Workbook Solutions: Moore General Relativity

$$\frac{d^2r}{d\lambda^2} = -\frac{GM}{r^2} + \frac{L^2}{r^3}$$

For the given metric, the non-zero Christoffel symbols are

$$\frac{d^2t}{d\lambda^2} = 0, \quad \frac{d^2x^i}{d\lambda^2} = 0$$ moore general relativity workbook solutions

$$ds^2 = -\left(1 - \frac{2GM}{r}\right) dt^2 + \left(1 - \frac{2GM}{r}\right)^{-1} dr^2 + r^2 d\Omega^2$$

Consider a particle moving in a curved spacetime with metric moore general relativity workbook solutions

Consider two clocks, one at rest at infinity and the other at rest at a distance $r$ from a massive object. Calculate the gravitational time dilation factor.

Derive the equation of motion for a radial geodesic. moore general relativity workbook solutions

where $\eta^{im}$ is the Minkowski metric.