Moment of inertia Derive the formula for the moment of inertia of a uniform thin rod of length L and mass M about an axis through its center, perpendicular to its face.

College Physics
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Author:Raymond A. Serway, Chris Vuille
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Chapter1: Units, Trigonometry. And Vectors
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**Moment of Inertia**

Derive the formula for the moment of inertia of a uniform thin rod of length \( L \) and mass \( M \) about an axis through its center, perpendicular to its face.

*Diagram Explanation:* 
The diagram shows a horizontal rod with a vertical dashed line through its center, indicating the axis of rotation.

Repeat the calculation, only now assume the rod has a density that increases uniformly from a value of \( \rho_0 \) on one end to \( 2\rho_0 \) on the other end.

**Suggestion**

For the second integration, it is important to define the density function correctly: It will be a straight line that includes the two points \((-L/2, \rho_0)\) and \((L/2, 2\rho_0)\). Find the slope of the line as rise over run, and the x-intercept, \( \rho(0) \).

Total mass of the rod, \( M \), will be the integral of the density function from \(-L/2\) to \( L/2 \).

If you solve the second integration correctly, including the value of the total mass, \( M \), in terms of \( \rho \), you should see a very interesting relationship between the two moments of inertia.
Transcribed Image Text:**Moment of Inertia** Derive the formula for the moment of inertia of a uniform thin rod of length \( L \) and mass \( M \) about an axis through its center, perpendicular to its face. *Diagram Explanation:* The diagram shows a horizontal rod with a vertical dashed line through its center, indicating the axis of rotation. Repeat the calculation, only now assume the rod has a density that increases uniformly from a value of \( \rho_0 \) on one end to \( 2\rho_0 \) on the other end. **Suggestion** For the second integration, it is important to define the density function correctly: It will be a straight line that includes the two points \((-L/2, \rho_0)\) and \((L/2, 2\rho_0)\). Find the slope of the line as rise over run, and the x-intercept, \( \rho(0) \). Total mass of the rod, \( M \), will be the integral of the density function from \(-L/2\) to \( L/2 \). If you solve the second integration correctly, including the value of the total mass, \( M \), in terms of \( \rho \), you should see a very interesting relationship between the two moments of inertia.
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