principle

principle of least action

The principle of least action states that physical systems evolve along paths that minimize the action functional.
26 related articles · 4 formulas · 2 who worked here

Description

Even in antiquity, Heron of Alexandria noticed that light reflects at equal angles, as if seeking the shortest path. In 1744, Pierre Louis Maupertuis formulated a general principle: nature always acts in the most economical way. Leonhard Euler and Joseph-Louis Lagrange developed the mathematics: for mechanical systems there is a Lagrange function L (difference between kinetic and potential energy), and its integral over time — the action S — must be minimal on the real trajectory. William Hamilton reformulated mechanics in terms of action, and Emmy Noether showed that from the invariance (unchangingness) of the action under transformations follow conservation laws — of energy, momentum, charge. Today, the principle of least action is the foundation of all theoretical physics.

History

Ancient mechanics (Heron) used the idea of the shortest path for light. Pierre Louis Maupertuis in 1744 proposed the teleological 'law of economy'. Leonhard Euler reformulated it for mechanics, and Joseph-Louis Lagrange (1788) created analytical mechanics on the basis of variational calculus. William Rowan Hamilton (1834–35) introduced the concept of action as a fundamental notion. Emmy Noether in 1918 established the connection between symmetries of the action and conservation laws. Henri Poincaré developed the theory of variational principles in celestial mechanics and relativity theory.

How it works

The principle applies to any systems with finite or infinite number of degrees of freedom provided that the equations of motion can be derived from a variational principle. Limitations: dissipative systems (with friction) may not be variational without introducing additional variables. In quantum mechanics, the principle of least action is a limiting case ℏ → 0, but quantum corrections are described by a sum over all trajectories. Modern theories, including string theory, rely on the Lagrangian form.

In practice

Allows building optimal trajectories for spacecraft and designing energy-efficient mechanisms.

Fun fact

Using this principle, Maxwell's equations for electromagnetism and the Schrödinger equation in quantum mechanics are derived.

Concept graph →

Formulas

$$\\Psi(t+\\tau) \\approx e^{\\tau W} e^{\\tau T} \\Psi(t)$$
Approximate evolution by splitting into simpler operators.
What is in the formula
ΨvariableWave function — wave function
tvariableTime — time second
τvariableTime step — time step second
e^{τW}operatorApplies the evolution operator for the W part — exponential operator
e^{τT}operatorApplies the evolution operator for the T part — exponential operator
\phi(t_{n+1},*)\approxe^{τw}e^{τt}\phi(t_n,*) · 2607.00335
$$\dot{\theta} = F(\theta) - \theta$$
Evolution of a state driven by expected increment minus current value.
What is in the formula
θvariableState vector — state vector
F(θ)variableExpected increment function — increment function
˙operatorDerivative with respect to time — time derivative
\dot{\theta}=f(\theta)-\theta · 2607.01148
$$\tau_P = \frac{2G}{1-\nu} \exp\left(-\frac{2\pi W}{b(1-\nu)}\right)$$
Minimum stress to move a dislocation through a crystal lattice.
What is in the formula
τ_PvariablePeierls-Nabarro stress — peierls nabarro stress pascal
Gvariableshear modulus of the crystal — shear modulus pascal
νvariablePoisson's ratio — poissons ratio
Wvariabledislocation width — dislocation width metre
bvariablemagnitude of the Burgers vector — burgers vector magnitude metre
τ_p=\frac{2g}{1-ν}\exp(-\frac{2πw}{b(1-ν)}) · 2606.29061
$$\nabla^2 \phi = V'(\phi)$$
Field minimizes Euclidean action in scalar theory.
What is in the formula
φvariableScalar field configuration — scalar field
∇²operatorLaplacian (sum of second spatial derivatives) — laplacian operator
\frac{\partial^2φ_b}{\partialx^2}+\frac{1}{x}\frac{\partialφ_b}{\partialx}=v'(φ_b) · 2607.06680

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