Euler-Lagrange Equation for Functional S

  • Thread starter Thread starter neworder1
  • Start date Start date
  • Tags Tags
    Euler-lagrange
Click For Summary
SUMMARY

The discussion focuses on deriving the Euler-Lagrange equation for a functional S defined on a rectangle P, with boundary conditions specified by a continuous and Lipschitz function f_{0}. The functional S is expressed as a double integral involving the squared partial derivatives of f with respect to x and y. The correct form of the Euler-Lagrange equation is established as ∂L/∂f - ∂/∂x(∂L/∂f_x) - ∂/∂y(∂L/∂f_y) = 0, where L is defined as (f_x)^2 + (f_y)^2, simplifying the problem of finding critical points of the functional S.

PREREQUISITES
  • Understanding of functional analysis and calculus of variations
  • Familiarity with the Euler-Lagrange equation
  • Knowledge of partial derivatives and their applications
  • Basic concepts of Lipschitz continuity
NEXT STEPS
  • Study the derivation of the Euler-Lagrange equation in multiple dimensions
  • Explore applications of the Euler-Lagrange equation in physics and engineering
  • Learn about variational methods in optimization problems
  • Investigate the implications of Lipschitz continuity in functional analysis
USEFUL FOR

Mathematicians, physicists, and engineers interested in calculus of variations, optimization problems, and the application of the Euler-Lagrange equation in various fields.

neworder1
Messages
64
Reaction score
0

Homework Statement



Let P be a rectangle , f_{0} : \partial P \rightarrow R) continuous and Lipschitz, C_{0} = \{ f \in C^{2}(P) : f=f_{0} \ on \ \partial P \}. and finally S : C_{0} \rightarrow R a functional:

S(f) = \int^b_a (\int^d_c (\frac{\partial f}{\partial x})^{2}\,dy)\,dx + \int^d_c (\int^a_b (\frac{\partial f}{\partial y})^{2}\,dx)\,dy.

Write Euler-Lagrange equation for S.

Homework Equations





The Attempt at a Solution



I tried writing: S(f) = \int^b_a (\int^d_c (\frac{\partial f}{\partial x})^{2} + (\frac{\partial f}{\partial y})^{2}\,dy)\,dx, so the proper Lagrangian would be L(x) = \int^d_c (\frac{\partial f}{\partial x})^{2} + (\frac{\partial f}{\partial y})^{2}\,dy.

Then the Euler-Lagrange equation should be \frac{d}{dx}\frac{\partial L}{\partial f^{'}_{x}} = 0 \leftrightarrow \frac{d}{dx}\frac{\partial }{\partial f^{'}_{x}}\int^d_c (\frac{\partial f}{\partial x})^{2}\,dy = 0, (L^{'} = \int^d_c (\frac{\partial f}{\partial x})^{2}\,dy) and now since \frac{dL^{'}}{dx} = \frac{\partial L^{'}}{\partial f_{x}^{'}}\frac{\partial f_{x}^{'}}{\partial x}, we can rewrite that as \frac{d}{dx}\frac{\frac{d}{dx}\int^d_c (\frac{\partial f}{\partial x})^{2}\,dy}{f_{xx}^{''}} = 0 \leftrightarrow \frac{d}{dx}\frac{\int^d_c \frac{\partial}{\partial x}(\frac{\partial f}{\partial x})^{2}\,dy}{f_{xx}^{''}} = 0 \leftrightarrow \frac{d}{dx}\frac{\int^d_c 2f_{x}^{'}f_{xx}^{''}\,dy}{f_{xx}^{''}} = 0. but what then?
 
Last edited:
Physics news on Phys.org
You are making this too hard. Let's call \frac{\partial f}{\partial x}=f_x and \frac{\partial f}{\partial y}=f_x. Then the form of the Euler-Lagrange equations for two independent variables is \frac{\partial L}{\partial f}-\frac{\partial}{\partial x} \frac{\partial L}{\partial f_x}-\frac{\partial}{\partial y}\frac{\partial L}{\partial f_y}=0 where L=(f_x)^2+(f_y)^2.
 

Similar threads

  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 18 ·
Replies
18
Views
3K
Replies
5
Views
2K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
2
Views
1K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 4 ·
Replies
4
Views
1K