Elliptical orbit centered at the origin

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SUMMARY

The discussion centers on deriving the polar equation for a particle in an elliptical orbit influenced by a central force, specifically a spring force. The polar equation is established as 1/r = sqrt(A + B*sin^2(θ), where A and B are constants. The force F(r) is confirmed to derive from Hooke's law, represented as F = -k(r - L), indicating that the potential must be harmonic in two dimensions for the orbit to remain elliptical.

PREREQUISITES
  • Understanding of polar coordinates and transformations
  • Familiarity with Hooke's law and spring forces
  • Knowledge of differential equations, particularly radial equations
  • Basic concepts of orbital mechanics and elliptical orbits
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  • Study the derivation of polar equations in orbital mechanics
  • Learn about the properties of harmonic potentials in two dimensions
  • Explore the application of differential equations in physical systems
  • Investigate the relationship between central forces and orbital shapes
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Students and professionals in physics, particularly those focusing on mechanics and orbital dynamics, as well as anyone interested in the mathematical modeling of forces and motion.

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Homework Statement


Under the influence of a central force F(r), a particle of mass m is observed to move in an elliptical orbit centered at the origin (the force center is not at one of the foci, as would be the case for a gravitational orbit)
a.) Show that the polar equation has the form 1/r = sqrt(A + B*sin^2(θ)) , where A and B are constants
b.) Show that the force f(r) comes from a simple spring (obeying Hooke's law) connected to the origin.

Homework Equations


Transformed radial equation u'' = -u - (mF)/(L^2u^2) where u = 1/r

The Attempt at a Solution


I know that in order to find r we must substitute F(r) in the equation. The problem is in this case the force comes from a spring or F = -kr, which when substituted into the eq, we will have u^3 in the denominator.
 
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F is not -kr, but -k(r - L), where L is the undistorted length of the spring.
 
mjc123 said:
F is not -kr, but -k(r - L), where L is the undistorted length of the spring.
If this was the case the orbit would not be elliptic. The potential needs to be a harmonic potential in two dimensions, which means that the force needs to vary as -kr and nothing else.
 

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