Classical mechanics

STR

This paper

$K_{c l} = \frac{1}{2} m v^{2}$

$K_{c l} = \frac{p^{2}}{2 m}$

$K_{r e} = m c^{2} - m_{0} c^{2}$

$K_{r e} = \frac{p_{r e}^{2}}{m + m_{0}}$

$K_{r e, n} = m_{e} c^{2} - m_{n} c^{2}$

$K_{r e, n} = \frac{p_{re, n}^{2}}{m_{e} + m_{n}}$

$K_{r e, n} = m_{e} c^{2} [1 - {(\frac{n^{2}}{n^{2} + α^{2}})}^{1 / 2}]$

$K_{re, n} = v_{p, n} p_{re, n}$

$K_{re, n} = m_{n} v_{g, n} v_{p, n}$

$K_{re, n} = c p_{re, n} {(\frac{m_{e} - m_{n}}{m_{e} + m_{n}})}^{1 / 2}$

$K_{re, n} = c p_{re, n} {[\frac{{(n^{2} + α^{2})}^{1 / 2} - n}{{(n^{2} + α^{2})}^{1 / 2} + n}]}^{1 / 2}$

$K_{re, n} = c p_{re, n} {(\frac{r_{re, n}^{-}}{r_{re, n}^{+}})}^{1 / 2}$