TEMPERATURE SWING ADSORPTION PROCESSES FOR GAS SEPARATION

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TEMPERATURE SWING ADSORPTION PROCESSES FOR GAS SEPARATION ( temperature-swing-adsorption-processes-for-gas-separation )

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Table C.3 Sample calculations for the governing conservation equations – continued tt 651[kgm-3] j ctt 3867[kgm-3] P,j T t  306.7 [K] g,j t  0.005 [s] utt 1.83[ms-1] j Ttt 308.4[K] g,j1 z  0.01 [m] ktt 0.035[Wm-1 K-1] G,j ktt 0.621[Wm-1 K-1] L,j Ttt 309.4[K] g,j2 Rtt  0.89 [W-1m K] eq,Heat,G,j Rtt  0.15 [W-1m K] eq,Heat,L,j Ttt 306.4[K] w,j Ag 1.735107 [m2] Microchannel energy conservation equation hg u hg  t z S S X S X S k  2T ads LDG G GDL G purge G  g S X S S S X k LDG L deso cool GDL L L Req,Heat,L,i Discretized form S S X S X S ktt  Ttt 2Ttt Ttt  ads LDG G GDL G purge G,j  g,j2 g,j1 g,j  S XS S S X 1  A g  z S S X S X S  1    eq,Heat,G 2 ads LDG G GDL G purgeR S XS S S X 1  T T   g w 0 Ag    LDG L deso cool GDL L  Ttt Tt ttctt g,j g,j ttcttutt g,j g,j1  Ttt Ttt jP,jtjP,jj z S XS S S Xktt  z2 Sads  SLDG  XG  SGDL  XG  Spurge Rtt  Ttt Ttt   LDG L deso cool GDL L L,j  1  e q,Heat ,G , j   g , j w, j  0 LDG L deso  R t   t  cool GDL L eq,Heat,L,j T t  307.5 [K] g,j (After iterations and implementing the switch procedure) 186

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