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8.1. Concepts: Tension and Compression

Introduction

Tension is the force exerted by a rope, string, or cable on one or more objects. Force of tension appears in flexible elements when an object is being suspended, pulled, swung, etc.

Compression is a force that appears in rigid elements, such as bars, beams, etc., when they are pushed or pressed against.

Examples of situations when force of tension is involved:

  1. A load hanging from a crane’s system of cables
  2. A wagon being pulled by a rope
    Figure 8.1. Examples of force of tension

Concepts

Tension questions with one cable (rope, string) involved

When an object hangs from a cable, string or rope, a tension will appear in the rope that balances the force of gravity acting on the object. The object will be in equilibrium.To draw a FBD for this situation we can imagine that we cut the rope and replace its effect by a force – force of tension.

Figure 8.3. Solving tension questions with one cable (rope, string) involved

In this situation, the object is in equilibrium on both x and y axes. Therefore:

[latex]\large \vec T = F_g[/latex]

If the object hung by the rope is now given an upward acceleration, [latex]a[/latex], then the object will not be in equilibrium on the y axis anymore.

In this case we write the net force using Newton’s second law and using the net force definition:

 

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

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

On the y axis:

[latex]\large F_{net} = m[/latex] X [latex]\large a[/latex], and

[latex]\large F_{net} = T - F_g[/latex]

So:

[latex]\large T - F_g = m[/latex] X [latex]\large a , \hspace{.2cm}[/latex]or [latex]\large \hspace{.2cm} T = F_g \hspace{.2cm}\text + \hspace{.2cm} m[/latex] X [latex]\large a[/latex]

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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.