Rotational Equilibrium Study Guide
In this lesson, we will approach a more complex system, a rigid object that has constraints that do not permit a linear motion but allow circular motion. We will define moment of inertia and torque inertia, and we will apply the conditions of equilibrium when rotational motion occurs in different systems.
Similar to the linear motion where we defined inertia, an object rotating around a fixed axis will keep this motion unless acted upon by an external influence. The same will happen with an object at rest: It will keep the state of rest unless acted upon.
Whereas mass is a measure of linear inertia, the measure of rotational inertia is the moment of inertia, or I. This quantity, as inertia, is proportional to the mass of the object but is also related to how the mass is distributed around the axis of rotation. The same object rotating around two different axes will resist rotation differently, and therefore have a different moment of inertia.
Note that the moment of inertia depends on the distribution of mass around an axis. The further the mass is from the axis, the more rotational inertia the object has and the harder it is to change the state of current motion. In this chapter, we will address the behavior of rigid objects. These are objects that will keep their shape and form while under external influence.
An object continues to stay at rest or move in a uniform circular motion as long as there is no external influence to change that motion. This property is called rotational inertia.
If you consider a metal rod or a wooden dowel of mass m and length L rotating in one of the two situations shown by Figure 9.1, you will have different responses to rotation.
In this figure, the rod rotates around the axis passing through the middle of the rod, halfway between the ends. In this case, the moment of inertia can be calculated as shown to be I = m · L2/12.
If we consider now an axis passing through the end of the rod, as shown in Figure 9.2, the moment of inertia can be calculated and the result is larger: I = m · L2/3 hence it is harder to start rotating the object or stop the object if it is in rotation when the axis of rotation is as shown in Figure 9.2.
Other useful expressions for the moment of inertia are shown in Figures 9.3 through 9.6.
In our discussions, we have studied two different types of motion: linear motion and rotational motion. The difference between the two lies in the path that the points of the rigid body follow in their motion. While in linear motion, the path is made out of parallel lines; in rotational motion, there is a spinning of the object around an axis.
The conditions of equilibrium are different for these two types of motion. Imagine the following examples. In the first example, you apply two equal but opposite forces on the steering wheel of your car (or boat) in the manner shown in Figure 9.7.
What is the result of the forces? If the wheel is anchored at the middle, there is no action following the interaction with the object. There is no rotation of the steering wheel around the axis of rotation.
Now let's apply the forces as shown in Figure 9.8. The object will rotate around the axis of rotation. However, in terms of the net force, there is no difference in the two cases. They can both be represented in the same way:
Net F = 0
The difference in the two cases is in the point of application of the force. So, analog to force, we need another quantity that includes force but also includes the distance to the point of application of the force. We call this new quantity torque.
Torque is proportional to the applied force, F, and to the lever arm, I:
T = FI
- The pivot point is the point through which the axis of rotation passes.
- The line of action is an extension of the direction of the force.
- The lever arm is the length of the perpendicular dropped from the pivot point to the line of action.
- The unit of measurement for torque is N · m.
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