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Chapter 1: Fundamental Concepts

1.8 Examples

Here are examples from Chapter 1 to help you understand these concepts better. These were taken from the real world and supplied by FSDE students in Summer 2021. If you’d like to submit your own examples, please send them to:
eosgood@upei.ca

Example 1.8.1: Vectors, Submitted by Tyson Ashton-Losee

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.

A digital drawing of a computer mouse is shown from above with an arrow labeled r pointing diagonally outward from its center. X and Y axes are displayed in the lower left corner.

 

A black wired computer mouse is placed on a white surface, viewed from above.
Source: Black Computer Mouse on Table | Old dusty black computer mou… | Flickr

2. Draw

A right triangle on an XY plane with base 6 cm on the X-axis, height 3.5 cm on the Y-axis, hypotenuse labeled r, and an angle theta (θ) at the origin.

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

[latex]\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}[/latex]

6. Review

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

 

Example 1.8.2: Vectors, Submitted by Brian MacDonald

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.
A person wearing a cap and life vest is fishing from a boat, holding a bent fishing rod over the sea.
Source: File:Deepsea.JPG – Wikimedia Commons

A digital drawing of a fishing rod angled at 45 degrees is 8 ft tall with a 25 ft fishing line. A 180 N fish is hooked at the end. An inset shows a reel with a handle 0.25 ft from its center.


2. Draw

Sketch:

Diagram of a right triangle on grid paper: vertical side AC is 8 ft, horizontal side AB is 0.25 ft, angle at C is 45°, and the hypotenuse CD measures 25 ft. Points A, B, C, and D are labeled.

Free-body diagram:

A right triangle with a green vertical side, angle θ, and two red downward arrows labeled FA and FD. The x and y axes are shown pointing right and up, respectively.

3. Knowns and Unknowns

Known:

  • rAB = 0.25 ft
  • rBC = 8 ft
  • rCD = 25 ft
  • FD = 180 N
  • θ = 45°

Unknown:

  • FA
  • vector rAD

4. Approach

Convert inches to meters, then use the equation below.

[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 TD

[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 FA

[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 rAD:

A vector diagram on a grid showing points A, B, C, and D. Vectors are drawn from A to B, B to C (black), and A to D (orange), with labeled distances and axes for x and y shown at the bottom left.

[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

Though yielding a very large number, the answer appears correct from the information given. 13,000 N of force is the amount of force Mark would need to apply to 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 a real scenario, 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, 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.

Example 1.8.3: Dot product and cross product, submitted by Anonymous ENGN 1230 Student

1. Problem

[latex]\underline{a}=[6\;\;\;5\;\;\;3]\;\;\;\underline{b}=[8\;\;\;1\;\;\;3][/latex]

a) Find 6a

b) Find [latex]a\cdot b[/latex]

c) Find [latex]a\times b[/latex]

d) Find [latex]2a\times b[/latex]


2. Draw

N/A

3. Knowns and Unknowns

Known:

  • a
  • b

Unknowns:

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

4. Approach

Use dot product and cross product equations

5. Analysis

Part a:

[latex]6\underline{a}=6*[6\;\;\;5\;\;\;3]\\6\underline{a}=[36\;\;\;30\;\;\;18][/latex]

Part b:

[latex]\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[/latex]

Part C:

[latex]\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}}[/latex]

Part D:

[latex]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}}[/latex]

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 a, c, and d have values in three directions, while b only has magnitude.

Example 1.8.4: Torque, Submitted by Luke McCarvill

1. Problem

To start riding her bicycle, Jane must push down on one of her bike’s pedals, which are on 16-centimetre-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?

Girl on a bike
Source: https://commons.wikimedia.org/wiki/File:Girl_on_a_Bike_(Imagicity_116).jpg

 

A green bicycle
Source: https://pixabay.com/illustrations/bicycle-cycle-two-wheeler-pedal-3168934/

2. Draw

A16 cm horizontal bar, with a downward force labeled Fₐ acting at the right end of the bar. The y- and x-axes are shown in the top left corner.

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 the 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 nonlinear.*

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 details.

Example 1.8.5: Torque, submitted by Hamza Ben Driouech

1. Problem

A person is pushing on a door with a force of 100 N. The door is at an angle α = 45° as shown in the sketch below.

a) Calculate the moment when r is 45 cm and 75 cm.

b) At what angle(s) is the moment zero? Explain why.

A sketch of a hand pushing a door

Assumptions: Model the force as a single point load acting on the door.


2. Draw

Sketch:

A sketch of the forces acting on the door at certain points

Free-body diagram:

A free-body diagram of the forces acting on the door at certain points

3. Knowns and Unknowns

Knowns:

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

Unknowns:

  • M1
  • M2
  • Angle when M is zero

4. Approach

Use the equation below.

[latex]M=|r|\cdot|F|\cdot\sin\theta[/latex]

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.

45 degree angle to the door

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

[latex]\theta=90^{\circ}-45^{\circ}[/latex]

[latex]\theta=45^{\circ}[/latex]

[latex]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[/latex]

Part b)

[latex]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}[/latex]

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.

Example 1.8.6: Bonus Vector Material, Submitted by Liam Murdock

1. Problem

George travelled a displacement of dg = [7   0  8] m from his car. George’s dog, named Sparky, on the other hand, travelled a displacement of ds = [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.

  1.  What is the displacement from George to his dog?
  2. What is Sparky’s velocity? (No need to draw.)
  3. What is Sparky’s speed? (No need to draw.)
A dog running in the field
Source: https://www.piqsels.com/en/public-domain-photo-oekac

 


2. Draw

A free-body diagram of the dog and George with dimensions shown

3. Knowns and Unknowns

Knowns:

  • dg = [7   0  8] m
  • ds = [0  6  6] m
  • t= 4 seconds

Unknowns:

  • vsg= ?
  • dsg= ?

4. Approach

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

 

5. Analysis

Part a:

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

Part b:

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

Part C:

[latex]V_{sg}=\sqrt{V_{sgx}^2+V_{sgy}^2+V_{sgz}^2}[/latex]
[latex]V_{sg}=\sqrt{1.75^2+(-1.5)^2+0.5^2}[/latex]
[latex]V_{sg}=2.36m/s[/latex]

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 George, 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 that 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 Sparky having to go positive 2 m in the z-direction to meet George.

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

 

Parts 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.

Example 1.8.7: Cross Product, Submitted By Victoria Keefe

1. Problem:
Using the cross product, find the torque on point A due to force F. Force F = (5 i – 2 j + k)N. The width of the platform is 1 meter, the height is 0.25 meters, and the length is 5 meters.

2: Sketch

N/A


3. Knowns and Unknowns

Knowns:

  • F = (5 i – 2 j + k)N
  • l = 5m
  • w = 1m
  • h = 0.25m

Unknown:

  • M

4: Approach

Use the equation: M = r x F

5. Analysis

[latex]r = (-1 \hat{i} + 0.25 \hat{j} + 5 \hat{k})m \\ \bar{F} = (5 \hat{i} - 2 \hat{j} + \hat{k})N \\  \bar{M} =[ [(0.25 \cdot 1) - (-2 \cdot 5)] \hat{i} - [(-1 \cdot 1) - (5 \cdot 5)] \hat{j} + [(-1 \cdot -2) - (5 \cdot 0.25)] \hat{k}]Nm \\ \bar{M} = (10.25 \hat{i} + 26 \hat{j} +0.75 \hat{k})Nm[/latex]

6.0 Review

The resulting moment has reasonable values and can be verified with a cross product calculator.

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Engineering Mechanics: Statics Copyright © by Libby (Elizabeth) Osgood; Gayla Cameron; Emma Christensen; Analiya Benny; Matthew Hutchison; and Deborah Areoye is licensed under a Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International License, except where otherwise noted.

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