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gas is defined by yo, and the partial pressures of each species are defined by Equations (2.5) and (2.6). P° N=NA+N V=VA+VB y=yo PAO = yoPo PBO = (1 - yo)Po (0) Po Po NA NB VA VB y=l y=0 B PBI =Po In state (1) of Figure 2.1, the gases are separated and the partial pressure of each gas has been raised to the total pressure. O n a molar basis, the avauability of each species at state (1) (ignoring velocity and gravitational terms) is defined as: Figure 2.1 (0)Mixed Reference System, and(1)Separated Gases. WAi=(HA\ -h Ao)-T o{s Ai -SAO) ¥BX ={HB\ -h Bo)-T o{s m-s Bo) Where: V|/AI= molar availability of species A at state (1) {J/mol} IIAI = molar enthalpy of species A at state (1) {J/mol} hAo = molar enthalpy of species A at the reference state {J/mol} To = reference temperature {K} (2-7) (2-8) PAI =Po (1) 10PDF Image | Energy Efficiency of Gas Separation Pressure Swing Adsorption
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