Motion of parallel-incoming particles in gravitational field

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SUMMARY

The discussion centers on the motion of a large parallel beam of incoming particles with mass m and uniform velocity v0 in a gravitational field created by a spherical planet of mass M and radius R. The conservation of energy and angular momentum equations are utilized to analyze the impact velocity and tangential components, but the participants conclude that insufficient information is provided to determine the fraction of particles that will reach the planet. Specifically, the diameter of the particle beam is critical, as it directly influences the number of particles that can achieve a perigee closer than the planet's radius.

PREREQUISITES
  • Understanding of classical mechanics principles, particularly conservation of energy and angular momentum.
  • Familiarity with gravitational fields and their effects on particle motion.
  • Knowledge of spherical mass distributions and their gravitational influence.
  • Basic proficiency in mathematical modeling of physical systems.
NEXT STEPS
  • Research the implications of conservation of energy in gravitational fields.
  • Study angular momentum conservation in particle dynamics.
  • Explore the effects of beam diameter on particle trajectories in gravitational fields.
  • Investigate numerical methods for simulating particle motion in gravitational fields.
USEFUL FOR

Physicists, astrophysicists, and students studying classical mechanics, particularly those interested in particle dynamics in gravitational fields.

Aaronaut
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Question:
There is a large parallel beam of incoming particles with mass m and uniform velocity v0 (v0≪c) in the presence of a gravitational field of a (spherical) planet with mass M and radius R. (without GR) The question is what fraction of the particles will eventually arrive at the planet.
Relevant formulas/attempt to solve
The conservation of Energy implies that
v20=v2−γMR,
which would give the norm of the velocity at the moment of impact. Furthermore, for the tangential component of the velocity could be at least in principle calculated using the conservation of angular momentum,
rv0,t=Rvt,
where r is the original distance vector of the particle. However, there is the problem, that since the case of a far-away particle is considered, r→∞, the left-hand expression is hard to evaluate. In addition, these equations still do not, at least from my point of view, contain enough information to calculate the fraction of particles arriving.
 
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Not sure I'm interpreting the question correctly. Are we to assume that the diameter of beam exceeds that of the planet, so it's a question of which particles would have a perigee closer than the radius of the planet? If so, I agree there's not enough information. We need to know the diameter of the beam.
 
I think the problem is to determine the radius of the particle beam, because it should be proportional to the number of particles.
 

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