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numbers where the difference between the predictions is the greatest. Additionally, breakthrough experiments using small particles are often conducted at low Reynolds numbers since the response time of gas analyzers make high velocity waves difficult to accurately measure. Since such a difference in koverall exists depending on the correlation used to estimate DL, it is critical to determine which one is more appropriate for use in process simulators. Table 4.1 Comparison of parameters used for estimates of koverall in Figure 4.2. Pressure = 267 kPa dp = 0.05 cm, Dp = 0.02 cm2/s, K=16.5 Case 1 Case 2 Case 3 Case 4 γ1 of DL 0.7 0.7 0.7 0.7 γ2 of DL 0.5 0.5 3 3 kf ∞ Eq. 4.2 ∞ Eq. 4.2 57PDF Image | LIMITS OF SMALL SCALE PRESSURE SWING ADSORPTION
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