Abstract
Environmental concerns and oil price rises and dependency promoted strong research in alternative fuel sources and vectors. Fischer-Tropsch products are considered a valid alternative to oil derivatives having the advantage of being able to share current infrastructures. As a renewable source of energy, synthesis gas obtained from biomass gasification presents itself as a sustainable alternative. However, prior to hydrocarbon conversion, the bio-syngas must be conditioned, which includes the removal of carbon dioxide for subsequent sequestration and capture. A pressure swing adsorption cycle was developed for the removal and concentration of CO2 from the bio-syngas stream. Activated carbon was chosen as adsorbent. The simulation results showed that it was possible to produce a (H2 + CO) product with a H2/CO stoichiometric ratio of 2.14 (suitable as feed stream for the Fischer-Tropsch reactor) and a CO2 product with a purity of 95.18%. A CO2 recovery of 90.3% was obtained. A power consumption of 3.36 MW was achieved, which represents a reduction of about 28% when compared to a Rectisol process with the same recovery.
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Abbreviations
- a p :
-
particle specific area (m−1)
- A :
-
virial coefficients (m2 mol−1)
- B :
-
virial coefficients (m4 mol−2)
- Bi i :
-
mass Biot number of component i, \((\mathit{Bi}_{i}=\frac{a_{p}k_{f}R_{p}^{2}}{\varepsilon _{p}8D_{p,i}})\) (–)
- C g,i :
-
gas phase concentration of component i (mol m−3)
- C g,T :
-
total gas phase concentration (mol m−3)
- C p :
-
gas mixture molar specific heat at constant pressure (J mol−1 K−1)
- \(\overline{C_{p,i}}\) :
-
average concentration of component i in the macropores (mol m−3)
- \(\hat{C}_{ps}\) :
-
particle specific heat at constant pressure (per mass unit) (J kg−1 K−1)
- \(\overline{C_{p,T}}\) :
-
average total concentration in the macropores (mol m−3)
- \(\hat{C}_{pw}\) :
-
wall specific heat at constant pressure (per mass unit) (J kg−1 K−1)
- C v :
-
gas mixture molar specific heat at constant volume (J mol−1 K−1)
- C v,ads,i :
-
molar specific heat of component i in the adsorbed phase at constant volume (J mol−1 K−1)
- C v,i :
-
molar specific heat of component i at constant volume (J mol−1 K−1)
- d p :
-
adsorbent particle diameter (m)
- d wi :
-
internal bed diameter (m)
- D ax :
-
axial dispersion coefficient (m2 s−1)
- D c,i :
-
micropore diffusivity of component i (m2 s−1)
- D p,i :
-
macropore diffusivity of component i (m2 s−1)
- h f :
-
film heat transfer coefficient between the gas and particle (J s−1 m−2 K−1 )
- h w :
-
film heat transfer coefficient between the gas and wall (J s−1 m−2 K−1 )
- k f :
-
film mass transfer coefficient (m s−1)
- K ∞ :
-
adsorption constant at infinite temperature (mol kg−1 bar−1)
- K H :
-
Henry constant (mol kg−1 bar−1)
- P :
-
pressure (Pa)
- \(\overline{q_{i}}\) :
-
average adsorbed phase concentration of component i (mol kg−1)
- \(q_{i}^{*}\) :
-
adsorbed concentration of component i in equilibrium with \(\overline{C_{p,i}}\) (mol kg−1)
- r c :
-
“microparticle” radius (m)
- R g :
-
ideal gas constant (J mol−1 K−1)
- R p :
-
adsorbent particle radius (m)
- t :
-
time (s)
- T g :
-
bulk phase temperature (K)
- T p :
-
solid temperature (K)
- T w :
-
wall temperature (K)
- u 0 :
-
superficial velocity (m s−1)
- y i :
-
gas phase molar fraction of component i (–)
- z :
-
axial position (m)
- α w :
-
ratio of the internal surface area to the volume of the column wall (m−1)
- (ΔH ads) i :
-
heat of adsorption of component i (J mol−1)
- ε :
-
bed porosity (–)
- ε p :
-
particle porosity (–)
- λ :
-
heat axial dispersion coefficient (J s−1 m−1 K−1)
- μ :
-
bulk gas mixture viscosity (kg m−1 s−1)
- ρ :
-
bulk gas mixture density (kg m−3)
- ρ b :
-
bed density (kg m−3)
- ρ p :
-
particle density (kg m−3)
- ρ w :
-
wall density (kg m−3)
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Ribeiro, A.M., Santos, J.C. & Rodrigues, A.E. Pressure swing adsorption for CO2 capture in Fischer-Tropsch fuels production from biomass. Adsorption 17, 443–452 (2011). https://doi.org/10.1007/s10450-010-9280-8
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DOI: https://doi.org/10.1007/s10450-010-9280-8