Verifying a Valid Inertia Tensor

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Discussion Overview

The discussion revolves around the conditions for a valid inertia tensor in multibody dynamics, specifically focusing on the relationship between principal moments of inertia and the physical validity of these values. Participants explore theoretical underpinnings, exceptions, and implications of these conditions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Kerry shares an experience with multibody dynamics software that flagged an invalid inertia tensor, prompting a question about the underlying principles that govern these values.
  • Some participants suggest that the relationship between principal moments of inertia is an original result from Euler.
  • There is a mention of the trace of a matrix being equal to the sum of its eigenvalues as a potential explanation for the conditions on the inertia tensor.
  • One participant notes exceptions to the rule, specifically for a point mass and an infinitely thin rod, which do not conform to the general relationship.
  • Another participant discusses the relationship 2*max(lambdai) < sum(lambdai) for a set of three non-colinear point masses, suggesting it as a basis for the validity of the inertia tensor.
  • Kerry seeks clarification on the physical meaning of the mathematical relationships discussed, particularly in relation to the center of gravity of the object.
  • There is a back-and-forth regarding the formulation of the test for the inertia tensor, with participants refining their understanding of the conditions involved.
  • Kerry expresses gratitude for a link to a paper that contains a proof related to the generalized perpendicular axis theorem, indicating it was a significant find for their inquiry.

Areas of Agreement / Disagreement

Participants express varying interpretations of the conditions for a valid inertia tensor, with some agreeing on the mathematical relationships while others highlight exceptions. The discussion remains unresolved regarding the complete understanding of the physical implications and derivations of these relationships.

Contextual Notes

Participants note limitations in their understanding and the need for specific reference frames when applying the discussed relationships. There is also acknowledgment of the dependency on definitions and the potential for confusion when not using the center of gravity as a reference.

KLoux
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Hello,

Recently I was using multibody dynamics software at work and when I ran the simulation it warned me that the values that I specified for the inertia tensor of one of the bodies was physically impossible. It turned out that I had mistyped one of the values and it was an easy fix, but it got me thinking - how did it know?

After some searching I found a source (which I cannot remember now) that said the sum of any two principle moments of inertia for an object must be greater than the third. After some testing of different shapes I think that this is true, but why? Is there a derivation anywhere? None of my textbooks mention this at all and the one source that I did manage to find didn't provide an explanation.

Thanks for your help!

-Kerry
 
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Hmm..this is one of Euler's original results, I think.
 
IIRC, this is a consequence of the fact that the trace of a matrix is equal to the sum of its eigenvalues.
 
Two exceptions to the rule: A point mass and an infinitely thin rod. A point mass has a null inertia tensor. The inertia tensor for an infinitely thin rod about its center of mass is a degenerate inertia tensor in which one of the principal moments is zero and the other two are equal to each other. The test fails for both of these cases, but neither case is real.

The eigenvalues of the inertia tensor of a set of three non-colinear point masses about the common center of mass will obey the relation 2*max(lambdai) < sum(lambdai). This is the basis for the relationship. If you somehow conjoin two objects that obey the relationship, the inertia tensor for the composite object will also obey the relationship.
 
robphy said:
Thanks for the link, but I must be missing what I'm supposed to be seeing?

Crosson said:
IIRC, this is a consequence of the fact that the trace of a matrix is equal to the sum of its eigenvalues.
What does this mean physically? If you're using principle axis as your reference frame, then the sum of the principle moments of inertia is equal to the sum of the principle moments of inertia? Can you elaborate?

D H said:
The eigenvalues of the inertia tensor of a set of three non-colinear point masses about the common center of mass will obey the relation 2*max(lambdai) < sum(lambdai). This is the basis for the relationship. If you somehow conjoin two objects that obey the relationship, the inertia tensor for the composite object will also obey the relationship.
Does this mean that the test is actually 2*max(lambdai) < sum(lambdai)? Reading your post made me remember that I forget to mention - I think it is important that you are using the CG of the object as your reference. You can sometimes pass the test even if your inertia tensor is not physically valid if you're using some other frame.

Thanks for all the replies!

-Kerry
 
KLoux said:
Does this mean that the test is actually 2*max(lambdai) < sum(lambdai)?

Your test is lambdai < lambdaj+lambdak. Adding lambdai to both sides of the expression yields 2*lambdai < sum(lambdaj), where j=1,2,3. This is trivially true for all but the largest eigenvalue. Hence your test is the same as mine.
 
D H said:
Your test is lambdai < lambdaj+lambdak. Adding lambdai to both sides of the expression yields 2*lambdai < sum(lambdaj), where j=1,2,3. This is trivially true for all but the largest eigenvalue. Hence your test is the same as mine.
Yes, yes... I should have actually looked at your equation - thanks for pointing this out

KLoux said:
Thanks for the link, but I must be missing what I'm supposed to be seeing?
Ah, the first two hits are links to a paper that contains a proof! I missed them because the paper isn't free (but luckily I still have friends at a university with a subscription to the American Journal of Physics). The generalized perpendicular axis theorem was exactly what I was looking for! Thank you robphy.

-Kerry
 

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