Let . Its gradient cannot vanish on the ellipsoid, since the origin is not on the surface. Thus the Lagrange multiplier equations capture every constrained stationary point:
The temperature is a sum of squares, so . Equality requires and . The surface constraint then gives the four coldest points:
These are all such points, because a sum of nonnegative terms can vanish only when each term vanishes.
Solve the Lagrange multiplier equations by separating cases according to which coordinates vanish, so that division by a coordinate loses no stationary points.
If and , the surface constraint gives
If and exactly one of is nonzero, the equation for that nonzero coordinate forces , while the equation gives . Hence there are no stationary points in that case.
If and , the two remaining equations give . The surface constraint therefore has equal contributions from and , giving four stationary points:
If all three coordinates are nonzero, the equations imply
so and . Substitution in the surface constraint gives, with ,
Thus the remaining eight stationary points and their temperatures are
For example, their common temperature follows from . The cases with and are exactly the coldest points already listed. This exhausts all possibilities, giving fourteen other stationary points in addition to those four.
For , the stationary points found in parts (a) and (b) have temperatures , , and . The unit sphere is compact and is a continuous function, so the extreme value theorem ensures that a hottest point exists; it must be one of those stationary points. Thus
For a direct bound, put . The identity gives , and
since . Equality forces , giving exactly the two points above.

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