3.6: Some kinematic identities
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Learning Objectives
- List of various kinematics equations and identities
In addition to the relations
D(v) = \sqrt{\frac{1+v}{1-v}}
and
v_c = \frac{v_1 + v_2}{1 + v_1 v_2}
the following identities can be handy. If stranded on a desert island you should be able to rederive them from scratch. Don’t memorize them.
v = \frac{D^2 - 1}{D^2 + 1}
\gamma = \frac{D^{-1} + D}{2}
v\gamma = \frac{D - D^{-1}}{2}
D(v)D(-v) = 1
\eta = \ln D
v = \tanh \eta
\gamma = \cosh \eta
v\gamma = \sinh \eta
\tanh (x+y) = \frac{\tanh x + \tanh y}{1 + \tanh x \tanh y}
D_c = D_1 D_2
\eta _c = \eta _1 + \eta _2
v_C \gamma _c = (v_1 + v_2)\gamma _1 \gamma _2
The hyperbolic trig functions are defined as follows:
\sinh x = \frac{e^x - e^{-x}}{2}
\cosh x = \frac{e^x + e^{-x}}{2}
\tanh x = \frac{\sinh x}{\cosh x}
Their inverses are built in to some calculators and computer software, but they can also be calculated using the following relations:
\sinh^{-1}x = \ln \left ( x + \sqrt{x^2 + 1} \right )
\cosh^{-1}x = \ln \left ( x + \sqrt{x^2 - 1} \right )
\tanh^{-1}x = \frac{1}{2}\ln \left ( \frac{1 + x}{1 - x} \right )
Their derivatives are, respectively, \left ( x^2 + 1 \right )^{-1/2}, \left ( x^2 - 1 \right )^{-1/2} and \left ( 1 - x^2 \right )^{-1}.