# Kepler's problem by H-J method

Kepler's problem is basically a problem related to central force. For simplicity we take inverse square force between nucleus of charge 'Ze' and electron of charge 'e'. In this case, Hamiltonian can be expressed as Where pr and pθ are the components of momentum for r and θ. Since the system is conservative and H doesn't involve time explicitly so,

H = α1 = E (say )...........2

As there is no time occuring in the expression of it so the generating function S in this case is Hamilton's characteristics function W. Thus, we can write

pi = ∂W/∂qi

pr = ∂W/∂r and pθ = ∂W/∂θ .............3

With the help of equation 3, equation 1 can be written as Using the method of variable separation, we have

W = Wr + Wθ ......5

Using eq 5 in eq 4, we get Again, we know that the angular momentum is always conserved in the central force problem i.e Hence complete solution becomes

W = Wθ + Wr θ1 = β + t For E<0, ∊ <1, the path of the particle is ellipse.

For E =0, ∊ = 1, the path of the particle is parabola.

For E>0, ∊ >1, the path of the particle is hyperbola.

Kepler's problem in actin angle variables

To exhibit all of the solution, we need to consider the motion in 3D space. In terms of spherical polar coordinate (r, θ, 𝜙), the Hamiltonian of the system is given by where V(r) = - k/r ...........2

If the variables in the corresponding H-J equation are separable, then W must have the form

W = W(r) + Wθ(θ) + W𝜙(𝜙)

with p𝜙 = ∂W𝜙 /∂𝜙 = α𝜙 pr = ∂Wr /∂r , pθ = ∂Wθ/∂θ

Thus the H-J equation reduce to The H-J equation then confirms that the quantity in the square bracket must be a constant. All the three of the action variables appear only in the form Jr + J +J𝜙. Hence all the frequencies are equal. The motion is completely degenrate. Thus the one frequency for the motion is given by if we evaluate the sum of J's in terms of the energy (E) from equations 11, the frequency is given by And the time period of the orbit is given by

𝜏 = 1/ γ Thus the equation 13 and 14 gives the frequency and time period for the motion in spherical polar coordinate system.

This note is taken from Classical Mechanics, MSC physics, Nepal.

This note is a part of the Physics Repository.