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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 D.2. Sample calculations for governing equations in the laboratory scale models – continued tt 0.3178[kgm-3] j t  0.1 [s] ut 10.940[ms-1] utt 10.726[ms-1] j utt 10.728[ms-1] j1 utt 10.724[ms-1] j1 z  0.0003 [m] j Ctt g,He, j Ctt g,N2 , j Ctt g,CO2 , j Ctt w,He,j Ctt w,N2 , j Ctt w,CO2 , j R R R Ag 1.735107 [m2] Mass , He Mass,N2 Mass,CO2  0.1605 [kg m-3]  0.0955 [kg m-3]  0.0703 [kg m-3]  0.1605 [kg m-3]  0.0955 [kg m-3]  0.05894 [kg m-3]  4411 [s m-2 ]  5748 [s m-2 ]  6834 [s m-2 ] Ptt 109.768[kgm-3] j1 Ptt 109.748[kgm-3] j1 tt 1.7838105 [kgm-1 s-1] j f  0.712 Dh 4.7104 [m] L  0.22 [m] Microchannel momentum conservation equation uuuCg,i Cw,iuP2uf u2 t z AR z z2 2D tt j utt ut j j  ttutt utt utt j1 j1 i g Mass,i h Ctt Ctt g,i, j w,i, j  t j j Ptt Ptt utt 2utt utt ARtt i g Mass,i,j 2 utt 2z j tt utt   j1 j1 tt j1 j j1 ftt j j 2z j z2 j 2Dh Ptt 109.758 [kPa] j 205

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