Calculating Moment of Inertia for a Rigid Body

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Homework Help Overview

The problem involves calculating the moment of inertia for a rigid body composed of three thin uniform rods arranged perpendicularly at their midpoints. The task is to demonstrate that the moment of inertia remains constant for any axis that passes through the origin.

Discussion Character

  • Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to determine if a coordinate transformation is necessary to relate the principal axes to an arbitrary axis through the origin. They question whether this transformation affects the diagonal elements of the inertia tensor.

Discussion Status

Some participants have noted that the principal moments of inertia are equal, suggesting that the inertia tensor is proportional to the unit matrix. This implies that any rotation will not alter the tensor of inertia, but there has not been explicit consensus on the necessity of a coordinate transformation.

Contextual Notes

There may be assumptions regarding the uniformity of the rods and the specific arrangement of the axes that are under discussion, but these have not been fully articulated.

ehrenfest
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Homework Statement


A rigid body consists of three thin uniform rods, each of mass m and length 2a, held mutually perpendicular at their midpoints. Show that the moment of inertia is the same for any axis passing through the origin.


Homework Equations





The Attempt at a Solution


I calculated the principal moments of inertia. To show this, do I need to find a coordinate transformation to take one of the principal axes to an arbitrary axis that goes through the origin and then show that the transformation does not change that element on the diagonal of the inertia tensor? Or is there another way to do this?
 
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The three principal moments of inertia are equal.
This means the tensor of inertia is proportional to the unit matrix,
so any rotation will not change the tensor of inertia.
It will still be the unit matrix in any rotated system.
 

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