A uniform rectangular flat plate has mass \(M\) and dimensions \(a\) by b. Use the parallel-axis theorem in conjunction with Table 10.2 to show that its rotational inertia about the side of length \(b\) is \(\frac{1}{3} M a^{2}\)

Short Answer

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The rotational inertia of the uniform rectangular flat plate about the side of length \(b\) is \(\frac{1}{3} M a^{2}\)

Step by step solution

01

Understand and visualize the problem

The problem is presenting a rectangular flat plate with mass \(M\) and dimensions \(a\) and \(b\). The task is to find the rotational inertia or moment of inertia about the side of length \(b\).
02

Ready the parallel-axis theorem

The parallel-axis theorem is given by \(I = I_{cm} + M d^2\), where, \(I\) is the moment of inertia about some axis parallel to and a distance \(d\) away from the axis passing through the center of mass, \(I_{cm}\) is the moment of inertia of the body about the axis through the center of mass, and \(M\) is the mass of the body, and \(d\) is the distance between the axis.
03

Compute the moment of inertia about an axis through the center of mass

From Table 10.2, the center of mass of a thin rectangular flat plate is given by \(I_{cm} = \frac{1}{12} M (a^2 + b^2)\). As the axis is about the side of length \(b\), the distance \(d\) between this axis and the axis through the center of mass is \(a/2\).
04

Apply the parallel-axis theorem

Substituting for \(I_{cm}\), \(M\), and \(d\) in the expression of the parallel-axis theorem, we get \(I = \frac{1}{12} M (a^2 + b^2) + M (\frac{a}{2})^2\). Since the axis is through the side of length \(b\), \(b^2\) does not need to be considered in the computation of \(I_{cm}\). Thus, the equation simplifies as: \(I = \frac{1}{12} Ma^2 + \frac{1}{4} Ma^2 = \frac{1}{3} Ma^2\).

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