Consider the motion of a point mass m in the potential V(r)

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SUMMARY

The discussion focuses on the motion of a point mass m in the potential V(r) = -k/r, where k > 0. Participants are tasked with demonstrating that there exists a solution x(t) representing circular motion with a constant frequency ω. The relationship between ω and the radius of the circular motion must be established, alongside proving the conservation of energy and angular momentum. Additionally, it is required to show that the radius of circular motion corresponds to the minimum of the effective potential.

PREREQUISITES
  • Understanding of classical mechanics, specifically Newtonian dynamics.
  • Familiarity with potential energy concepts and effective potential.
  • Knowledge of angular momentum and energy conservation principles.
  • Basic proficiency in calculus, particularly integration and parametric equations.
NEXT STEPS
  • Study the derivation of circular motion equations in classical mechanics.
  • Learn about effective potential and its significance in orbital mechanics.
  • Explore the conservation laws of energy and angular momentum in closed systems.
  • Investigate the mathematical techniques for computing arc lengths in parametric curves.
USEFUL FOR

This discussion is beneficial for physics students, educators, and anyone interested in classical mechanics, particularly those studying orbital dynamics and conservation laws in motion.

Muskovite
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Homework Statement



Consider the motion of a point mass m in the potential
V(r)=-k/r , k>0

Show that there is a solution x(t) of the equations of motion which is a circular motion
with constant circular frequency ω. Determine the relation between ω and the radius of the
circular motion. Show explicitely that energy and angular momentum are conserved along
the motion curve, by computing their values. Show also that the radius of the circular
motion coincides with the radius where the corresponding eective potential takes its
minimum.

Homework Equations


γ(t)=(rcos(ωt); r sin(wt)); r > 0; ω> 0;

The Attempt at a Solution


I am not really sure where to start. Maybe one can find the arc length for a piece of the curve γ, using this
s(t0,t1)=∫ from t0 to t1√(∑γ'k^2dx) and then go into the details, but for the moment I can't conjure up anything.
Any help would be highly appreciated.
 
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It's hard to know what approach you are expected to use. Can you give us a little information about the concepts that you are currently studying that you feel are relevant to the question?

I don't understand your integral for the arc length. Can you explain how you arrived at the expression for the integrand and why you feel that an expression for arc length will help to solve the problem? Is the k in the integrand the same k that appears in the potential? Does your integrand have the right dimensions to represent length?
 

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