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By this we are saying that at time tc the mole fraction at the entrance of the bed is yc. This can be generalized for all time, with yc becoming the mole fraction at the left end of the bed, yi. f=-^-[i (A-i) ]2 w +yi P AU2 However, until the front of the simple wave reaches the end of the bed, the gas leaves with mole fraction yB. The position of the simple wave at the end of this constant mole fraction step is labeled tB in Figure 3.7, and the equation describing this time is given below. P AU2 Equation (3.37) is valid for the remaining time from t = tB to t = tpu and can be solved for yi in terms of t. Only one root of the resulting quadratic has values of yi less than 1. The solution of yi(t) over the entire range 0 < t < tpu is presented below. yi(t) = yB ;0PDF Image | Energy Efficiency of Gas Separation Pressure Swing Adsorption
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