Gravitational potential of a thin ring

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SUMMARY

The discussion focuses on determining the gravitational potential of a thin ring with radius 'a' and mass 'M' when a mass 'm' is placed within the plane of the ring, specifically for distances 'r' less than 'a'. Participants emphasize the importance of using the law of cosines to set up the integral and highlight the necessity of considering the radial components of gravitational force due to symmetry. Additionally, the discussion touches on finding the equilibrium position and analyzing its stability through small displacement expansions.

PREREQUISITES
  • Understanding of gravitational potential and forces
  • Familiarity with integral calculus
  • Knowledge of the law of cosines
  • Concept of equilibrium and stability in physics
NEXT STEPS
  • Study the derivation of gravitational potential for various mass distributions
  • Learn about stability analysis in gravitational systems
  • Explore advanced integral calculus techniques for physics applications
  • Investigate the implications of symmetry in gravitational fields
USEFUL FOR

Students and professionals in physics, particularly those studying gravitational systems, as well as educators looking to enhance their understanding of gravitational potential and stability analysis in mechanics.

DerekDnl
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Hello, I am not sure how to set up this integral. Its a little more advanced than I am used too. Any ideas?


Consider a thin ring of radius a and mass M. A mass m is placed in the plane of the ring (not in the center!). Determine the gravitational potential for r < a. Find a position of equilibrium and determine whether it is stable or unstable. (Hint: Consider a small displacement from the equilibrium position and do an expansion.)


I think I have to use the law of cosines. But why would I need to do an expansion?
 
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Welcome to PF.

Consider that wherever you are inside the ring you basically only need to be concerned about the component of the gravitational force that is in the radial direction. By symmetry anything normal to the radius will be canceled out left to right won't it?

So for any point a distance r away from the center all you need to do is develop an expression that describes, for each element about the ring the gravitational component that projects to the radius your mass is on.
 

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