Free · Open · Based on MIT OpenCourseWare
Learn how the universe began, expanded, and came to look the way it does.
Open Cosmology is a free, complete programme in physics — four undergraduate years from classical mechanics and electromagnetism through relativity, quantum and statistical physics to the early universe, with the calculus, differential equations and linear algebra they rest on, and a fifth, graduate year for dark matter, the growth of structure and general relativity — rewritten from MIT lectures as clear explanations, interactive graphs and worked examples. Cosmology is the destination: the expanding universe, the Big Bang, the cosmic microwave background, inflation, dark matter and dark energy.
The destination: cosmology
Year IV of the path. Each theme follows MIT 8.286 The Early Universe, with extra pages where a topic needs more room — the dark matter and structure formation pages come from the graduate course 8.902 in Year V.
The expanding universe
Hubble's law, the scale factor, comoving coordinates and cosmological redshift: what it means for space itself to expand.
- The Doppler effect and special relativity
- The homogeneous expanding universe
- Cosmological redshift
- Why a static universe cannot work
Dynamics of expansion
How gravity and the matter content decide the fate of the universe: the Friedmann equation, critical density and the age of the universe.
- The expanding sphere and the equation for a(t)
- The Friedmann equation
- Open, closed and flat universes
- The age of the universe and the Big Bang singularity
Geometry of space and spacetime
Closed, open and flat universes, the spacetime metric and the paths light and matter follow through curved space.
- The open universe and the age of any matter universe
- Non-Euclidean geometry
- The metric of a sphere and of a closed universe
- Curvature and expansion — the Robertson–Walker metric
The Big Bang and the cosmic microwave background
Black-body radiation, the thermal history of the early universe and the afterglow released when atoms first formed.
- Mass, energy and the dilution of radiation
- Matter–radiation equality and the pressure of light
- The radiation-dominated universe
- Black-body radiation
Dark energy
The cosmological constant, vacuum energy and the Type Ia supernova evidence that the expansion is accelerating.
- The age of the universe with vacuum energy
- How bright is a distant supernova?
- The supernova evidence for acceleration
- The puzzle of the vacuum energy, and Einstein's mistake about Friedmann
Inflation
The flatness, horizon and monopole problems of the conventional Big Bang, and the rapid early expansion that solves them.
- The Big Bang and its prequel — an overview of inflation
- Eternal inflation, dark energy and the landscape
- The anthropic argument and the multiverse — and where the course begins
- The horizon problem
Dark matter
Rotation curves, galaxy clusters, gravitational lensing and the CMB all point to matter we cannot see. Extra pages beyond MIT's lecture list; sources assigned per page.
- Why structure formation needs cold dark matter
- Where dark matter comes from — freeze-out, hot and cold
Structure formation
How tiny density ripples grew by gravity into galaxies and the cosmic web. Extra pages beyond MIT's lecture list; sources assigned per page.
- How small ripples grow — linear perturbation theory
- Why structure formation needs cold dark matter
- Measuring structure — the power spectrum and the correlation function
- When ripples collapse — the spherical collapse model
Galaxies
What galaxies look like, how stars move in them, and how they evolve chemically.
8.902 lectures 1, 2, 3, 4, 5, 6, 7, 8, 9 · pages coming
8.902 overview →Cosmology
The cosmological principle, the expanding universe and inflation, from the astrophysicist's side.
8.902 lectures 10, 11, 12 · pages coming
8.902 overview →Structure formation
How tiny density ripples grow by gravity, why cold dark matter is needed, and how structure is measured.
- How small ripples grow — linear perturbation theory
- Why structure formation needs cold dark matter
- Measuring structure — the power spectrum and the correlation function
- When ripples collapse — the spherical collapse model
The CMB and the early universe
CMB anisotropies, the thermal history of dark matter, nucleosynthesis and the Lyman-alpha forest.
8.902 overview →Cosmology in general relativity
The FLRW metric and the Friedmann equations derived from Einstein's field equation.
8.962 lectures 18, 19 · pages coming
8.962 overview →The programme, read backwards
Cosmology stands on the rest of physics. Read the path backwards to see what each step needs, or start at Year 1 and walk forward.
- Year VGraduate year: astrophysics and general relativity
- Year IVCosmology
- Year IIIStatistical and advanced quantum physics
The hot early universe is a gas in thermal equilibrium: blackbody radiation, the Boltzmann factor and entropy explain the CMB spectrum and the thermal history after the Big Bang. Quantum fields and their fluctuations are the seeds of all cosmic structure in inflationary cosmology; spin and identical particles decide how many particle species filled the early universe. Reaction rates and scattering cross sections decide when particles fell out of equilibrium in the early universe — the basis of Big Bang nucleosynthesis and of dark-matter relic abundances.
- Year IIWaves, relativity, the quantum, and the mathematics behind them8.03SC Physics III: Vibrations and Waves18.03 Differential Equations8.033 Relativity18.06 Linear Algebra8.04 Quantum Physics I
Redshift starts as a wave phenomenon (the Doppler effect), and the sound waves of the early plasma left the acoustic peaks we see in the CMB. The Friedmann equation is a differential equation for a(t); oscillators, waves and the growth of small density ripples into galaxies are all described by differential equations. Light travel time, the relativistic Doppler effect and E = mc² are used throughout cosmology, and the spacetime metric is the starting point for curved, expanding space. Quantum mechanics is written in linear algebra, a spacetime metric is a matrix, and rotations — like the one that proves a closed universe is the same everywhere — are orthogonal matrices. Photon energies and the hydrogen atom explain recombination — when the universe became transparent and the CMB was released — and the spectral lines used to measure redshift.
- Year IMechanics, electromagnetism and calculus8.01SC Classical Mechanics618.01 Single Variable Calculus8.02T Electricity and Magnetism18.02 Multivariable Calculus
Cosmology describes the whole universe with the tools of mechanics: vectors and rates of change (Hubble's law is a velocity proportional to a position vector), Newton's gravity (the Friedmann equation can be derived from a Newtonian expanding sphere), and energy conservation (which decides whether the universe expands forever). Every rate of change in cosmology is a derivative — the Hubble rate ȧ/a, the deceleration ä — and ages, horizon distances and volumes of the universe are integrals. Almost everything we know about the universe arrives as electromagnetic radiation. Maxwell's equations explain light, its spectrum and energy flux — the basis of the cosmic microwave background and of measuring distances with standard candles. Gauss's law, Poisson's equation and flux integrals — the tools behind Maxwell's equations and the Newtonian model of the expanding universe — are multivariable calculus.
How each page works
- Prerequisites first. Every page lists what you need before it, and where it leads in cosmology.
- Live graphs. Plots are computed from the formulas, with sliders to change the parameters.
- Every formula cited. Each equation links to the MIT lecture or notes it comes from.
- Practice. Step-by-step worked examples, a quiz and flashcards on every page.
- Listen. A read-aloud button speaks the page, maths included.