- #1
jds17
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Hi, I love the lectures by David Tong. Usually I can follow his calculations (but I am not yet so far into the lectures...). But one that I just cannot do is the derivation of the energy in (4.16), the expression being ##E = \frac {mk^2} {2 l^2} (e^2 - 1)##, where l is the constant angular momentum of the orbit of the single point particle, m its mass, V(r) = - k/r the expression for the potential and e the eccentricity of the orbit.
I just don't see how using the expression ##\frac {dr} {d\theta} = \frac {r_0 e \sin(\theta)} {(1+e \cos(\theta))^2}## (page 59) in the expression of the energy using the effective potential cancels out the angle ##\theta##. Of course it has to work since the energy is a constant of motion, but no matter what trigonometric manipulations I use, it does not cancel out the angle.
In case it is not so readable I have attached the relevant sections from the lecture
I just don't see how using the expression ##\frac {dr} {d\theta} = \frac {r_0 e \sin(\theta)} {(1+e \cos(\theta))^2}## (page 59) in the expression of the energy using the effective potential cancels out the angle ##\theta##. Of course it has to work since the energy is a constant of motion, but no matter what trigonometric manipulations I use, it does not cancel out the angle.
In case it is not so readable I have attached the relevant sections from the lecture
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