1.II.35C

General Relativity
Part II, 2005

Suppose (x(τ),t(τ))(x(\tau), t(\tau)) is a timelike geodesic of the metric

ds2=dx21+x2(1+x2)dt2d s^{2}=\frac{d x^{2}}{1+x^{2}}-\left(1+x^{2}\right) d t^{2}

where τ\tau is proper time along the world line. Show that dt/dτ=E/(1+x2)d t / d \tau=E /\left(1+x^{2}\right), where E>1E>1 is a constant whose physical significance should be stated. Setting a2=E21a^{2}=E^{2}-1, show that

dτ=dxa2x2,dt=Edx(1+x2)a2x2.d \tau=\frac{d x}{\sqrt{a^{2}-x^{2}}}, \quad d t=\frac{E d x}{\left(1+x^{2}\right) \sqrt{a^{2}-x^{2}}} .

Deduce that xx is a periodic function of proper time τ\tau with period 2π2 \pi. Sketch dx/dτd x / d \tau as a function of xx and superpose on this a sketch of dx/dtd x / d t as a function of xx. Given the identity

aaEdx(1+x2)a2x2=π\int_{-a}^{a} \frac{E d x}{\left(1+x^{2}\right) \sqrt{a^{2}-x^{2}}}=\pi

deduce that xx is also a periodic function of tt with period 2π2 \pi.

Next consider the family of metrics

ds2=[1+f(x)]2dx21+x2(1+x2)dt2,d s^{2}=\frac{[1+f(x)]^{2} d x^{2}}{1+x^{2}}-\left(1+x^{2}\right) d t^{2},

where ff is an odd function of x,f(x)=f(x)x, f(-x)=-f(x), and f(x)<1|f(x)|<1 for all xx. Derive expressions analogous to ()(*) above. Deduce that xx is a periodic function of τ\tau and also that xx is a periodic function of tt. What are the periods?