# CFD Simulation for Separation of Carbon Dioxide-Methane Mixture by Pressure Swing Adsorption

Authors: K. Rambabu; L. Muruganandam; S. Velu
Journal: International Journal of Chemical Engineering
 (2014)

---

## Abstract

A developing technology for gas separations is pressure swing adsorption, which has been proven to be more economical and energy efficient compared to other separation methods like cryogenic distillation and membrane separation. A pressure swing adsorption (PSA) column, with carbon dioxide-methane as feed mixture and 6-FDA based polyimides as the adsorbent, was modeled and simulated in this work. Ansys Fluent 12.1, along with supplementary user defined functions, was used to develop a 2D transient Eulerian laminar viscous flow model for the PSA column. The model was validated by comparing the simulated results with established analytical models for PSA. The developed numerical model was used to determine the carbon dioxide concentration in the column as a function of time based on different operating conditions. Effect of various operating parameters like pressure, temperature, and flow rate on the separation efficiency has been studied and reported. Optimization studies were carried out to obtain suitable operating conditions for the feed gases separation. Simulation studies were carried out to determine the separation length required for complete separation of the feed mixture corresponding to different inlet feed concentrations which were entering the column at a given flow rate.


---

## Body

## 1. Introduction

Traditionally, industrial gas separation is done by chemical and physical absorption, membrane separation, and low temperature distillation [1]. Owing to high energy consumption and associated problems like cost and process degradation, newer avenues are being explored. With different kinds of adsorbents available, each offering a wide range of equilibrium properties, adsorption is being seen as a viable option for gas separation, especially for binary gas mixtures [2]. Separation processes utilizing adsorption are low cost and energy efficient alternatives in comparison with other separation processes particularly at low to moderate throughput [3].Adsorption is mainly performed by periodic variations of pressure and temperature of the system. Temperature swing adsorption (TSA) is widely used for removal of trace amounts of pollutants such as volatile organic compounds from gaseous streams [4]. However, TSA needs precise process controls, huge columns, and longer operating time compared to pressure swing adsorption (PSA) and hence, TSA is preferred for systems having strong adsorbing nature with respect to the adsorbent [5].Pressure swing adsorption is based on Skarstrom cycle [6] in which feed mixture is sent in at high pressures. Separation takes place due to selective adsorption of one or more feed components by the adsorbent and the rate of adsorption is regulated by the operating pressure of the process. The adsorbed component (adsorbate) is recovered later by reducing the pressure of the column. Adsorption involves contacting a free fluid phase (gas or liquid) with a rigid particulate phase which has the property of selectively taking up and storing one or more solute species originally contained in the fluid [7]. The strength of the surface interaction between the adsorbent and adsorbate depends on the nature of the solid adsorbent, the fluid adsorbate, and the system’s thermodynamic properties, especially density and pressure.Consequently, different adsorbents adsorb feed components with different affinities which are regulated by the thermodynamics of the system. This gives raise to the wide range of processes in PSA processes with respect to the adsorbent used.Two separations of particular commercial interest that have been mostly reported in the literature are the carbon dioxide-methane (CO2-CH4) separation and oxygen-air separation. Separation of oxygen from air by PSA using zeolite 5A as adsorbent has been studied experimentally [8, 9]. Modelling of the oxygen separation from air by PSA using 13X zeolite as adsorbent has been carried out by equilibrium model with a linear isotherm for oxygen and a polynomial isotherm for nitrogen [10]. Experimental studies on the separation of the carbon dioxide-methane system using membrane technology have been reported in scientific literature [11]. Simulation study on the effect of gas solubility in the adsorbent with respect to feed mixture separation is also made for CO2-CH4 system using PSA [12]. However, the effect of operating parameters on the separation efficiency of the system has not been explored so far.Removal of carbon dioxide from natural gas is extremely important in order to meet the transportation pipeline specifications as well as produce natural gas from associated gas dug out from oil wells [11, 13]. The most common adsorbents used in PSA separation processes for carbon dioxide-methane system are inorganic adsorbents like zeolite, activated charcoal, and polymer adsorbents like polysulfone and polyacetate. The 6-FDA based polyimides have been reported to be a promising adsorbent material for gas separation [14]. The hexafluoroisopropylidene linkage in the polyimides enhances the permselectivity of the 6-FDA based polyimides for the binary systems [15]. Polyimides also show excellent mechanical strength as well as temperature and chemical resistance [16].In this study, the separation process of CO2-CH4 system was modeled based on dynamic pressure-swing adsorption process with FDA based polyimides particles as adsorbent. CFD package, Ansys Fluent 12.1, along with supplementary user defined functions was used to develop a 2D transient Eulerian laminar viscous flow model for the adsorption column. The objective of the investigation was to simulate the developed numerical model to study the individual feed component’s concentration distribution and separation efficiency with respect to time and column operating parameters.


## 2. Process Modelling

### 2.1. Model Setup and Analysis

A typical model of the PSA adsorption column is shown in Figure1. The model was developed and simulated using Ansys Fluent 12.1. The details of the adsorption column model were taken as used in earlier related work [12] and are shown in Table 1. The fluid was taken to be incompressible, Newtonian, and in a laminar flow regime. Carbon dioxide-methane system at standard conditions was chosen as the feed mixture in a 50%-50% volume concentration. The porous medium approach was used in the simulation of the fluid flow in the packed bed since the adsorbent inside the packed bed can be treated as porous medium. The porous medium is assumed to be isotropic. The approach uses an additional mass source term to the standard fluid flow equations to account for the flow resistance due to the porous medium. The mixing and transport of binary species are modeled by solving conservation equations describing convection and diffusion for each component species. The following assumptions have been made in the modelling approach.(i)
The process is assumed to be isothermal.
(ii)
Ideal gas law is applicable.
(iii)
Plug flow is assumed; that is, there is no axial or radial dispersion.
(iv)
The mass transfer rate is given by linear driving force (LDF) model.Table 1
Parameters used in separation of binary gas mixtures.
Molar feed composition
CO2-CH4 (50%-50% by volume)
Adsorbent
Polyimide (6FDA-ODA)
Particle radius,μm
100
Bed length, m
0.35
Bed diameter, m
0.06
Bed voidage
0.5
Operating temperature, K
300
Operating pressure, atm
20
Glass transition temperature
~450 KFigure 1
Schematic of the PSA column model with feed inlet and outlet.User defined functions were introduced to incorporate source terms in order to include the effects of solubility and diffusivity. The effect of temperature on permeability was incorporated in the source term by (1) using the data given in Table 2 [17]. PISO scheme was used as the pressure velocity coupling algorithm. The governing equation for fluid flow in isotropic porous media is given by (2). Incorporating the source term, S
∅, in (2) would enable to define concentration points of adsorbed gas. Thus, the mass and momentum conservation equations for the discussed model are given by (3) and (4), respectively. Inertial and viscous resistance encountered by the fluid are incorporated in the model by the last two terms. Permeability (α) is calculated using Darcy’s law (see equation (5)) due to the presence of porous media. The linear driving force model describing the mass transfer phenomena for PSA is given by (6) and (7). The governing equations were discretized by second-order upwind scheme:
(1)
P
=
λ
o
exp
⁡
(
E
P
R
T
)
,
(2)
∂
(
γ
ρ
Φ
)
∂
t
+
∇
•
(
γ
ρ
V
→
Φ
)
=
∇
•
(
γ
Γ
∇
Φ
)
+
γ
S
Φ
,
(3)
∂
(
γ
ρ
)
∂
t
+
∇
•
(
γ
ρ
V
→
)
±
∇
•
(
ε
D
p
,
i
∇
•
(
γ
ρ
)
)
=
0
,
(4)
∂
(
γ
ρ
V
→
)
∂
t
+
∇
•
(
γ
ρ
V
→
V
→
)
=
-
γ
∇
P
+
∇
•
(
γ
τ
→
)
+
γ
B
f
⟶
-
(
μ
α
+
C
2
ρ
2
|
V
|
→
)
V
→
,
(5)
α
=
d
p
2
ε
3
150
(
1
-
ε
)
2
,
(6)
∂
q
i
∂
t
=
k
i
(
q
i
*
-
q
i
)
,
(7)
k
i
=
60
D
p
,
i
d
p
2
.Table 2
Activation energies for permeation for 6-FDA based membranes at 35°C and 20 atm.
CO2
CH4
Kinetic diameter(
Å
)
3.30
3.80
λ
0 (Barrer)
17.25
0.20
E
p (kcal/mol)
4.74
0.92


### 2.2. Model Validation

The adsorption of small molecules in glassy polymers is described best by the dual mode (DM) sorption model [18, 19]. The dual sorption mechanism is given as a combination of Henry’s law of solubility and Langmuir adsorption [18]. Henry’s law accounts for the dissolution of the penetrant molecule in the continuous polymer chain matrix and its sorption in microvoids is described by Langmuir model. According to DM sorption model, the gas concentration in the polymer is given by the following equation as a function of operating pressure:
(8)
C
=
C
D
+
C
H
=
k
D
p
+
C
H
′
b
p
(
1
+
b
p
)
,
where C is the concentration of the gas adsorbed in unit volume of the polymer, C
D is the gas concentration by dissolution, C
H is the gas concentration by hole filling, p is the applied pressure, k
D is dissolution constant, C
H
′ is the hole saturation constant, and b is the affinity constant.DM model assumes that both modes occur simultaneously and are always in equilibrium [18, 20]. The diffusion coefficient is independent of concentration. The values of the parameters for the DM sorption model for carbon dioxide sorbed in polyimide are specified in Table 3 [21].Table 3
DM sorption model parameters for carbon dioxide sorbed in polyimide.
k
D (cm3 of CO2/cm3 of adsorbent bar)
1.56
C
H
′ (cm3 of CO2/cm3 of adsorbent)
54.6
b (bar−1)
0.544Validation of the numerical model was conducted by studying the steady state adsorbed CO2 concentration as a function of operating pressure and comparing with the CO2 concentration obtained using analytical DM model. As shown in Figure 2, the behaviour of the numerical model is in accordance with the analytical DM sorption model. The variation in the amount of CO2 adsorbed per unit volume of adsorbent between the DM model and numerical model reported an average error of 8.7% (in magnitude), calculated over the operating pressure for the adsorption column. The error between the DM model and the proposed numerical model could be due to the truncation, discretization, and round-off phenomena in the simulation. The deviation between numerical model and the DM model was very much less in comparison to the deviation between Langmuir model and the DM model (average error of 42.5%) and the deviation between Henry model and the DM model (average error of 34.9%).Figure 2
Comparison of DM model and numerical model.


### 2.3. Simulation

Carbon dioxide-methane mixture at a volume composition of 50%-50% was given as the inlet feed stream. At the end of the cycle the mole fraction of carbon dioxide was reduced to 0.05 from 0.5 due to the adsorption of carbon dioxide in the column. The result of the unsteady state simulation is presented in Figure3. It is evident from Figure 3 that the concentration of methane at a given spatial position increased with time of adsorption. It was also evident that the rate of adsorption at a given point in the column decreased with the time of adsorption. This was due to the decreasing concentration gradient between the feed stream and the adsorbent material.Figure 3
Concentration of methane as a function of time.


#### 2.3.1. Effect of Pressure

Simulation results showed that decreasing the operating pressure leads to better separation. As shown in Figure4, the separation ratio (ratio of concentration of CO2 to concentration of CH4) decreased along the length of the column as pressure was reduced from 15 atm to 1 atm.Figure 4
Pressure effects on separation ratio (flow velocity = 0.15 m/sec and temperature = 200 K).


#### 2.3.2. Effect of Temperature

For most gases, solubility increases with increase in temperature till the glass transition temperature is reached. Simulations were carried out at 200 K, 300 K, and 400 K keeping the pressure constant. It was observed that separation increases with increase in temperature. The temperature effect on the adsorption is shown in Figure5.Figure 5
Temperature effects on separation ratio (flow velocity = 0.15 m/sec and pressure = 15 atm).


#### 2.3.3. Effect of Flowrate

Flowrate of the feed stream is an important factor affecting the separation process. The model was simulated for three different flow rates—0.1 m/s, 0.01 m/s, and 0.001 m/s. The highest degree of separation was obtained at 0.001 m/s, as evident from Figure6.Figure 6
Effect of feed velocity on the separation ratio (pressure = 5 atm and temperature = 200 K).


### 2.4. Optimization

The optimum operating conditions for carrying out the pressure swing adsorption for the separation of carbon dioxide-methane mixture at a volume composition of 50%-50% entering the column at a velocity of 0.001 m/s was obtained by simulating the model at different operating pressures and temperatures. Pressure was reduced from 20 atm to 1 atm and the temperature dependence study was performed for 200 K, 300 K, and 400 K. For every run, the separation ratio was calculated and plotted to find the optimum conditions for operating the PSA column. The results are presented in Figure7. The optimization study revealed that a separation length of about 0.125 m guaranteed 100% separation for the specified feed inlet conditions. Optimum operating conditions were found to be 1 atm and 400 K.Figure 7
Optimization studies on separation ratio on operation conditions (feed velocity = 0.001 m/s).Further, as a comparative study, simulations were carried out to determine the separation length required for complete separation of the feed corresponding to different initial concentrations of the feed mixture. The results obtained are presented in Table4.Table 4
Dependence studies of separation length on initial concentration of feed.
Position of the column (m)
Concentration of CO2 (kmol/m
3
L
L
L) along the column length for different initial concentrations of feed mixture
95% CO2 in feed
85% CO2 in feed
75% CO2 in feed
65% CO2 in feed
55% CO2 in feed
45% CO2 in feed
35% CO2 in feed
25% CO2 in feed
15% CO2 in feed
5% CO2 in feed
0.306
0
0
0
0
0
0
0
0
0
0
0.253
0
0
0
0
0
0
0
0
0
0
0.201
0
0
0
0
0
0
0
0
0
0
0.157
0.000481
0
0
0
0
0
0
0
0
0
0.105
0.080044
0.053567
0.02707
0.005331
0
0
0
0
0
0
0.052
0.419499
0.345991
0.277279
0.212829
0.152186
0.09501
0.0409
0.001032
0
0
0.017
1.49493
1.15133
0.88624
0.675398
0.503622
0.36095
0.24045
0.137306
0.047937
0.00695As a future scope of study for the pressure swing adsorption using 6-FDA-ODA particles bed, a more improved model (3-dimensional) incorporating most of the real time correlations, radial variation studies and temperature dependence studies for the adsorption process are to be carried out.


## 2.1. Model Setup and Analysis

A typical model of the PSA adsorption column is shown in Figure1. The model was developed and simulated using Ansys Fluent 12.1. The details of the adsorption column model were taken as used in earlier related work [12] and are shown in Table 1. The fluid was taken to be incompressible, Newtonian, and in a laminar flow regime. Carbon dioxide-methane system at standard conditions was chosen as the feed mixture in a 50%-50% volume concentration. The porous medium approach was used in the simulation of the fluid flow in the packed bed since the adsorbent inside the packed bed can be treated as porous medium. The porous medium is assumed to be isotropic. The approach uses an additional mass source term to the standard fluid flow equations to account for the flow resistance due to the porous medium. The mixing and transport of binary species are modeled by solving conservation equations describing convection and diffusion for each component species. The following assumptions have been made in the modelling approach.(i)
The process is assumed to be isothermal.
(ii)
Ideal gas law is applicable.
(iii)
Plug flow is assumed; that is, there is no axial or radial dispersion.
(iv)
The mass transfer rate is given by linear driving force (LDF) model.Table 1
Parameters used in separation of binary gas mixtures.
Molar feed composition
CO2-CH4 (50%-50% by volume)
Adsorbent
Polyimide (6FDA-ODA)
Particle radius,μm
100
Bed length, m
0.35
Bed diameter, m
0.06
Bed voidage
0.5
Operating temperature, K
300
Operating pressure, atm
20
Glass transition temperature
~450 KFigure 1
Schematic of the PSA column model with feed inlet and outlet.User defined functions were introduced to incorporate source terms in order to include the effects of solubility and diffusivity. The effect of temperature on permeability was incorporated in the source term by (1) using the data given in Table 2 [17]. PISO scheme was used as the pressure velocity coupling algorithm. The governing equation for fluid flow in isotropic porous media is given by (2). Incorporating the source term, S
∅, in (2) would enable to define concentration points of adsorbed gas. Thus, the mass and momentum conservation equations for the discussed model are given by (3) and (4), respectively. Inertial and viscous resistance encountered by the fluid are incorporated in the model by the last two terms. Permeability (α) is calculated using Darcy’s law (see equation (5)) due to the presence of porous media. The linear driving force model describing the mass transfer phenomena for PSA is given by (6) and (7). The governing equations were discretized by second-order upwind scheme:
(1)
P
=
λ
o
exp
⁡
(
E
P
R
T
)
,
(2)
∂
(
γ
ρ
Φ
)
∂
t
+
∇
•
(
γ
ρ
V
→
Φ
)
=
∇
•
(
γ
Γ
∇
Φ
)
+
γ
S
Φ
,
(3)
∂
(
γ
ρ
)
∂
t
+
∇
•
(
γ
ρ
V
→
)
±
∇
•
(
ε
D
p
,
i
∇
•
(
γ
ρ
)
)
=
0
,
(4)
∂
(
γ
ρ
V
→
)
∂
t
+
∇
•
(
γ
ρ
V
→
V
→
)
=
-
γ
∇
P
+
∇
•
(
γ
τ
→
)
+
γ
B
f
⟶
-
(
μ
α
+
C
2
ρ
2
|
V
|
→
)
V
→
,
(5)
α
=
d
p
2
ε
3
150
(
1
-
ε
)
2
,
(6)
∂
q
i
∂
t
=
k
i
(
q
i
*
-
q
i
)
,
(7)
k
i
=
60
D
p
,
i
d
p
2
.Table 2
Activation energies for permeation for 6-FDA based membranes at 35°C and 20 atm.
CO2
CH4
Kinetic diameter(
Å
)
3.30
3.80
λ
0 (Barrer)
17.25
0.20
E
p (kcal/mol)
4.74
0.92


## 2.2. Model Validation

The adsorption of small molecules in glassy polymers is described best by the dual mode (DM) sorption model [18, 19]. The dual sorption mechanism is given as a combination of Henry’s law of solubility and Langmuir adsorption [18]. Henry’s law accounts for the dissolution of the penetrant molecule in the continuous polymer chain matrix and its sorption in microvoids is described by Langmuir model. According to DM sorption model, the gas concentration in the polymer is given by the following equation as a function of operating pressure:
(8)
C
=
C
D
+
C
H
=
k
D
p
+
C
H
′
b
p
(
1
+
b
p
)
,
where C is the concentration of the gas adsorbed in unit volume of the polymer, C
D is the gas concentration by dissolution, C
H is the gas concentration by hole filling, p is the applied pressure, k
D is dissolution constant, C
H
′ is the hole saturation constant, and b is the affinity constant.DM model assumes that both modes occur simultaneously and are always in equilibrium [18, 20]. The diffusion coefficient is independent of concentration. The values of the parameters for the DM sorption model for carbon dioxide sorbed in polyimide are specified in Table 3 [21].Table 3
DM sorption model parameters for carbon dioxide sorbed in polyimide.
k
D (cm3 of CO2/cm3 of adsorbent bar)
1.56
C
H
′ (cm3 of CO2/cm3 of adsorbent)
54.6
b (bar−1)
0.544Validation of the numerical model was conducted by studying the steady state adsorbed CO2 concentration as a function of operating pressure and comparing with the CO2 concentration obtained using analytical DM model. As shown in Figure 2, the behaviour of the numerical model is in accordance with the analytical DM sorption model. The variation in the amount of CO2 adsorbed per unit volume of adsorbent between the DM model and numerical model reported an average error of 8.7% (in magnitude), calculated over the operating pressure for the adsorption column. The error between the DM model and the proposed numerical model could be due to the truncation, discretization, and round-off phenomena in the simulation. The deviation between numerical model and the DM model was very much less in comparison to the deviation between Langmuir model and the DM model (average error of 42.5%) and the deviation between Henry model and the DM model (average error of 34.9%).Figure 2
Comparison of DM model and numerical model.


## 2.3. Simulation

Carbon dioxide-methane mixture at a volume composition of 50%-50% was given as the inlet feed stream. At the end of the cycle the mole fraction of carbon dioxide was reduced to 0.05 from 0.5 due to the adsorption of carbon dioxide in the column. The result of the unsteady state simulation is presented in Figure3. It is evident from Figure 3 that the concentration of methane at a given spatial position increased with time of adsorption. It was also evident that the rate of adsorption at a given point in the column decreased with the time of adsorption. This was due to the decreasing concentration gradient between the feed stream and the adsorbent material.Figure 3
Concentration of methane as a function of time.


### 2.3.1. Effect of Pressure

Simulation results showed that decreasing the operating pressure leads to better separation. As shown in Figure4, the separation ratio (ratio of concentration of CO2 to concentration of CH4) decreased along the length of the column as pressure was reduced from 15 atm to 1 atm.Figure 4
Pressure effects on separation ratio (flow velocity = 0.15 m/sec and temperature = 200 K).


### 2.3.2. Effect of Temperature

For most gases, solubility increases with increase in temperature till the glass transition temperature is reached. Simulations were carried out at 200 K, 300 K, and 400 K keeping the pressure constant. It was observed that separation increases with increase in temperature. The temperature effect on the adsorption is shown in Figure5.Figure 5
Temperature effects on separation ratio (flow velocity = 0.15 m/sec and pressure = 15 atm).


### 2.3.3. Effect of Flowrate

Flowrate of the feed stream is an important factor affecting the separation process. The model was simulated for three different flow rates—0.1 m/s, 0.01 m/s, and 0.001 m/s. The highest degree of separation was obtained at 0.001 m/s, as evident from Figure6.Figure 6
Effect of feed velocity on the separation ratio (pressure = 5 atm and temperature = 200 K).


## 2.3.1. Effect of Pressure

Simulation results showed that decreasing the operating pressure leads to better separation. As shown in Figure4, the separation ratio (ratio of concentration of CO2 to concentration of CH4) decreased along the length of the column as pressure was reduced from 15 atm to 1 atm.Figure 4
Pressure effects on separation ratio (flow velocity = 0.15 m/sec and temperature = 200 K).


## 2.3.2. Effect of Temperature

For most gases, solubility increases with increase in temperature till the glass transition temperature is reached. Simulations were carried out at 200 K, 300 K, and 400 K keeping the pressure constant. It was observed that separation increases with increase in temperature. The temperature effect on the adsorption is shown in Figure5.Figure 5
Temperature effects on separation ratio (flow velocity = 0.15 m/sec and pressure = 15 atm).


## 2.3.3. Effect of Flowrate

Flowrate of the feed stream is an important factor affecting the separation process. The model was simulated for three different flow rates—0.1 m/s, 0.01 m/s, and 0.001 m/s. The highest degree of separation was obtained at 0.001 m/s, as evident from Figure6.Figure 6
Effect of feed velocity on the separation ratio (pressure = 5 atm and temperature = 200 K).


## 2.4. Optimization

The optimum operating conditions for carrying out the pressure swing adsorption for the separation of carbon dioxide-methane mixture at a volume composition of 50%-50% entering the column at a velocity of 0.001 m/s was obtained by simulating the model at different operating pressures and temperatures. Pressure was reduced from 20 atm to 1 atm and the temperature dependence study was performed for 200 K, 300 K, and 400 K. For every run, the separation ratio was calculated and plotted to find the optimum conditions for operating the PSA column. The results are presented in Figure7. The optimization study revealed that a separation length of about 0.125 m guaranteed 100% separation for the specified feed inlet conditions. Optimum operating conditions were found to be 1 atm and 400 K.Figure 7
Optimization studies on separation ratio on operation conditions (feed velocity = 0.001 m/s).Further, as a comparative study, simulations were carried out to determine the separation length required for complete separation of the feed corresponding to different initial concentrations of the feed mixture. The results obtained are presented in Table4.Table 4
Dependence studies of separation length on initial concentration of feed.
Position of the column (m)
Concentration of CO2 (kmol/m
3
L
L
L) along the column length for different initial concentrations of feed mixture
95% CO2 in feed
85% CO2 in feed
75% CO2 in feed
65% CO2 in feed
55% CO2 in feed
45% CO2 in feed
35% CO2 in feed
25% CO2 in feed
15% CO2 in feed
5% CO2 in feed
0.306
0
0
0
0
0
0
0
0
0
0
0.253
0
0
0
0
0
0
0
0
0
0
0.201
0
0
0
0
0
0
0
0
0
0
0.157
0.000481
0
0
0
0
0
0
0
0
0
0.105
0.080044
0.053567
0.02707
0.005331
0
0
0
0
0
0
0.052
0.419499
0.345991
0.277279
0.212829
0.152186
0.09501
0.0409
0.001032
0
0
0.017
1.49493
1.15133
0.88624
0.675398
0.503622
0.36095
0.24045
0.137306
0.047937
0.00695As a future scope of study for the pressure swing adsorption using 6-FDA-ODA particles bed, a more improved model (3-dimensional) incorporating most of the real time correlations, radial variation studies and temperature dependence studies for the adsorption process are to be carried out.


## 3. Conclusions

A CFD model based on pressure swing adsorption was developed for binary gas mixture separation, namely, CO2-CH4, using 6-FDA based polyimides as adsorbent. The model was validated against the analytical dual mode sorption model for adsorption of gases (CO2) on glassy polymers. The model was used to determine the carbon dioxide concentration in the column as a function of time based on different operating conditions. Analysis clearly indicated that providing an optimal residence time by lowering the velocity of the flow produces the maximum separation efficiency. For a fixed column length of 0.035 m, an optimal residence time of 50 seconds corresponding to a flow velocity of 0.001 m/s yielded a separation efficiency of around 97%. Lowering the operating pressure leads to better separation as permeability of gases is inversely proportional to the operating pressure. Increasing the temperature of the adsorption bed produced better separation of the gases. As an outcome of optimization studies, a reference table specifying the separation length required for complete separation of the feed mixture entering the adsorption column at different initial concentrations (with a flow velocity of 0.001 m/s) was also presented.



---

*Source: 402756-2014-06-19.xml*