Torques in rotational equilibrium

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SUMMARY

In rotational equilibrium, the net torque about any point on an object or any point in space must be zero. This is demonstrated using a balanced seesaw, where the torque contributions vary depending on the chosen pivot point. When calculating torque around the pivot point, the force at that point does not contribute to torque, while forces at other points do. Understanding that the physical pivot remains constant while the reference point for torque calculations can change is crucial for grasping this concept.

PREREQUISITES
  • Understanding of torque and its calculation
  • Familiarity with the concept of rotational equilibrium
  • Basic knowledge of forces and moments in physics
  • Ability to visualize and analyze mechanical systems, such as seesaws
NEXT STEPS
  • Study the principles of torque and rotational dynamics in detail
  • Learn about the conditions for static equilibrium in mechanical systems
  • Explore examples of torque calculations using different pivot points
  • Investigate the implications of torque in real-world applications, such as engineering structures
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Students of physics, educators teaching mechanics, and anyone interested in understanding the principles of rotational dynamics and equilibrium.

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Homework Statement



Why, for any system that is in rotational equilibrium, the torque about 1) any point on the object or 2) any point in space, must be zero.

Homework Equations



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The Attempt at a Solution



What I do not understand is, why the torque about ANY point on the object is zero? Isn't it only about the point of rotation/center of gravity? Say, if I have a seesaw that is balanced (therefore it's in rotational equilibrium?) on both side. If I move the pivot point away from the middle, the equilibrium will not exist anymore, right? How can this be for torque about ANY point?

Also, as 2) stated in the original question, about ANY POINT IN SPACE, too? I.e. A balanced seesaw with torque about a random position on the moon??

There got to be something important here I missed or didn't understand. Can someone clarify these for me? Thank you!
 
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If you have a balanced seesaw and you look at torques around the pivot point then the force at the pivot point doesn't contribute any torque because it's at the pivot point. And it doesn't rotate because the torques sum to zero. If you compute the torques around some other point, like an endpoint of the seesaw, then the force at the end of the seesaw now contributes no torque, but now the force at the pivot does. But they still have to sum to zero because it still doesn't rotate. Write down a concrete example and try it.
 
Dick said:
If you have a balanced seesaw and you look at torques around the pivot point then the force at the pivot point doesn't contribute any torque because it's at the pivot point. And it doesn't rotate because the torques sum to zero. If you compute the torques around some other point, like an endpoint of the seesaw, then the force at the end of the seesaw now contributes no torque, but now the force at the pivot does. But they still have to sum to zero because it still doesn't rotate. Write down a concrete example and try it.

Thank you so much Dr.! Now it makes sense! I think the reason I couldn't understand this before was I always assumes that the actual pivot point "moves" with different ways of torque calculation! After all, the physical pivot for the seesaw is still at the same location but the imaginary rotation center used for torque calculation changes for different ways torque combination! :)
 

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