Page 294 - Pressure Swing Adsorption
P. 294

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-
   289   290   291   292   293   294   295   296   297   298   299