Problem sheet 1

Lecture: Introduction to general relativity, 2023-2024

Deadline: Nov 3rd, 2023 (3 weeks)

Topic: special relativity

Please send the solutions via email to korzynski@cft.edu.pl. I prefer PDF's (for example LaTeX-generated) or common graphic formats (for example scans of your hand-written notes).


Problem 1

Let vv be the velocity (standard 3-velocity) of an inertial frame PP with respect to another one, QQ. Define the rapidity θ\theta as a dimensionless scalar given by

θ(v)=artanhv,\theta(v) = \textrm{artanh}\, v,

or, equivalently, by the condition v=tanhθv = \tanh \theta.

  1. Prove that the Lorentz transformation matrix from PP to QQ in a two-dimentsional Minkowski space, with 2 spatial dimensions suppressed, takes the form of
Λ=(coshθsinhθsinhθcoshθ).\Lambda = \begin{pmatrix} \cosh \theta & -\sinh \theta \\ -\sinh\theta & \cosh\theta\end{pmatrix}.
  1. Prove that θ(v)=θ(v)\theta(-v) = -\theta(v).

  2. Additivity of rapidity. Prove that if the inertial frame BB moves with respect to AA with rapidity θAB\theta_{AB}, while CC moves with respect to BB with rapidity θBC,\theta_{BC}, then CC moves with respect to AA with θAC\theta_{AC} given by

θAC=θAB+θBC.\theta_{AC} = \theta_{AB} + \theta_{BC}.

Problem 2

Derivation of the time dilation formula.

Consider a clock CPC_P stationary in an inertial frame PP and another one, called CQC_Q, stationary in QQ, see Fig. 1.

QQ moves with respect to PP with velocity vv. Assume that both CPC_P and CQC_Q read 0 when the two clocks pass point O\cal O.

  1. Calculate the coordinate time x0x^0 in PP of the moment when CQC_Q reads a fixed time t>0t > 0. Show that x0>tx^0 > t, i.e. clock CQC_Q appears to run slower than CPC_P for an observer in PP.

  2. Calculate the coordinate time x~0\tilde x^0 in QQ of the moment when CPC_P reads the same time tt. Show that x~0>t\tilde x^0 > t, i.e. clock CPC_P appears to run slower than CQC_Q for an oberver in QQ.

  3. Explain why the two results above are not contradictory.