Constrained variations and multipliers
Restrict perturbations to a constraint tangent space and derive a valid multiplier equation under a constraint qualification.
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The question for today
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 with homogeneous perturbation space . Let the objective and a scalar equality constraint be continuously Fréchet differentiable nearby. If a differentiable feasible curve through the candidate has tangent , differentiating the equality gives . Thus feasible tangents lie in the kernel of the constraint derivative. A tangent condition alone does not make the straight line exactly feasible for a nonlinear constraint.
For an area constraint , the constraint is affine, so zero-integral directions preserve it exactly along straight lines. For a normalization , the tangent condition is , but the second-order term 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.
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 for the augmented functional. If both quantities are integrals, apply the Euler–Lagrange calculation to the augmented density . 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.
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.
Work it through
The least derivative energy for unit area
Minimize over subject to . Use the augmented functional .
The constraint derivative is nonzero on , so the scalar constraint qualification holds. The augmented Euler–Lagrange equation is .
Zero endpoints give . Its integral is , so and . The energy is .
For any feasible difference , both endpoint traces and its integral vanish. Hence , and the energy difference is , positive for every nonzero feasible difference.
The constrained minimizer is uniquely 6x(1 − x), with energy six and multiplier twelve in the declared sign convention.
The living notebook
Explore the model
Interactive lab · function
Quadratic scaling inside an admissible family
Consider the trial shapes , whose area is and energy is . Reset and set both instrument coefficient and position ; its height predicts normalized energy for area . Reset and set both ; 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.
- y at chosen x
- 0.608
- Tangent slope · 2ax
- 1.35
- Signed area · ax³/3
- 0.182
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.
Pause & reason
Check your understanding
Your turn
Try it yourself
Repeat the area-constrained derivative-energy problem with prescribed area . 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 , so and . Its energy is . More generally the minimum is , consistent with the energy's quadratic scaling and the area constraint's linear scaling.
Keep the idea
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.
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