Euler-Lagrange Equation

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## History

## Statement

## Examples

## Generalizations

### Single function of single variable with higher derivatives

### Several functions of single variable with single derivative

### Single function of several variables with single derivative

### Several functions of several variables with single derivative

### Single function of two variables with higher derivatives

### Several functions of several variables with higher derivatives

## Generalization to manifolds

## See also

## Notes

## References

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

Euler%E2%80%93Lagrange Equation

In the calculus of variations, the **Euler equation**^{[1]} is a second-order partial differential equation whose solutions are the functions for which a given functional is stationary. It was developed by Swiss mathematician Leonhard Euler and Italian mathematician Joseph-Louis Lagrange in the 1750s.

Because a differentiable functional is stationary at its local extrema, 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, according to Hamilton's principle of stationary action, the evolution of a physical system is described by the solutions to the Euler equation for the action of the system. In this context Euler equations are usually called **Lagrange equations**. 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.

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]}

The Euler-Lagrange equation is an equation satisfied by a function * q*
of a real argument

where:

- is the function to be found:

- such that is differentiable, , and .

- is the derivative of :

- denotes the tangent bundle to along the curve , (disjoint) union of all tangent spaces (see tangent space) to at the points of curve .

- is a real-valued function with continuous first partial derivatives:

- being the tangent bundle of defined by
- .

The Euler-Lagrange equation, then, is given by

Here and denote the partial derivatives of with respect to the second and third arguments, respectively.

If the dimension of the space is greater than 1, this is a system of differential equations, one for each component:

A standard example is finding the real-valued function *y*(*x*) on the interval [*a*, *b*], such that *y*(*a*) = *c* and *y*(*b*) = *d*, for which the path length along the curve traced by *y* is as short as possible.

the integrand function being .

The partial derivatives of *L* are:

By substituting these into the Euler-Lagrange equation, we obtain

that is, the function must have a constant first derivative, and thus its graph is a straight line.

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.

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]}

A multi-dimensional generalization comes from considering a function on n variables. If is some surface, then

is extremized only if *f* satisfies the partial differential equation

When *n* = 2 and functional is the energy functional, this leads to the soap-film minimal surface problem.

If there are several unknown functions to be determined and several variables such that

the system of Euler-Lagrange equations is^{[4]}

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 *n*-th order such that

then the Euler-Lagrange equation is^{[4]}

which can be represented shortly as:

wherein are indices that span the number of variables, that is, here they go from 1 to 2. Here summation over the indices is only over in order to avoid counting the same partial derivative multiple times, for example appears only once in the previous equation.

If there 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 *n*-th 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 the summation over the is avoiding counting the same derivative several times, just as in the previous subsection. This can be expressed more compactly as

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:

- Lagrangian mechanics
- Hamiltonian mechanics
- Analytical mechanics
- Beltrami identity
- Functional derivative

**^**Fox, Charles (1987).*An introduction to the calculus of variations*. Courier Dover Publications. ISBN 978-0-486-65499-7.**^**A short biography of Lagrange Archived 2007-07-14 at the Wayback Machine**^**Courant & Hilbert 1953, p. 184- ^
^{a}^{b}^{c}Courant, R; Hilbert, D (1953).*Methods of Mathematical Physics*. Vol. I (First English ed.). New York: Interscience Publishers, Inc. ISBN 978-0471504474.CS1 maint: ref=harv (link) **^**Weinstock, R. (1952).*Calculus of Variations with Applications to Physics and Engineering*. New York: McGraw-Hill.

- "Lagrange equations (in mechanics)",
*Encyclopedia of Mathematics*, EMS Press, 2001 [1994] - Weisstein, Eric W. "Euler-Lagrange Differential Equation".
*MathWorld*. - "Calculus of Variations".
*PlanetMath*. - Gelfand, Izrail Moiseevich (1963).
*Calculus of Variations*. Dover. ISBN 0-486-41448-5. - Roubicek, T.:
*Calculus of variations. Chap.17 in: Mathematical Tools for Physicists. (Ed. M. Grinfeld) J. Wiley, Weinheim, 2014, ISBN 978-3-527-41188-7, pp.551-588.*

This article uses material from the Wikipedia page available here. It is released under the Creative Commons Attribution-Share-Alike License 3.0.

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