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Physics LibreTexts

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}.


This page titled 3.6: Some kinematic identities is shared under a CC BY-SA 4.0 license and was authored, remixed, and/or curated by Benjamin Crowell via source content that was edited to the style and standards of the LibreTexts platform.

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