General Relativity

Einstein's Masterpiece: Gravity is the curvature of spacetime. Mass-energy tells spacetime how to curve, and spacetime tells mass-energy how to move.

General Relativity

A comprehensive graduate-level course on Einstein's theory of gravity—from tensor calculus and differential geometry through the Einstein field equations to black holes, cosmology, and gravitational waves.

Course Overview

General Relativity, formulated by Albert Einstein in 1915, is the modern theory of gravitation. It describes gravity not as a force, but as a manifestation of the curvature of spacetime caused by mass and energy. This course provides a rigorous mathematical treatment of GR, starting from differential geometry and culminating in applications to black holes, cosmology, and gravitational wave astronomy.

What You'll Learn

  • • Tensor analysis and differential geometry
  • • Riemann curvature tensor and Einstein equations
  • • Schwarzschild and Kerr solutions
  • • Black hole physics and thermodynamics
  • • Cosmological models (FLRW universe)
  • • Gravitational waves and LIGO detections
  • • Singularity theorems and quantum gravity
  • • Numerical relativity and modern applications

Prerequisites

Course Structure

5 Parts covering 29 chapters • From differential geometry to quantum gravity • Includes detailed derivations, worked examples, and observational evidence • Suitable for advanced undergraduates and graduate students

Course Parts

Key Equations

Einstein Field Equations

$G_{\mu\nu} + \Lambda g_{\mu\nu} = \frac{8\pi G}{c^4} T_{\mu\nu}$

The fundamental equations of General Relativity: spacetime curvature (left side) is determined by matter-energy content (right side).

Schwarzschild Metric

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

Describes spacetime outside a spherically symmetric mass. Event horizon at r_s = 2GM/c².

Geodesic Equation

$\frac{d^2x^\mu}{d\tau^2} + \Gamma^\mu_{\alpha\beta}\frac{dx^\alpha}{d\tau}\frac{dx^\beta}{d\tau} = 0$

Free particles follow geodesics—the straightest possible paths in curved spacetime.

Related Courses

"Matter tells spacetime how to curve, and spacetime tells matter how to move."— John Archibald Wheeler

Learning Path & Prerequisites

Prerequisite
Foundation
Core
Advanced
Application

Hover over nodes to see connections. Click to lock selection. Colored nodes link to course content.