Flash Evaporation Physics
VACUUM-DRIVEN PHASE-CHANGE SEPARATION FROM FIRST PRINCIPLES
Flash evaporation is the rapid phase transition from liquid to vapor that occurs when pressure drops below the saturation point at a given temperature. Water at 25°C boils when ambient pressure falls below 23.8 torr (3.17 kPa). The transition is abrupt: latent heat is drawn from the liquid itself, cooling the remaining volume and driving a self-limiting evaporation front that propagates through the exposed surface in milliseconds.
The Separation Mechanism
Dissolved solids, heavy metals, and biological contaminants have vapor pressures many orders of magnitude below water's at any relevant temperature. Sodium chloride, for example, has a vapor pressure below 10−10 torr at 25°C. When water flashes to vapor under vacuum, these contaminants remain in the liquid phase. The separation is not filtration — it is a thermodynamic boundary. No membrane, no chemical pretreatment, no fouling surface.
Governing Physics
The flash evaporation rate depends on the degree of superheat — the difference between the liquid temperature and the saturation temperature at the reduced pressure. For water at 25°C flashing into a 10 torr environment, the superheat is approximately 10°C. The evaporation mass flux follows:
where α is the evaporation coefficient (0.01–1.0 depending on surface conditions), R is the gas constant, T is temperature, and M is molecular mass. For clean water surfaces, α ≈ 0.04.
The energy cost of evaporation is the latent heat: 2,260 kJ/kg at 100°C, rising to 2,442 kJ/kg at 25°C. Any practical flash system must recover this latent heat from the condensing vapor to achieve competitive energy efficiency. Without heat recovery, flash distillation consumes roughly 680 kWh/m3. With multi-effect heat recovery, the theoretical minimum approaches 1.8 kWh/m3. Phase Flash targets 3–5 kWh/m3 in deployed systems.
Comparison with Conventional Desalination
The Engineering Challenge
Conventional multi-stage flash plants operate at 2–4 flash events per minute. Phase Flash targets hundreds of cycles per minute through radial expansion chamber geometry and rapid re-pressurization. The bottleneck is condensation rate: vapor must condense fast enough to clear the chamber for the next flash cycle. Diamond condenser surfaces provide the thermal conductivity (2,200 W/m·K, five times copper) needed to sustain high-frequency cycling.