I don't understand this idea about torque

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Total torque T can be translated in space without affecting the system's overall behavior, but it will slightly alter the angular momentum about the A-B axis. Applying a force to flip a gyroscope changes the direction of its angular momentum rather than creating torque along the A-B axis. The system conserves angular momentum, meaning any change in one direction necessitates a compensatory change in another. In gyroscope dynamics, rapid spinning allows for significant changes in angular momentum direction with minimal force application. Understanding these principles is crucial for analyzing gyroscopic motion effectively.
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First, not related to this figure, if there is a total torque T acting on a body, can I move this vector around the space by translation? Will I affect the system?Second, I don’t understand why can’t there be torque along the A-B axis. For example, if I apply a force to flip the gyroscope, the gyroscope will definitely turn around and there will be an increase of angular momentum along the A-B axis.Thank you.

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If you apply a torque so that the system rotates about the A-B axis, you do change by a very slight amount the angular momentum about the A-B axis. That portion of angular momentum is for the most part ignored in this analysis. The more important effect is that you will change the direction of the angular momentum of the spinning gyroscope. The change in the angular momentum of the spinning gyro could very well point downward, i.e. ## \Delta \vec{L}= \vec{L}_2-\vec{L}_1 ##, from the spinning gyro, can readily occur in the minus z direction, if you push downward on the near side of the frame that holds the gyro. ## \\ ## Since you did not apply any torque in the z direction, total z angular momentum needs to be conserved, and there will be an increase in the angular momentum of the system in the +z-direction to offset this. Basically there will be an increase in ## \Omega ##. Otherwise you would need to apply a torque in the minus z-direction to prevent this increase in ## \Omega ##. ## \\ ## Additional note: In these gyroscope problems, you can often assume the gyro to be spinning quite rapidly, so that ## \vec{L}_1 ## and ## \vec{L}_2 ## are quite large and of equal amplitude. A small change in direction from ## \vec{L}_1 ## to ## \vec{L}_2 ## can result in a very large ## \Delta \vec{L} ##, whose direction can be readily computed.
 
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