Dirichlet energy

{{Short description|Mathematical measure of a function's variability}}

In mathematics, the Dirichlet energy is a measure of how variable a function is. More abstractly, it is a quadratic functional on the Sobolev space {{math|H1}}. The Dirichlet energy is intimately connected to Laplace's equation and is named after the German mathematician Peter Gustav Lejeune Dirichlet.

Definition

Given an open set {{math|Ω ⊆ Rn}} and a differentiable function {{math|u : Ω → R}}, the Dirichlet energy of the function {{math|u}} is the real number

:E[u] = \frac 1 2 \int_\Omega \| \nabla u(x) \|^2 \, dx,

where {{math|∇u : Ω → Rn}} denotes the gradient vector field of the function {{math|u}}.

Properties and applications

Since it is the integral of a non-negative quantity, the Dirichlet energy is itself non-negative, i.e. {{math|E[u] ≥ 0}} for every function {{math|u}}.

Solving Laplace's equation -\Delta u(x) = 0 for all x \in \Omega, subject to appropriate boundary conditions, is equivalent to solving the variational problem of finding a function {{math|u}} that satisfies the boundary conditions and has minimal Dirichlet energy.

Such a solution is called a harmonic function and such solutions are the topic of study in potential theory.

In a more general setting, where {{math|Ω ⊆ Rn}} is replaced by any Riemannian manifold {{math|M}}, and {{math|u : Ω → R}} is replaced by {{math|u : M → Φ}} for another (different) Riemannian manifold {{math|Φ}}, the Dirichlet energy is given by the sigma model. The solutions to the Lagrange equations for the sigma model Lagrangian are those functions {{math|u}} that minimize/maximize the Dirichlet energy. Restricting this general case back to the specific case of {{math|u : Ω → R}} just shows that the Lagrange equations (or, equivalently, the Hamilton–Jacobi equations) provide the basic tools for obtaining extremal solutions.

See also

  • {{annotated link|Dirichlet's principle}}
  • {{annotated link|Dirichlet eigenvalue}}
  • {{annotated link|Total variation}}
  • {{annotated link|Bounded mean oscillation}}
  • {{annotated link|Harmonic map}}
  • {{annotated link|Capacity of a set}}

References

  • {{cite book | author=Lawrence C. Evans | title=Partial Differential Equations | publisher=American Mathematical Society | year=1998 | isbn=978-0821807729 }}

Category:Calculus of variations

Category:Partial differential equations