Lagrange multipliers on Banach spaces

In the field of calculus of variations in mathematics, the method of Lagrange multipliers on Banach spaces can be used to solve certain infinite-dimensional constrained optimization problems. The method is a generalization of the classical method of Lagrange multipliers as used to find extrema of a function of finitely many variables.

The Lagrange multiplier theorem for Banach spaces

Let X and Y be real Banach spaces. Let U be an open subset of X and let f : UR be a continuously differentiable function. Let g : UY be another continuously differentiable function, the constraint: the objective is to find the extremal points (maxima or minima) of f subject to the constraint that g is zero.

Suppose that u0 is a constrained extremum of f, i.e. an extremum of f on

g^{-1} (0) = \{ x \in U \mid g(x) = 0 \in Y \} \subseteq U.

Suppose also that the Fréchet derivative Dg(u0) : XY of g at u0 is a surjective linear map. Then there exists a Lagrange multiplier λ : YR in Y, the dual space to Y, such that

\mathrm{D} f (u_{0}) = \lambda \circ \mathrm{D} g (u_{0}). \quad \mbox{(L)}

Since Df(u0) is an element of the dual space X, equation (L) can also be written as

\mathrm{D} f (u_{0}) = \left( \mathrm{D} g (u_{0}) \right)^{*} (\lambda),

where (Dg(u0))(λ) is the pullback of λ by Dg(u0), i.e. the action of the adjoint map (Dg(u0)) on λ, as defined by

\left( \mathrm{D} g (u_{0}) \right)^{*} (\lambda) = \lambda \circ \mathrm{D} g (u_{0}).

Connection to the finite-dimensional case

In the case that X and Y are both finite-dimensional (i.e. linearly isomorphic to Rm and Rn for some natural numbers m and n) then writing out equation (L) in matrix form shows that λ is the usual Lagrange multiplier vector; in the case n = 1, λ is the usual Lagrange multiplier, a real number.

Application

In many optimization problems, one seeks to minimize a functional defined on an infinite-dimensional space such as a Banach space.

Consider, for example, the Sobolev space X = H01([1, +1]; R) and the functional f : XR given by

f(u) = \int_{-1}^{+1} u'(x)^{2} \, \mathrm{d} x.

Without any constraint, the minimum value of f would be 0, attained by u0(x) = 0 for all x between 1 and +1. One could also consider the constrained optimization problem, to minimize f among all those uX such that the mean value of u is +1. In terms of the above theorem, the constraint g would be given by

g(u) = \frac{1}{2} \int_{-1}^{+1} u(x) \, \mathrm{d} x - 1.

However this problem can be solved as in the finite dimensional case since the Lagrange multiplier  \lambda is only a scalar.

See also

References

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