Questions about acceleration in SR

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The discussion focuses on calculating the world line of a rocket undergoing constant proper acceleration in an inertial frame, starting from rest. The equation for the world line is derived, showing that it forms hyperbolas with lightlike asymptotes in a Minkowski space. Key properties of these hyperbolas include their orthogonality to lines through their center and their parametrization by hyperbolic trigonometric functions. The conversation also touches on the concept of rapidity, which is additive across different inertial frames, and the relationship between proper acceleration and coordinate acceleration. Overall, the thread provides insights into the geometric interpretation of acceleration in special relativity.
  • #31
DrGreg said:
So we can write

<br /> \Lambda_{\phi} = e^{Z\phi}<br />​

Indeed :smile:

Regards, Hans
 
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  • #32
  • #33
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...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 ...

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

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

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

and therefor:

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

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