Help Me Analyze Particle Moving in Inverse Cubic Force Field

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SUMMARY

The discussion focuses on analyzing the motion of a particle in an inverse cubic force field described by the equation F = -Amr^-3. Key concepts include the conservation of angular momentum (L = m r^2 θ') and total energy (E = (1/2) m (r')^2 + (1/2) m r^2 θ'^2 + V(R)). The user seeks guidance on determining the potential function V(R) and analyzing possible orbits for different energy states (E = 0, E < 0, E > 0) while maintaining non-zero angular momentum.

PREREQUISITES
  • Understanding of classical mechanics principles, particularly central force motion
  • Familiarity with polar coordinates and their applications in physics
  • Knowledge of conservation laws, specifically angular momentum and energy
  • Basic proficiency in calculus, particularly integration for potential energy calculations
NEXT STEPS
  • Study the derivation of potential energy functions from force equations, specifically V(R) from F = -dV/dR
  • Explore the characteristics of orbits under central forces, focusing on energy conditions for bound and unbound orbits
  • Investigate the implications of angular momentum conservation on orbital shapes and stability
  • Learn about LaTeX for displaying mathematical expressions clearly in discussions and documentation
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This discussion is beneficial for physics students, educators, and researchers interested in classical mechanics, particularly those studying orbital dynamics in conservative force fields.

Odyssey
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Urgent! I really need help please!

Sorry for posting this question again. Lemme try to rephrase my question if it helps :frown: . Please help me get started on this question. I am really stuck and time is running out! :cry: I don't want the answer, I just need some pointers to get me going and headed in the right direction.

A particle moves in an inverse cubic, central, conservative force field. The force is
F = -Amr^-3,

where A = some constant,
m = mass of particle (pt. mass)
r = distance

I know that the angular momentum L (its 3 components) are conserved under a central force. The total energy is also conserved since the force is conservative.

L = m r^2 θ'
E = (1/2) m (r')^2 + (1/2) m r^2 θ'^2 + V(R)
The 2 equations above are written in polar coordinate form.

Is V(R) = - / F? (/ = integral...sorry) :frown:

How should I go about in describing the possible orbits of a particle moving under the influence of such a force? I have to consider the following cases: E = 0, E < 0, and E > 0, for non-zero angular momentum cases.

I need some desperate guidelines to get me started. Please give some advices. Thanks in advance! :redface:
 
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What is V(R)? If you need to display integrals or other math. symbols, use LaTex.
 
V(R) is the potential as a function of R.
 

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