I would like to share some insight on how different trajectories can form in a *central field*. I'll use laws of Newtonian gravitation and I would limit myself to examples in gravitation.

In a two body system, we normally assume the heavier to be fixed. I will *not*. Also, I will proceed by taking the motion of the reduced mass of the system.

Going down to basic equations, coordinate of C.M. becomes \[\vec R = \dfrac{m_1\vec r_1 + m_2\vec r_2}{M}\] where \(M = m_1 + m_2\). Now, using \(\vec r = \vec r_1 - \vec r_2\), \[\vec r_1 = \vec R + \dfrac{m_2}M \vec r\\\vec r_2 = \vec R - \dfrac{m_1}M \vec r\]

Note that the momentum \(\vec P = M\dot {\vec R} = 0\) implies that the centre of mass is stationary (\(\vec R = 0\))

Looking at Kinetic Energy, \[\begin{align*}T &= \dfrac12\left(m_1\dot r_1^2+m_2\dot r_2^2\right)\\ &=\dfrac12\left[m_1\left(\dot R + \dfrac{m_2}M \dot r\right)^2+m_1\left(\dot R - \dfrac{m_1}M \dot r\right)^2\right]\\ &=\dfrac12 M\dot R^2+\dfrac12 \mu\dot r^2 \end{align*}\] where \(\mu = \dfrac{m_1m_2}M\), the reduced mass of the system. It's time for us to shift to the centre of mass frame of reference.

From now on, all standard variables will be referred on the C.M. frame.

In C.M. frame, for example, our kinetic energy becomes, \(T = \dfrac12 \mu\dot r^2\).

Let our central force and it's potential be \[\vec F = -f(r)\ \hat r\\U = U(r)\]

The angular momentum of the system (w.r.t. CM) will become, \[\vec L = \left(m_1r_1^2+m_2r_2^2\right)\omega = \mu r^2 \dot \theta\]

Using \(\dot{\vec r} = \dot r \ \hat r + r\dot\theta\ \hat\theta\), \[T = \dfrac12 \mu\left(\dot r^2 + r^2\dot\theta^2\right)\]

Thus, the total energy, \[\begin{align*} E &= T+U\\ &= \dfrac12 \mu\left(\dot r^2 + r^2\dot\theta^2\right) + U(r)\\ &= \dfrac12 \mu\dot r^2 + \dfrac{L^2}{2\mu r^2} + U(r)\\ E&= \dfrac12 \mu\dot r^2 + U_{\text{eff}}\end{align*}\] where \(U_{\text{eff}} = \dfrac{L^2}{2\mu r^2} + U(r)\)

*Note: I've written rotational kinetic energy in terms of \(L\) is because \(\theta\) term is messy and \(L\) is constant.*

*This will be updated*

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