Page 290 - Pressure Swing Adsorption
P. 290

,j  I
 266   PRESSURE SWING ADSORPTION
          EXTENSIONS OF THE PSA CONCEPT                                267
 Driven   H&allng   so:
 Platon   Halt-Cycle
                                                                      (73)
          Each  cycle  therefore  leads  to  a  net  upward  movement  of  the  solute.  as
          illustrated in  Figure 7.l(b). Over a large.number of cycles a very high degree
          of separatton can be  achieved between  the two reservoirs.
             The  main  drawback  of  oararnetnc  pumping  1s  that  1t  was  originally
          env1s1oned  and  reduced  to  practice  as  a  batch  process.  In  fact,  published
          accounts  of experimental  attempts  indicate  that  perhaps  50  or more  cycles
                                                                      2
 Heating   are  necessary  to  ::.tpproach  cyclic  steady  state.  Pigford  and  co-workers at-
 and      tempted  to  remedy  that  by  suggesting  a  similar  process,  which  they  called
 Cooling   Cooling   "cycling zone  adsorption."  Their concept  was  to  admit  feed  to  the  first  of
 Jacket   Half-Cycle   several  zones  (fixed  beds  of adsorbent)  connected  m  senes,  rather  than  to
          dnve it  back and forth  through a single fixed  bed, as in  parametnc pumping.
 Dr1vlng1--~;z:1
 Platon   They were able to relate the number of zones for continuous operation to the
          corresponding  number of batchwise  cycles.  Nevertheiess,  to  achieve  a  good
 (a)
          separation in  a contmuous system requiring several fixed  beds has smce been
          shown to be .1ust  as 1moract1cal as a batchwise system that reqmred enormous
          ttme (i.e., several  days).
             It  1s  often  said  that  PSA  separations  arc  similar  to  paramctnc  pumping
 HOT   COLO   HOT   COLO   with  pressure  rather  than  temperature  as  the  controlling  thermodyn::.tm1c
          variable.  However,  the  relationship  between  parametric  pumping  and  a



                                                            12
                                                            vl-----



                                                                  13
 (b)
 Figure  7.1  Thermal· parametriC  pump  showing  (a)  the  principle  of operatmn  and
 (b) the zigzag progressfon of the concentration profile m successive cycles.

                                            I I'     ,;/
 easily  understood  from  equilibrium  theory.  The  wave  velocity  is  given  by
 (Ea. 2.50):
 V   (7.1)
 ,I + ((! - <)/<) dq* /de                             16
                                           15
 If adsorption  ts  exothermic:
 da*)   (dq*)   (7.2)   Figure  7.2  A  pressure swing  parametnc  pump  (the  "molecular gate").  1-6, motor
 (Tc  hot  <  -Tc  cold   and drive;  7-11, adjustable stroke pistons;  13,  adsorbent bed;  12,12', product drawoff
          oomts;  15,16,  feed  and  ore-drier. (From  Keller and  Kuo,::  with  perm1ss1on.)
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