Stuck on derivation of Euler's equations in rigid body dynamics

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The discussion centers on the derivation of Euler's equations for rigid body dynamics, specifically regarding the moment of inertia tensor and its dependence on the body's position. It highlights the importance of using a "body frame" that rotates with the rigid body, allowing for accurate measurements of angular momentum. The confusion arises when considering angular velocity in the body frame, as it seems contradictory to assume the body is stationary relative to this frame. The clarification provided indicates that angular momentum is measured in terms of the components along the rotating axes at a given moment, rather than implying the body is motionless. Understanding this distinction is crucial for grasping the dynamics of rigid body rotation.
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i was reading about derivation of Euler's equations for rotational dynamics (john taylor, classical mechanics, chapter 10) when i got stuck on one of the reasonings
essentially it refers to the moment of inertia tensor, since the tensor itself about a point is dependent on the position of the rigid body (hence the tensor would have to be a function of time) hence it is argued that it would be helpful to construct a "body frame" fixed within the body with its axis pointing at the principal axis of rotation of the body, this body frame would rotate along with the body (since it is fixed within the body). then came the part i didnt understand, it said the angular momentum measured in the body frame is L = w, where denotes the diagonal matrix and w the angular velocity. however since the frame is fixed inside the body, should the rigid body be stationary relative to the frame and hence w is zero? what is wrong with my reasoning?
 
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I had the same question when I first encountered Euler Rigid body equations. What the author means by "L in rotating frame" is the components of L along the rotating axes at that instant.
 
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