advanced30 min studyLesson 344 in Mathematics

Constrained variations and multipliers

Restrict perturbations to a constraint tangent space and derive a valid multiplier equation under a constraint qualification.

On this page

What you’ll understand

  • Identify tangent directions to an integral constraint.
  • State the surjectivity hypothesis needed for a normal multiplier.
  • Solve an area-constrained quadratic variational problem and certify its minimum.

An energy-minimizing shape may also need to enclose a prescribed area, preserve mass, or satisfy a normalization. The constraint changes which perturbations are allowed. A Lagrange multiplier converts the first-order constrained condition into an unconstrained stationarity equation for an augmented functional, but the conversion has a hypothesis: the constraint must vary independently near the candidate. Without that regularity, a formal multiplier can fail to exist. Even when the equation is valid, it supplies candidates rather than a proof that a constrained minimizer exists or is globally best.

The tangent condition is a linearized constraint

Work in a Banach space of functions, for example a fixed-trace affine subset of H1(a,b)H^1(a,b) with homogeneous perturbation space H01H_0^1. Let the objective and a scalar equality constraint be continuously Fréchet differentiable nearby. If a differentiable feasible curve through the candidate has tangent hh, differentiating the equality gives DG[u](h)=0DG[u](h)=0. Thus feasible tangents lie in the kernel of the constraint derivative. A tangent condition alone does not make the straight line u+εhu+\varepsilon h exactly feasible for a nonlinear constraint.

For an area constraint G[u]=∫uG[u]=\int u, the constraint is affine, so zero-integral directions preserve it exactly along straight lines. For a normalization G[u]=∫u2G[u]=\int u^2, the tangent condition is ∫uh=0\int uh=0, but the second-order term ε2∫h2\varepsilon^2\int h^2 changes the norm along the uncorrected line. One can instead normalize a nearby perturbed function to construct a feasible curve. Keeping exact feasibility separate from its linearization prevents incorrect second-variation calculations on constrained problems.

G[u]=m,DG[u](h)=0;G[u]=∫abu2dx⇒DG[u](h)=2∫abuh dxG[u]=m,\qquad DG[u](h)=0;\qquad G[u]=\int_a^bu^2dx\Rightarrow DG[u](h)=2\int_a^buh\,dx
The derivative describes tangent feasibility. A nonlinear equality generally requires higher-order correction to construct an exactly feasible perturbation.↔ Scroll wide equations horizontally.

A normal multiplier needs a regular constraint

For finitely many equality constraints in a Banach space, a standard multiplier theorem applies when the objective and constraints are continuously Fréchet differentiable and the derivative of the constraint map onto the finite-dimensional constraint space is surjective. At a constrained local minimum, the objective derivative is then a linear combination of the constraint derivatives. For one scalar constraint this qualification means its derivative is not the zero functional. The theorem follows from the local level-set structure supplied by the implicit-function theorem.

Choose the sign convention J−λ(G−m)J-\lambda(G-m) for the augmented functional. If both quantities are integrals, apply the Euler–Lagrange calculation to the augmented density F−λgF-\lambda g. The multiplier is one constant for one global scalar equality, because the equality is a single number. A pointwise constraint instead involves a field of restrictions and can require a function-valued multiplier in an appropriate dual space. These are different problems; replacing an integral constraint by a pointwise equation radically changes the admissible set.

DJ[u]=λDG[u],(Fu−λgu)−ddx(Fv−λgv)=0when G[u]=∫abg(x,u,u′)dxDJ[u]=\lambda DG[u],\qquad (F_u-\lambda g_u)-\frac{d}{dx}(F_v-\lambda g_v)=0\quad\text{when }G[u]=\int_a^bg(x,u,u')dx
The scalar multiplier is justified by the stated differentiability and surjectivity conditions. Boundary terms must still be treated using the actual endpoint constraints.↔ Scroll wide equations horizontally.

The multiplier is not the entire optimality proof

Constraint qualifications cannot be omitted. In the finite-dimensional example minimizing a linear function subject to a squared variable equal to zero, the feasible set contains only zero, yet the constraint derivative there is zero while the objective derivative is not. No normal multiplier represents the objective derivative. Similar degeneracies can occur in function spaces. A failed qualification does not mean there is no constrained minimizer; it means this particular normal-multiplier conclusion is unavailable without another argument.

For convex quadratic energies with an affine integral constraint, a complete comparison is often simple. Once the candidate satisfies the multiplier equation, its first-order cross term against any feasible difference is the multiplier times the zero constraint difference. What remains is a positive quadratic energy. This proves uniqueness and global minimality in the specified class. For nonconvex functionals or nonlinear constraints, second-order tangent corrections and competing branches matter, so solving an augmented differential equation alone is not enough.

The least derivative energy for unit area

Minimize J[u]=12∫01(u′)2dxJ[u]=\tfrac12\int_0^1(u')^2dx over H01(0,1)H_0^1(0,1) subject to ∫01u dx=1\int_0^1u\,dx=1. Use the augmented functional J−λ(G−1)J-\lambda(G-1).

  1. The constraint derivative h↦∫hh\mapsto\int h is nonzero on H01H_0^1, so the scalar constraint qualification holds. The augmented Euler–Lagrange equation is −u′′=λ-u''=\lambda.

  2. Zero endpoints give u=(λ/2)x(1−x)u=(\lambda/2)x(1-x). Its integral is λ/12\lambda/12, so λ=12\lambda=12 and u∗=6x(1−x)u_*=6x(1-x). The energy is 12⋅36⋅(1/3)=6\tfrac12\cdot36\cdot(1/3)=6.

  3. For any feasible difference hh, both endpoint traces and its integral vanish. Hence ∫u∗′h′=12∫h=0\int u_*'h'=12\int h=0, and the energy difference is 12∫(h′)2\tfrac12\int(h')^2, positive for every nonzero feasible difference.

The result

The constrained minimizer is uniquely 6x(1 − x), with energy six and multiplier twelve in the declared sign convention.

Explore the model

Interactive lab

Interactive lab · function

Quadratic scaling inside an admissible family

Consider the trial shapes uc=6c x(1−x)u_c=6c\,x(1-x), whose area is cc and energy is 6c26c^2. Reset and set both instrument coefficient a=1a=1 and position x=0.5x=0.5; its height 0.250.25 predicts normalized energy J/6=0.25J/6=0.25 for area c=0.5c=0.5. Reset and set both a=1,x=1a=1,x=1; predict normalized energy one. The instrument parameter x represents area c in this scalar comparison, not spatial position in the string; it does not enforce the full constraint space.

Quadratic scaling inside an admissible familyThis lab uses only y = ax². Playback traces the curve within the fixed integration interval from 0 to x; it does not estimate numerical error or change the chosen point. Current readings: y at chosen x: 0.608; Tangent slope · 2ax: 1.35; Signed area · ax³/3: 0.182. All parameters are adjustable with the labeled controls below.−2.4−1.201.22.4−9−4.504.59xy(x, ax²)
y = ax²TangentSigned integral
y at chosen x
0.608
Tangent slope · 2ax
1.35
Signed area · ax³/3
0.182
t = 0 s

This lab uses only y = ax². Playback traces the curve within the fixed integration interval from 0 to x; it does not estimate numerical error or change the chosen point. Parameter changes pause playback and recompute the model at the current elapsed time. Reset restores both parameters and returns time to zero. Playback starts paused. Adjust either parameter, then choose Play or Step.

Look forAn integral constraint selects a shape amplitude, and quadratic energy scales with its square.

Check your understanding

Why is the multiplier for one global integral equality a constant rather than an arbitrary function of position?

Try it yourself

Repeat the area-constrained derivative-energy problem with prescribed area m=1/2m=1/2. Find the shape, multiplier, and minimum energy.

Take a moment to make a prediction or work it out on paper. Open a hint when you need one.

Give me a hint

Use the general solution (λ/2)x(1 − x), and impose the new integral before computing the energy.

Compare with the solution

The area is λ/12\lambda/12, so λ=6\lambda=6 and u∗=3x(1−x)u_*=3x(1-x). Its energy is 12⋅9⋅(1/3)=3/2\tfrac12\cdot9\cdot(1/3)=3/2. More generally the minimum is 6m26m^2, consistent with the energy's quadratic scaling and the area constraint's linear scaling.

Take it with you

  • Feasible tangents satisfy the linearized constraint, not necessarily exact straight-line feasibility.
  • A normal multiplier theorem needs a constraint qualification.
  • An augmented Euler–Lagrange equation still needs feasibility and a minimality argument.

Read further

Original sources and deeper explanations to follow at your own pace.

Optional progress, saved in this browser when available. Revisit any lesson at any time.

Lesson not marked complete.