Page 160 - Pressure Swing Adsorption
P. 160

134   PRESSURE SWING ADSORPTION   I,   EQUILIBRIUM THEORY           135

 0.5   I   I  I  I  111   Table 4.1.  Conditions and Results of PSA Experiments with Combined Feed and
                 Cocurrent Blowdown  27

            Run       il,       ilu                             ~ (o/c)
 0.4                                      R,:,pl     Riti-:ory
 c
 $           l        12.77     10.43      25.4       26.5       -1.1
 C
 0           2        13.18     10.95      28.4       27.1        1.3
 a.          3        17.41
 E   0.3                        14.35      29.6       31.4       - 1.8
 0   0       4       22.91      19.03      34.1       34.6       -0.5
 0
             5       33.73      25.12      35.9       38.5       -2.6
             6       33.29      21.06      37.4       39.1       - 1.7
 0.2
 >-
 ""
 w
 >
 0               27
 ()     apparatus.  The theory for this  type  of cycle  was  discussed  m  Section  4.4.4.
 w   O.i
 "'     The  application  was  to  split  oxygen  from  air  with  zerilite  13X.  Six  experi-
 .j     ments  were  conducted  m  which  two  pressure  ratios  were  varied  mdeoen-
 0.0  1 oo   1 Q3   !   dently.  A  summary of the conditions and results 1s  given in Table 4. L
          The  average  absoiute  deviation  of  the  light  product  recovery  between
        theory  and  these  experiments  was  only  1.5%, just  as  it  was  for  the  exoen-
        ments  havmg  constant pressure  durmg  the  feed  steo. This  close  agreement
        provides additional evidence that the local equilibrium theory 1s  mdeed valid,
 Figure 4.13  Expenmental recovery versus predicted recovery (according to Eo. 4.27)
 for  oxygen (and argon) separation from  air usmg SA zeolite at 45° C.  20   and ts  relatively insensitive to the cycle  and ooeratmg cbndit1ons.
          Finally, a set of experiments has  been conducted in which a  nnse step was
        mtroduced,  m order  to  extract  the  heavy  comoonent  as  a  pure  product.  In
 from  6.5  to 840,  and  the  average temperatures were 45  and 60° C.  It should   addition,  the  purge  steo  was  left  mcomolete,  m  order  to  achieve  high
 be  noted  that  argon, which  appears  as  about  1 %  m  dry air,  adsorbs  nearly   recovery of the light component. The ·relevant  theory 1s  described  in  Section
 ident1cally  to oxygen,  so  the  targeted "oure"  light product  1s  actually  about   4.4.5. The specific application was to split  dry air to get. oxygen (with  residual
 95% oxygen and 5% argon. Product recovery was of primary mterest, smce It   argon) and nitrogen usmg zeolite 5A as the adsorbent.  in those exoenments
                                                                       1
 1s  predicted ouantitativeiy by  the  theory.  Results of the expenments and  the   a  single  bed  was  used,  and  pressure  rat10s  were  vaned  between  6  and  20.
 predictions of Eq.  4.27  are  shown  m  Figure 4.13.  Recall  that  there  are  no   Generally, it was possible to reduce the level  of imourities m the products to
 !
 adjustable parameters in the model, so the extent of agreement is  not due to   about  1 %  (i.e.,  0  2   m  N ,  and  N  2   m  0  2 )  anct  to  achieve  corresoonding
 and  oredicted  recoveries was  1.5%,  and  the  product  purity  averaged  99.6%  I   oroduct recovenes between  27% and 90%. The  oredicted  and exoenmental
                             2
 emomcal  fitting.  The  average  absolute  deviation  between  the  experimental
 i      recoveries  of both  oroducts  agreed  well,  even  though ,they  vaned  with  the
 (mtrogen-free oxygen and argon). These experiments provide strong evidence   i   applied pressure ratio, as shown m  Figures 4.!4(a) and {b).
 that, for this system, the equilibnum theory 1s  essentially correct.   '   In  addition,  Figure  4.15  shows  a  cross-plot  of  the  experimental  resuits
 !
 Although the results described are reassuring, they focus on the high-pres-  from  those  exoenments,  along  with  results  obtamed  bty  Sircar  22   for  a  very
 sure  feed  step;  the  pressunzation,  purge,  and  especially  blowdown  are   I   similar  cycle.  The  axes  depicted  are  product  purity  and  recovery.  Sircar's
 ancillary  steps.  So  a  major  Question  still  remams  as  to  the  validity  of   '  !   results  show  a  commonly  observed  trend:  as  recovel':}'  mcreases,  product
 equilibrmm theories when ·pressure changes  are vital to the cycle,  rather than   · purity decreases.  The  data  from  the  exoenments  described,  however,  show
 oract1cally  lmmatenal.  This  issue  was  examined  in  two  separate  types  of   that ounty can  be  maintamed at  high  levels as  recovery increases, without  a
 experiments.  The  first  type  of  experiment  looked  at  the  accelerat10n  or   significant increase in oower consurnot,on.
 deceleration  of  the  shock  wave  durmg  the  feed  step,  in  conJunctton  with   To conclude this sect10n, 1t  appears that the equilibrium theory 1s  accurate
 decreasmg  or  mcreasing  pressure,  resoectiveiy.  26   Comoarmg  experimental   and reliable for different PSA cycles, even  for  relatively difficult  separations.
 results with  predictions  of the  theory  showed  nearly  perfect  agreement for   Parenthetically,  1t  should  be  mentioned  that  other  expenmental  evidence,
 both mcreasing and ctecreasmg pressure. Second, PSA experiments involvmg   · shown m  Figure 4.3, indicates that the eouilibrmm  theory should be valid for
 simultaneous feed and cocurrent blowdown have been conducted in a two-bed   a wide range of applications,  although  the  degree of agreement depends on
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