Chapter 2: Problem 9
9\. How many successive velocity increments of \(\frac{1}{2} c\) from the instantaneous rest frame are needed to produce a resultant velocity of (i) \(0.99 c\), (ii) \(0.999 c\) ? [Answer. 5,7 .
Chapter 2: Problem 9
9\. How many successive velocity increments of \(\frac{1}{2} c\) from the instantaneous rest frame are needed to produce a resultant velocity of (i) \(0.99 c\), (ii) \(0.999 c\) ? [Answer. 5,7 .
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Get started for freeIn a given frame, a particle A moves hyperbolically with proper acceleration \(\alpha\) from rest at \(t=0\). At \(t=0\) a photon B is emitted in the same direction, a distance \(c^{2} / \alpha\) behind A. Prove that in A's instantaneous rest frames the distance \(A B\) is always \(c^{2} / \alpha\).
If \(\phi=\tanh ^{-1}(u / c)\), and \(\mathrm{e}^{2 \phi}=z\), prove that \(n\) consecutive velocity increments \(u\) from the instantaneous rest frame produce a velocity \(c\left(z^{n}-1\right) /\left(z^{n}+1\right)\)
The rapidity \(\phi\), of a particle moving with velocity \(u\), is defined by \(\phi=\tanh ^{-1}(u / c)\) [cf. Exercise I (12)]. Prove that collinear rapidities are additive, i.e. if A has rapidity \(\phi\) relative to B, and B has rapidly \(\psi\) relative to \(\mathrm{C}\), then \(\mathrm{A}\) has rapidity \(\phi+\psi\) relative to \(\mathrm{C}\).
Given that \(g\), the acceleration of gravity at the earth's surface, is \(\sim 9.8 \mathrm{~m} \mathrm{~s}^{-2}\), and that a year has \(\sim 3.2 \times 10^{7}\) seconds, verify that, in units of years and light years, \(g \approx 1\). A rocket moves from rest in an inertial frame \(S\) with constant proper acceleration \(g\) (thus giving maximum comfort to its passengers). Find its Lorentz factor relative to \(\mathrm{S}\) when its own clock indicates times \(\tau=1\) day, 1 year, 10 years. Find also the corresponding distances and times travelled in S. If the rocket accelerates for 10 years of its own time, then decelerates for 10 years, and then repeats the whole manoeuvre in the reverse direction, what is the total time elapsed in \(\mathrm{S}\) during the rocket's absence?
A certain piece of elastic breaks when it is stretched to twice its unstretched length. At time \(t=0\), all points of it are accelerated longitudinally with constant proper acceleration \(\alpha\), from rest in the unstretched state. Prove that the elastic breaks at \(t=\sqrt{3} c / \alpha\).
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