⚠️ DRAFT HANDOUT - NOT FINALIZED BY INSTRUCTOR - DO NOT PRINT YET

MATH-283 (Calculus III) Curriculum

Session 03 - Dot and Cross Product

Handout Worksheet
Fall Semester 2026
Session Objectives & Overview

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

  • Review core multivariable mathematical concepts and engineering calculus prerequisites.

Micro-Lecture

Engineering Context: Quantifying Force

In this session, we investigate the mathematical principles of Dot and Cross Product and explore how engineers apply these concepts to analyze real-world physical and structural systems.

Skill Block 1

Worked Example

Find the dot product of uβƒ—=⟨6,7⟩\vec{u} = \langle 6, 7 \rangleu=⟨6,7⟩ and vβƒ—=⟨7,βˆ’6⟩\vec{v} = \langle 7, -6 \ranglev=⟨7,βˆ’6⟩.

Worked Solution:

Here is the step-by-step solution to the problem presented in the image:

Problem Statement

Find the dot product of uβƒ—=⟨6,7⟩\vec{u} = \langle 6, 7 \rangleu=⟨6,7⟩ and vβƒ—=⟨7,βˆ’6⟩\vec{v} = \langle 7, -6 \ranglev=⟨7,βˆ’6⟩.

Formula

For two 2D vectors uβƒ—=⟨ux,uy⟩\vec{u} = \langle u_x, u_y \rangleu=⟨ux​,uyβ€‹βŸ© and vβƒ—=⟨vx,vy⟩\vec{v} = \langle v_x, v_y \ranglev=⟨vx​,vyβ€‹βŸ©, the dot product is calculated as:

uβƒ—β‹…vβƒ—=(uxβ‹…vx)+(uyβ‹…vy)\vec{u} \cdot \vec{v} = (u_x \cdot v_x) + (u_y \cdot v_y)uβ‹…v=(ux​⋅vx​)+(uy​⋅vy​)

Step-by-Step Calculation
  1. Identify the components of each vector:
  • ux=6u_x = 6ux​=6, uy=7u_y = 7uy​=7

  • vx=7v_x = 7vx​=7, vy=βˆ’6v_y = -6vy​=βˆ’6

  1. Substitute the values into the formula:

uβƒ—β‹…vβƒ—=(6β‹…7)+(7β‹…βˆ’6)\vec{u} \cdot \vec{v} = (6 \cdot 7) + (7 \cdot -6)uβ‹…v=(6β‹…7)+(7β‹…βˆ’6)

  1. Simplify the terms:

uβƒ—β‹…vβƒ—=42+(βˆ’42)\vec{u} \cdot \vec{v} = 42 + (-42)uβ‹…v=42+(βˆ’42)

  1. Combine the results:

u⃗⋅v⃗=0\vec{u} \cdot \vec{v} = 0u⋅v=0

Final Answer

The dot product is 000.

(Note: Since the dot product is exactly zero, these two vectors are orthogonal or perpendicular to each other).

Active Practice Problem

Find the dot product of uβƒ—=3i^βˆ’2j^\vec{u} = 3\hat{i} - 2\hat{j}u=3i^βˆ’2j^​ and vβƒ—=4i^βˆ’5j^\vec{v} = 4\hat{i} - 5\hat{j}v=4i^βˆ’5j^​.

Workspace
Solution

Here is the step-by-step solution to the problem in the image:

Problem Statement

Find the dot product of uβƒ—=3i^βˆ’2j^\vec{u} = 3\hat{i} - 2\hat{j}u=3i^βˆ’2j^​ and vβƒ—=4i^βˆ’5j^\vec{v} = 4\hat{i} - 5\hat{j}v=4i^βˆ’5j^​.

Formula

When vectors are written in unit vector notation (i^,j^\hat{i}, \hat{j}i^,j^​), the dot product multiplies the corresponding components together:

uβƒ—β‹…vβƒ—=(uxβ‹…vx)+(uyβ‹…vy)\vec{u} \cdot \vec{v} = (u_x \cdot v_x) + (u_y \cdot v_y)uβ‹…v=(ux​⋅vx​)+(uy​⋅vy​)

Step-by-Step Calculation
  1. Identify the components of each vector:
  • uβƒ—\vec{u}u: ux=3u_x = 3ux​=3, uy=βˆ’2u_y = -2uy​=βˆ’2

  • vβƒ—\vec{v}v: vx=4v_x = 4vx​=4, vy=βˆ’5v_y = -5vy​=βˆ’5

  1. Substitute the values into the formula:

uβƒ—β‹…vβƒ—=(3β‹…4)+(βˆ’2β‹…βˆ’5)\vec{u} \cdot \vec{v} = (3 \cdot 4) + (-2 \cdot -5)uβ‹…v=(3β‹…4)+(βˆ’2β‹…βˆ’5)

  1. Multiply the components:
  • For the i^\hat{i}i^ components: 3β‹…4=123 \cdot 4 = 123β‹…4=12

  • For the j^\hat{j}j^​ components: βˆ’2β‹…βˆ’5=10-2 \cdot -5 = 10βˆ’2β‹…βˆ’5=10

  1. Add the results together:

u⃗⋅v⃗=12+10\vec{u} \cdot \vec{v} = 12 + 10u⋅v=12+10

u⃗⋅v⃗=22\vec{u} \cdot \vec{v} = 22u⋅v=22

Final Answer

The dot product is 222222.

Extra Practice & Extensions

Regroup 1

  • Review common misconceptions and clarify key notations.

Skill Block 2

Worked Example

Calculate pβƒ—Γ—qβƒ—\vec{p} \times \vec{q}p​×q​ using a determinant if pβƒ—=2i^+4j^\vec{p} = 2\hat{i} + 4\hat{j}p​=2i^+4j^​ and qβƒ—=βˆ’4i^βˆ’5j^\vec{q} = -4\hat{i} - 5\hat{j}q​=βˆ’4i^βˆ’5j^​.

Worked Solution:

Here is the step-by-step solution to the problem in the image:

Problem Statement

Calculate pβƒ—Γ—qβƒ—\vec{p} \times \vec{q}p​×q​ using a determinant if pβƒ—=2i^+4j^\vec{p} = 2\hat{i} + 4\hat{j}p​=2i^+4j^​ and qβƒ—=βˆ’4i^βˆ’5j^\vec{q} = -4\hat{i} - 5\hat{j}q​=βˆ’4i^βˆ’5j^​.

Formula

Even though these vectors are in 2D (i^\hat{i}i^ and j^\hat{j}j^​ components), the cross product requires a 3D space because the resulting vector points perpendicular to the xyxyxy-plane (along the k^\hat{k}k^ axis). We treat the k^\hat{k}k^ components as 000:

pβƒ—Γ—qβƒ—=∣i^j^k^pxpypzqxqyqz∣\vec{p} \times \vec{q} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ p_x & p_y & p_z \\ q_x & q_y & q_z \end{vmatrix}p​×q​=​i^px​qx​​j^​py​qy​​k^pz​qz​​​

Step-by-Step Calculation
  1. Set up the matrix determinant with pz=0p_z = 0pz​=0 and qz=0q_z = 0qz​=0:

pβƒ—Γ—qβƒ—=∣i^j^k^240βˆ’4βˆ’50∣\vec{p} \times \vec{q} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 2 & 4 & 0 \\ -4 & -5 & 0 \end{vmatrix}p​×q​=​i^2βˆ’4​j^​4βˆ’5​k^00​​

  1. Expand the determinant along the top row:

pβƒ—Γ—qβƒ—=i^∣40βˆ’50βˆ£βˆ’j^∣20βˆ’40∣+k^∣24βˆ’4βˆ’5∣\vec{p} \times \vec{q} = \hat{i}\begin{vmatrix} 4 & 0 \\ -5 & 0 \end{vmatrix} - \hat{j}\begin{vmatrix} 2 & 0 \\ -4 & 0 \end{vmatrix} + \hat{k}\begin{vmatrix} 2 & 4 \\ -4 & -5 \end{vmatrix}p​×q​=i^​4βˆ’5​00β€‹β€‹βˆ’j^​​2βˆ’4​00​​+k^​2βˆ’4​4βˆ’5​​

  1. Evaluate each 2x2 minor:
  • i^\hat{i}i^ component: (4β‹…0)βˆ’(0β‹…βˆ’5)=0(4 \cdot 0) - (0 \cdot -5) = 0(4β‹…0)βˆ’(0β‹…βˆ’5)=0

  • j^\hat{j}j^​ component: (2β‹…0)βˆ’(0β‹…βˆ’4)=0(2 \cdot 0) - (0 \cdot -4) = 0(2β‹…0)βˆ’(0β‹…βˆ’4)=0

  • k^\hat{k}k^ component: (2β‹…βˆ’5)βˆ’(4β‹…βˆ’4)=βˆ’10βˆ’(βˆ’16)=βˆ’10+16=6(2 \cdot -5) - (4 \cdot -4) = -10 - (-16) = -10 + 16 = 6(2β‹…βˆ’5)βˆ’(4β‹…βˆ’4)=βˆ’10βˆ’(βˆ’16)=βˆ’10+16=6

  1. Combine the components:

pβƒ—Γ—qβƒ—=0i^βˆ’0j^+6k^\vec{p} \times \vec{q} = 0\hat{i} - 0\hat{j} + 6\hat{k}p​×q​=0i^βˆ’0j^​+6k^

pβƒ—Γ—qβƒ—=6k^\vec{p} \times \vec{q} = 6\hat{k}p​×q​=6k^

Final Answer

The cross product is 6k^6\hat{k}6k^ (or ⟨0,0,6⟩\langle 0, 0, 6 \rangle⟨0,0,6⟩).

Active Practice Problem

Calculate rβƒ—Γ—Fβƒ—\vec{r} \times \vec{F}rΓ—F where rβƒ—=⟨3,2⟩\vec{r} = \langle 3, 2 \rangler=⟨3,2⟩ and Fβƒ—=βŸ¨βˆ’2,5⟩\vec{F} = \langle -2, 5 \rangleF=βŸ¨βˆ’2,5⟩.

Workspace
Solution

Here is the step-by-step solution to the problem in the image:

Problem Statement

Calculate rβƒ—Γ—Fβƒ—\vec{r} \times \vec{F}rΓ—F where rβƒ—=⟨3,2⟩\vec{r} = \langle 3, 2 \rangler=⟨3,2⟩ and Fβƒ—=βŸ¨βˆ’2,5⟩\vec{F} = \langle -2, 5 \rangleF=βŸ¨βˆ’2,5⟩.

Formula

For 2D vectors lying in the xyxyxy-plane, we extend them into 3D by setting their zzz-components to 000 (rz=0r_z = 0rz​=0 and Fz=0F_z = 0Fz​=0). The cross product is computed using a 3Γ—33 \times 33Γ—3 determinant:

rβƒ—Γ—Fβƒ—=∣i^j^k^rxryrzFxFyFz∣\vec{r} \times \vec{F} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ r_x & r_y & r_z \\ F_x & F_y & F_z \end{vmatrix}rΓ—F=​i^rx​Fx​​j^​ry​Fy​​k^rz​Fz​​​

Step-by-Step Calculation
  1. Set up the determinant matrix:

rβƒ—Γ—Fβƒ—=∣i^j^k^320βˆ’250∣\vec{r} \times \vec{F} = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 3 & 2 & 0 \\ -2 & 5 & 0 \end{vmatrix}rΓ—F=​i^3βˆ’2​j^​25​k^00​​

  1. Expand the determinant along the top row:

rβƒ—Γ—Fβƒ—=i^∣2050βˆ£βˆ’j^∣30βˆ’20∣+k^∣32βˆ’25∣\vec{r} \times \vec{F} = \hat{i}\begin{vmatrix} 2 & 0 \\ 5 & 0 \end{vmatrix} - \hat{j}\begin{vmatrix} 3 & 0 \\ -2 & 0 \end{vmatrix} + \hat{k}\begin{vmatrix} 3 & 2 \\ -2 & 5 \end{vmatrix}rΓ—F=i^​25​00β€‹β€‹βˆ’j^​​3βˆ’2​00​​+k^​3βˆ’2​25​​

  1. Evaluate the 2x2 minors:
  • i^\hat{i}i^ component: (2β‹…0)βˆ’(0β‹…5)=0(2 \cdot 0) - (0 \cdot 5) = 0(2β‹…0)βˆ’(0β‹…5)=0

  • j^\hat{j}j^​ component: (3β‹…0)βˆ’(0β‹…βˆ’2)=0(3 \cdot 0) - (0 \cdot -2) = 0(3β‹…0)βˆ’(0β‹…βˆ’2)=0

  • k^\hat{k}k^ component: (3β‹…5)βˆ’(2β‹…βˆ’2)=15βˆ’(βˆ’4)=15+4=19(3 \cdot 5) - (2 \cdot -2) = 15 - (-4) = 15 + 4 = 19(3β‹…5)βˆ’(2β‹…βˆ’2)=15βˆ’(βˆ’4)=15+4=19

  1. Combine the components:

rβƒ—Γ—Fβƒ—=0i^βˆ’0j^+19k^\vec{r} \times \vec{F} = 0\hat{i} - 0\hat{j} + 19\hat{k}rΓ—F=0i^βˆ’0j^​+19k^

r⃗×F⃗=19k^\vec{r} \times \vec{F} = 19\hat{k}r×F=19k^

Final Answer

The cross product is 19k^19\hat{k}19k^ (or written in component form as ⟨0,0,19⟩\langle 0, 0, 19 \rangle⟨0,0,19⟩).

Extra Practice & Extensions

Regroup 2

  • Reflect on the physical modeling applications and mathematical setups.

Skill Block 3

Worked Example

Find aβƒ—β‹…bβƒ—\vec{a} \cdot \vec{b}aβ‹…b if ∣aβƒ—βˆ£=16Β N|\vec{a}| = 16\text{ N}∣a∣=16Β N, ∣bβƒ—βˆ£=5Β m|\vec{b}| = 5\text{ m}∣b∣=5Β m, and the angle between aβƒ—\vec{a}a and bβƒ—\vec{b}b is 77∘77^\circ77∘. Express the answer rounded to two decimal places.

Worked Solution:

Here is the step-by-step solution to the problem in the image:

Problem Statement

Find aβƒ—β‹…bβƒ—\vec{a} \cdot \vec{b}aβ‹…b if ∣aβƒ—βˆ£=16Β N|\vec{a}| = 16\text{ N}∣a∣=16Β N, ∣bβƒ—βˆ£=5Β m|\vec{b}| = 5\text{ m}∣b∣=5Β m, and the angle between aβƒ—\vec{a}a and bβƒ—\vec{b}b is 77∘77^\circ77∘. Express the answer rounded to two decimal places.

Formula

When given the magnitudes of two vectors and the angle ΞΈ\thetaΞΈ between them, the geometric definition of the dot product is used:

aβƒ—β‹…bβƒ—=∣aβƒ—βˆ£βˆ£bβƒ—βˆ£cos⁑θ\vec{a} \cdot \vec{b} = |\vec{a}| |\vec{b}| \cos \thetaaβ‹…b=∣a∣∣b∣cosΞΈ

Step-by-Step Calculation
  1. Identify the given values:
  • Magnitude of aβƒ—\vec{a}a: ∣aβƒ—βˆ£=16|\vec{a}| = 16∣a∣=16

  • Magnitude of bβƒ—\vec{b}b: ∣bβƒ—βˆ£=5|\vec{b}| = 5∣b∣=5

  • Angle: ΞΈ=77∘\theta = 77^\circΞΈ=77∘

  1. Substitute the values into the formula:

aβƒ—β‹…bβƒ—=16β‹…5β‹…cos⁑(77∘)\vec{a} \cdot \vec{b} = 16 \cdot 5 \cdot \cos(77^\circ)aβ‹…b=16β‹…5β‹…cos(77∘)

  1. Simplify the multiplication:

16β‹…5=8016 \cdot 5 = 8016β‹…5=80

aβƒ—β‹…bβƒ—=80β‹…cos⁑(77∘)\vec{a} \cdot \vec{b} = 80 \cdot \cos(77^\circ)aβ‹…b=80β‹…cos(77∘)

  1. Calculate the cosine value (ensure your calculator is in Degree mode):

cos⁑(77∘)β‰ˆ0.224951\cos(77^\circ) \approx 0.224951cos(77∘)β‰ˆ0.224951

  1. Multiply to find the dot product:

aβƒ—β‹…bβƒ—β‰ˆ80β‹…0.224951=17.99608\vec{a} \cdot \vec{b} \approx 80 \cdot 0.224951 = 17.99608aβ‹…bβ‰ˆ80β‹…0.224951=17.99608

  1. Round to two decimal places:

aβƒ—β‹…bβƒ—β‰ˆ18.00\vec{a} \cdot \vec{b} \approx 18.00aβ‹…bβ‰ˆ18.00

Final Answer

The dot product is 18.0018.0018.00 (or 18.00Β J18.00\text{ J}18.00Β J / Nβ‹…m\text{N} \cdot \text{m}Nβ‹…m if keeping track of the physical work units).

Active Practice Problem

Find the work (in Joules) done by the force Fβƒ—=⟨4,βˆ’4,4⟩\vec{F} = \langle 4, -4, 4 \rangleF=⟨4,βˆ’4,4⟩ (in Newtons) acting on a particle as it moves from point P(βˆ’7,βˆ’2,5)P(-7, -2, 5)P(βˆ’7,βˆ’2,5) to point Q(8,βˆ’7,βˆ’5)Q(8, -7, -5)Q(8,βˆ’7,βˆ’5) along a straight line. The coordinates of PPP and QQQ are measured in meters.

Units:

  • 1Β N=1Β kgβ‹…m/s21\text{ N} = 1\text{ kg} \cdot \text{m/s}^21Β N=1Β kgβ‹…m/s2
  • 1Β J=1Β Nβ‹…m1\text{ J} = 1\text{ N} \cdot \text{m}1Β J=1Β Nβ‹…m
Workspace
Solution

Here is the step-by-step solution to the problem in the image:

Problem Statement

Find the work (in Joules) done by the force Fβƒ—=⟨4,βˆ’4,4⟩\vec{F} = \langle 4, -4, 4 \rangleF=⟨4,βˆ’4,4⟩ (in Newtons) acting on a particle as it moves from point P(βˆ’7,βˆ’2,5)P(-7, -2, 5)P(βˆ’7,βˆ’2,5) to point Q(8,βˆ’7,βˆ’5)Q(8, -7, -5)Q(8,βˆ’7,βˆ’5) along a straight line. The coordinates of PPP and QQQ are measured in meters.

Formula

Work (WWW) done by a constant force vector F⃗\vec{F}F over a displacement vector d⃗\vec{d}d is given by the dot product:

W=F⃗⋅d⃗W = \vec{F} \cdot \vec{d}W=F⋅d

Where the displacement vector d⃗\vec{d}d from a starting point PPP to an ending point QQQ is calculated as:

dβƒ—=PQβƒ—=⟨xQβˆ’xP,Β yQβˆ’yP,Β zQβˆ’zP⟩\vec{d} = \vec{PQ} = \langle x_Q - x_P, \ y_Q - y_P, \ z_Q - z_P \rangled=PQ​=⟨xQβ€‹βˆ’xP​,Β yQβ€‹βˆ’yP​,Β zQβ€‹βˆ’zPβ€‹βŸ©

Step-by-Step Calculation
Step 1: Find the displacement vector d⃗\vec{d}d

Subtract the coordinates of the initial point P(βˆ’7,βˆ’2,5)P(-7, -2, 5)P(βˆ’7,βˆ’2,5) from the final point Q(8,βˆ’7,βˆ’5)Q(8, -7, -5)Q(8,βˆ’7,βˆ’5):

  • dx=8βˆ’(βˆ’7)=8+7=15d_x = 8 - (-7) = 8 + 7 = 15dx​=8βˆ’(βˆ’7)=8+7=15

  • dy=βˆ’7βˆ’(βˆ’2)=βˆ’7+2=βˆ’5d_y = -7 - (-2) = -7 + 2 = -5dy​=βˆ’7βˆ’(βˆ’2)=βˆ’7+2=βˆ’5

  • dz=βˆ’5βˆ’5=βˆ’10d_z = -5 - 5 = -10dz​=βˆ’5βˆ’5=βˆ’10

So, the displacement vector is:

dβƒ—=⟨15,βˆ’5,βˆ’10⟩ m\vec{d} = \langle 15, -5, -10 \rangle\text{ m}d=⟨15,βˆ’5,βˆ’10⟩ m

Step 2: Calculate the work using the dot product

Now, take the dot product of the force vector Fβƒ—=⟨4,βˆ’4,4⟩\vec{F} = \langle 4, -4, 4 \rangleF=⟨4,βˆ’4,4⟩ and the displacement vector dβƒ—=⟨15,βˆ’5,βˆ’10⟩\vec{d} = \langle 15, -5, -10 \rangled=⟨15,βˆ’5,βˆ’10⟩:

W=Fβƒ—β‹…dβƒ—=(4β‹…15)+(βˆ’4β‹…βˆ’5)+(4β‹…βˆ’10)W = \vec{F} \cdot \vec{d} = (4 \cdot 15) + (-4 \cdot -5) + (4 \cdot -10)W=Fβ‹…d=(4β‹…15)+(βˆ’4β‹…βˆ’5)+(4β‹…βˆ’10)

Step 3: Simplify the terms
  • 4β‹…15=604 \cdot 15 = 604β‹…15=60

  • βˆ’4β‹…βˆ’5=20-4 \cdot -5 = 20βˆ’4β‹…βˆ’5=20

  • 4β‹…βˆ’10=βˆ’404 \cdot -10 = -404β‹…βˆ’10=βˆ’40

Combine the values:

W=60+20βˆ’40W = 60 + 20 - 40W=60+20βˆ’40

W=40Β JW = 40\text{ J}W=40Β J

Final Answer

The work done by the force is 40Β Joules40\text{ Joules}40Β Joules.

Extra Practice & Extensions

Regroup 3

  • Verify calculations and mathematical reasoning.

Synthesis Wrap-up

  • Core takeaways from Session 03 and overview of homework homework assignment: The Dot Product The Cross Product.