Calculating the Inertia Tensor of a Homogeneous Sphere

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Homework Help Overview

The discussion revolves around calculating the moments of inertia for a homogeneous sphere, specifically focusing on the inertia tensor and its components. The original poster attempts to set up the integral for the inertia tensor using both Cartesian and polar coordinates.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the setup of the integral for the inertia tensor, questioning the definitions of variables and the correctness of the integrand. There is a focus on ensuring the proper formulation of the integral and the implications of choosing specific components for calculation.

Discussion Status

The discussion is ongoing, with participants providing feedback on the original poster's attempts and suggesting reconsideration of the integrand. There is an exploration of different approaches to calculating the moments of inertia, with no explicit consensus reached yet.

Contextual Notes

Participants note potential errors in the integrand and the importance of correctly identifying the components of the inertia tensor. There is also mention of the need to simplify the problem by focusing on specific components of the inertia tensor.

Storm Butler
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Homework Statement



Calculate the moments of Inertia I_{1}, I_{2}, I_{3} for a homogenous sphere

Homework Equations



I_{jk}=\intx^{2}_{l}\delta_{ik}-x_{i}x_{k}dV


The Attempt at a Solution



For I_{x} i set up the equation using the above equation in cartesian coordinates and then i switched into polar coordinates and i get the following integral
\rho\int\int\int(r^{2}-rsin(\vartheta)cos(\phi))r^{2}sin(\vartheta)d\phid\varthetadr
with 0\leqr\leqR, 0\leq\phi\leq2\pi, and 0\leq\vartheta\leqpi

when i solve this integral i get I=\rho\frac{4}{5}\piR^{2} and then setting \rho= \frac{M}{4/3\piR^{3}<br /> }
so after simplifying i end up with I=\frac{3}{5}MR^{2}
But the answer i believe is \frac{2}{5}MR^{2} , so i don't really know where is went wrong.
 
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How did you end up with that integral? What are i an k in your expression? Remember that the principal moments of inertia are the diagonal terms in Iij. Start by making the easiest choice for i=j and then think if you have to calculate more.
 
as i started to type i response i realized my integrand was essentially r^{2}-x. when i should have been r^{2}-x^{2}. So what i should have is r^{4}-r^{4}sin(\vartheta)^{3}cos\phi^{2}

If i integrate this then i get 2/5\pi^{2}R^{5}. which looks better.
 
although if i then multiply this by rho i get 3/10\piMR^{2}...
 
Storm Butler said:
as i started to type i response i realized my integrand was essentially r^{2}-x. when i should have been r^{2}-x^{2}. So what i should have is r^{4}-r^{4}sin(\vartheta)^{3}cos\phi^{2}

If i integrate this then i get 2/5\pi^{2}R^{5}. which looks better.

That's not right either, one sin(θ) should be in the integration measure. Perhaps it would be easier to calculate only the zz-component of I. Why is this enough?
 

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