I don't understand this idea about torque

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This discussion centers on the principles of torque and angular momentum in gyroscopic systems. It establishes that while applying torque can influence the angular momentum vector, the primary effect is the alteration of the direction of angular momentum rather than its magnitude. Specifically, when a force is applied to a gyroscope, it can lead to an increase in angular momentum in the z-direction, necessitating a balance through conservation laws. The analysis emphasizes that the rapid spinning of the gyroscope allows for significant changes in angular momentum direction with minimal applied torque.

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Clara Chung
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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.

The full example is attached if it is helpful.
 

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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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