Period of small oscillations in central potential

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SUMMARY

The discussion focuses on determining the period of small oscillations for a particle in a central potential defined by V(r) = -k(e^{-αr})/r. The effective potential is expressed as V_eff(r) = -k(e^{-αr})/r + (l²)/(2mr²), where l represents angular momentum. The minimum of the effective potential occurs at r_0, allowing for circular motion. The period of oscillations around this orbit is independent of the particle's energy or angular momentum.

PREREQUISITES
  • Understanding of central potential and effective potential in classical mechanics
  • Familiarity with the concepts of angular momentum and centrifugal potential
  • Knowledge of oscillatory motion and its mathematical representation
  • Basic proficiency in calculus, particularly in solving differential equations
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  • Research the derivation of the period of small oscillations in classical mechanics
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This discussion is beneficial for physicists, particularly those specializing in classical mechanics, as well as students studying dynamics and oscillatory systems.

Chen
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Hi,

A particle is subjected to a central potential of:

V(r) = -k\frac{e^{-\alpha r}}{r}
Where k, \alpha are known, positive constants.

If we make this problem one-dimensional, the effective potential of the particle is given by:
V_{eff}(r) = -k\frac{e^{-\alpha r}}{r} + \frac{l^2}{2 m r^2}
Where the second term is the "centrifugal potential", l is the absolute value of the angular momentum the particle has.

Now suppose that this effective potential has a minimum at r_0, which is known, so that if placed there the particle will have a circular motion.

The question is - what is the period of small oscillations (in the r-dimension) around the circular orbit?
The answer needn't depend on the energy of the particle or its angular momentum.

Thanks,
Chen
 
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