Gravitational force due to sphere

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SUMMARY

The discussion focuses on calculating the speed of a particle falling from infinity to the center of a thin hollow spherical shell with radius R and surface mass density ρ. The gravitational force acting on the particle is derived from the shell's center of mass, and the problem emphasizes the use of conservation of energy principles. The gravitational potential energy at infinity is zero, and as the particle approaches the shell, the gravitational force increases. The key equations involved include F = -GMm/r² and the concept that only the mass within the radius r attracts the particle once it is inside the shell.

PREREQUISITES
  • Understanding of gravitational force and potential energy
  • Familiarity with conservation of energy principles
  • Knowledge of calculus for analyzing forces over distance
  • Concept of center of mass in spherical shells
NEXT STEPS
  • Study gravitational potential energy calculations in spherical shells
  • Learn about the implications of the shell theorem in gravitational physics
  • Explore advanced topics in calculus related to infinite series and sums
  • Investigate the dynamics of particles in gravitational fields
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Physics students, educators, and anyone interested in gravitational mechanics and energy conservation principles in spherical systems.

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Homework Statement

Consider a thin hollow fixed spherical shell of radius R and surface mass density rho. A particle initially at rest falls in from infinity. What is its speed when it reaches the center of the shell?

(Assume that a tiny hole has been cut in the shell to let the particle thru.)

Known:

rho, distance between centers of masses, R, G

Homework Equations



F = -GMm/r^2

The Attempt at a Solution

The source of the force acts through the center of the sphere, right? So I know the force, but the problem says the particle falls from infinity (I'm assuming I'd need to use calculus here then)

The gravitational force from the sphere acting on the particle is originating from the sphere's center of mass, and pulling it towards that center radially. The part that tricks me is bringing the test particle in from infinity, so the g-force is pretty much zero at that point in time, and slowly increases at it gets closer. Seems like I require an infinite sum here, but not sure how to realize that.
 
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Use conservation of energy. At infinity, the gravitational potential energy is zero, and the particle is in rest, so its KE=0, too. What is the formula for the gravitational potential energy?

When reaching the sphere, and entering into it, getting at a distance r<R from the centre, only that mass attracts the particle that is confined in the sphere of radius r. What is the force in the empty sphere?

ehild
 

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