Chapter 2 Review of Forces and Moments - Brown University
Chapter 2 Review of Forces and Moments - Brown University
Chapter 2 Review of Forces and Moments - Brown University
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<strong>Forces</strong> exerted by springs<br />
A solid object (e.g. a rubber b<strong>and</strong>) can be made to exert forces by stretching it. The forces exerted by a<br />
solid that is subjected to a given deformation depend on the shape <strong>of</strong> the component, the materials it is<br />
made from, <strong>and</strong> how it is connected to its surroundings. Solid objects can also exert moments, or torques<br />
– we will define these shortly. <strong>Forces</strong> exerted by solid components in a machine or structure are<br />
complicated, <strong>and</strong> will be discussed in detail separately. Here, we restrict attention to the simplest case:<br />
forces exerted by linear springs.<br />
A spring scale is a good example <strong>of</strong> a linear spring. You can attach it<br />
to something at both ends. If you stretch or compress the spring, it<br />
will exert forces on whatever you connected to.<br />
The forces exerted by the ends <strong>of</strong> the spring always act along the line<br />
<strong>of</strong> the spring. The magnitude <strong>of</strong> the force is (so long as you don’t<br />
stretch the spring too much) given by the formula<br />
F = k( L−<br />
a)<br />
where a is the un-stretched spring length; L is the stretched length,<br />
<strong>and</strong> k is the spring stiffness.<br />
In the SI system, k has units <strong>of</strong> N/m.<br />
Note that when you draw a picture showing the forces exerted by a<br />
spring, you must always assume that the spring is stretched, so that<br />
the forces exerted by the spring are attractive. If you don’t do this,<br />
your sign convention will be inconsistent with the formula<br />
F = k( L− a)<br />
, which assumes that a compressed spring (L