Page 293 - Pressure Swing Adsorption
P. 293

I I
             270                                   PRESSURE SWING ADSORPTION
                                                                                               EXTENSIONS  OF THE PSA CONCEPT
                                                                                                                                                            271
             these  sm1Ple  arguments;  ootirnai  performance  is  obtamed  when  the  phase
             angle difference is  about 45°  and the ratio of the piston strokes ts about 3.5:1.              \
               As  a  separation  process  the  pressure  swmg  oarametnc  pump  has  two
             maJor  advantages:
             I.  It  can  produce  two  oure  products;  so  complete  resolution  of  a  hinary
                                                                                                                                       hot space
               nuxture  may  lie  achieved  without  the  complexity  of the  purge  and  nnse                                         (wod~ing gas 1s
               steps  that  are  reauirect  to  accomplish  this  in  the  normai  PSA  mode  (sec                                    /  found in  here
                                                                                                                                       while it expands)
               Sect10n  6.3).
             2.  The  system  can  be  easily  designed  to  provide  efficient  energy  recovery,                                    ,-regenerator
               since,  on  the -exoans1on  stroke,  the 01stons  are  dnven  by  the  pressure of
                the gas. Conseivation of this energy for use in the next compression stroke                             displacer      ~cooler
                c3n be easily accomolished either usmg a flywheel  or by coupling together
                two  umts operatmg-out of phase.
               There  1s,  however,  one  serious  disadvantage:  the  pistons  and  cylinders
             must be large enough to accommodate virtually all the gas desorbed from the                                              cold space
             bed  at  the lowest  pressure of the cycle.  For a  bench-scale  umt this  1s  not a                                     (working gas 1s
                                                                                                                                     ~ found in  here
             serious problem,  but  it  does present a serious obstacle to scaleup.                                                   when compressed)
                                                                                    I
             7 .2  Thermally Coupled PSA


              In the previous section we considered the molecular gate as a oressure-driven   l   Figure 7.4  The pnnc1ple of operation of the  Stiriing engme (dispiacer type).
              oarametnc  oumo.  This  system  is  also  closely  related  to  the  Stirling  engine
              and thus to a  nOvei  class of processes that  utilize oenodic vanatiOns in  both
              pressure and  temperature together with  an oscillating  gas  flow  to  effect  an   working gas,  and the  eqmvaient  amount of heat is  transferred  from  the cold
              energetically efficient separation. The basic elements of a Stirling engme are   region to the  hot region.
              shown  in  Figure  7.4.  As  in  the  molecular  gate  there  are  two  01stons:  a   In order to reduce unnecessary heat  losses, a  regenerative  heat exchanger
              pressure piston  and a displacer, in  an arrangement that ts  similar tn  essence   IS  mclucted  between  the  hot  and  cold  regions.  This  is  essentially  a  soace
              to  that shewn  in  Figure 7 .2.  The working  gas  1s  transferred backWarcts  and
                                                                                              oackect  with  high-heat-capacity matenal that 01cks  up  heat from  the  hot gas
              forward  between  the  ''hot  space"  and  the  "cold  space"  by  the  displacer
                                                                                              as  It  flows  to  the  cold  space,  stores  1t.  and  transfers  it  to  the  cold  gas
              otston.  There  is  very  littie  difference  in  pressure  between  the  hot  and  cold
                                                                                              returning from  the cold space on  the  next  stroke of the displacer.
              ~paces:  so  the  disoiacer  does  very  little  mechamcal  work.  However,  the   A thermally coupled PSA (TCPSA) system can be  thought of as a Stirling
                                                                                                                                    4
              Pressure  throughOll~  the  system  varies  sinusoidally  as  a  result of the  move-  engme in which  the regenerator 1s  packed with a selective adsorbent and the
              ment  of the  pressure  piston.  When 'the  system  operates  as  an  engme,  gas
                                                                                              gas  to  be  separated  1s  the  working  fluid.  Two  possible  arrangements  are
              expands  m  the  hot  space  and  flows  mto  the  cold  space,  ctnvmg  down  the
                                                                                              shown  m  Figure  7.5.  The  arrangement  shown  m  Figure  7.5(a)  is  directly
              pressure mston. The displacer then moves  down,  transfernng the cold gas at
                                                                                              analogous  to  the  displacer-type  Stiriing  engme  (Figure  7.4).  The  disoiacer
              low  pressure  back  to  the  hot  space.  The  pressure  piston  is  then  raised,
                                                                                              transfers  the  cold  gas,  at  high  pressure,  from  the  cold  space.  through  the
              mcreasing  the  pressure  m  the  system,  while  the  gas  m  the ·hot  space  ts
                                                                                              adsorbent bed, where the preferentially adsorbed component 1s  retained. The
              heated, causmg a  further  nse m  pressure,  and the cycle  is  repeated.  In  this   heat of adsorption  raises  the  temperature of the gas flowing  through  to  the
              mode  of operation  the  net  effect  is  that  heat  1s  transferred  by  the  gas from
                                                                                              hot  spa·ce,  where  Jt  1s  heated  further  from  an  external  heat  source.  The
              the  hot  to -cold  regions and an eqUivalent amount of work  is  delivered to the   pressure  in  the  system  1s  then  decreased  and  the  hot  g11s  1s  passed  back
              pressure  piston. The system can also he operated in  reverse  as a  heat  pumo   through  the  adsorbent  bed.  The  prcfcrcnt1a/ly adsorbed  species  is  dcsorhed
              or  refrigeratm;.  In  that  mode,  work  1s  dOne  by  the  pressure  piston  on  the
                                                                                              and  earned  down  with  the gas  tlow,  which  1s  cooled  by  the  heat of desorp-
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