Questions about acceleration in SR

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DrGreg said:
So we can write

[tex] \Lambda_{\phi} = e^{Z\phi}[/tex]​

Indeed :smile:

Regards, Hans
 
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kev said:
That looks a LOT like the polar equation for a logarithimic spiral http://mathworld.wolfram.com/LogarithmicSpiral.html . Do you think there is any connection?
Note that Z is a matrix here...[tex]e^{Z\phi} ~=~ I~+~Z\phi ~+~ \frac{1}{2!}Z^2\phi^2~+~ \frac{1}{3!}Z^3\phi^3~+~ \frac{1}{4!}Z^4\phi^4~+~ \frac{1}{5!}Z^5\phi^5 ...[/tex]

But higher powers of Z simply become either Z or Z^2

[tex]Z~ = Z^3 = Z^5 = ... = \left(\begin{array}{cccc}<br /> 0 & 0 & 0 & 1 \\<br /> 0 & 0 & 0 & 0 \\<br /> 0 & 0 & 0 & 0 \\<br /> 1 & 0 & 0 & 0 \\<br /> \end{array}\right)[/tex]

[tex]Z^2 = Z^4 = Z^6 = ... = \left(\begin{array}{cccc}<br /> 1 & 0 & 0 & 0 \\<br /> 0 & 0 & 0 & 0 \\<br /> 0 & 0 & 0 & 0 \\<br /> 0 & 0 & 0 & 1 \\<br /> \end{array}\right)[/tex]

and therefor:

[tex]e^{Z\phi} ~=~ I ~+~ \sinh(\phi)\left(\begin{array}{cccc}<br /> 0 & 0 & 0 & 1 \\<br /> 0 & 0 & 0 & 0 \\<br /> 0 & 0 & 0 & 0 \\<br /> 1 & 0 & 0 & 0 \\<br /> \end{array}\right) ~+~ (\cosh(\phi)-1)\left(\begin{array}{cccc}<br /> 1 & 0 & 0 & 0 \\<br /> 0 & 0 & 0 & 0 \\<br /> 0 & 0 & 0 & 0 \\<br /> 0 & 0 & 0 & 1 \\<br /> \end{array}\right) ~=~ \left(\begin{array}{cccc}<br /> \cosh\phi & 0 & 0 & \sinh\phi \\<br /> 0 & 1 & 0 & 0 \\<br /> 0 & 0 & 1 & 0 \\<br /> \sinh\phi & 0 & 0 & \cosh\phi \\<br /> \end{array}\right)[/tex]
Regards, Hans