Use for the perturbation variable and for its dual variable. The full Fenchel conjugate is . One signed-marginal convention is
The primal problem of convex perturbation duality is and its dual problem of convex perturbation duality is . The signed dual marginal is concave; some conventions instead use as a convex marginal. The definitions above fix all signs. Weak duality follows from . Also , so .
For a sufficient strong duality condition, assume is jointly proper convex, is proper with finite, and is finite and continuous in a neighborhood of . More generally suffices in finite dimensions. A supporting subgradient then exists, and
Thus the dual is attained with no gap. This condition does not by itself assert attainment of the primal infimum; that needs an additional compactness or coercivity argument.
The same subgradient describes sensitivity analysis in convex perturbation duality: bounds the optimum's change under perturbation. When is finite convex near zero, its one-sided directional derivative is . If , then is differentiable there and
These conditions allow first-order sensitivity predictions; without differentiability the subgradient set gives directional bounds. Multipliers can measure the value of relaxing constraints, quantify changes in noise tolerance, and guide parameter choice without resolving every perturbed problem. For the constraint convention in part (b), the noise-budget sensitivity is negative the nonnegative constraint multiplier.
A shadow price measures the marginal improvement from relaxing an inequality optimization constraint. Use for in a minimization problem. With strong duality and a differentiable optimal value function, .[ref]
In the quadratic minimization with a moving upper bound, direct differentiation gives
The derivative at is zero from both sides, although has different one-sided derivatives there. The value of additional room has faded continuously to zero just as the active constraint stops restricting the optimizer.
At , , and . Raising the bound to lowers the value to : the first-order prediction is a change of , while the exact change is . At , the same relaxation leaves and . At , tightening by costs , a second-order effect despite the zero Lagrange multiplier.
Figure 1.
The derivative of the optimal value is the negative inequality multiplier
. Details.
There is also a global statement in this example. Keeping the Lagrange multiplier at the value associated with , the Lagrange dual function changes by . Weak duality therefore gives
At this is , the supporting tangent shown in the diagram. This bound remains valid for large changes, whereas the derivative predicts only the first-order effect. If the value function is not differentiable, an optimal Lagrange multiplier can instead supply a supporting subgradient, rather than a unique marginal rate. This is the same idea used in sensitivity analysis in convex perturbation duality.