As the substance in a liquid body crosses
the boundary from liquid to gas (see green arrow in
phase diagram), the liquid changes into
gas at a finite rate, while the amount of liquid decreases. When this happens within a heterogeneous environment,
surface tension in the liquid body pulls against any solid structures the liquid might be in contact with. Delicate structures such as
cell walls, the dendrites in
silica gel, and the tiny machinery of microelectromechanical devices, tend to be broken apart by this surface tension as the liquid–gas–solid junction moves by. To avoid this, the sample can be brought via two possible alternate paths from the liquid phase to the gas phase without crossing the liquid–gas boundary on the phase diagram. In
freeze-drying, this means going around to the left (low temperature, low pressure; blue arrow). However, some structures are disrupted even by the
solid–gas boundary. Supercritical drying, on the other hand, goes around the line to the right, on the high-temperature, high-pressure side (red arrow). This route from liquid to gas does not cross any
phase boundary, instead passing through the
supercritical region, where the distinction between gas and liquid ceases to apply. Densities of the liquid phase and vapor phase become equal at critical point of drying. ==Fluids==