Postgraduate Science

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Special Relativity

Lorentz transformations, time dilation, and the geometry of spacetime.

Einstein's two postulates — the laws of physics are the same in all inertial frames, and the speed of light $c$ is invariant — force the coordinate change between frames to be the Lorentz transformation:

$$t' = \gamma(t - vx/c^2), \quad x' = \gamma(x - vt), \qquad \gamma = \frac{1}{\sqrt{1 - v^2/c^2}}.$$

Consequences include time dilation $\Delta t = \gamma \Delta\tau$, length contraction $L = L_0/\gamma$, and a unified spacetime interval

$$ds^2 = -c^2 dt^2 + dx^2 + dy^2 + dz^2$$

that is invariant under boosts. Energy and momentum unify into the four-momentum $p^\mu = (E/c, \mathbf p)$ with $E^2 = (pc)^2 + (mc^2)^2$.

Interactive: time dilation via light clock

A photon bouncing between two mirrors traces a longer path in the moving frame — so the moving clock ticks slower by factor $\gamma$.

Quiz

1. The Lorentz factor $\gamma$ equals:
2. The relativistic energy-momentum relation is:
3. The spacetime interval $ds^2 = -c^2 dt^2 + d\mathbf x^2$ is:
4. A rod of proper length $L_0$ moving with speed $v$ along its length has measured length:
5. Two events have an invariant spacetime separation $\Delta s^2 > 0$. Their order: