5⟩\vec{n} = \langle 4, -2, 5 \ranglen=⟨4,βˆ’2,5⟩.

  3. Construct the Equation with Point P(βˆ’2,3,1)P(-2, 3, 1)P(βˆ’2,3,1): State the Point-Normal Form:

    a(xβˆ’x0)+b(yβˆ’y0)+c(zβˆ’z0)=0a(x - x_0) + b(y - y_0) + c(z - z_0) = 0a(xβˆ’x0​)+b(yβˆ’y0​)+c(zβˆ’z0​)=0
    Substitute a=4,b=βˆ’2,c=5a = 4, b = -2, c = 5a=4,b=βˆ’2,c=5 and x0=βˆ’2,y0=3,z0=1x_0 = -2, y_0 = 3, z_0 = 1x0​=βˆ’2,y0​=3,z0​=1:
    4(xβˆ’(βˆ’2))βˆ’2(yβˆ’3)+5(zβˆ’1)=04(x - (-2)) - 2(y - 3) + 5(z - 1) = 04(xβˆ’(βˆ’2))βˆ’2(yβˆ’3)+5(zβˆ’1)=0
    4(x+2)βˆ’2(yβˆ’3)+5(zβˆ’1)=04(x + 2) - 2(y - 3) + 5(z - 1) = 04(x+2)βˆ’2(yβˆ’3)+5(zβˆ’1)=0
    4x+8βˆ’2y+6+5zβˆ’5=04x + 8 - 2y + 6 + 5z - 5 = 04x+8βˆ’2y+6+5zβˆ’5=0
    4xβˆ’2y+5z+9=04x - 2y + 5z + 9 = 04xβˆ’2y+5z+9=0
    4xβˆ’2y+5z=βˆ’94x - 2y + 5z = -94xβˆ’2y+5z=βˆ’9


Show your steps and calculations here.

Regroup 1

  • Key Takeaway: A plane in 3D is completely determined by a single normal vector nβƒ—=⟨a,b,c⟩\vec{n} = \langle a, b, c \ranglen=⟨a,b,c⟩ and a single anchor point P0(x0,y0,z0)P_0(x_0, y_0, z_0)P0​(x0​,y0​,z0​).
  • Common Misconception: Students often try to find the "slope" of a plane as a single scalar number. Emphasize that planes do not have a single slope; their 3D spatial orientation is dictated entirely by their 3-component normal vector nβƒ—\vec{n}n.
  • Cross Product Check: Remind students that when finding a plane through three points, reversing the cross product order (ACβƒ—Γ—ABβƒ—\vec{AC} \times \vec{AB}ACΓ—AB) produces βˆ’nβƒ—-\vec{n}βˆ’n, which yields the exact same geometric plane after multiplying both sides of the equation by βˆ’1-1βˆ’1.

Skill Block 2

Worked Example A: Tangent Plane to an Oscillating Trigonometric Surface

Find the equation of the tangent plane to the surface z=sin⁑(xy)z = \sin(xy)z=sin(xy) at the coordinate (x0,y0)=(0,Ο€)(x_0, y_0) = (0, \pi)(x0​,y0​)=(0,Ο€), where z0=0z_0 = 0z0​=0.

Worked Solution:
  1. Verify the Surface Height at the Given Coordinate:

    z0=f(0,Ο€)=sin⁑(0β‹…Ο€)=sin⁑(0)=0z_0 = f(0, \pi) = \sin(0 \cdot \pi) = \sin(0) = 0z0​=f(0,Ο€)=sin(0β‹…Ο€)=sin(0)=0

  2. Compute General First-Order Partial Derivatives: Apply the Trigonometric Chain Rule (treating the alternate variable as a constant coefficient):

    fx(x,y)=βˆ‚βˆ‚x[sin⁑(xy)]=cos⁑(xy)β‹…βˆ‚βˆ‚x(xy)=ycos⁑(xy)f_x(x, y) = \frac{\partial}{\partial x}[\sin(xy)] = \cos(xy) \cdot \frac{\partial}{\partial x}(xy) = y\cos(xy)fx​(x,y)=βˆ‚xβˆ‚β€‹[sin(xy)]=cos(xy)β‹…βˆ‚xβˆ‚β€‹(xy)=ycos(xy)
    fy(x,y)=βˆ‚βˆ‚y[sin⁑(xy)]=cos⁑(xy)β‹…βˆ‚βˆ‚y(xy)=xcos⁑(xy)f_y(x, y) = \frac{\partial}{\partial y}[\sin(xy)] = \cos(xy) \cdot \frac{\partial}{\partial y}(xy) = x\cos(xy)fy​(x,y)=βˆ‚yβˆ‚β€‹[sin(xy)]=cos(xy)β‹…βˆ‚yβˆ‚β€‹(xy)=xcos(xy)

  3. Evaluate the Partial Derivatives at (0,Ο€)(0, \pi)(0,Ο€):

    fx(0,Ο€)=Ο€β‹…cos⁑(0β‹…Ο€)=Ο€β‹…cos⁑(0)=Ο€(1)=Ο€f_x(0, \pi) = \pi \cdot \cos(0 \cdot \pi) = \pi \cdot \cos(0) = \pi(1) = \pifx​(0,Ο€)=Ο€β‹…cos(0β‹…Ο€)=Ο€β‹…cos(0)=Ο€(1)=Ο€
    fy(0,Ο€)=0β‹…cos⁑(0β‹…Ο€)=0β‹…cos⁑(0)=0(1)=0f_y(0, \pi) = 0 \cdot \cos(0 \cdot \pi) = 0 \cdot \cos(0) = 0(1) = 0fy​(0,Ο€)=0β‹…cos(0β‹…Ο€)=0β‹…cos(0)=0(1)=0

  4. Substitute Components into the Tangent Plane Formula: State the Tangent Plane Equation (defined in Tangent Planes):

    z=z0+fx(x0,y0)(xβˆ’x0)+fy(x0,y0)(yβˆ’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​)(xβˆ’x0​)+fy​(x0​,y0​)(yβˆ’y0​)
    Substitute z0=0,x0=0,y0=Ο€,fx(0,Ο€)=Ο€,fy(0,Ο€)=0z_0 = 0, x_0 = 0, y_0 = \pi, f_x(0, \pi) = \pi, f_y(0, \pi) = 0z0​=0,x0​=0,y0​=Ο€,fx​(0,Ο€)=Ο€,fy​(0,Ο€)=0:
    z=0+Ο€(xβˆ’0)+0(yβˆ’Ο€)z = 0 + \pi(x - 0) + 0(y - \pi)z=0+Ο€(xβˆ’0)+0(yβˆ’Ο€)
    z=Ο€xz = \pi xz=Ο€x

  5. Express in General Linear Form:

    Ο€xβˆ’z=0\pi x - z = 0Ο€xβˆ’z=0

    • Geometric Insight: Because fy(0,Ο€)=0f_y(0, \pi) = 0fy​(0,Ο€)=0, slicing the surface parallel to the yyy-axis produces an instantaneous slope of zero. The tangent plane tilts upward in the positive xxx-direction with slope Ο€\piΟ€, but remains perfectly flat along the yyy-direction.

Practice Problem 5: Concept & Reading Check

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

  • (a) Explain how the surface normal vector nβƒ—=⟨fx(x0,y0),fy(x0,y0),βˆ’1⟩\vec{n} = \langle f_x(x_0, y_0), f_y(x_0, y_0), -1 \ranglen=⟨fx​(x0​,y0​),fy​(x0​,y0​),βˆ’1⟩ is derived from the cross product of the two coordinate trace tangent vectors Tβƒ—x\vec{T}_xTx​ and Tβƒ—y\vec{T}_yTy​. Where does the constant component βˆ’1-1βˆ’1 come from?
  • (b) In Worked Example A, explain why the yyy-term vanishes from the tangent plane equation z=Ο€xz = \pi xz=Ο€x. What does this indicate about the slope of the surface along the cross-section x=0x = 0x=0?
  • (c) In Supersonic Nose Cone Aerodynamic Pressure (Aerospace & Mechanical Engineering), why is finding the unit normal vector n^\hat{n}n^ to the tangent plane essential for calculating the aerodynamic pressure force Fβƒ—p=βˆ’pn^ dA\vec{F}_p = -p \hat{n} \, dAFp​=βˆ’pn^dA?
Solution Key:
  • (a) As derived in Tangent Planes, 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 an xxx-trace curve whose tangent vector is Tβƒ—x=⟨1,0,fx(x0,y0)⟩\vec{T}_x = \langle 1, 0, f_x(x_0, y_0) \rangleTx​=⟨1,0,fx​(x0​,y0​)⟩. Slicing with x=x0x = x_0x=x0​ produces a yyy-trace curve whose tangent vector is Tβƒ—y=⟨0,1,fy(x0,y0)⟩\vec{T}_y = \langle 0, 1, f_y(x_0, y_0) \rangleTy​=⟨0,1,fy​(x0​,y0​)⟩. Because both vectors lie within the tangent plane, their cross product is perpendicular to the plane:
    Tβƒ—xΓ—Tβƒ—y=∣i^j^k^10fx01fy∣=βŸ¨βˆ’fx,βˆ’fy,1⟩\vec{T}_x \times \vec{T}_y = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & 0 & f_x \\ 0 & 1 & f_y \end{vmatrix} = \langle -f_x, -f_y, 1 \rangleTx​×Ty​=​i^10​j^​01​k^fx​fy​​​=βŸ¨βˆ’fx​,βˆ’fy​,1⟩
    Multiplying by βˆ’1-1βˆ’1 produces the downward-pointing normal nβƒ—=⟨fx,fy,βˆ’1⟩\vec{n} = \langle f_x, f_y, -1 \ranglen=⟨fx​,fy​,βˆ’1⟩. The constant βˆ’1-1βˆ’1 arises directly from rearranging the explicit surface equation zβˆ’f(x,y)=0z - f(x, y) = 0zβˆ’f(x,y)=0 into point-normal form.
  • (b) In Worked Example A, evaluating fy(x,y)=xcos⁑(xy)f_y(x, y) = x\cos(xy)fy​(x,y)=xcos(xy) at (0,Ο€)(0, \pi)(0,Ο€) gives fy(0,Ο€)=0β‹…cos⁑(0)=0f_y(0, \pi) = 0 \cdot \cos(0) = 0fy​(0,Ο€)=0β‹…cos(0)=0. In the tangent plane equation z=z0+fx(xβˆ’x0)+fy(yβˆ’y0)z = z_0 + f_x(x - x_0) + f_y(y - y_0)z=z0​+fx​(xβˆ’x0​)+fy​(yβˆ’y0​), the term 0(yβˆ’Ο€)=00(y - \pi) = 00(yβˆ’Ο€)=0, leaving z=Ο€xz = \pi xz=Ο€x. Geometrically, this means that along the vertical trace slice x=0x = 0x=0, the surface has zero instantaneous inclination (a horizontal crest), so moving along yyy produces no vertical elevation change on the tangent plane.
  • (c) In Supersonic Nose Cone Aerodynamic Pressure (Aerospace & Mechanical Engineering), physical fluid mechanics dictates that static gas pressure exerts compressive stress strictly perpendicular to any immersed solid surface. The unit normal vector n^=nβƒ—βˆ₯nβƒ—βˆ₯\hat{n} = \frac{\vec{n}}{\|\vec{n}\|}n^=βˆ₯nβˆ₯n​ extracted from the tangent plane defines the exact spatial direction of incoming air molecule momentum transfer. Aerodynamicists integrate βˆ’pn^ dA-p \hat{n} \, dAβˆ’pn^dA over the nose cone to resolve resultant forces into vehicle lift and drag.
Show your steps and calculations here.

Practice Problem 6

Find the equation of the tangent plane to the elliptic paraboloid z=x2+y2z = x^2 + y^2z=x2+y2 at the point (1,2,5)(1, 2, 5)(1,2,5). Write the final result in general linear form (ax+by+cz=dax + by + cz = dax+by+cz=d).

Solution Key:
  1. Verify the Point on the Surface:

    z0=f(1,2)=12+22=1+4=5z_0 = f(1, 2) = 1^2 + 2^2 = 1 + 4 = 5z0​=f(1,2)=12+22=1+4=5
    The point of tangency is P0(1,2,5)P_0(1, 2, 5)P0​(1,2,5).

  2. Compute General Partial Derivatives: State the Power Rule for Partial Derivatives:

    fx(x,y)=βˆ‚βˆ‚x(x2+y2)=2xf_x(x, y) = \frac{\partial}{\partial x}(x^2 + y^2) = 2xfx​(x,y)=βˆ‚xβˆ‚β€‹(x2+y2)=2x
    fy(x,y)=βˆ‚βˆ‚y(x2+y2)=2yf_y(x, y) = \frac{\partial}{\partial y}(x^2 + y^2) = 2yfy​(x,y)=βˆ‚yβˆ‚β€‹(x2+y2)=2y

  3. Evaluate Derivatives at (1,2)(1, 2)(1,2):

    fx(1,2)=2(1)=2f_x(1, 2) = 2(1) = 2fx​(1,2)=2(1)=2
    fy(1,2)=2(2)=4f_y(1, 2) = 2(2) = 4fy​(1,2)=2(2)=4

  4. Substitute into Tangent Plane Formula: State the Tangent Plane Equation:

    z=z0+fx(x0,y0)(xβˆ’x0)+fy(x0,y0)(yβˆ’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​)(xβˆ’x0​)+fy​(x0​,y0​)(yβˆ’y0​)
    z=5+2(xβˆ’1)+4(yβˆ’2)z = 5 + 2(x - 1) + 4(y - 2)z=5+2(xβˆ’1)+4(yβˆ’2)
    z=5+2xβˆ’2+4yβˆ’8z = 5 + 2x - 2 + 4y - 8z=5+2xβˆ’2+4yβˆ’8
    z=2x+4yβˆ’5z = 2x + 4y - 5z=2x+4yβˆ’5

  5. Convert to Standard General Form:

    2x+4yβˆ’z=52x + 4y - z = 52x+4yβˆ’z=5

    • Normal Vector Note: The surface normal vector is nβƒ—=⟨2,4,βˆ’1⟩=2i^+4j^βˆ’k^\vec{n} = \langle 2, 4, -1 \rangle = 2\hat{i} + 4\hat{j} - \hat{k}n=⟨2,4,βˆ’1⟩=2i^+4j^β€‹βˆ’k^.
Show your steps and calculations here.

Practice Problem 7

Find the equation of the tangent plane to the radical surface z=x+yz = \sqrt{x + y}z=x+y​ at the point (3,1,2)(3, 1, 2)(3,1,2).

Solution Key:
  1. Verify the Surface Height:

    z0=f(3,1)=3+1=4=2z_0 = f(3, 1) = \sqrt{3 + 1} = \sqrt{4} = 2z0​=f(3,1)=3+1​=4​=2

  2. Compute General Partial Derivatives: Let u(x,y)=x+yu(x, y) = x + yu(x,y)=x+y. Applying the Chain Rule:

    fx(x,y)=12(x+y)βˆ’1/2β‹…βˆ‚βˆ‚x(x+y)=12x+yf_x(x, y) = \frac{1}{2}(x + y)^{-1/2} \cdot \frac{\partial}{\partial x}(x + y) = \frac{1}{2\sqrt{x + y}}fx​(x,y)=21​(x+y)βˆ’1/2β‹…βˆ‚xβˆ‚β€‹(x+y)=2x+y​1​
    fy(x,y)=12(x+y)βˆ’1/2β‹…βˆ‚βˆ‚y(x+y)=12x+yf_y(x, y) = \frac{1}{2}(x + y)^{-1/2} \cdot \frac{\partial}{\partial y}(x + y) = \frac{1}{2\sqrt{x + y}}fy​(x,y)=21​(x+y)βˆ’1/2β‹…βˆ‚yβˆ‚β€‹(x+y)=2x+y​1​

  3. Evaluate at the Point (3,1)(3, 1)(3,1):

    fx(3,1)=123+1=12(2)=14f_x(3, 1) = \frac{1}{2\sqrt{3 + 1}} = \frac{1}{2(2)} = \frac{1}{4}fx​(3,1)=23+1​1​=2(2)1​=41​
    fy(3,1)=123+1=12(2)=14f_y(3, 1) = \frac{1}{2\sqrt{3 + 1}} = \frac{1}{2(2)} = \frac{1}{4}fy​(3,1)=23+1​1​=2(2)1​=41​

  4. Substitute into Tangent Plane Formula: State the Tangent Plane Equation:

    z=z0+fx(x0,y0)(xβˆ’x0)+fy(x0,y0)(yβˆ’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​)(xβˆ’x0​)+fy​(x0​,y0​)(yβˆ’y0​)
    z=2+14(xβˆ’3)+14(yβˆ’1)z = 2 + \frac{1}{4}(x - 3) + \frac{1}{4}(y - 1)z=2+41​(xβˆ’3)+41​(yβˆ’1)
    z=2+14xβˆ’34+14yβˆ’14z = 2 + \frac{1}{4}x - \frac{3}{4} + \frac{1}{4}y - \frac{1}{4}z=2+41​xβˆ’43​+41​yβˆ’41​
    z=14x+14y+1z = \frac{1}{4}x + \frac{1}{4}y + 1z=41​x+41​y+1

  5. Clear Fractions to Obtain General Form: Multiply the entire equation by 444:

    4z=x+y+4β€…β€ŠβŸΉβ€…β€Šx+yβˆ’4z=βˆ’44z = x + y + 4 \implies x + y - 4z = -44z=x+y+4⟹x+yβˆ’4z=βˆ’4

Show your steps and calculations here.

Practice Problem 8

Find the equation of the tangent plane to the surface z=xexyz = x e^{xy}z=xexy at the point (2,0,2)(2, 0, 2)(2,0,2).

Solution Key:
  1. Verify the Point on the Surface:

    z0=f(2,0)=2e2β‹…0=2e0=2(1)=2z_0 = f(2, 0) = 2 e^{2 \cdot 0} = 2 e^0 = 2(1) = 2z0​=f(2,0)=2e2β‹…0=2e0=2(1)=2
    The point of tangency is P0(2,0,2)P_0(2, 0, 2)P0​(2,0,2).

  2. Compute General Partial Derivatives:

    • For fx(x,y)f_x(x, y)fx​(x,y): Apply the Multivariable Product Rule because xxx appears both as a linear factor and in the exponential exponent:
      fx(x,y)=βˆ‚βˆ‚x[x]β‹…exy+xβ‹…βˆ‚βˆ‚x[exy]=1β‹…exy+x(yexy)=exy(1+xy)f_x(x, y) = \frac{\partial}{\partial x}[x] \cdot e^{xy} + x \cdot \frac{\partial}{\partial x}[e^{xy}] = 1 \cdot e^{xy} + x(y e^{xy}) = e^{xy}(1 + xy)fx​(x,y)=βˆ‚xβˆ‚β€‹[x]β‹…exy+xβ‹…βˆ‚xβˆ‚β€‹[exy]=1β‹…exy+x(yexy)=exy(1+xy)
    • For fy(x,y)f_y(x, y)fy​(x,y): The leading factor xxx is treated as a constant coefficient. Apply the Exponential Chain Rule:
      fy(x,y)=xβ‹…βˆ‚βˆ‚y[exy]=x(xexy)=x2exyf_y(x, y) = x \cdot \frac{\partial}{\partial y}[e^{xy}] = x(x e^{xy}) = x^2 e^{xy}fy​(x,y)=xβ‹…βˆ‚yβˆ‚β€‹[exy]=x(xexy)=x2exy
  3. Evaluate Partial Derivatives at (2,0)(2, 0)(2,0): Notice that the exponent is xy=2(0)=0xy = 2(0) = 0xy=2(0)=0, so e0=1e^0 = 1e0=1:

    fx(2,0)=e0(1+2β‹…0)=1(1+0)=1f_x(2, 0) = e^0(1 + 2 \cdot 0) = 1(1 + 0) = 1fx​(2,0)=e0(1+2β‹…0)=1(1+0)=1
    fy(2,0)=22e0=4(1)=4f_y(2, 0) = 2^2 e^0 = 4(1) = 4fy​(2,0)=22e0=4(1)=4

  4. Substitute into Tangent Plane Formula: State the Tangent Plane Equation:

    z=z0+fx(x0,y0)(xβˆ’x0)+fy(x0,y0)(yβˆ’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​)(xβˆ’x0​)+fy​(x0​,y0​)(yβˆ’y0​)
    z=2+1(xβˆ’2)+4(yβˆ’0)z = 2 + 1(x - 2) + 4(y - 0)z=2+1(xβˆ’2)+4(yβˆ’0)
    z=2+xβˆ’2+4yβ€…β€ŠβŸΉβ€…β€Šz=x+4yz = 2 + x - 2 + 4y \implies z = x + 4yz=2+xβˆ’2+4y⟹z=x+4y

  5. Convert to Standard General Form:

    x+4yβˆ’z=0x + 4y - z = 0x+4yβˆ’z=0

    • Normal Vector Note: The surface normal vector is nβƒ—=⟨1,4,βˆ’1⟩=i^+4j^βˆ’k^\vec{n} = \langle 1, 4, -1 \rangle = \hat{i} + 4\hat{j} - \hat{k}n=⟨1,4,βˆ’1⟩=i^+4j^β€‹βˆ’k^.

Show your steps and calculations here.

Regroup 2

  • Key Takeaway: The tangent plane to z=f(x,y)z = f(x, y)z=f(x,y) at (x0,y0)(x_0, y_0)(x0​,y0​) has the explicit formula z=z0+fx(xβˆ’x0)+fy(yβˆ’y0)z = z_0 + f_x(x - x_0) + f_y(y - y_0)z=z0​+fx​(xβˆ’x0​)+fy​(yβˆ’y0​). Its normal vector is always nβƒ—=⟨fx,fy,βˆ’1⟩\vec{n} = \langle f_x, f_y, -1 \ranglen=⟨fx​,fy​,βˆ’1⟩.
  • Common Misconception: Students often confuse z0z_0z0​ with zero. Emphasize that z0=f(x0,y0)z_0 = f(x_0, y_0)z0​=f(x0​,y0​) must always be calculated first unless explicitly provided in the problem prompt.
  • Product Rule Alert: When calculating partial derivatives of functions like xexyx e^{xy}xexy, remind students to check whether the differentiated variable appears multiple times in the expression, requiring the product rule.

Skill Block 3

Worked Example A: Estimating a Radical Expression via Linear Approximation

Use a linear approximation at the base point (2,1)(2, 1)(2,1) to estimate the value of f(2.1,0.9)f(2.1, 0.9)f(2.1,0.9) for the function f(x,y)=x2+yf(x, y) = \sqrt{x^2 + y}f(x,y)=x2+y​.

Worked Solution:
  1. Evaluate the True Function at the Base Point (2,1)(2, 1)(2,1):

    f(2,1)=22+1=4+1=5f(2, 1) = \sqrt{2^2 + 1} = \sqrt{4 + 1} = \sqrt{5}f(2,1)=22+1​=4+1​=5​

  2. Compute General First-Order Partial Derivatives: Apply the Generalized Power Rule to f(x,y)=(x2+y)1/2f(x, y) = (x^2 + y)^{1/2}f(x,y)=(x2+y)1/2:

    fx(x,y)=12(x2+y)βˆ’1/2(2x)=xx2+yf_x(x, y) = \frac{1}{2}(x^2 + y)^{-1/2}(2x) = \frac{x}{\sqrt{x^2 + y}}fx​(x,y)=21​(x2+y)βˆ’1/2(2x)=x2+y​x​
    fy(x,y)=12(x2+y)βˆ’1/2(1)=12x2+yf_y(x, y) = \frac{1}{2}(x^2 + y)^{-1/2}(1) = \frac{1}{2\sqrt{x^2 + y}}fy​(x,y)=21​(x2+y)βˆ’1/2(1)=2x2+y​1​

  3. Evaluate the Partial Derivatives at (2,1)(2, 1)(2,1):

    fx(2,1)=222+1=25f_x(2, 1) = \frac{2}{\sqrt{2^2 + 1}} = \frac{2}{\sqrt{5}}fx​(2,1)=22+1​2​=5​2​
    fy(2,1)=1222+1=125f_y(2, 1) = \frac{1}{2\sqrt{2^2 + 1}} = \frac{1}{2\sqrt{5}}fy​(2,1)=222+1​1​=25​1​

  4. Construct the Linearization Function L(x,y)L(x, y)L(x,y): State the Linear Approximation Formula (defined in Linear Approximations):

    L(x,y)=f(x0,y0)+fx(x0,y0)(xβˆ’x0)+fy(x0,y0)(yβˆ’y0)L(x, y) = f(x_0, y_0) + f_x(x_0, y_0)(x - x_0) + f_y(x_0, y_0)(y - y_0)L(x,y)=f(x0​,y0​)+fx​(x0​,y0​)(xβˆ’x0​)+fy​(x0​,y0​)(yβˆ’y0​)
    L(x,y)=5+25(xβˆ’2)+125(yβˆ’1)L(x, y) = \sqrt{5} + \frac{2}{\sqrt{5}}(x - 2) + \frac{1}{2\sqrt{5}}(y - 1)L(x,y)=5​+5​2​(xβˆ’2)+25​1​(yβˆ’1)

  5. Evaluate at the Perturbed Target Point (2.1,0.9)(2.1, 0.9)(2.1,0.9): Calculate coordinate displacements:

    Ξ”x=xβˆ’x0=2.1βˆ’2=0.1\Delta x = x - x_0 = 2.1 - 2 = 0.1Ξ”x=xβˆ’x0​=2.1βˆ’2=0.1
    Ξ”y=yβˆ’y0=0.9βˆ’1=βˆ’0.1\Delta y = y - y_0 = 0.9 - 1 = -0.1Ξ”y=yβˆ’y0​=0.9βˆ’1=βˆ’0.1
    Substitute into L(x,y)L(x, y)L(x,y):
    L(2.1,0.9)=5+25(0.1)+125(βˆ’0.1)L(2.1, 0.9) = \sqrt{5} + \frac{2}{\sqrt{5}}(0.1) + \frac{1}{2\sqrt{5}}(-0.1)L(2.1,0.9)=5​+5​2​(0.1)+25​1​(βˆ’0.1)
    L(2.1,0.9)=5+0.25βˆ’0.055=5+0.155L(2.1, 0.9) = \sqrt{5} + \frac{0.2}{\sqrt{5}} - \frac{0.05}{\sqrt{5}} = \sqrt{5} + \frac{0.15}{\sqrt{5}}L(2.1,0.9)=5​+5​0.2β€‹βˆ’5​0.05​=5​+5​0.15​
    Using the numerical approximation 5β‰ˆ2.23607\sqrt{5} \approx 2.236075β€‹β‰ˆ2.23607:
    L(2.1,0.9)β‰ˆ2.23607+0.152.23607β‰ˆ2.23607+0.06708=2.30315L(2.1, 0.9) \approx 2.23607 + \frac{0.15}{2.23607} \approx 2.23607 + 0.06708 = 2.30315L(2.1,0.9)β‰ˆ2.23607+2.236070.15β€‹β‰ˆ2.23607+0.06708=2.30315

    • Accuracy Check: The exact value is f(2.1,0.9)=2.12+0.9=4.41+0.9=5.31β‰ˆ2.30434f(2.1, 0.9) = \sqrt{2.1^2 + 0.9} = \sqrt{4.41 + 0.9} = \sqrt{5.31} \approx 2.30434f(2.1,0.9)=2.12+0.9​=4.41+0.9​=5.31β€‹β‰ˆ2.30434. The linear approximation error is only ∣2.30434βˆ’2.30315∣=0.00119|2.30434 - 2.30315| = 0.00119∣2.30434βˆ’2.30315∣=0.00119 (0.05%0.05\%0.05% relative error).

Practice Problem 9: Concept & Reading Check

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

  • (a) What is the mathematical and geometric connection between the Tangent Plane equation and the Linearization function L(x,y)L(x, y)L(x,y)?
  • (b) In Worked Example A, explain why (2,1)(2, 1)(2,1) was chosen as the base point rather than evaluating f(2.1,0.9)f(2.1, 0.9)f(2.1,0.9) directly. What two criteria should guide the selection of a base point (x0,y0)(x_0, y_0)(x0​,y0​)?
  • (c) In Autonomous Drone Thrust State Estimation (Robotics & Computer Engineering), why does the quadcopter's flight computer use a linear approximation rather than evaluating the non-linear equation T(x,y)=ln⁑(x2+ey)T(x, y) = \ln(x^2 + e^y)T(x,y)=ln(x2+ey) in real-time?
Solution Key:
  • (a) As defined in Linear Approximations, the equation z=L(x,y)=f(x0,y0)+fx(x0,y0)(xβˆ’x0)+fy(x0,y0)(yβˆ’y0)z = L(x, y) = f(x_0, y_0) + f_x(x_0, y_0)(x - x_0) + f_y(x_0, y_0)(y - y_0)z=L(x,y)=f(x0​,y0​)+fx​(x0​,y0​)(xβˆ’x0​)+fy​(x0​,y0​)(yβˆ’y0​) is algebraically and geometrically identical to the point-normal equation of the tangent plane. The linearization function L(x,y)L(x, y)L(x,y) treats the flat tangent plane as an explicit mathematical function whose outputs approximate the curved surface z=f(x,y)z = f(x, y)z=f(x,y) in the immediate vicinity of the base point.
  • (b) In Worked Example A, evaluating f(2.1,0.9)=5.31f(2.1, 0.9) = \sqrt{5.31}f(2.1,0.9)=5.31​ requires a high-precision radical root extraction algorithm that cannot be done by hand. In contrast, the base point (2,1)(2, 1)(2,1) yields 22+1=52^2 + 1 = 522+1=5, giving clean analytical derivatives. In general, an optimal base point (x0,y0)(x_0, y_0)(x0​,y0​) must satisfy two criteria: (1) Clean Evaluation: f(x0,y0)f(x_0, y_0)f(x0​,y0​) and its partial derivatives must evaluate to simple, known numbers; and (2) Proximity: the displacements Ξ”x=xβˆ’x0\Delta x = x - x_0Ξ”x=xβˆ’x0​ and Ξ”y=yβˆ’y0\Delta y = y - y_0Ξ”y=yβˆ’y0​ must be small so that higher-order curvature errors remain negligible.
  • (c) In Autonomous Drone Thrust State Estimation (Robotics & Computer Engineering), the quadcopter's 32-bit flight controller updates motor commands at 400Β Hz400\text{ Hz}400Β Hz (2.5Β ms2.5\text{ ms}2.5Β ms loop cycle). Computing floating-point transcendental functions (logarithms and exponentials) consumes substantial clock cycles and battery energy. By executing the linear approximation L(x,y)=yL(x, y) = yL(x,y)=y, the microcontroller executes a single register read operation in nanoseconds while introducing less than 0.35%0.35\%0.35% error, well within motor actuator tolerances.
Show your steps and calculations here.

Practice Problem 10

Use the linear approximation of f(x,y)=x2+y2f(x, y) = x^2 + y^2f(x,y)=x2+y2 at the base point (1,1)(1, 1)(1,1) to estimate f(1.1,0.9)f(1.1, 0.9)f(1.1,0.9). Compare your estimate with the exact value and calculate the approximation error.

Solution Key:
  1. Evaluate Baseline Value at Base Point (1,1)(1, 1)(1,1):

    f(1,1)=12+12=1+1=2f(1, 1) = 1^2 + 1^2 = 1 + 1 = 2f(1,1)=12+12=1+1=2

  2. Compute General Partial Derivatives and Evaluate at (1,1)(1, 1)(1,1):

    fx(x,y)=2xβ€…β€ŠβŸΉβ€…β€Šfx(1,1)=2(1)=2f_x(x, y) = 2x \implies f_x(1, 1) = 2(1) = 2fx​(x,y)=2x⟹fx​(1,1)=2(1)=2
    fy(x,y)=2yβ€…β€ŠβŸΉβ€…β€Šfy(1,1)=2(1)=2f_y(x, y) = 2y \implies f_y(1, 1) = 2(1) = 2fy​(x,y)=2y⟹fy​(1,1)=2(1)=2

  3. Construct the Linearization Function L(x,y)L(x, y)L(x,y): State the Linearization Equation:

    L(x,y)=f(1,1)+fx(1,1)(xβˆ’1)+fy(1,1)(yβˆ’1)L(x, y) = f(1, 1) + f_x(1, 1)(x - 1) + f_y(1, 1)(y - 1)L(x,y)=f(1,1)+fx​(1,1)(xβˆ’1)+fy​(1,1)(yβˆ’1)
    L(x,y)=2+2(xβˆ’1)+2(yβˆ’1)L(x, y) = 2 + 2(x - 1) + 2(y - 1)L(x,y)=2+2(xβˆ’1)+2(yβˆ’1)

  4. Evaluate at Target Point (1.1,0.9)(1.1, 0.9)(1.1,0.9): Identify displacements: Ξ”x=1.1βˆ’1=0.1\Delta x = 1.1 - 1 = 0.1Ξ”x=1.1βˆ’1=0.1 and Ξ”y=0.9βˆ’1=βˆ’0.1\Delta y = 0.9 - 1 = -0.1Ξ”y=0.9βˆ’1=βˆ’0.1.

    L(1.1,0.9)=2+2(0.1)+2(βˆ’0.1)=2+0.2βˆ’0.2=2.0L(1.1, 0.9) = 2 + 2(0.1) + 2(-0.1) = 2 + 0.2 - 0.2 = 2.0L(1.1,0.9)=2+2(0.1)+2(βˆ’0.1)=2+0.2βˆ’0.2=2.0

  5. Compare with Exact Value and Calculate Error:

    f(1.1,0.9)=(1.1)2+(0.9)2=1.21+0.81=2.02f(1.1, 0.9) = (1.1)^2 + (0.9)^2 = 1.21 + 0.81 = 2.02f(1.1,0.9)=(1.1)2+(0.9)2=1.21+0.81=2.02
    ApproximationΒ Error=∣f(1.1,0.9)βˆ’L(1.1,0.9)∣=∣2.02βˆ’2.00∣=0.02\text{Approximation Error} = |f(1.1, 0.9) - L(1.1, 0.9)| = |2.02 - 2.00| = 0.02ApproximationΒ Error=∣f(1.1,0.9)βˆ’L(1.1,0.9)∣=∣2.02βˆ’2.00∣=0.02

    • Curvature Insight: The first-order linear contributions canceled exactly (+0.2βˆ’0.2=0+0.2 - 0.2 = 0+0.2βˆ’0.2=0). The remaining discrepancy of 0.020.020.02 represents second-order surface curvature: (Ξ”x)2+(Ξ”y)2=(0.1)2+(βˆ’0.1)2=0.01+0.01=0.02(\Delta x)^2 + (\Delta y)^2 = (0.1)^2 + (-0.1)^2 = 0.01 + 0.01 = 0.02(Ξ”x)2+(Ξ”y)2=(0.1)2+(βˆ’0.1)2=0.01+0.01=0.02.
Show your steps and calculations here.

Practice Problem 11

Use a linear approximation at the base point (4,0)(4, 0)(4,0) to estimate f(4.1,βˆ’0.1)f(4.1, -0.1)f(4.1,βˆ’0.1) for the radical function f(x,y)=x+y+4f(x, y) = \sqrt{x + y + 4}f(x,y)=x+y+4​.

Solution Key:
  1. Evaluate Baseline Value at Base Point (4,0)(4, 0)(4,0):

    f(4,0)=4+0+4=8=22β‰ˆ2.82843f(4, 0) = \sqrt{4 + 0 + 4} = \sqrt{8} = 2\sqrt{2} \approx 2.82843f(4,0)=4+0+4​=8​=22β€‹β‰ˆ2.82843

  2. Compute General Partial Derivatives: Applying the Chain Rule to f(x,y)=(x+y+4)1/2f(x, y) = (x + y + 4)^{1/2}f(x,y)=(x+y+4)1/2:

    fx(x,y)=12x+y+4,fy(x,y)=12x+y+4f_x(x, y) = \frac{1}{2\sqrt{x + y + 4}}, \quad f_y(x, y) = \frac{1}{2\sqrt{x + y + 4}}fx​(x,y)=2x+y+4​1​,fy​(x,y)=2x+y+4​1​

  3. Evaluate Derivatives at (4,0)(4, 0)(4,0):

    fx(4,0)=124+0+4=128=142=28f_x(4, 0) = \frac{1}{2\sqrt{4 + 0 + 4}} = \frac{1}{2\sqrt{8}} = \frac{1}{4\sqrt{2}} = \frac{\sqrt{2}}{8}fx​(4,0)=24+0+4​1​=28​1​=42​1​=82​​
    fy(4,0)=124+0+4=128=142=28f_y(4, 0) = \frac{1}{2\sqrt{4 + 0 + 4}} = \frac{1}{2\sqrt{8}} = \frac{1}{4\sqrt{2}} = \frac{\sqrt{2}}{8}fy​(4,0)=24+0+4​1​=28​1​=42​1​=82​​

  4. Construct Linearization and Evaluate at (4.1,βˆ’0.1)(4.1, -0.1)(4.1,βˆ’0.1): State the Linear Approximation Formula:

    L(x,y)=f(4,0)+fx(4,0)(xβˆ’4)+fy(4,0)(yβˆ’0)L(x, y) = f(4, 0) + f_x(4, 0)(x - 4) + f_y(4, 0)(y - 0)L(x,y)=f(4,0)+fx​(4,0)(xβˆ’4)+fy​(4,0)(yβˆ’0)
    L(x,y)=22+142(xβˆ’4)+142yL(x, y) = 2\sqrt{2} + \frac{1}{4\sqrt{2}}(x - 4) + \frac{1}{4\sqrt{2}}yL(x,y)=22​+42​1​(xβˆ’4)+42​1​y
    Substitute Ξ”x=4.1βˆ’4=0.1\Delta x = 4.1 - 4 = 0.1Ξ”x=4.1βˆ’4=0.1 and Ξ”y=βˆ’0.1βˆ’0=βˆ’0.1\Delta y = -0.1 - 0 = -0.1Ξ”y=βˆ’0.1βˆ’0=βˆ’0.1:
    L(4.1,βˆ’0.1)=22+142(0.1)+142(βˆ’0.1)L(4.1, -0.1) = 2\sqrt{2} + \frac{1}{4\sqrt{2}}(0.1) + \frac{1}{4\sqrt{2}}(-0.1)L(4.1,βˆ’0.1)=22​+42​1​(0.1)+42​1​(βˆ’0.1)
    L(4.1,βˆ’0.1)=22+0.1βˆ’0.142=22+0=22β‰ˆ2.82843L(4.1, -0.1) = 2\sqrt{2} + \frac{0.1 - 0.1}{4\sqrt{2}} = 2\sqrt{2} + 0 = 2\sqrt{2} \approx 2.82843L(4.1,βˆ’0.1)=22​+42​0.1βˆ’0.1​=22​+0=22β€‹β‰ˆ2.82843

    • Remarkable Geometric Note: Notice that Ξ”x+Ξ”y=0.1βˆ’0.1=0\Delta x + \Delta y = 0.1 - 0.1 = 0Ξ”x+Ξ”y=0.1βˆ’0.1=0, so the exact evaluation is f(4.1,βˆ’0.1)=4.1βˆ’0.1+4=8=22f(4.1, -0.1) = \sqrt{4.1 - 0.1 + 4} = \sqrt{8} = 2\sqrt{2}f(4.1,βˆ’0.1)=4.1βˆ’0.1+4​=8​=22​. Because the level curves of this surface are parallel lines x+y=Cx + y = Cx+y=C, the linear approximation yielded the exact true value.
Show your steps and calculations here.

Practice Problem 12

The storage capacity of a cylindrical industrial chemical tank is given by V(r,h)=Ο€r2hV(r, h) = \pi r^2 hV(r,h)=Ο€r2h. During construction, field measurements record a radius of r=2.0Β mr = 2.0\text{ m}r=2.0Β m with a maximum measurement uncertainty of dr=Β±0.02Β mdr = \pm 0.02\text{ m}dr=Β±0.02Β m and a height of h=5.0Β mh = 5.0\text{ m}h=5.0Β m with an uncertainty of dh=Β±0.05Β mdh = \pm 0.05\text{ m}dh=Β±0.05Β m.

  1. Compute the total differential dVdVdV in terms of r,h,dr,r, h, dr,r,h,dr, and dhdhdh.
  2. Use dVdVdV to estimate the maximum worst-case absolute error in the calculated volume.
  3. Determine the maximum relative error dVV\frac{dV}{V}VdV​ and percentage error in the storage volume.
Solution Key:
  1. Compute Partial Derivatives and State Total Differential: State the Total Differential Formula (defined in Differentials and Error Propagation):

    dV=βˆ‚Vβˆ‚rdr+βˆ‚Vβˆ‚hdhdV = \frac{\partial V}{\partial r} dr + \frac{\partial V}{\partial h} dhdV=βˆ‚rβˆ‚V​dr+βˆ‚hβˆ‚V​dh
    Differentiate V(r,h)=Ο€r2hV(r, h) = \pi r^2 hV(r,h)=Ο€r2h:
    βˆ‚Vβˆ‚r=2Ο€rh,βˆ‚Vβˆ‚h=Ο€r2\frac{\partial V}{\partial r} = 2\pi r h, \quad \frac{\partial V}{\partial h} = \pi r^2βˆ‚rβˆ‚V​=2Ο€rh,βˆ‚hβˆ‚V​=Ο€r2
    dV=2Ο€rh dr+Ο€r2 dhdV = 2\pi r h \, dr + \pi r^2 \, dhdV=2Ο€rhdr+Ο€r2dh

  2. Estimate Maximum Absolute Error at (r,h)=(2.0,5.0)(r, h) = (2.0, 5.0)(r,h)=(2.0,5.0): Evaluate sensitivity coefficients:

    βˆ‚Vβˆ‚r(2,5)=2Ο€(2.0)(5.0)=20Ο€\frac{\partial V}{\partial r}(2, 5) = 2\pi(2.0)(5.0) = 20\piβˆ‚rβˆ‚V​(2,5)=2Ο€(2.0)(5.0)=20Ο€
    βˆ‚Vβˆ‚h(2,5)=Ο€(2.0)2=4Ο€\frac{\partial V}{\partial h}(2, 5) = \pi(2.0)^2 = 4\piβˆ‚hβˆ‚V​(2,5)=Ο€(2.0)2=4Ο€
    Apply worst-case tolerances ∣drβˆ£β‰€0.02Β m|dr| \le 0.02\text{ m}∣drβˆ£β‰€0.02Β m and ∣dhβˆ£β‰€0.05Β m|dh| \le 0.05\text{ m}∣dhβˆ£β‰€0.05Β m using the Triangle Inequality:
    ∣dV∣maxβ‘β‰€βˆ£βˆ‚Vβˆ‚r∣∣dr∣+βˆ£βˆ‚Vβˆ‚h∣∣dh∣|dV|_{\max} \le \left|\frac{\partial V}{\partial r}\right| |dr| + \left|\frac{\partial V}{\partial h}\right| |dh|∣dV∣maxβ€‹β‰€β€‹βˆ‚rβˆ‚Vβ€‹β€‹βˆ£dr∣+β€‹βˆ‚hβˆ‚Vβ€‹β€‹βˆ£dh∣
    ∣dV∣max⁑≀(20Ο€)(0.02)+(4Ο€)(0.05)=0.40Ο€+0.20Ο€=0.60Ο€β‰ˆ1.8850Β m3|dV|_{\max} \le (20\pi)(0.02) + (4\pi)(0.05) = 0.40\pi + 0.20\pi = 0.60\pi \approx 1.8850\text{ m}^3∣dV∣max​≀(20Ο€)(0.02)+(4Ο€)(0.05)=0.40Ο€+0.20Ο€=0.60Ο€β‰ˆ1.8850Β m3

  3. Compute Relative and Percentage Error: The nominal tank volume is V(2,5)=Ο€(2.0)2(5.0)=20π m3β‰ˆ62.8319Β m3V(2, 5) = \pi(2.0)^2(5.0) = 20\pi\text{ m}^3 \approx 62.8319\text{ m}^3V(2,5)=Ο€(2.0)2(5.0)=20π m3β‰ˆ62.8319Β m3. State the Relative Error Formula:

    dVV=2Ο€rh dr+Ο€r2 dhΟ€r2h=2drr+dhh\frac{dV}{V} = \frac{2\pi r h \, dr + \pi r^2 \, dh}{\pi r^2 h} = 2\frac{dr}{r} + \frac{dh}{h}VdV​=Ο€r2h2Ο€rhdr+Ο€r2dh​=2rdr​+hdh​
    Substitute relative measurement uncertainties:
    drr=0.022.0=0.01(1.0%),dhh=0.055.0=0.01(1.0%)\frac{dr}{r} = \frac{0.02}{2.0} = 0.01 \quad (1.0\%), \quad \frac{dh}{h} = \frac{0.05}{5.0} = 0.01 \quad (1.0\%)rdr​=2.00.02​=0.01(1.0%),hdh​=5.00.05​=0.01(1.0%)
    dVV=2(0.01)+0.01=0.02+0.01=0.030\frac{dV}{V} = 2(0.01) + 0.01 = 0.02 + 0.01 = 0.030VdV​=2(0.01)+0.01=0.02+0.01=0.030
    PercentageΒ Error=0.030Γ—100%=3.0%\text{Percentage Error} = 0.030 \times 100\% = 3.0\%PercentageΒ Error=0.030Γ—100%=3.0%

    • Engineering Sensitivity Takeaway: Because the radius is squared in the volume formula (r2r^2r2), its relative measurement uncertainty contributes with a weight factor of 222, while height contributes with a weight factor of 111. Precision control on radius is twice as critical to tank capacity accuracy as height.

Show your steps and calculations here.

Regroup 3

  • Key Takeaway: The total differential dz=fxdx+fydydz = f_x dx + f_y dydz=fx​dx+fy​dy approximates the true change Ξ”z\Delta zΞ”z by measuring vertical displacement along the flat tangent plane rather than the curved surface.
  • Common Misconception: Students often forget to take absolute values when estimating maximum worst-case error. If dr=Β±0.02dr = \pm 0.02dr=Β±0.02 and dh=Β±0.05dh = \pm 0.05dh=Β±0.05, the worst-case scenario occurs when both errors push the output in the same direction, requiring ∣fx∣∣dx∣+∣fy∣∣dh∣|f_x| |dx| + |f_y| |dh|∣fxβ€‹βˆ£βˆ£dx∣+∣fyβ€‹βˆ£βˆ£dh∣.
  • Relative Error Shortcut: In power products of the form f(x,y)=Cxmynf(x, y) = C x^m y^nf(x,y)=Cxmyn, logarithmic differentiation reveals that relative error is simply dff=mdxx+ndyy\frac{df}{f} = m \frac{dx}{x} + n \frac{dy}{y}fdf​=mxdx​+nydy​, providing an instantaneous mental check for engineering tolerance studies.

Synthesis Wrap-up

  • Core Takeaways from Session 10:
    1. Planes in 3D Space: Uniquely oriented by a normal vector nβƒ—=⟨a,b,c⟩\vec{n} = \langle a, b, c \ranglen=⟨a,b,c⟩. The scalar equation a(xβˆ’x0)+b(yβˆ’y0)+c(zβˆ’z0)=0a(x-x_0) + b(y-y_0) + c(z-z_0) = 0a(xβˆ’x0​)+b(yβˆ’y0​)+c(zβˆ’z0​)=0 expresses that every displacement vector in the plane is orthogonal to nβƒ—\vec{n}n.
    2. Tangent Planes to Surfaces: For any differentiable multivariable surface z=f(x,y)z = f(x, y)z=f(x,y), the surface normal vector is nβƒ—=⟨fx,fy,βˆ’1⟩\vec{n} = \langle f_x, f_y, -1 \ranglen=⟨fx​,fy​,βˆ’1⟩, yielding the tangent plane z=z0+fx(xβˆ’x0)+fy(yβˆ’y0)z = z_0 + f_x(x-x_0) + f_y(y-y_0)z=z0​+fx​(xβˆ’x0​)+fy​(yβˆ’y0​).
    3. Linearization & Differentials: The tangent plane acts as a local computational proxy L(x,y)L(x, y)L(x,y). The total differential dz=fxdx+fydydz = f_x dx + f_y dydz=fx​dx+fy​dy provides a rapid first-order tool for propagating measurement tolerances and analyzing system sensitivities.
  • Overview of Knewton Alta Homework:
    • Tangent Planes and Linear Approximations of Functions of Several Variables: Focus on calculating partial derivatives accurately, converting equations between point-normal and standard general forms, evaluating linearizations at nearby offsets Ξ”x,Ξ”y\Delta x, \Delta yΞ”x,Ξ”y, and bounding total differentials in physical measurement applications.