For a unit-speed space curve, set
These form the Frenet trihedron. With the signed torsion convention compatible with the question, the Frenet-Serret formulas are
For an oriented surface with unit normal , the signed geodesic curvature is
On the unit sphere . Since , differentiation gives
Write . Then , and differentiating this expression and comparing the coefficient with gives
Thus, wherever the displayed quantities are defined,
Finally,
which is the stated curvature decomposition for a spherical curve.
For a positively oriented simple closed curve bounding a disc on the unit sphere, the local Gauss-Bonnet theorem gives
Here , so
At fixed length , maximizing the enclosed area is therefore exactly the same as minimizing .
From part (a),
As is orthogonal to ,
To compute , only its component matters. Differentiating contributes , while differentiating contributes through . Every other term is normal to . Hence
At an area critical point the assumed first-variation identity holds for every smooth compactly supported where :
The fundamental lemma of the calculus of variations gives
on each component of . Thus is constant there. A nonzero constant component cannot have a boundary point where continuity makes . Since the closed curve is connected, either or it is one nonzero constant everywhere. Therefore every area-maximizing curve has constant geodesic curvature.
For a unit-speed spherical curve,
the normal component is because
, and the tangential normal component is the definition of . If is constant, then
Moreover . Hence the whole curve lies in the fixed plane
so it is planar.
The preceding parts show that an area maximizer among curves of fixed length is a plane section of the sphere, hence a circle. If its smaller cap has angular radius , then
For this circle,
No curve of the same length encloses more area than the maximizing circle. Equivalently every curve enclosing the smaller area satisfies the spherical isoperimetric inequality
with equality precisely for circles.

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