1. Problem

After a long day of studying, a student sitting at their computer moves the cursor from the bottom left of the screen to the top right in order to close a web browser. The computer mouse was displaced 6 cm along the x-axis and 3.5 cm along the y-axis. Draw the resultant vector and calculate the distance traveled.

 

2. Draw

3. Knowns and Unknowns

Known:

• x = 6 cm
• y = 3.5 cm

Unknown:

• r
• θ

4. Approach

Use SOH CAH TOA, first find θ, then r

5. Analysis

\begin{aligned}
&\tan \theta=\frac{y}{x} \\
&\tan \theta=\frac{3.5 \mathrm{~cm}}{6 \mathrm{~cm}} \\
&\theta=\tan ^{-1}\left(\frac{3.5}{6}\right) \\
&\theta=30.256^{\circ} \\
&\sin \theta=\frac{y}{r} \\
&r=\frac{y}{\sin \theta} \\
&r=\frac{3.5 \mathrm{~cm}}{\sin \left(30.256^{\circ}\right)} \\
&r=6.946 \mathrm{~cm} \\
&r=6.9 \mathrm{~cm}
\end{aligned}

6. Review

It makes sense that the angle is less that 45, because y is smaller than x. Also, if you use Pythagorean theorem to find r, you get the same answer.

1. Problem

Mark is fishing in the ocean with his favourite fishing rod. The distance between the tip of the rod and the reel is 8 ft and the length of the reel handle is 0.25 ft. The angle between the fishing rod and fishing line is 45 degrees. If Mark catches a fish when 25 ft of the fishing line is released while the fish is diving down with a force of 180 N, how much force does Mark need to apply (push down) to the reel handle to bring in the fish? Draw the position vector of the fish relative to the reel.

Assumptions:

• Mark can reel in the fish when he generates more torque with the handle than the amount of torque that the fish is applying to the reel while pulling on the line.
• The fishing line comes out of the reel in a straight line at a 90-degree angle.

2. Draw

Sketch:

Free-body diagram:

3. Knowns and Unknowns

Known:

• r_AB = 0.25 ft
• r_BC = 8 ft
• r_CD = 25 ft
• F_D = 180 N
• θ = 45°

Unknown:

• F_A
• vector r_AD

4. Approach

Convert inches to meters, then use the below equation.

[latex]T=|r| *|F| * \sin \theta\\[/latex]

5. Analysis

Step 1: convert inches to meters

[latex]\begin{align} &25 \mathrm{ft} * \frac{12 \mathrm{in}}{1 \mathrm{ft}} * \frac{2.54 \mathrm{cm}}{\operatorname{1in} } * \frac{\operatorname{1m}}{100 \mathrm{cm}}=7.62 \mathrm{m}\\\\ &\quad\mathrm{and}\\\\ &0.25 \mathrm{ft} * \frac{12  \mathrm{in}}{1\mathrm{ft}} * \frac{2.54 \mathrm{cm}}{\operatorname{1in} } * \frac{\mathrm{1m}}{100 \mathrm{cm}}=0.0762 \mathrm{m}\\ \end{align}[/latex]

Step 2: solve for T_D

[latex]\begin{aligned}&T_{D}=\left|r_{C D}\right| * \left|F_{D}\right| * \sin \theta\\ &T_{D}=(7.62 m)(180 N) \sin \left(45^{\circ}\right)\\ &T_{D}=969.86766 \mathrm{Nm} \end{aligned}[/latex]

Step 3: Solve for F_A

[latex]\begin{aligned}&T_{A}=\left|r_{AB}\right| * \left|F_{A}\right| * \sin \theta\\ &\text { Assume } T_{A}=T_{D}\\ &F_{A}=\frac{T_{D}}{\left|r_{AB}\right| * \sin \theta} \\ &F_{A}=\frac{969.86766 \mathrm{ Nm}}{0.0762 \mathrm{~m} * \sin \left(90^{\circ}\right)} \\ &F_{A}=12 727.9 \mathrm{N} \\ &F_{A}=13 000 \mathrm{N} \end{aligned}[/latex]

Vector r_AD:

[latex]\begin{aligned} &\vec r_{A D}=\vec r_{A B}+\vec r_{B C}+\vec r_{C D} \\ &\vec {r}_{A D}=\left[\begin{array}{c} 0.25 \\ 0 \end{array}\right] f t+\left[\begin{array}{l} 0 \\ 8 \end{array}\right] f t+\left[\begin{array}{c} 25 \sin 45^{\circ} \\ -25 \cos 45^{\circ} \end{array}\right] f t \\ &\vec r_{A D}=\left[\begin{array}{cc} 17.93 \\ -9.68 \end{array}\right] ft \end{aligned}[/latex]

6. Review

The answer, though yielding a very large number, appears to be correct from the information given. 13,000 N of force is the amount of force Mark would need to apply the reel handle to generate the same amount of force that the fish creates. 13,000 N in reality is too much for one to generate but also in real scenario’s one would not have to generate the same amount of force to reel in the fish to reel gearing, the amount of torque generated by the fishing rod itself and etc. In other words 13 000 N of force is too high in a real scenario but with the assumptions given in the problem, the number seems reasonable. The answer also has the correct unit, N.

1. Problem

2. Draw

N/A

3. Knowns and Unknowns

Known:

• a
• b

Unknowns:

• 6b,
• [latex]a\cdot b[/latex]
• [latex]a\times b[/latex]
• [latex]2a\times b[/latex]

4. Approach

Use dot product, cross product equations

5. Analysis

Part a:

$$6\underline{b}=6*[6\;\;\;5\;\;\;3]\\6\underline{b}=[36\;\;\;30\;\;\;18]$$

Part b:

$$\underline{a}\cdot\underline{b}=[6\;\;\;5\;\;\;3]\cdot[8\;\;\;1\;\;\;3]\\=6\cdot 8+5\cdot 1+3\cdot3\\=48+5+9\\\underline{a}\cdot\underline{b}=62$$

Part c:

$$\underline{a}\times\underline{b}=\begin{bmatrix}
\underline{\hat{i}} &\underline{\hat{j}} & \underline{\hat{k}} \\
6 & 5 & 3 \\
8 & 1 & 3
\end{bmatrix}\\(5\cdot 3-3\cdot 1)\underline{\hat{i}}-(6\cdot 3-3\cdot 8)\underline{\hat{j}}+(6\cdot 1-5\cdot 8)\underline{\hat{k}}\\\underline{a}\times\underline{b}=12\underline{\hat{i}}+6\underline{\hat{j}}-34\underline{\hat{k}}$$

Part d:

$$ 2\underline{a}=2*[6\;\;\;5\;\;\;3]=[12\;\;\;10\;\;\;6]\\\underline{b}=[8\;\;\;1\;\;\;3]\\2\underline{a}\times\underline{b} = \begin{bmatrix}
\underline{\hat{i}} & \underline{\hat{j}} & \underline{\hat{k}} \\
12 & 10 & 6 \\
8 & 1 & 3
\end{bmatrix} \\=(10\cdot 3-6\cdot 1)\underline{\hat{i}}-(12\cdot 3-6\cdot 8)\underline{\hat{j}}+(12\cdot 1-10\cdot 8)\underline{\hat{k}}\\2\underline{a}\times\underline{b}=24\underline{\hat{i}}+12\underline{\hat{j}}-68\underline{\hat{k}}$$

6. Review

The answer to part d is double the answer for part c, which makes sense. It also makes sense that the answers to b, c, and d have values in three directions, while a only has magnitude.

To start riding her bicycle, Jane must push down on one of her bike’s pedals which are on 16 centimeter long crank arms. Jane can push directly downwards with her legs with a force of 100N. Jane notices that the pedal’s starting position can sometimes make it more or less useful in generating torque.

a) What is the ideal angle that Jane’s bike pedal should be at in order to generate the most torque? Prove this mathematically. (Assume we only care about the very start of her very first push, and choose a reference frame for the angle that makes most sense for you).

b) What angle(s) should the bike pedal be at if Jane wants to generate exactly half of the maximum amount of torque?

c) Is there any position(s) at which the pedal will create zero torque? Where are they and why?

 

2. Draw

3. Knowns and Unknowns

Knowns:

[latex]\begin{aligned} &\vec r=\left[\begin{array}{c} 0.16 \\ 0 \\ 0 \end{array}\right] m \\ &\vec F_{A}=\left[\begin{array}{c} 0 \\ -100 \\ 0 \end{array}\right] N \end{aligned}[/latex]

Unknowns:

• position of r for maximum torque
• position of r for half of maximum torque
• position of r for zero torque, and why

4. Approach

For part a), I will find a general equation for torque based on the given values in terms of θ, then analyze the function for its maxima

For part b), I will find the magnitude of 50% of maximum torque and then reverse-engineer the equation to determine what angle(s) the pedal needs to be at to satisfy the equation.

For part c), I will look back at my equation and find when the equation equals zero, then try to understand why given the example problem.

5. Analysis

Part a:

[latex]\begin{aligned} &T=\left|\vec F_{A}\right| * \left|\vec r\right| * \sin \theta \\ &T=(100 N) *(0.16 m) * \sin \theta \\ &T=16 \sin \theta \mathrm{Nm} \\ &\quad\left\{90^{\circ}+360^{\circ} k ; k \in \mathbb{Z}\right\} \end{aligned}[/latex]

Thinking about the shape of the sine function in the first period, the maximum occurs at 90 degrees.

You could say algebraically that the maximum is at 90, 450, 810 etc., but these angles all represent the same position on the wheel. Therefore, we will use 90.

Part b:

[latex]\begin{aligned} &T_1=\left|F_{A}\right| *|r| * \sin \theta \\ &T_1=(100 N)*(0.16 m)* \sin 90^{\circ} \\ &T_1=16 N m \end{aligned}[/latex]

Find 50% of the maximum torque:

[latex]T_2=\frac{T_1}{2}[/latex]
[latex]\frac{16 Nm}{2}=8 Nm[/latex]

Rearrange T₂ equation: [latex]T_{2}=\left|F_{A}\right| *|{r}|  \sin \theta[/latex]
[latex]\begin{aligned}&\sin \theta=\frac{T_{2}}{\left| F_{A}\right| * \left| r \right|} \\ &\sin \theta=\frac{8 N m}{(100 N)*(0.16 m)} \\ &\sin \theta=0.5 \\ &\theta=30^{\circ}, 150^{\circ}, etc \end{aligned}[/latex]

Therefore, Jane could push at 30 from vertical, or 150 from vertical to create half the torque.

*Interesting to note is that half the angle does not yield half the torque; the angle is 30, not 45. This is because the sine function is non-linear.*

Part c:

T = 16 sinθ tells us that the angles of 0 and 180 will give us zero torque.

This makes sense given that pushing straight down on a stable pendulum will not cause the pendulum to rotate!

Likewise, if you just stand on your pedals, you’re providing lots of downward force, but creating zero torque since the crank arm and the direction of the force are parallel (or antiparallel)!

6. Review

These answers have the correct units (Nm and degrees) and are within a reasonable order of magnitude based on the given information. See logic/explanations above for more detail.

1. Problem

2. Draw

Sketch:

Free-body diagram:

3. Knowns and Unknowns

Knowns:

• F = 100N
• r₁ = 45cm
• r₂ = 75cm
• α = 45°

Unknowns:

• M₁
• M₂
• Angle when M is zero

4. Approach

Use equation below.

$$ M=|r|\cdot|F|\cdot\sin\theta$$

5. Analysis

Part a)

The angle we were given is not technically the one we should use in the moment equation. The angle should be between r and F. Therefore, we have to find the new angle.

As shown below, the angle we find is also 45°. Now we can continue and solve for M₁ and M₂.

$$\theta=90^{\circ}-45^{\circ}$$

$$\theta=45^{\circ}$$

$$ M_1=|r_1|\cdot|F|\cdot\sin\theta\\M_1=0.45m\cdot 100N\cdot\sin(45^{\circ})\\m_1=31.82Nm\\\\M_2=|r_2|\cdot |F|\cdot\sin\theta\\M_2=0.75m\cdot 100N\cdot\sin(45^{\circ})\\M_2=53.03Nm$$

Part b)

$$M=|r|\cdot|F|\cdot\sin\theta\\if \sin\theta=0, M=0\\\sin\theta=0\\\theta=\sin^{-1}(0)\\\theta=0^{\circ}, 180^{\circ}, 360^{\circ}$$

Answer: the moment is zero when the angle between the force and the moment arm is 0° or 180° (360 would represent the same angle as 0°, as would 540°, etc.)

6. Review

It makes sense that the moment is zero when the door is either closed or wide open, because when we apply a force at those positions, no movement of the door is possible.

1. Problem

George traveled a displacement of d_g = [7   0  8] m from his car. George’s dog named Sparky on the other hand traveled a displacement of d_s = [0  6  6] m from George’s car. George called Sparky’s name and the dog ran to George’s position. It took Sparky four seconds to get there.

a. What is the displacement from George to his dog?
b. What is Sparky’s velocity? (no need to draw)
c. What is Sparky’s speed? (no need to draw)

 

 

2. Draw

3. Knowns and Unknowns

Knowns:

• d_g = [7   0  8] m
• d_s = [0  6  6] m
• t= 4 seconds

Unknowns:

• v_sg= ?
• d_sg= ?

4. Approach

We are going to use vector operations (both subtraction and division), velocity – displacement relationship, velocity – speed relationship, and Pythagoras theorem to solve this problem.

5. Analysis

Part a:

$$ d_{sg}=d_{g}-d_{s}$$
$$ d_{sg}=[7\;\;\;0\;\;\;8]m-[0\;\;\;6\;\;\;6]m$$
$$ d_{sg}=[7-0\;\;\;0-6\;\;\;8-6]m$$
$$ d_{sg}=[7\;\;\;-6\;\;\;2]m$$

Part b:

$$ v_{sg}=d_{sg}/t$$
$$v_{sg}=[7\;\;\;-6\;\;\;2]m/4s$$
$$v_{sg}=[7/4\;\;\;-6/4\;\;\;2/4]m/s$$
$$v_{sg}=[1.75\;\;\;-1.5\;\;\;0.5]m/s$$

Part c:

$$V_{sg}=\sqrt{V_{sgx}^2+V_{sgy}^2+V_{sgz}^2}$$
$$V_{sg}=\sqrt{1.75^2+(-1.5)^20.5^2}$$
$$ V_{sg}=2.36m/s$$

6. Review

Part a:

One way to review the question is to walk through the solution verbally. Our solution shows that for Sparky to get to Gerorge, he must walk 7 m in the positive x-direction (almost out of the page), 6 m in the negative y-direction (left), and finally 2 m in the positive z-direction (up).

Firstly, since the dog initially did not go in the x-direction it makes sense Sparky would have to copy George’s exact x movement. Secondly, since George did not move in the y – direction, it would make sense that Sparky would just have to retrace his steps and if he initially went 6 m right, he would have to go 6 m left. Thirdly, George and Sparky both went upwards, but George went 2 m higher with an altitude of 8 m compared to Sparky’s 6 m correlating to Spraky having to go positive 2 m in the z – direction to meet Geroge.

Therefore, since all the movements make sense for Sparky to meet George (using logic), the answer is proven to be right.

Part b and c:

Since B and C correlate to the same magnitude they can be reviewed together. From a quick search, an average dog tops out at a speed of 19 miles per hour. We can convert this to SI units:

[latex]\frac{19 \text { miles }}{1 h r}\left(\frac{1 \mathrm{~km}}{0.621371 \text { miles }}\right)\left(\frac{1000 \mathrm{~m}}{1 \mathrm{~km}}\right)\left(\frac{1 \mathrm{hr}}{3600}\right)=8.49 \mathrm{~m} / \mathrm{s}[/latex]

The top speed of an average dog is 8.49 m/s. So 2.36m/s is approximately a quarter of the top speed of an average dog. Sparky probably was not sprinting at full speed and he could be a slower dog breed, making  2.36m/s a reasonable answer.