  We define the pressure of a porous medium in terms of the grand potential,
and compute its value in a nano-confined or nano-porous medium, meaning a
medium where thermodynamic equations need be adjusted for smallness. On the
nano-scale, the pressure depends in a crucial way on the size and shape of the
pores. According to Hill, two pressures are needed to characterize this
situation; the integral pressure and the differential pressure. Using Hill's
formalism for a nano-porous medium, we derive an expression for the difference
between the integral and the differential pressures in a spherical phase
$\alpha$ of radius $R$, $\hat{p}^\alpha-p^\alpha = {\gamma}/{R}$. We recover
the law of Young-Laplace for the differential pressure difference across the
same curved surface. We discuss the definition of a representative volume
element for the nano-porous medium and show that the smallest REV is half a
unit cell in the direction of the pore in the fcc lattice. We also show, for
the first time, how the pressure profile through a nano-porous medium can be
defined and computed away from equilibrium.
