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<br />Calculations of various flow rates and limitations include: <br /> <br /> (1) BPR; <br />f\) [ 1-(50/TOO,) TDS. - 50 l............. (53) <br />00 BPR ~ <br />c..;l = max or <br />""" 900/C - 1 80,000 - TDS. <br /> a. ~ <br /> ~ <br /> (2) Cb by Eq. 48; <br /> (3) Cw; <br /> <br />Cw <br />Cw <br /> <br />= C (3.2 <br />P <br />by Eq. 50 <br /> <br />- BPR) (no cooling towers) <br />(no cooling towers) <br /> <br />. . . . . . . . . . . . . . . (54) <br /> <br />(4) C. by; <br />~ <br /> <br />Ci = Cp (1.15 + BPR) (cooling towers) ................. (55) <br /> <br />Ci by Eq. 52 (no cooling towers) <br /> <br />The mathematical cost simulation for VTE-MSF process is <br />given in Table 2. <br /> <br />Vapor Compression - VTE-MSF <br /> <br />An alternative to generating the necessary process heat <br />through steam is to employ another enthalpy principle, i.e. that <br />as a vapor is compressed, its pressure and temperature increase. <br />A vapor compressor takes the low temperature water vapor from <br />the VTE outlets, compresses it to increase the temperature and <br />then feeds it back into the next MSF stage, thereby replacin~ <br />the high temperature steam supply. <br /> <br />The applicable conditions for the VC-VTE-MSF process are <br />the same as noted previously except this process favors rela- <br />tively warm feedwaters. Hydraulic characteristics for BPR are <br />determined from Eq. 53. Brine volume is then calculated using <br />Eq. 48, and cooling waters by: <br /> <br />Cw <br />Cw <br /> <br />= Cp (2.2 <br />= C (1.5 <br />P <br /> <br />- BPR) <br />- BPR) <br /> <br />(cooling towers) .................. (56) <br />(no cooling towers) ............... (57) <br /> <br />Total intake rate is computed by: <br /> <br />C. = c (1.1 + BPR) ................................... (58) <br />~ P <br />or for systems not using cooling towers, Eq. 52. <br />A summary of the cost simulation is given in Table 3. <br /> <br />36 <br />