Page 202 - Pressure Swing Adsorption
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 178   PRESSURE SWING ADSORPTION   DYNAMIC  MODELING OF A  PSA SYSTEM   179

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                               Figure 5.1  (Continued).


 TIME,  S   Extended Langmuir Model
 (al
 Figure 5.1  (a)  Pressure  profile  m a  small  PSA column seoaratmg air on 5A zeolite   (5.13)
 for oxygen production. The steps in sequence are depressunzaoon (30 s), purge_ (30 s),
 pressunzat1on (30 s),  and production (90 s). The pressure drop during the production   !=I
 step 1s  due to additional product withdrawal  for purging the other bed. Column size:
 90  cm  Oength)XlO  cm  ·(i.d.),  bed  voidage=0.35.  (From  Ref.  31;  reprmted  with
 permission.)  (b)  A  representative  pressure-tune  history  m  a  small  PSA  column
 separntmg  air  on  molecular  sieve  RS-10  for  mtrogen  production.  The  steps  m   LRC Model
 seQuencc  arc  oressurizalion  (15  s),  high-pressure  feed  (35  s),  blowdown  (6  s),  and
 purge (3  s). Column size:  101.6 cm  (length) X 2.08 cm  (i.d.),  bed voidage = 0.6.  (From   qf   b;cf;
 Ref.  32;  reprmted with  permission.)   _.c,_  = ---n,,.c.--     (5.14)
             qis       "'"'
                   1 +  L, b,.cf;
                       ,- !
 accurate  representation of the Henry·s  Law  region 1s  obviously  essential;  so   The  LRC model  1s  essentially  the  mult1comoonent  extension  of the  hybrid
 from  this perspective the Langmutr equation 1s  preferable.   Langmuir-Freundlich  eouatmn.  In  the  Langmmr-Freundlich  eouat10n  the
 The bulk PSA separation processes that have so far been modeled are for   concentration terms are raised to arbitrary exponents to provide an improved
 tile  most  part  bin·~~1es.  together with  a  few  ternary systems.  To predict  the   empincal  fit  of  the  smgle-component  data.  Both  extended  Langinmr  and
 ~uxture  isotherms  the extended  Langmuir  modei,  the  loading  ratio  correla-  LRC mocteis  orovide  explicit  expressions  for  the  adsorbed  phase  concentra•
 tion (LRC) and  ideal adsorbed solution theory OAS) have  been  applied.   tions.  so  no  iteration  1s  needed  during  the  simulation.  By  contrast.  the  IAS
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