Page 176 - Pressure Swing Adsorption
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 150   PRESSURE SWING ADSORPTION   EQUILIBRIUM THEORY                151

 Thus,  the  net  effect  of  ternoerature  shifts  during  this  four-steo  cycle  is   PSA  WITH  INCREASING  PRESSURE
 positive.  That  1s,  the  recovery  of  the  light  component  should  be  somewhat
 greater when  the  natural  temperature  shifts  occur  than  if  the  system  were
 forced  to  remam  isothermal.  The  net  effect  IS  expected  to  be  mmor  since,   40
 according to the basis chosen, only the ourge and feed  streams are affected,
 and  the mcrease of the ourge stream should be small relative to the decrease
 of the feect ·stream.   35
               u
 Before  leaving  this  subject,  1t  is  worthwhile  to  point out that the  conclu-
 sion Just  reached  1s  not general: different cycies will  resoonct to temperature   w
 shifts  differently.  For  example,  for  cycies  in  which  the  heavy  component  is   a:   30
               ::,
 oroctuced  durmg blowdown (cf.  Section 4.4.5),  the most  imoortant stream m   f-
               <(
 determmmg  recovery  is  the  blowdown  step.  This  steo  involves  a  large   a:
               w
 temoerature drop (relative  to the  pressurization,  high-pressure  oroduct, and   CL   25
               :,:
               w
 rinse steps) due to desorption and depressunzatlon. As can be seen from EQ.   I-
 4.41, the net effect ·is that the adsorbent retains more of the heavy component   20
 than 1t would under isothermal conditions (i.e .•  the magmtude of the second
 term on the right-hand side is  larger), so recovery is diminished.
 Aside  -from  gaining  a  better  understanding  of  PSA  systems  via  their   15
 inherent  thermal  response,  there is  an even greater mcent1ve  to understand   10   20   30   40   50   60   70
 this  behavior. To elaborate, in many PSA systems 1t  is  important to orevent   TIME   (s)
 complete  breakthrough,  (e.g.,  durmg  feed  and  cocurrent  blowdown  steps),
 which would reduce the purity of the product.  Conversely, if breakthrough  IS   Figure 4.22  Bed temperature histones for  a combined pressunzauon  and  feed  step.
 not  imminent  at  the  end of these  steps,  the  product  recovery  cannot  be  as   The numbers  1 through  5 indicate  thermocoupie  locations  m the  bed,  from  near  the
 high  as  possible,  smce  any  purified  gas  left  m the column  1s  exhausted with   feed  end to  near the  product end. The  application  is oroduttmn of oxygen  from  a1r
        with zeolite 5A. The pressure  mcreases linearly with  ume  from  ~.O  to  5.2  atm.  26
 the  byproduct.  Simiiariy,  a  rmse  step  should  be  allowed  to  proceed  until
 breakthrough is Just  como1ete.  To go  further would  reduce  recovery,  and  to
 stop prematurely would reduce ourity. Accordingly, both high product punty   used  to control  feed  and  rinse  step times  for  the  five-step  t.')'cle  experiments
 and  high-recovery  PSA  performance  can  be  achieved  by  termmatmg  such   described in  Section 4.5  lcf.  Figures 14(a) and (b)].
 steos  very  precisely.  A  minor  problem  ts  that  many  comoosit1on  sensmg
 instruments  have  long  response  times  or  large  samole  volumes,  so  that
 on•line  measurements  are  often  unpractical.  That  is  where  the  thermal   4.9  Pressurization and Blowdown Steps
 response comes m,
 The  fact · that  the  shock  wave  of temperature usually  comcides  with  the   Until  now,  attention  has  been  focused  on  comoJete  PSA  cycies  and  overall
 composition front' can be exoloited to control the t1mmg.  Evidence for that is   effects. There are, however, cases in which  the individual steps are important.
 shown  both  m  Figure 4.20,  which  was  described  oreviousiy,  and  m  Figure   For example, when  the  heavy  component of a  mixture )s valuable,  it  may  be
 4.22,  in which, again, oxygen 1s  being separated from  air.  In  the iatter figure,   des1red  as  the sole  product or  as  a  co-oroduct.  In  that  case,  the  blowdown
 the pressure increases from  2.0  to 5.2 atm.  as feed  1s  being admitted to  and   step,  in  particular, 1s  vitai  to  the  performance  of the  PSA svstem,  and  1t  1s
 product  is  bemg  slowly  released  from  the  column.  As  can  be  seen,  the   important to know the comoosition  of the effluent as a: function  of pressure,
 average temperature m the bed rises, but the sharpness and magmtude of the   or to  predict  the composition  profile  m the  bed  at the end of blowdown.  In
 temperature  front  are  essentially  the same  as  when  pressure was  constant.   other s1tuat1ons  (e.g.,  mvolvmg pressunzat10n  by feed  or by  an  intermediate
 26
 Eqmvaient, but reverse effects occur when the bed pressure decreases.  The   product from  a parallel bed) 1t  may be of interest to oredict the  composition
 possibility of controlling the step  times  in  this manner can orevent reduced   profile in  the bed dunng pressunzatwn.
 recovery  [e.g.,  due  to  diminished  adsorbent  capacity  or  when  operatmg   Jn  that vein,  perhaps the first  treatment of composition  profiles at various
 conditions (or ambient conditions) vary significantly]. Jn fact,  this concept was   extents of pressurization was given  hy  Flores  Fcrn;ndez and  Kenney.  25   They
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