
The Vlasov equation describes the time evolution of the distribution function of charged particles in a plasma under the influence of electromagnetic fields.In 1938, Soviet physicist Anatoly Vlasov noticed that in a rarefied plasma, collisions are rare, and the main role is played by self-consistent electromagnetic fields. He wrote down an equation that became the foundation of plasma physics. It describes how a cloud of charged particles floats in its own electric field, like a flock of birds spiraling in an invisible vortex. The right-hand side of the equation is zero — no 'bird' collides with another, but each feels the overall attraction-repulsion. This approach made it possible to explain Langmuir waves in plasma and, decades later, the contraction of dark matter in galaxies. The flock scatters and closes again, obeying an invisible conductor.
Anatoly Alexandrovich Vlasov in 1938 published the work 'On the Vibrational Properties of an Electron Gas', where he proposed the collisionless equation. The idea met with resistance — Landau, Tamm, and others criticized the lack of accounting for collisions. Nevertheless, the equation became a standard in plasma physics, and later in astrophysics for modeling gravitating systems. In 1945, Vlasov generalized it to the case of solids.
Self-consistent solution: the distribution function determines the sources of fields, the fields determine the evolution of the distribution. Used in numerical PIC (particle-in-cell) codes for modeling laser plasma, solar wind, galaxy dynamics. Applicability limit: valid when the collision frequency is much less than the plasma frequency; at not too high densities. For collisional plasma, a collision operator is necessary.
Used to model plasma in fusion devices, galaxy dynamics, and the evolution of dark matter.
Vlasov sent his paper to Einstein, who, though not immediately, recognized its value. Today, the Vlasov equation is the basis of most computer simulations of cosmic plasma.
| concentration | variable | local concentration of the diffusing species — concentration mole per cubic metre |
| t | variable | time — time second |
| flux | variable | diffusive flux vector — diffusive flux mole per square metre per second |
| d/dt | operator | rate of change with respect to time — time derivative |
| divergence | operator | measures the net outflow of a vector field per unit volume — divergence operator |














