Frequently Made Errors in Mechanics - Moments - Comments

AI Thread Summary
The discussion focuses on common errors in mechanics, particularly regarding the equation of momentum for rigid bodies. It highlights that the equation is valid only when point A is either a stationary point or the center of mass, and using it for the instantaneous center of rotation is incorrect. Additionally, it emphasizes that the term involving angular velocity is zero in planar problems but must be considered in three-dimensional scenarios. The inertia tensor must also refer to the body-fixed point A for accurate calculations. Understanding these nuances will improve calculations involving torques and moments of inertia in physics.
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Frequently Made Errors in Mechanics - Moments

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Nice post, Haruspex. I'll have to come back to this when I start my physics and mechanics classes.
 
Nice work haruspex!
 
Having read this, my future calcs involving torques and moments of inertia will be much faster and easier.
 
Nice article. I just want to add some comment on the equation of momentum for rigid body and on some very frequent errors that arise in this regard.
The equation of momentum is
$$J_A\dot{\boldsymbol \omega}+\boldsymbol\omega\times J_A\boldsymbol\omega=\boldsymbol M_A.\qquad (*)$$ Here ##J_A,\boldsymbol\omega## are the operator of inertia about the point ##A## and the angular velocity of the rigid body respectively; ##\boldsymbol M_A## is the torque about the point ##A## applied to the rigid body.

But what is the point ##A##? If ##A## is a stationary point of the rigid body or its center of mass then equation (*) is correct.
In general, it is incorrect to use formula (*) for ##A## to be instantaneous centre of rotation; it is incorrect even for planar problems.

Another frequent error is concerned to the term ##\boldsymbol\omega\times J_A\boldsymbol\omega##. This term is equal to zero identically in planar problems. But one can not forget it in essentially 3D problems.
 
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One should also note that the tensor of inertia, ##J_A##, must refer to the body-fixed point ##A##.
 
vanhees71 said:
ne should also note that the tensor of inertia, JAJ_A, must refer to the body-fixed point AA.
sureaccidentally I came across an article
https://www.jstor.org/stable/2973359?seq=1#page_scan_tab_contents
perhaps It should be noted about a general formula. Let a point ##A## be any point of the rigid body. Then
$$J_A\dot{\boldsymbol\omega}+\boldsymbol\omega\times J_A\boldsymbol\omega+m\boldsymbol{AS}\times \boldsymbol a_A=\boldsymbol M_A;$$
where ##S## is the center of mass, ##m## is the mass of the rigid body, ##\boldsymbol a_A## is the acceleration of the point ##A##.
 
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