Understanding Rigid Body Rotation: Principles and Observations

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A body frame rotates with the body and does not need to align with the rotation axis, while the angular momentum vector is always aligned with this axis. An observer on the body surface perceives no motion relative to the body, and the principal axis of rotation is determined by the body's symmetry, which may differ from the actual rotation axis. The discussion raises questions about the existence of a body angular velocity vector as perceived by an observer in the body frame and the implications of precession observed from an external static frame. Observers can identify rotation through the Coriolis force, and principal coordinates can exist even without clear symmetry. The relationship between the angular momentum vector and precession in the rotating frame remains a key point of inquiry.
Tian En
Just to confirm a few points:
  1. A body frame rotates with a body. It need not be aligned to the rotation axis.
  2. Angular momentum vector always aligned with rotation axis (not deviates from it).
  3. An observer on the body surface (body frame) observes no motion on a body.
  4. Principal axis of rotation comes from the symmetry of the body.
  5. Principal axis of rotation need not be rotation axis itself.
For point 3, is there a body angular velocity vector in the first place as observed by the observer in the body frame? I think if the observer is in the external static frame, he can then observe the body precesses and hence the existence of angular momentum vector.

Thanks.
 
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An observer can always determine the rotation of his coordinate system from the Coriolis force.
 
Tian En said:
Principal axis of rotation comes from the symmetry of the body.

There exists principal coordinates even when there is no evident symmetry.
 
Is angular momentum vector of the rotating body precessing in the frame of an observer in the rotating body?
 
I built a device designed to brake angular velocity which seems to work based on below, i used a flexible shaft that could bow up and down so i could visually see what was happening for the prototypes. If you spin two wheels in opposite directions each with a magnitude of angular momentum L on a rigid shaft (equal magnitude opposite directions), then rotate the shaft at 90 degrees to the momentum vectors at constant angular velocity omega, then the resulting torques oppose each other...

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