For a regular isoperimetric constraint, introduce a constant Lagrange multiplier and set . With fixed endpoint values, the Euler-Lagrange equation is
If and have no explicit dependence, the Beltrami identity gives the first integral
The regularity assumption excludes the exceptional case in which the constraint itself has zero first variation for every admissible perturbation.
Parametrize the surface of revolution by . The magnitude of is . Integrating the resulting surface area element over , and integrating the circular cross-sectional areas for the volume, gives
Here because it is a radius. For a regular connected closed surface, take in the interior; the closing endpoints can have unbounded even when the surface itself is smooth.
After dividing by , its integrand is . The Euler-Lagrange equation and Beltrami identity become
As tends to zero at an endpoint, also tends to zero, so . On the positive interior this implies and, writing ,
The Euler-Lagrange equation also yields . Therefore
including at the maximum where . Integrating and using the first integral gives
Thus the regular extremal is a sphere. The two zeros fix its center and radius:
Equivalently, the prescribed volume fixes . If are fixed in advance, their separation and the prescribed volume must be compatible with these equations; there is no positive regular stationary profile of the stated type for an incompatible volume.
For minimality, the three-dimensional isoperimetric inequality states that every sufficiently regular closed surface enclosing volume has
with equality precisely for a sphere. Our extremal has and , so it attains equality and is a global minimum of area at the fixed volume. This also makes clear the connected-surface assumption behind uniqueness: allowing several disconnected components introduces stationary collections of spheres, rather than the single positive generating profile used here.

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