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MATH-283 (Calculus III) Curriculum

Session 05 - Vector-Valued Functions and Derivatives

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: Motion in Mechanical Systems

In this session, we investigate the mathematical principles of Vector-Valued Functions and Derivatives and explore how engineers apply these concepts to analyze real-world physical and structural systems.

Skill Block 1

Worked Example

Determine the domain of r⃗(t)=⟨t+2,−9t+3,−7t−5⟩\vec{r}(t) = \left\langle \sqrt{t+2}, \frac{-9}{t+3}, \frac{-7}{\sqrt{t-5}} \right\rangler(t)=⟨t+2​,t+3−9​,t−5​−7​⟩ and plot the function using Desmos.

Worked Solution:

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

Problem Statement

Determine the domain of the vector-valued function:

r⃗(t)=⟨t+2,−9t+3,−7t−5⟩\vec{r}(t) = \left\langle \sqrt{t+2}, \frac{-9}{t+3}, \frac{-7}{\sqrt{t-5}} \right\rangler(t)=⟨t+2​,t+3−9​,t−5​−7​⟩

To find the domain of a vector-valued function, we must find the intersection of the domains of its individual component functions (x(t)x(t)x(t), y(t)y(t)y(t), and z(t)z(t)z(t)).

1. Analyze the xxx-component: x(t)=t+2x(t) = \sqrt{t+2}x(t)=t+2​
  • The term inside a square root must be greater than or equal to zero.

  • Set up the inequality:

t+2≥0  ⟹  t≥−2t + 2 \ge 0 \implies t \ge -2t+2≥0⟹t≥−2

  • Domain of x(t)x(t)x(t): [−2,∞)[-2, \infty)[−2,∞)
2. Analyze the yyy-component: y(t)=−9t+3y(t) = \frac{-9}{t+3}y(t)=t+3−9​
  • The denominator cannot equal zero.

  • Set up the equation:

t+3≠0  ⟹  t≠−3t + 3 \neq 0 \implies t \neq -3t+3=0⟹t=−3

  • Domain of y(t)y(t)y(t): (−∞,−3)∪(−3,∞)(-\infty, -3) \cup (-3, \infty)(−∞,−3)∪(−3,∞)
3. Analyze the zzz-component: z(t)=−7t−5z(t) = \frac{-7}{\sqrt{t-5}}z(t)=t−5​−7​
  • The term inside the square root must be non-negative (t−5≥0t - 5 \ge 0t−5≥0).

  • Additionally, because the square root is in the denominator, it cannot be equal to zero (t−5≠0t - 5 \neq 0t−5=0).

  • Combining these restrictions yields:

t−5>0  ⟹  t>5t - 5 > 0 \implies t > 5t−5>0⟹t>5

  • Domain of z(t)z(t)z(t): (5,∞)(5, \infty)(5,∞)
Finding the Intersection

Now, we intersect the three individual domains to find where all components are simultaneously defined:

  1. t≥−2t \ge -2t≥−2

  2. t≠−3t \neq -3t=−3

  3. t>5t > 5t>5

Since any value of ttt that is strictly greater than 555 automatically satisfies t≥−2t \ge -2t≥−2 and t≠−3t \neq -3t=−3, the restriction t>5t > 5t>5 dictates the overall domain.

Final Answer
  • Inequality Notation: t>5t > 5t>5

  • Interval Notation: (5,∞)(5, \infty)(5,∞)

Desmos Plotting Tip

To plot this 3D vector-valued function in Desmos (specifically using the Desmos 3D Grapher), you can input the curve using the parameter ttt exactly as written:

Plaintext

r(t) = (sqrt(t+2), -9/(t+3), -7/sqrt(t-5))

Be sure to set the parameter bounds for ttt starting from just above 555 (e.g., 5 < t < 15) to see the curve render correctly!

Active Practice Problem

Determine the domain and plot using Desmos:

r⃗(t)=⟨3t−4,t+7,6t−1⟩\vec{r}(t) = \left\langle \sqrt{3t-4}, \sqrt{t+7}, \frac{6}{t-1} \right\rangler(t)=⟨3t−4​,t+7​,t−16​⟩

Workspace
Solution
Problem Statement

Determine the domain of the vector-valued function:

r⃗(t)=⟨3t−4,t+7,6t−1⟩\vec{r}(t) = \left\langle \sqrt{3t-4}, \sqrt{t+7}, \frac{6}{t-1} \right\rangler(t)=⟨3t−4​,t+7​,t−16​⟩


Step-by-Step Solution

To find the domain of this vector-valued function, we find the domain of each component independently and then determine where they intersect.

1. Analyze the xxx-component: x(t)=3t−4x(t) = \sqrt{3t-4}x(t)=3t−4​
  • The expression inside the square root must be greater than or equal to zero.
    3t−4≥0  ⟹  3t≥4  ⟹  t≥433t - 4 \ge 0 \implies 3t \ge 4 \implies t \ge \frac{4}{3}3t−4≥0⟹3t≥4⟹t≥34​
  • Domain of x(t)x(t)x(t): [43,∞)\left[\frac{4}{3}, \infty\right)[34​,∞)
2. Analyze the yyy-component: y(t)=t+7y(t) = \sqrt{t+7}y(t)=t+7​
  • The expression inside the square root must be greater than or equal to zero.
    t+7≥0  ⟹  t≥−7t + 7 \ge 0 \implies t \ge -7t+7≥0⟹t≥−7
  • Domain of y(t)y(t)y(t): [−7,∞)[-7, \infty)[−7,∞)
3. Analyze the zzz-component: z(t)=6t−1z(t) = \frac{6}{t-1}z(t)=t−16​
  • The denominator cannot equal zero.
    t−1≠0  ⟹  t≠1t - 1 \neq 0 \implies t \neq 1t−1=0⟹t=1
  • Domain of z(t)z(t)z(t): (−∞,1)∪(1,∞)(-\infty, 1) \cup (1, \infty)(−∞,1)∪(1,∞)

Finding the Intersection

Now, find the interval where all three conditions are satisfied at the same time:

  1. t≥43t \ge \frac{4}{3}t≥34​ (which is approximately 1.331.331.33)
  2. t≥−7t \ge -7t≥−7
  3. t≠1t \neq 1t=1
  • Looking at the first condition (t≥43t \ge \frac{4}{3}t≥34​), any value in this range is automatically greater than −7-7−7.
  • Furthermore, since 43>1\frac{4}{3} > 134​>1, the restriction t≠1t \neq 1t=1 is already excluded automatically because 111 is strictly less than 43\frac{4}{3}34​.

Therefore, the condition t≥43t \ge \frac{4}{3}t≥34​ is the limiting restriction that satisfies all components.

Final Answer
  • Inequality Notation: t≥43t \ge \frac{4}{3}t≥34​
  • Interval Notation: [43,∞)\left[\frac{4}{3}, \infty\right)[34​,∞)

Extra Practice & Extensions

r⃗(t)=⟨t+2t−1,4−t,3t−6⟩\vec{r}(t) = \left\langle \frac{\sqrt{t+2}}{t-1}, \sqrt{4-t}, \frac{3}{\sqrt{t-6}} \right\rangler(t)=⟨t−1t+2​​,4−t​,t−6​3​⟩

Regroup 1

  • Review common misconceptions and clarify key notations.

Skill Block 2

Worked Example

Find the derivative of the vector valued function and the principal unit tangent vector:

r⃗(t)=−ti^−t4j^−6t2k^\vec{r}(t) = -t\hat{i} - t^{4}\hat{j} - 6t^{2}\hat{k}r(t)=−ti^−t4j^​−6t2k^

Worked Solution:
Problem Statement

Find the derivative of the vector-valued function and the principal unit tangent vector:

r⃗(t)=−ti^−t4j^−6t2k^\vec{r}(t) = -t\hat{i} - t^{4}\hat{j} - 6t^{2}\hat{k}r(t)=−ti^−t4j^​−6t2k^


Part 1: Find the Derivative r⃗′(t)\vec{r}^{\prime}(t)r′(t)

To find the derivative of a vector-valued function, differentiate each component with respect to ttt individually using the power rule:

  • i^\hat{i}i^-component: ddt[−t]=−1\frac{d}{dt}[-t] = -1dtd​[−t]=−1
  • j^\hat{j}j^​-component: ddt[−t4]=−4t3\frac{d}{dt}[-t^4] = -4t^3dtd​[−t4]=−4t3
  • k^\hat{k}k^-component: ddt[−6t2]=−12t\frac{d}{dt}[-6t^2] = -12tdtd​[−6t2]=−12t

r⃗′(t)=−i^−4t3j^−12tk^\vec{r}^{\prime}(t) = -\hat{i} - 4t^{3}\hat{j} - 12t\hat{k}r′(t)=−i^−4t3j^​−12tk^


Part 2: Find the Principal Unit Tangent Vector T^(t)\hat{T}(t)T^(t)

The principal unit tangent vector is found by dividing the tangent vector r⃗′(t)\vec{r}^{\prime}(t)r′(t) by its magnitude ∣r⃗′(t)∣|\vec{r}^{\prime}(t)|∣r′(t)∣:

T^(t)=r⃗′(t)∣r⃗′(t)∣\hat{T}(t) = \frac{\vec{r}^{\prime}(t)}{|\vec{r}^{\prime}(t)|}T^(t)=∣r′(t)∣r′(t)​

1. Calculate the Magnitude ∣r⃗′(t)∣|\vec{r}^{\prime}(t)|∣r′(t)∣:

∣r⃗′(t)∣=(−1)2+(−4t3)2+(−12t)2|\vec{r}^{\prime}(t)| = \sqrt{(-1)^2 + (-4t^3)^2 + (-12t)^2}∣r′(t)∣=(−1)2+(−4t3)2+(−12t)2​
∣r⃗′(t)∣=1+16t6+144t2|\vec{r}^{\prime}(t)| = \sqrt{1 + 16t^6 + 144t^2}∣r′(t)∣=1+16t6+144t2​

Rearranging the terms in standard descending order:

∣r⃗′(t)∣=16t6+144t2+1|\vec{r}^{\prime}(t)| = \sqrt{16t^6 + 144t^2 + 1}∣r′(t)∣=16t6+144t2+1​

2. Divide r⃗′(t)\vec{r}^{\prime}(t)r′(t) by its magnitude:

T^(t)=−i^−4t3j^−12tk^16t6+144t2+1\hat{T}(t) = \frac{-\hat{i} - 4t^{3}\hat{j} - 12t\hat{k}}{\sqrt{16t^6 + 144t^2 + 1}}T^(t)=16t6+144t2+1​−i^−4t3j^​−12tk^​


Final Answer
  • Derivative:

    r⃗′(t)=−i^−4t3j^−12tk^\vec{r}^{\prime}(t) = -\hat{i} - 4t^{3}\hat{j} - 12t\hat{k}r′(t)=−i^−4t3j^​−12tk^

  • Principal Unit Tangent Vector:

    T^(t)=−116t6+144t2+1i^−4t316t6+144t2+1j^−12t16t6+144t2+1k^\hat{T}(t) = \frac{-1}{\sqrt{16t^6 + 144t^2 + 1}}\hat{i} - \frac{4t^3}{\sqrt{16t^6 + 144t^2 + 1}}\hat{j} - \frac{12t}{\sqrt{16t^6 + 144t^2 + 1}}\hat{k}T^(t)=16t6+144t2+1​−1​i^−16t6+144t2+1​4t3​j^​−16t6+144t2+1​12t​k^

Active Practice Problem

Given r⃗(t)=−6t3i^−3t7j^−−3t4k^\vec{r}(t) = -6t^{3}\hat{i} - 3t^{7}\hat{j} - \frac{-3}{t^{4}}\hat{k}r(t)=−6t3i^−3t7j^​−t4−3​k^ and f(t)=t4f(t) = \sqrt[4]{t}f(t)=4t​, calculate:

  1. ddt[r⃗(t)]\frac{d}{dt}[\vec{r}(t)]dtd​[r(t)]
  2. ddt[r⃗(f(t))]\frac{d}{dt}[\vec{r}(f(t))]dtd​[r(f(t))]
Workspace
Solution
Problem Statement

Given r⃗(t)=−6t3i^−3t7j^−−3t4k^\vec{r}(t) = -6t^{3}\hat{i} - 3t^{7}\hat{j} - \frac{-3}{t^{4}}\hat{k}r(t)=−6t3i^−3t7j^​−t4−3​k^ and f(t)=t4f(t) = \sqrt[4]{t}f(t)=4t​, calculate:

  1. ddt[r⃗(t)]\frac{d}{dt}[\vec{r}(t)]dtd​[r(t)]
  2. ddt[r⃗(f(t))]\frac{d}{dt}[\vec{r}(f(t))]dtd​[r(f(t))]

Step-by-Step Solution

First, let's rewrite the given vector-valued function r⃗(t)\vec{r}(t)r(t) and scalar function f(t)f(t)f(t) in simplified power form to make differentiation easier:

r⃗(t)=−6t3i^−3t7j^+3t−4k^\vec{r}(t) = -6t^{3}\hat{i} - 3t^{7}\hat{j} + 3t^{-4}\hat{k}r(t)=−6t3i^−3t7j^​+3t−4k^
f(t)=t1/4f(t) = t^{1/4}f(t)=t1/4


Part 1: Calculate ddt[r⃗(t)]\frac{d}{dt}[\vec{r}(t)]dtd​[r(t)]

To find the derivative, use the power rule on each component individually:

  • i^\hat{i}i^-component: ddt[−6t3]=−18t2\frac{d}{dt}[-6t^3] = -18t^2dtd​[−6t3]=−18t2
  • j^\hat{j}j^​-component: ddt[−3t7]=−21t6\frac{d}{dt}[-3t^7] = -21t^6dtd​[−3t7]=−21t6
  • k^\hat{k}k^-component: ddt[3t−4]=−12t−5=−12t5\frac{d}{dt}[3t^{-4}] = -12t^{-5} = -\frac{12}{t^5}dtd​[3t−4]=−12t−5=−t512​

ddt[r⃗(t)]=−18t2i^−21t6j^−12t5k^\frac{d}{dt}[\vec{r}(t)] = -18t^{2}\hat{i} - 21t^{6}\hat{j} - \frac{12}{t^{5}}\hat{k}dtd​[r(t)]=−18t2i^−21t6j^​−t512​k^


Part 2: Calculate ddt[r⃗(f(t))]\frac{d}{dt}[\vec{r}(f(t))]dtd​[r(f(t))]

There are two common methods to solve this: by substitution first, or by using the Vector Chain Rule. Let's use Method 1: Direct Substitution as it is often simpler.

Step 1: Substitute f(t)=t1/4f(t) = t^{1/4}f(t)=t1/4 into r⃗(t)\vec{r}(t)r(t)

r⃗(f(t))=−6(t1/4)3i^−3(t1/4)7j^+3(t1/4)−4k^\vec{r}(f(t)) = -6\left(t^{1/4}\right)^{3}\hat{i} - 3\left(t^{1/4}\right)^{7}\hat{j} + 3\left(t^{1/4}\right)^{-4}\hat{k}r(f(t))=−6(t1/4)3i^−3(t1/4)7j^​+3(t1/4)−4k^
r⃗(f(t))=−6t3/4i^−3t7/4j^+3t−1k^\vec{r}(f(t)) = -6t^{3/4}\hat{i} - 3t^{7/4}\hat{j} + 3t^{-1}\hat{k}r(f(t))=−6t3/4i^−3t7/4j^​+3t−1k^

Step 2: Differentiate with respect to ttt Now, apply the power rule to each component of this composite vector function:

  • i^\hat{i}i^-component: ddt[−6t3/4]=−6⋅34t−1/4=−92t−1/4\frac{d}{dt}[-6t^{3/4}] = -6 \cdot \frac{3}{4}t^{-1/4} = -\frac{9}{2}t^{-1/4}dtd​[−6t3/4]=−6⋅43​t−1/4=−29​t−1/4
  • j^\hat{j}j^​-component: ddt[−3t7/4]=−3⋅74t3/4=−214t3/4\frac{d}{dt}[-3t^{7/4}] = -3 \cdot \frac{7}{4}t^{3/4} = -\frac{21}{4}t^{3/4}dtd​[−3t7/4]=−3⋅47​t3/4=−421​t3/4
  • k^\hat{k}k^-component: ddt[3t−1]=3⋅(−1)t−2=−3t−2\frac{d}{dt}[3t^{-1}] = 3 \cdot (-1)t^{-2} = -3t^{-2}dtd​[3t−1]=3⋅(−1)t−2=−3t−2

ddt[r⃗(f(t))]=−92t1/4i^−21t3/44j^−3t2k^\frac{d}{dt}[\vec{r}(f(t))] = -\frac{9}{2t^{1/4}}\hat{i} - \frac{21t^{3/4}}{4}\hat{j} - \frac{3}{t^2}\hat{k}dtd​[r(f(t))]=−2t1/49​i^−421t3/4​j^​−t23​k^


Final Answers
  1. ddt[r⃗(t)]=−18t2i^−21t6j^−12t5k^\frac{d}{dt}[\vec{r}(t)] = -18t^{2}\hat{i} - 21t^{6}\hat{j} - \frac{12}{t^{5}}\hat{k}dtd​[r(t)]=−18t2i^−21t6j^​−t512​k^

  2. ddt[r⃗(f(t))]=−92t1/4i^−21t3/44j^−3t2k^\frac{d}{dt}[\vec{r}(f(t))] = -\frac{9}{2t^{1/4}}\hat{i} - \frac{21t^{3/4}}{4}\hat{j} - \frac{3}{t^2}\hat{k}dtd​[r(f(t))]=−2t1/49​i^−421t3/4​j^​−t23​k^

Extra Practice & Extensions

v⃗(t)=⟨tsin⁡(2t),2tln⁡(t−3),t2t−2⟩ m/s\vec{v}(t) = \left\langle t \sin(2t), 2t \ln(t-3), \frac{t^{2}}{t-2} \right\rangle \text{ m/s}v(t)=⟨tsin(2t),2tln(t−3),t−2t2​⟩ m/s

  • Find the acceleration of the car, a⃗(t)\vec{a}(t)a(t). Hint: acceleration is the derivative of velocity with respect to time.
  • Find the acceleration and principal unit tangent vector at t=20t = 20t=20 s.

Regroup 2

  • Reflect on the physical modeling applications and mathematical setups.

Skill Block 3

Worked Example

Evaluate the indefinite integral:

∫⟨5cos⁡(7t),3cos⁡(4t),−9t⟩dt\int \left\langle 5 \cos(7t), 3 \cos(4t), \frac{-9}{t} \right\rangle dt∫⟨5cos(7t),3cos(4t),t−9​⟩dt

Worked Solution:
Problem Statement

Evaluate the indefinite integral:

∫⟨5cos⁡(7t),3cos⁡(4t),−9t⟩dt\int \left\langle 5 \cos(7t), 3 \cos(4t), \frac{-9}{t} \right\rangle dt∫⟨5cos(7t),3cos(4t),t−9​⟩dt


To integrate a vector-valued function, integrate each component function independently with respect to ttt. Remember to include a constant of integration for each component, which can ultimately be combined into a single constant vector C⃗\vec{C}C.

1. Integrate the xxx-component: f(t)=5cos⁡(7t)f(t) = 5 \cos(7t)f(t)=5cos(7t)

Using uuu-substitution where u=7tu = 7tu=7t and du=7 dtdu = 7\,dtdu=7dt:

∫5cos⁡(7t) dt=5⋅17sin⁡(7t)+C1=57sin⁡(7t)+C1\int 5 \cos(7t) \, dt = 5 \cdot \frac{1}{7} \sin(7t) + C_1 = \frac{5}{7} \sin(7t) + C_1∫5cos(7t)dt=5⋅71​sin(7t)+C1​=75​sin(7t)+C1​

2. Integrate the yyy-component: g(t)=3cos⁡(4t)g(t) = 3 \cos(4t)g(t)=3cos(4t)

Similarly, using uuu-substitution where u=4tu = 4tu=4t and du=4 dtdu = 4\,dtdu=4dt:

∫3cos⁡(4t) dt=3⋅14sin⁡(4t)+C2=34sin⁡(4t)+C2\int 3 \cos(4t) \, dt = 3 \cdot \frac{1}{4} \sin(4t) + C_2 = \frac{3}{4} \sin(4t) + C_2∫3cos(4t)dt=3⋅41​sin(4t)+C2​=43​sin(4t)+C2​

3. Integrate the zzz-component: h(t)=−9th(t) = \frac{-9}{t}h(t)=t−9​

Using the standard logarithmic integration rule ∫1t dt=ln⁡∣t∣\int \frac{1}{t} \, dt = \ln|t|∫t1​dt=ln∣t∣:

∫−9t dt=−9ln⁡∣t∣+C3\int \frac{-9}{t} \, dt = -9 \ln|t| + C_3∫t−9​dt=−9ln∣t∣+C3​


Combining the Components

We can write out the final vector in standard component form, merging the individual integration constants (C1,C2,C3C_1, C_2, C_3C1​,C2​,C3​) into a single constant vector C⃗=⟨C1,C2,C3⟩\vec{C} = \langle C_1, C_2, C_3 \rangleC=⟨C1​,C2​,C3​⟩:

∫⟨5cos⁡(7t),3cos⁡(4t),−9t⟩dt=⟨57sin⁡(7t),34sin⁡(4t),−9ln⁡∣t∣⟩+C⃗\int \left\langle 5 \cos(7t), 3 \cos(4t), \frac{-9}{t} \right\rangle dt = \left\langle \frac{5}{7} \sin(7t), \frac{3}{4} \sin(4t), -9 \ln|t| \right\rangle + \vec{C}∫⟨5cos(7t),3cos(4t),t−9​⟩dt=⟨75​sin(7t),43​sin(4t),−9ln∣t∣⟩+C


Final Answer

⟨57sin⁡(7t),34sin⁡(4t),−9ln⁡∣t∣⟩+C⃗\left\langle \frac{5}{7} \sin(7t), \frac{3}{4} \sin(4t), -9 \ln|t| \right\rangle + \vec{C}⟨75​sin(7t),43​sin(4t),−9ln∣t∣⟩+C

Active Practice Problem

Given that an object has a velocity of v⃗(t)=[t3i^,1t+2j^,e8tk^] ft/s\vec{v}(t) = \left[ \sqrt[3]{t}\hat{i}, \frac{1}{t+2}\hat{j}, e^{8t}\hat{k} \right] \text{ ft/s}v(t)=[3t​i^,t+21​j^​,e8tk^] ft/s:

  • Use an indefinite integral to find the displacement vector of the object.
  • Use a definite integral to find the displacement vector of the object over the interval 1≤t≤51 \le t \le 51≤t≤5.
Solution Key:
Problem Statement

Given that an object has a velocity of v⃗(t)=[t3i^,1t+2j^,e8tk^] ft/s\vec{v}(t) = \left[ \sqrt[3]{t}\hat{i}, \frac{1}{t+2}\hat{j}, e^{8t}\hat{k} \right] \text{ ft/s}v(t)=[3t​i^,t+21​j^​,e8tk^] ft/s:

  • Use an indefinite integral to find the displacement vector of the object.
  • Use a definite integral to find the displacement vector of the object over the interval 1≤t≤51 \le t \le 51≤t≤5.

To find the displacement vector from a velocity vector function, we integrate each component function independently. For easier integration, rewrite the velocity function using fractional exponents:

v⃗(t)=t1/3i^+1t+2j^+e8tk^\vec{v}(t) = t^{1/3}\hat{i} + \frac{1}{t+2}\hat{j} + e^{8t}\hat{k}v(t)=t1/3i^+t+21​j^​+e8tk^


Part 1: Indefinite Integral for Displacement Vector r⃗(t)\vec{r}(t)r(t)

Integrate each component individually with respect to ttt:

  • i^\hat{i}i^-component: Use the power rule (∫tndt=tn+1n+1\int t^n dt = \frac{t^{n+1}}{n+1}∫tndt=n+1tn+1​):

    ∫t1/3 dt=t4/34/3=34t4/3+C1\int t^{1/3} \, dt = \frac{t^{4/3}}{4/3} = \frac{3}{4}t^{4/3} + C_1∫t1/3dt=4/3t4/3​=43​t4/3+C1​

  • j^\hat{j}j^​-component: Use the standard logarithmic rule:

    ∫1t+2 dt=ln⁡∣t+2∣+C2\int \frac{1}{t+2} \, dt = \ln|t+2| + C_2∫t+21​dt=ln∣t+2∣+C2​

  • k^\hat{k}k^-component: Use the exponential rule (∫eatdt=1aeat\int e^{at} dt = \frac{1}{a}e^{at}∫eatdt=a1​eat):

    ∫e8t dt=18e8t+C3\int e^{8t} \, dt = \frac{1}{8}e^{8t} + C_3∫e8tdt=81​e8t+C3​

Combine the components and merge the constants C1,C2,C3C_1, C_2, C_3C1​,C2​,C3​ into a single constant vector C⃗\vec{C}C:

r⃗(t)=(34t4/3)i^+(ln⁡∣t+2∣)j^+(18e8t)k^+C⃗\vec{r}(t) = \left( \frac{3}{4}t^{4/3} \right)\hat{i} + \left( \ln|t+2| \right)\hat{j} + \left( \frac{1}{8}e^{8t} \right)\hat{k} + \vec{C}r(t)=(43​t4/3)i^+(ln∣t+2∣)j^​+(81​e8t)k^+C


Part 2: Definite Integral over the Interval 1≤t≤51 \le t \le 51≤t≤5

To find the total displacement over the time interval [1,5][1, 5][1,5], evaluate the definite integral component-by-component using the antiderivatives found above:

Δr⃗=∫15v⃗(t) dt\Delta\vec{r} = \int_{1}^{5} \vec{v}(t) \, dtΔr=∫15​v(t)dt

1. Evaluate the i^\hat{i}i^-component:

[34t4/3]15=34(5)4/3−34(1)4/3=34(54/3−1)≈5.66\left[ \frac{3}{4}t^{4/3} \right]_{1}^{5} = \frac{3}{4}(5)^{4/3} - \frac{3}{4}(1)^{4/3} = \frac{3}{4}\left(5^{4/3} - 1\right) \approx 5.66[43​t4/3]15​=43​(5)4/3−43​(1)4/3=43​(54/3−1)≈5.66

2. Evaluate the j^\hat{j}j^​-component:

[ln⁡∣t+2∣]15=ln⁡∣5+2∣−ln⁡∣1+2∣=ln⁡(7)−ln⁡(3)=ln⁡(73)≈0.847\left[ \ln|t+2| \right]_{1}^{5} = \ln|5+2| - \ln|1+2| = \ln(7) - \ln(3) = \ln\left(\frac{7}{3}\right) \approx 0.847[ln∣t+2∣]15​=ln∣5+2∣−ln∣1+2∣=ln(7)−ln(3)=ln(37​)≈0.847

3. Evaluate the k^\hat{k}k^-component:

[18e8t]15=18e8(5)−18e8(1)=18(e40−e8)≈2.94×1016\left[ \frac{1}{8}e^{8t} \right]_{1}^{5} = \frac{1}{8}e^{8(5)} - \frac{1}{8}e^{8(1)} = \frac{1}{8}\left(e^{40} - e^8\right) \approx 2.94 \times 10^{16}[81​e8t]15​=81​e8(5)−81​e8(1)=81​(e40−e8)≈2.94×1016

Combine the components into the final displacement vector:

Δr⃗=[34(54/3−1)]i^+[ln⁡(73)]j^+[18(e40−e8)]k^\Delta\vec{r} = \left[ \frac{3}{4}\left(5^{4/3} - 1\right) \right]\hat{i} + \left[ \ln\left(\frac{7}{3}\right) \right]\hat{j} + \left[ \frac{1}{8}\left(e^{40} - e^8\right) \right]\hat{k}Δr=[43​(54/3−1)]i^+[ln(37​)]j^​+[81​(e40−e8)]k^


Final Answers
  • Indefinite Integral Vector:

    r⃗(t)=(34t4/3)i^+(ln⁡∣t+2∣)j^+(18e8t)k^+C⃗\vec{r}(t) = \left( \frac{3}{4}t^{4/3} \right)\hat{i} + \left( \ln|t+2| \right)\hat{j} + \left( \frac{1}{8}e^{8t} \right)\hat{k} + \vec{C}r(t)=(43​t4/3)i^+(ln∣t+2∣)j^​+(81​e8t)k^+C

  • Definite Integral (Exact Value):

    Δr⃗=[34(54/3−1)]i^+[ln⁡(73)]j^+[18(e40−e8)]k^\Delta\vec{r} = \left[ \frac{3}{4}\left(5^{4/3} - 1\right) \right]\hat{i} + \left[ \ln\left(\frac{7}{3}\right) \right]\hat{j} + \left[ \frac{1}{8}\left(e^{40} - e^8\right) \right]\hat{k}Δr=[43​(54/3−1)]i^+[ln(37​)]j^​+[81​(e40−e8)]k^

Show your steps and calculations here.

Regroup 3

  • Verify calculations and mathematical reasoning.

Synthesis Wrap-up

  • Core takeaways from Session 05 and overview of homework homework assignment: Vector-Valued Functions and Space Curves Calculus of Vector-Valued Functions.