
A Lagrangian is a mathematical function used to describe the dynamics of a system, often applied in optimization and motion analysis.The Lagrangian is a function depending on the coordinates and velocities of all parts of a system. Instead of considering forces, as in Newtonian mechanics, one operates with energies: kinetic (energy of motion) and potential (energy of position). From the principle of least action it follows that the actual motion of a system occurs such that the total difference of these energies along the trajectory is minimal. This approach is particularly convenient for systems with constraints, e.g., a pendulum on an inextensible string, and allows one to derive the equations of motion (Euler-Lagrange equations).
First presented by Joseph-Louis Lagrange in 'Analytical Mechanics' (1788) with the goal of constructing mechanics without geometric constructions. In the 19th century, William Rowan Hamilton reformulated it into Hamiltonian formalism. Henri Poincaré developed the theory of dynamical systems. Emmy Noether in 1918 proved the theorem linking continuous symmetries of the Lagrangian to conserved quantities. In quantum field theory, the Lagrangian became the basis of the Standard Model.
For a system with generalized coordinates q_i, the Lagrangian is written as L(q, q̇, t) = T − V. The Euler-Lagrange equations are obtained by requiring the variation of the action to be zero. For example, for a particle in a potential field, L = ½ m ẋ² − V(x). Noether's theorem states: to each continuous symmetry of the Lagrangian there corresponds a conserved integral of motion (energy, momentum, etc.).
Used for calculating the orbits of planets, trajectories of rockets, optimizing mechanical devices, and in the foundations of quantum theory.
Lagrange's method made it possible to solve problems that were too complex for the direct application of Newton's laws, such as the motion of many-body systems with constraints.
| x | variable | Position of the particle — position metre |
| γ | variable | Damping coefficient — damping coefficient per second |
| ω | variable | Natural angular frequency of the oscillator — angular frequency radian per second |
| η(t) | variable | Random force (noise) as a function of time — random force newton per kilogram |
| d²/dt² | operator | Second derivative with respect to time — second time derivative |
| d/dt | operator | First derivative with respect to time — first time derivative |
| r | variable | distance between two points — distance metre |
| ν | variable | smoothness parameter |
| l | variable | length scale parameter — length metre |
| σ | variable | variance amplitude — variance square metre |
| Γ | operator | Gamma function, generalizes factorial — gamma function |
| K_ν | operator | Modified Bessel function of the second kind of order ν — modified bessel function second kind |
| S_E | variable | Euclidean action — action joule second |
| L_E | variable | Euclidean Lagrangian — lagrangian joule |
| τ | variable | Euclidean time — time second |
| ∫ | operator | Integration over Euclidean time — integral operator |
| dτ | operator | Infinitesimal time element — differential element |











