Permeability — where it appears
Named by 4 essays across 2 fields — each of them below, with the objects they name alongside it.
A wall that is not quite there
A porous surface has structure on every scale below the pore, and no calculation resolves it. The whole of it can be replaced by one length — the square root of the permeability — and the replacement is exact to first order, with what it leaves out identifiable as the flow the wall itself carries.
A velocity nobody has
The velocity in Darcy's law is the flow rate divided by the whole cross-section, solid included — a speed no fluid particle in the bed ever has. Averaging buys a linear law and charges for it in exactly this coin, and the constant that comes with it is an area of about a square micron.
A permeability that is only the geometry
Kozeny–Carman says that a porous medium's permeability follows from its porosity and its specific surface. Both are real, both are exactly measurable, and they do not determine the answer: forty-nine tube bundles built with identical values of each span a factor of eighty-two in permeability.
A filter is slowed by what it has caught
Push a slurry through a cloth and within minutes the cloth no longer matters: the particles it has caught form a cake, the cake is a packed bed, and every litre filtered makes the bed thicker for the next. The filtrate grows only as the square root of time. And if the cake is soft, it packs tighter against the cloth the harder it is pushed, until more pressure buys almost nothing.
Named alongside it
The objects these essays reach for when they reach for this one.
Darcy's lawMeasurementPacked bedPorosityAveragingScalingBoundary conditionChannel flowClosureCompressibilityConserved quantityCorrelation