Understanding Angular Momentum in Rigid Body Rotation

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Angular momentum for a rigid body can be expressed as the product of its moment of inertia and angular velocity only when rotating about an axis of symmetry, as the moment of inertia is a tensor that simplifies in this case. When rotation occurs around a non-symmetry axis, the angular momentum does not align with the rotation axis due to the tensor's non-diagonal nature. This concept is often covered in mechanics textbooks, but explanations can be lacking for high school students. An example illustrating this phenomenon could clarify the relationship between angular momentum and rotation axes. Understanding these principles is crucial for grasping the complexities of rigid body dynamics.
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Why can only the angular momentum of a rigid body rotating about an axis of symmetry be expressed as the product of the body's moment of inertia and its angular velocity?
 
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The "moment of inertia" is actually a tensor. If a body is rotated about an axis that is not a symmetry axis (or, more generally, an axis for which the tensor is not diagonal), the angular momentum in not in the direction of the axis of rotation.
This is discussed in Mechanics terxtbooks.
 
Hmm.
I still don't really understand why not and my textbook doesn't supply much of an explanation.
Could someone please explain more thoroughly in terms a high school physics student might be privy to?
 
clem said:
If a body is rotated about an axis that is not a symmetry axis [..] the angular momentum [is] not in the direction of the axis of rotation.
Would you describe (or cite) an example of that?
 
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