HUNGARIAN JOURNAL 
OF INDUS1RIAL CHEMISTRY 

VESZPREM 
Vol. 30. pp. 103- 105 (2002) 

ON THE PURIFICATION OF GASES CONTAINING IMPURITIES OF SMALL 
CONCENTRATION 

C. BOY ADJIEV 

(Bulgarian Academy of Sciences, Institute of Chemical Engineering, "Acad. G.Bontchev" str.,Bl.l03, 1113 Sofia, 
BULGARIA) 

Received: November 05, 2001 

A theoretical analysis was made of the methods used for the purification of gas, containing impurities of small 
concentrations. A comparison is proposed between absorption and adsorption methods. It is shown that adsorption 
processes are more advantageous in these cases. 

Keywords: gas purification, absorption, adsorption, comparative analysis 

Introduction 

Numerous ecology problems are related to the 
purification of air from its impurities.~ The main problem 
occurred in the case, when the concentration of the 
impurity is really small. In these cases absorption in a 
packed column is frequently used. A high absorption 
rate should be realized by a suitable chemical reaction 
between the gas impurity and a liquid absorbent. In 
reality, the absorption rate is usually very small and as a 
result, a very high absorption column has to be applied, 
to reach the expected efficiency. 

Absorption 

If a gas of Q(m3 Is) flow rate has to be purified from its 
impurity with concentration of C (kg I m3 gas) in a 
packed column (diameter d (m) and a height of the 
active zone h (m), height of the packing). 

The concentration of the impurity (an active 
component of the gas) is equal to zero as result of the 
chemical reaction between this component and the 
absorbent. In this case the concentration difference in 
the equation of the mass transfer rate is equal to C . The 
concentration difference is changing along the active 
zone height. Thus, it should be used the average value 

of the concentration difference ilC(kg / m3 gas}: 

Contact information: E-mail: chboyadj @bas.bg 

.tlC (1) 

where 

C1 and C2 (kg I m3 gas) are the inlet and exit 
concentrations of the active component in two ends of 
the active zone. 

The chemisorption rate in the column is J (kg/ s) 
and the volumetric chemisorption rate is 

j (kg I s.m3 active zone). 
If u (m/ s), V {m3 ) are the gas velocity and active 

zone volume, then: 

7Td2 
V = S.h, Q = S.u, S == --. (2) 

4 

If k (m3 gas/ s.m3 actve zone} is the volumetric mass 
transfer coefficient and 

ks (m3 gas/ s.m2 mass transferswface) is the surface 
mass transfer coefficient, the chemisorption rate 
equation has the following form: 

(3) 

where 

s(m2 masstransfersuiface/m3 actvezone) is the 
specific mass transfer surface in the active zone. 

Eq.( 3) shows that if the volume concentration of the 
active component is small and the diameter of the 



104 

Table 1 Comparison between the absorption and the adsorption: 

Q=0.4m%ec, C=0.01kg/m3, 1J.==99% 
.N2 Parameters 

1 The gas velocity, u {Jnjs) 
2The column section, s (m~) 
3The column diameter, d (m) 
4The volume mass transfer coefficient, k (s-1 ) 
5The active zone volume, v (m1 ) 
6The active zone height, h (m) 
7The relative decreasing of the volume, A V Vn 3 ) 
8The relative increasing of the height, M (m) 

9The stoichiometric quantity of a liquid phase, l (m 3 Is) 
1 OThe real quantity a liquid phase, L (m 3 j s) 
11 The relative increasing of the liquid phase .AL (m 3 Is) 
12The relative increasing of the consummations for the liquid phase, I1E 
13The pressure drops, !J.rp mm H

2
0 

column is constant, the increasing rate of chemisorption 
is a result of the active zone height increase or the 
increase of the volume mass transfer coefficient: 

(4) 

Under the chemisorption conditions, when the gas 
velocity and chemical reaction rate are constant, the 
mass transfer coefficient does not change significantly. 
Thus, from Eq.(4) follows that the increase of the input 
concentration C1 (respectively AC) needs the increase 

of the specific mass transfer surface, s . 
The specific active surface in packed columns is 

limited by the specific surface of the packing. As a 
result. it is not possible to i'ncrease the volumetric mass 
transfer coefficient, i.e. for increasing of the column 
height. This shows that it is better to use adsorption 
process for gas purification because its specific mass 
transfer surface is significantly greater compared to 
packed columns. 

The chemisorption in the active zone may be 
realized by means of absorption in a packed column 

(s=l02 m2/m 3 ) or by the adsorption of a synthetic 
adsorbent (s= 108 m2 /m 3 ) .. because the ratio of the 
volumetric mass transfer coefficients of the adsorption 

and absorption is 10
4

• 

The experimental data for volumetric mass transfer 
coefficient in the case the sa}. adsorption by synthetic 
anionite shows that 

k = 12.1 u m3 gas/ s.m3 active zone. {S) 
The experimental data for the gas absorption in the 

packed column [4] show that the volumetric mass 
transfer coefficient in gas phase for Raschig rings 
(502t50x2)mm is 

k = l.4kg/m 3 .bar.s. {6} 

Adsorption 

0.7 

0.57 

0.85 

8.5 

0.046 

0.081 

25 

3.3 w-s 
3.3 w-s 

1 
80 

0.1 

4 

2.25 

1.2 

0.32 

0.081 

1 

25 

3.3 to·5 

3.3 w·s 
1 

1 
24 

Absorption 
1 

0.4 

0.71 

0.5 

0.79 

2 

25 

3.3 w-s 
6710"5 

20 

500 

24 

if the gas velocity is 1 m/ s and the liquid flow rate is 
6m3/m

2
h. 

From (6) it is immediately obtained, that: 

k = 0.5 m 3 gas/ s.m3 active zone. (7) 

These data allow possibility to make a comparative 
analysis on the absorption and adsorption, on the basis 
of the next example (Table 1.). 

Let to purify airflow of Q = 0.4m3 /s with 
concentration of 802 C =0.0lkgjm

3 with 11 =99%. 
Efficiency. The values of the process parameters of 
chemisorption under the absorption and adsorption 
conditions are shown in the Table 1. The results in the 
Table show that an increase of the volume AV and M 
in the case of absorption, compared to the adsorption. 

In the Table 1 the stoichiometric quantity of the 

liquid phase l (m 3 Is) 200 g /l Na2 co3 is obtained 
immediately. The real quantities of the liquid phase 

L~n3 / s) are obtained immediately under the adsorption 
condition L = l from the liquid flow rate under an . 
absorption condition. The relative increase of the liquid 
flow rate in the case of absorption compared to the 
absorption condition M can be obtained immediately. 
The consummations of the liquid phase movement are 
linear function of the liquid flow rate L and the active 
zone height. h. As a result. the consummation of the 
relative increase AE is /J.L : M = AL.Ah . 

Raschig rings (50x50x5) mm are used for the 
pressure drops comparison. The second adsorption data 
are valid in the case of lower gas velocity (u = 0.1 m/ s). 

Conclusions 

The obtained results show that the adsorption process is 
significantly more effective for gas purification 
compared to the absorption, when the concentration 
impurities are small. 



In these conditions the saturation of the adsorbent is 
very slow and this is another cause for a real use of 
adsorption processes for solving ecology problems. 

SYMBOLS 

C concentration, (kg/ m3 gas) 

C1, C2 input and output concentration of the active 

component, (kg/ m3 gas) 

A.C average value of the concentration difference, 

(kg/m 3 gas) 

d column diameter, (m) 
DE relative increasing of the consummations for 

liquid phase, 
h column height, (m) 
A.h increasing of the column height, (m) 
1 chemisorption rate, (kg/ s) 
j 

k 

volume chemisorption rate, 

(kg/ s.m3 active zone) 

volume mass transfer coefficient, 

(m3 gas/ s.m3 active zone) 
surface mass transfer 

coefficient, 

(m3 gas/ s.m2 mass transfer surface) 

L 

u 

Q 
s 

u 

v 
A.V 

1] 

8.cp 

105 

stoichiometric quantity of the liquid phase, 

(m 3 /s) 
real quantity of the liquid phase, (m 3 /s) 
relative increasing of the liquid flow rate, 

(m3 /s) 
gas flow rate, (m 3 / s) 

specific mass transfer surface, 

(m 2 mass transfer surface/ m 3 active zone) 

gas velocity, (m/ s) 
active zone volume, (m3 ) 

increasing active zone volume, (m3 ) 

purification degree, (%) 
pressure drops, mm H 20 

REFERENCES 

1. L. PANTOVCHIEV A and CHR. BOY ADJIEV: Bulg. 
Chern. Commun., 1995, 28, .N2 %, 780-794 

2. CHR. BOYADJIEV, L. PANTOVCHIEVA and J. 
CHRISTOV: Theor. Found. Chern. Eng., 2000, 34, 2, 
141-144 

3. J. CHRISTOV, CHR. BOYADJIEV and L. 
PANTOFCHIEVA; Theor. Found. Chern. Eng., 2000, 
34, 5, 439-443 

4. V. M. RAMM: Gas Absorption, Chemistry, Moscow, 
1976 


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