Page 214 - Pressure Swing Adsorption
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 190   PRESSURE SWING ADSORPTION   DYNAMIC MODELING  OF A  PSA SYSTEM   191



 7
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 LOF  model
                     CL
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 0   0
 0   2   3   4   5                                          0
                         0     4     8     12    16   20   22.5
 Product  rate  (cc/sl
 (CJ                                  TIME.MIN
 Pigure 5.4  (c) Effect of product withdrawal  rate  (experiments 7-9 in Table 5.4) on   Figure 5.S  Effluent concentration at steadv state obtained from a  PSA cvcJc  seoarat-
 punty  and  recovery  of  oxygen  product  m  a  dual~bed  PSA  air  separation  process   mg 49.5:59.5:1.0  H :CH :H S mixture  on  activated  carboff showmg  the  close  agree-
                           4
                              2
                       2
 operated  on  a  Skarstrom  cycle.  Equilibnum  and  kinetic  data  and  other  common   ment  between  numencallv  solved  eauilibnum  model(--) and  LDF  model  (---).
 parameter values used  for computing  the  LDF model  predictions are given  m  Table   (0), ( □) and (t:..)  represent  exocnmCn1al  data  for  CH  4 ,  H ,  and  I-1 S,  reSpcct1vclv.
                                                             2
                                                      2
 5.3.  (From  Ret 22)   (From Ref. 8;  reonnted with  pcrm1ss1on.)
         presented  m  Figure  5.2  together  with  the  other  coffelattons.  It  1s  evident
         from  Figure 5.7  that  the  LDF model  usrng  the  fl  values  derived  from  this
         calibration can correctly predict the effects of varying the product withdrawal
 Table S.S.  Effect of Mass Transfer Resistance on Product Purity
         rate  and  the  high  operating  pressure  m  the  range  2.36-3.72  atm.  The
 and Recovery (PSA Oxygen)"
         calibrated .0  values approach the limiting value of 15  for  large cycle  times.  It
 Feed   Product   Mole%   Recovery   is  important to note  that  this  particular observation  is  specific  to  the  system
 rate   rate   kA   k,   02in   of0 2   and the operating conditions and therefore should not'be taken as a universal
 3
 3
 No.   (cm /s)   (cm /s)   (s - ')   (s- I)   product   (%)
         upper limit for the calibrated  fl  values m  the  iong-cycle-t1me  region.
 1   25.0   LIJ   62.0   19.7   93A0   21U0
 2   25.0   LI3   20.0   6.6   93.29   20.08
 3   25.0   Ll3   62.0   !9,7   76.70   16.50   5.2.2  Variable-Diffusiv1ty Micropore Diffusion  Model
 4   25.0   l.13   20.0   6.6   75.78   16.30
         In most of the studies m which  the LDF model has be.en successfully applied
 For  I  nnd  2:  i1dsorption  pressure - 1.48  ;1tm,  blowdown  prt!ssure - 1.0,  purge  pressure - I.07  atm,   to  PSA separations  based  on  kinetic  select1v1ty,  key  parameter values  have
 cycle  ume - JOO  s;  for  1  and  4:  11dsorpt1on  pressure - J.QO  atm,  hlowdown  pressure= l.O,  purge   been chosen emoincally  by  matching  the  model  oredkt10ns  to exoenmental
 pressure= I. I aim. cvcle  ume = 250 s.  Other parameters as 1n  Table 5.3.
 .   -
 Source:  From Ref. 22.   data.  In this situation  the  model  oredict1ons can  be considered  reliable only
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