Summary
Flash evaporation (or partial evaporation) is the partial vapor that occurs when a saturated liquid stream undergoes a reduction in pressure by passing through a throttling valve or other throttling device. This process is one of the simplest unit operations. If the throttling valve or device is located at the entry into a pressure vessel so that the flash evaporation occurs within the vessel, then the vessel is often referred to as a flash drum. If the saturated liquid is a single-component liquid (for example, propane or liquid ammonia), a part of the liquid immediately "flashes" into vapor. Both the vapor and the residual liquid are cooled to the saturation temperature of the liquid at the reduced pressure. This is often referred to as "auto-refrigeration" and is the basis of most conventional vapor compression refrigeration systems. If the saturated liquid is a multi-component liquid (for example, a mixture of propane, isobutane and normal butane), the flashed vapor is richer in the more volatile components than is the remaining liquid. Uncontrolled flash evaporation can result in a boiling liquid expanding vapor explosion (BLEVE). The flash evaporation of a single-component liquid is an isenthalpic process and is often referred to as an adiabatic flash. The following equation, derived from a simple heat balance around the throttling valve or device, is used to predict how much of a single-component liquid is vaporized. {| border="0" cellpadding="2" |- |align=right|where: | |- !align=right| |align=left|= weight ratio of vaporized liquid / total mass |- !align=right| |align=left|= upstream liquid enthalpy at upstream temperature and pressure, J/kg |- !align=right| |align=left|= flashed vapor enthalpy at downstream pressure and corresponding saturation temperature, J/kg |- !align=right| |align=left|= residual liquid enthalpy at downstream pressure and corresponding saturation temperature, J/kg |} If the enthalpy data required for the above equation is unavailable, then the following equation may be used.
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