Euler–Lagrange equation
In calculus of variations, the Euler–Lagrange equation, Euler's equation,^{[1]} or Lagrange's equation (although the latter name is ambiguous—see disambiguation page), is a secondorder partial differential equation whose solutions are the functions for which a given functional is stationary. It was developed by SwissRussian mathematician Leonhard Euler and FrenchItalian mathematician JosephLouis Lagrange in the 1750s.
Because a differentiable functional is stationary at its local maxima and minima, the Euler–Lagrange equation is useful for solving optimization problems in which, given some functional, one seeks the function minimizing (or maximizing) it. This is analogous to Fermat's theorem in calculus, stating that at any point where a differentiable function attains a local extremum, its derivative is zero.
In Lagrangian mechanics, because of Hamilton's principle of stationary action, the evolution of a physical system is described by the solutions to the Euler–Lagrange equation for the action of the system. In classical mechanics, it is equivalent to Newton's laws of motion, but it has the advantage that it takes the same form in any system of generalized coordinates, and it is better suited to generalizations. In classical field theory there is an analogous equation to calculate the dynamics of a field.
Contents
 1 History
 2 Statement
 3 Examples
 4 Variations for several functions, several variables, and higher derivatives
 4.1 Single function of single variable with higher derivatives
 4.2 Several functions of one variable
 4.3 Single function of several variables
 4.4 Several functions of several variables
 4.5 Single function of two variables with higher derivatives
 4.6 Several functions of several variables with higher derivatives
 5 Generalization to Manifolds
 6 See also
 7 Notes
 8 References
History
The Euler–Lagrange equation was developed in the 1750s by Euler and Lagrange in connection with their studies of the tautochrone problem. This is the problem of determining a curve on which a weighted particle will fall to a fixed point in a fixed amount of time, independent of the starting point.
Lagrange solved this problem in 1755 and sent the solution to Euler. Both further developed Lagrange's method and applied it to mechanics, which led to the formulation of Lagrangian mechanics. Their correspondence ultimately led to the calculus of variations, a term coined by Euler himself in 1766.^{[2]}
Statement
The Euler–Lagrange equation is an equation satisfied by a function, q, of a real argument, t, which is a stationary point of the functional
where:
 is the function to be found:
 such that is differentiable, , and ;
 ; is the derivative of :
 TX being the tangent bundle of X defined by
 ;
 L is a realvalued function with continuous first partial derivatives:
The Euler–Lagrange equation, then, is given by
where L_{x} and L_{v} denote the partial derivatives of L with respect to the second and third arguments, respectively.
If the dimension of the space X is greater than 1, this is a system of differential equations, one for each component:

Derivation of onedimensional Euler–Lagrange equation The derivation of the onedimensional Euler–Lagrange equation is one of the classic proofs in mathematics. It relies on the fundamental lemma of calculus of variations.
We wish to find a function which satisfies the boundary conditions , , and which extremizes the functional
We assume that is twice continuously differentiable.^{[3]} A weaker assumption can be used, but the proof becomes more difficult.^{[citation needed]}
If extremizes the functional subject to the boundary conditions, then any slight perturbation of that preserves the boundary values must either increase (if is a minimizer) or decrease (if is a maximizer).
Let be the result of such a perturbation of , where is small and is a differentiable function satisfying . Then define
where .
We now wish to calculate the total derivative of with respect to ε.
It follows from the total derivative that
So
When ε = 0 we have g_{ε} = f, F_{ε} = F(x, f(x), f'(x)) and J_{ε} has an extremum value, so that
The next step is to use integration by parts on the second term of the integrand, yielding
Using the boundary conditions ,
Applying the fundamental lemma of calculus of variations now yields the Euler–Lagrange equation

Alternate derivation of onedimensional Euler–Lagrange equation Given a functional
on with the boundary conditions and , we proceed by approximating the extremal curve by a polygonal line with segments and passing to the limit as the number of segments grows arbitrarily large.
Divide the interval into equal segments with endpoints and let . Rather than a smooth function we consider the polygonal line with vertices , where and . Accordingly, our functional becomes a real function of variables given by
Extremals of this new functional defined on the discrete points correspond to points where
Evaluating this partial derivative gives
Dividing the above equation by gives
and taking the limit as of the righthand side of this expression yields
The left hand side of the previous equation is the functional derivative of the functional . A necessary condition for a differentiable functional to have an extremum on some function is that its functional derivative at that function vanishes, which is granted by the last equation.
Examples
A standard example is finding the realvalued function on the interval [a, b], such that f(a) = c and f(b) = d, the length of whose graph is as short as possible. The length of the graph of f is:
the integrand function being L(x, y, y′) = √1 + y′ ² evaluated at (x, y, y′) = (x, f(x), f′(x)).
The partial derivatives of L are:
By substituting these into the Euler–Lagrange equation, we obtain
that is, the function must have constant first derivative, and thus its graph is a straight line.
Variations for several functions, several variables, and higher derivatives
Single function of single variable with higher derivatives
The stationary values of the functional
can be obtained from the Euler–Lagrange equation^{[4]}
under fixed boundary conditions for the function itself as well as for the first derivatives (i.e. for all ). The endpoint values of the highest derivative remain flexible.
Several functions of one variable
If the problem involves finding several functions () of a single independent variable () that define an extremum of the functional
then the corresponding Euler–Lagrange equations are^{[5]}
Single function of several variables
A multidimensional generalization comes from considering a function on n variables. If Ω is some surface, then
is extremized only if f satisfies the partial differential equation
When n = 2 and is the energy functional, this leads to the soapfilm minimal surface problem.
Several functions of several variables
If there are several unknown functions to be determined and several variables such that
the system of Euler–Lagrange equations is^{[4]}
Single function of two variables with higher derivatives
If there is a single unknown function f to be determined that is dependent on two variables x_{1} and x_{2} and if the functional depends on higher derivatives of f up to nth order such that
then the Euler–Lagrange equation is^{[4]}
which can be represented shortly as:
where are indices that span the number of variables, that is they go from 1 to 2. Here summation over the indices is implied according to Einstein notation.
Several functions of several variables with higher derivatives
If there is are p unknown functions f_{i} to be determined that are dependent on m variables x_{1} ... x_{m} and if the functional depends on higher derivatives of the f_{i} up to nth order such that
where are indices that span the number of variables, that is they go from 1 to m. Then the Euler–Lagrange equation is
where summation over the is implied according to Einstein notation. This can be expressed more compactly as
Generalization to Manifolds
Let be a smooth manifold, and let denote the space of smooth functions . Then, for functionals of the form
where is the Lagrangian, the statement is equivalent to the statement that, for all , each coordinate frame trivialization of a neighborhood of yields the following equations:
See also
Look up Euler–Lagrange equation in Wiktionary, the free dictionary. 
 Lagrangian mechanics
 Hamiltonian mechanics
 Analytical mechanics
 Beltrami identity
 Functional derivative
Notes
 ↑ Lua error in package.lua at line 80: module 'strict' not found.
 ↑ A short biography of Lagrange
 ↑ Courant & Hilbert 1953, p. 184
 ↑ ^{4.0} ^{4.1} ^{4.2} Lua error in package.lua at line 80: module 'strict' not found.
 ↑ Weinstock, R., 1952, Calculus of Variations With Applications to Physics and Engineering, McGrawHill Book Company, New York.
References
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 Weisstein, Eric W., "EulerLagrange Differential Equation", MathWorld.
 Calculus of Variations at PlanetMath.org.
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 Roubicek, T.: Calculus of variations. Chap.17 in: Mathematical Tools for Physicists. (Ed. M. Grinfeld) J. Wiley, Weinheim, 2014, ISBN 9783527411887, pp.551588.