Find rotation matrix that diagonalizes given inertia tensor

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Homework Help Overview

The problem involves finding a rotation matrix that diagonalizes a given moment of inertia tensor for a rigid body. The inertia tensor is presented in a specific coordinate frame, and the task is to transform it into a diagonal form using a rotation matrix.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to diagonalize the inertia tensor using eigenvectors to form the rotation matrix. They also explore a specific rotation about the x3 axis and question how to determine the angle for this transformation. Other participants confirm the validity of the initial approach and discuss the relationship between rotation matrices and their properties.

Discussion Status

Some participants have provided guidance on the approaches taken, with one confirming that the initial method should work. The original poster has revisited their calculations and found success in diagonalizing the tensor. However, they express a desire for further clarification on the physical interpretation of the rotation matrix derived from the eigensystem.

Contextual Notes

There is a mention of the need to normalize eigenvectors and the relationship between rotation matrices and their transposes. The discussion includes considerations of angles and directional cosines in the context of the transformation.

mindarson
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Homework Statement



In a particular coordinate frame, the moment of inertia tensor of a rigid body is given by

I = {{3,40},{4,9,0},{0,0,12}}

in some units. The instantaneous angular velocity is given by ω = (2,3,4) in some units. Find a rotation matrix a that transforms to a new coordinate system in which the inertia tensor becomes diagonal.

Homework Equations



I' = RIR^-1

The Attempt at a Solution



I've tried a couple of approaches. First, I figure that I'm essentially just trying to diagonalize a matrix (the problem does not specify a particular transformation, just one that will diagonalize the tensor). So I used the equation above and found the diagonalizing matrix R by finding the eigenvectors of I and using them as the columns of the diagonalizing matrix R. I do not see any reason why this will not work, but when I checked it the matrix I came up with for R did not diagonalize I. But maybe my computations were hasty.

My second approach was to assume a certain transformation, i.e. a rotation of the body about, say, the x3 axis. Then the rotation matrix would be

R = {{cosθ, sinθ, 0},{-sinθ,cosθ,0},{0,0,1}}

and its inverse is

R^-1 ={{cosθ,-sinθ,0},{sinθ,cosθ,0},{0,0,1}}

I then compute the matrix I' = RIR^-1 and try to find a rotation angle θ that causes the off-diagonal elements to vanish. However, I have no idea how to proceed to find this angle. (Solve another system of equations?) Also, I have a distinct feeling that the solution should not be quite this complicated.

Can anyone give guidance?
 
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Your initial approach should have done the trick.
 
Thank you for your reply! I tried my initial approach again, and this time it did work to diagonalize the tensor. I think I just was hasty in my calculations.

However, I wonder if you can help me think this through. I do not feel too comfortable just calling the matrix I found via the eigensystem a 'rotation matrix' without actually dealing explicitly with the angles and functions of the angles through which the coordinate system has been rotated. Is there a way, at least in principle, to arrive at this rotation matrix using my second approach, i.e. by using the transformation matrix that uses the directional cosines? Then I would feel more comfortable with my answer from a physical, versus just a formal, perspective.

But thanks again for your confirmation!
 
Both approaches are identical. One property of a rotation matrix R which you might have overlooked is that R Transpose = R inverse.

See wiki articles on Mass Moment ofIinertia and Rotation Matrix for the math.
 
Just normalize your eigenvectors. You should be able to see by inspection what ##\cos\theta## and ##\sin\theta## are equal to.
 

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