Take and extend it by zero outside . The zero extension of W01 belongs to and the Sobolev inequality gives
Because has finite measure, the Holder inequality gives
Thus
The reverse estimate follows directly from . After adjusting constants,
This is the Poincare inequality on .
For , define the Sobolev conjugate exponent
The Sobolev inequality, also called the Gagliardo--Nirenberg--Sobolev inequality, states that there is a constant such that
for every , and hence by completion for every for which the right formulation applies.
Interpolation between and , followed by the three-dimensional Sobolev inequality, gives
Apply this with and use part i:
Orthogonal projection is contractive in , so
The Sobolev constant is dimensionless after using the periodic-domain normalization, so the estimate is scale invariant.
For , the Sobolev conjugate exponent is defined by
The first-order Sobolev inequality maps one derivative in to the function in .