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7.2. Solved Examples: Force of Friction and Normal Force; Free Body Diagrams

Example 1

A 17 kg toolbox sits on a level floor. A worker uses a rope and pulls the toolbox with a force F (see diagram below). The coefficients of static friction and kinetic friction between the toolbox and the floor are 0.65, respectively 0.40.

  1. Find the pulling force needed to just set the toolbox in motion.
  2. If then, the toolbox continues to move with an acceleration of 0.20 m/s2, find the new force needed to maintain this acceleration.
Toolbox diagram
[CAP] Figure 7.5.Free-body diagram of a toolbox being pulled with force F.
Given:
[latex]\small m = 17 \text{ kg}[/latex]
[latex]\small mu_s = 0.65[/latex]
[latex]\small mu_k = 0.40[/latex]
[latex]\small a = 0.20 \text{ m/s}^2[/latex]
Find:
[latex]\small \text{(a)} \quad F = ?[/latex]
[latex]\small \text{(b)} \quad F_1 = ?[/latex]

a) Solution:

The pulling force must overcome the friction for the toolbox to start moving.

[latex]\large F > F_f[/latex], but [latex]F_f = \mu_s F_N[/latex]

Analyze the motion on the axis (axes). Ask the question: Is this a situation of equilibrium?

Since [latex]F_N[/latex] is positioned on the y axis, we need to ask the equilibrium question about the y axis.

On the y axis we have a situation of equilibrium because the toolbox is not moving on the y axis. This means that:

[latex]\large F_{\text{net}, y} = 0[/latex]

[latex]\large F_{\text{net}, y} = F_N - F_g = 0, \quad \text{or} \quad F_N = F_g[/latex]

On the other hand,

[latex]\large F_g = m \times g[/latex]

Substitute the expressions into [latex]\large F_f[/latex] :

[latex]\large F_f = \mu_s \times m \times g = 0.65 \times 17 \times 9.8 = 108.29 \text{ N}[/latex]

Answer:

[latex]\large F > 108.29 \text{ N}[/latex]

b) Solution:

Analyze the motion on the axis (axes). Ask the question: Is this a situation of equilibrium?

Since F is positioned on the x axis, we need to ask the equilibrium question about the x axis.

On the x axis we do not have a situation of equilibrium because the toolbox is moving with an acceleration.

In this case we use Newton’s second law and the net force on the x axis to solve the question:

[latex]\large \text{(a)} \quad F_{\text{net}} = m \times a[/latex]

[latex]\large \text{(b)} \quad F_{\text{net}} = F - F_f[/latex]

Since expressions a) and b) represent the same net force, we can equal them:

[latex]\large F - F_f = m \times a[/latex]

Solving for F:

[latex]\large F = F_f + m \times a = \mu_k \times m \times g + m \times a = 0.40 \times 17 \times 9.8 + 17 \times 0.20 = 70.04 \text{ N}[/latex]
Answer:

[latex]\large F = 70.04 \text{ N}[/latex]

[A] Notes

  1. Recall: Equilibrium occurs when either the object is at rest, or it moves at a constant speed.
    Equations to use:

    [latex]\large F_{\text{net}, x} = 0[/latex]

    [latex]\large F_{\text{net}, y} = 0[/latex]

  2. Recall: An object moving with an acceleration is not in a situation of equilibrium.Equations to use:

    [latex]\large F_{\text{net}} = m \times a[/latex]

    [latex]\large F_{\text{net}} = \sum \overline{F}[/latex]

Try it!

  1. A sled is being pulled by a child with a rope that makes a 30° angle with the vertical. The sled is moving horizontally at a constant speed. Which one of the following statements are true?
    1. Equilibrium situation on both x and y axes
    2. Equilibrium situation only on y
    3. Equilibrium situation only on x
  2. The normal force is always directed:
    1. Parallel to the contact surface
    2. Opposing the motion of the object
    3. Perpendicular on the contact surface
  3. If an object moves horizontally at a constant speed due of a horizontal pulling force of 50 N, what is the force of friction?
    1. Not enough information to calculate it
    2. 50 N
    3. 490 N

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College Physics – Fundamentals and Applications Copyright © by Daniela Stanescu, Centennial College is licensed under a Creative Commons Attribution-NonCommercial 4.0 International License, except where otherwise noted.