Adsorption rate characteristics of methane and CO
2
in coal samples
from Raniganj and Jharia coalfields of India
Santanu Bhowmik
a,
⁎, Pratik Dutta
b
a
Department of Geoscience, University of Calgary, 2500 University Drive NW, Calgary, Alberta, Canada T2N 1N4
b
Bengal Engineering and Science University, Shibpur, P.O. Botanic Garden, Howrah - 711103, West Bengal, India
abstract article info
Article history:
Received 9 November 2012
Received in revised form 3 February 2013
Accepted 6 February 2013
Available online 16 February 2013
Keywords:
Coalbed methane
Adsorption rate characteristics
Diffusion
Pressure-dependency
Pore diffusion model
Linear approximation of unipore model
A set of six sub-bituminous to high-volatile bituminous coal samples was chosen to analyze the adsorption rate
during the isotherm tests. The isotherm tests were conducted at 30 °C on dry, powdered coal samples up to a max-
imum experimental pressure of ~ 8 MPa and ~ 6.5 MPa for methane and CO2, respectively. It was observed that the
rate of adsorption for CO2 is higher than that for methane for the same experimental pressure–temperature con-
dition and, for a particular pressure step, the equilibrium was reached earlier for CO2 compared to methane. It was
also observed that at an increased pressure range, the rates of adsorption and the diffusion were generally
decreased. The experimental data were fitted to unipore diffusion model but this model failed to predict the
experimental adsorption kinetics data for the entire time range. However, the modification of unipore model, as
suggested by Mianowski and Marecka (2009), was able to satisfactorily predict the experimental kinetics data at
various pressure stages for the entire time range with the introduction of a kinetic parameter, C, accounting for
the effect of gas diffusivity. The adsorption kinetics data was “unusable” at the initial time range due to variation
in temperature–pressure in the sample cell after gas was injected. It was also observed that this “unusable” data
is small at lower pressure range (~15 s), but could be significant (~30–50 s) at higher-pressure range.
© 2013 Elsevier B.V. All rights reserved.
1. Introduction
It is well known that gas production from a coalbed methane (CBM)
reservoir is a combined process of desorption, diffusion and Darcy flow.
So, the success of a CBM operation depends on the gas storage in the
coal matrix, the diffusion of the gases occurred in inter-molecular and
molecule to pore-wall boundaries, and the fluid flow through the coal
natural fracture system. Mass transfer of gas through the coal primary po-
rosity is dominated by diffusion where fluid flow occurs in random man-
ner, from high-concentration zone to low concentration zone, towards
the secondary porosity. Pressure driven mass transfer, if any, is assumed
to be negligible or incorporated with the diffusion (Gas Research Institute
(GRI), 1996). It is also known that diffusion is a complex process of bulk
diffusion (inter-molecular), Knudsen diffusion (molecule to pore-wall in-
teractions) and surface diffusion (mass transfer from sorbed state to free
state) (GRI, 1996; Pan et al., 2010; Smith and Williams, 1984a).
Studies reported on the sorption kinetics of methane and CO
2
in coal
are very few. Ruppel et al. (1974) stated that release of methane from
small coal particles due to desorption is interlinked with diffusion. As
methane is physically adsorbed into coal, the time required for desorp-
tion is negligible compared to that for diffusion. Nandi and Walker
(1975) studied the diffusion of methane from anthracite, medium vola-
tile and high volatile A (HVA) bituminous powdered coal samples up
to a pressure of 400 psi and observed a positive variation of effective
diffusivities with pressure, though the effect is reduced from anthracite
to HVA bituminous coal. They also observed that effective diffusivity in-
creases with increasing methane concentration and decreasing particle
size of coal. Smith and Williams (1984b) conducted pulse tracer analysis
for laboratory measurement of the diffusivity parameters for methane in
coal taking into consideration the desorption and diffusion of methane
for both short and long times. Ciembroniewicz and Marecka (1993)
conducted sorption of CO
2
at low temperatures of two Polish coals and
identified the kinetic parameters. The factors on which the fractional up-
take depends were also identified. Finally, the experimental data were
evaluated to observe the combined effect of absorption and adsorption.
Some of the earlier studies also discussed about the effect of exper-
imental condition and/or coal type. It was seen that effective diffusiv-
ities increased with a decrease in particle size (Busch et al., 2004; Cui
et al., 2004; Gruszkiewicz et al., 2009; Li et al., 2010; Marecka and
Mianowiski, 1998; Nandi and Walker, 1975; Siemons et al., 2003). It is
established that an increase in temperature reduces the gas sorption
capacity. So, at lower temperatures sorption capacity increases and
hence, more time is required for equilibrium and diffusion rate also re-
duces (Busch et al., 2004; Charriere et al., 2010). However, Li et al.
(2010) found no dependencies with temperature for methane and
CO
2
. Diffusion studies conducted at variable experimental pressure
displayed a direct relationship — i.e., diffusion parameters increased for
an increased pressure (Busch et al., 2004; Charriere et al., 2010; Nandi
and Walker, 1975). However, the opposite trend of inverse relationship
is also reported (Cui et al., 2004). But for all studies, it was observed
that CO
2
diffusion rate is higher than that of methane at the same
International Journal of Coal Geology 113 (2013) 50–59
⁎ Corresponding author. Tel.: +1 403 803 9307.
E-mail address: santanu789@gmail.com (S. Bhowmik).
0166-5162/$ – see front matter © 2013 Elsevier B.V. All rights reserved.
http://dx.doi.org/10.1016/j.coal.2013.02.005
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