J. of Supercritical Fluids 54 (2010) 178–189
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The Journal of Supercritical Fluids
journal homepage: www.elsevier.com/locate/supflu
Analysis of the kinetics of regeneration of bidispersed activated
granular carbon, by supercritical carbon dioxide
B. Bensebia
a,b
, A. Dahmani
a
, O. Bensebia
a
, D. Barth
c,∗
a
Laboratoire de Thermodynamique et de Modélisation Moléculaire, Faculté de Chimie, Université des Sciences et de la Technologie
Houari Boumediene, BP 32, El Alia, Alger 16111, Algeria
b
Département de Génie des Procédés, Université Hassiba Ben Bouali de Chlef, BP 151, 02000-Chlef, Algeria
c
Laboratoire des Sciences du Génie Chimique, Nancy-Université, CNRS, 1 rue Grandville, BP 20451, F 54001-Nancy, France
article info
Article history:
Received 21 October 2009
Received in revised form 15 April 2010
Accepted 17 April 2010
Keywords:
Supercritical desorption
Bidisperse solids
Macropore diffusion
Micropore diffusion
abstract
A desorption of m-xylene by supercritical CO
2
under different temperatures (40, 50 and 60
◦
C) and pres-
sures (80, 100 and 128 bar) has been modelled using the analytical solution expressing the desorption
yield for bidisperse granular activated carbon. This solution is in the form of an infinite double series.
The coefficients of which were calculated by solving the transcendental equation using the method of
Newton–Raphson. Solutions of first and second order of this equation determine the coefficients of the
analytical solution. The results of this modelling, including macropore and micropore diffusion, show
very good concordancy between experimental and simulated data for all operating conditions, which
confirms the appropriateness of this model for this type of adsorbent considered. Only the equilibrium
adsorption constant “K
C
” was used as adjustable parameter. The values of K
C
varied between 13.32 and
121.33 and the maximum average deviation between estimated and fitted values not exceeding 6.54%.
On the other hand, it has been particularly highlighted for the experimental conditions studied, that the
contribution of resistance due to external transfer and axial dispersion were negligible and that the resis-
tance due to macropore diffusion was consistent and it was possible to reduce the time of desorption by
reducing the size of the grain.
© 2010 Published by Elsevier B.V.
1. Introduction
Many potential applications have been proposed which involve
desorption of solutes from solid using SCF solvents: these include
activated carbon regeneration [1–7] using SC-CO
2
. To design large
scale supercritical desorption process is necessary to understand
in which way dynamic desorption is influenced by process vari-
ables as mass transfer effects, equilibrium considerations but also
the texture of the solid. The models developed [8–16] are gen-
erally based on the differential mass balance equations for the
different phases and different assumptions about the resistance
to mass transfer and solute–solid, solute–solvent interactions. The
common assumption in the above-cited models is the monodis-
perse pore structure within the adsorbent particle. It has been
demonstrated [17,18] that erroneous diffusivities may result if dif-
fusion data in a bidisperse grain are analyzed as a monodisperse
porous material. Then, to interpret accurately the transport phe-
nomena in adsorbent with broad pore size distribution (such as
∗
Corresponding author. Tel.: +33 3 83 17 50 27; fax: +33 3 83 32 29 75.
E-mail addresses: danielle.barth@ensic.nancy.fr,
Danielle.Barth@eeigm.inpl-nancy.fr (D. Barth).
activated carbon) the real porous structure must be taken into
account [19].
It is generally accepted that microporous adsorbents, such as
activated carbon, are bidisperse [20] and have both micropores
as well as macropores. The description of transport processes in
such bidisperse solids is difficult due to the complex and largely
unknown nature of the pore network, and a variety of structural
idealization have been proposed based on which approximate
methods for diffusion and adsorption have been developed. The
simplest and most popular of these idealizations considers the
solid particle as comprising an aggregate of microporous spherical
microparticles, with the inter-microparticles macropores provid-
ing the channels for intragranular transport. The pore size of the
micropores is of the order of molecular dimension, and there-
fore, molecules of solute inside the micropore never escape the
attraction potential of the pore walls. This means that molecules
in the free form do not exist and only adsorbed molecules exist
in the micropore. During the desorption process, these adsor-
bate molecules diffuse (in the adsorbed state) under a gradient
of concentration to reach the mouths of micropores where des-
orption equilibrium with the fluid in the macropores takes place.
These large macropores basically act as passage way for desorbed
molecules to diffuse from the interior of the grain (macropores) to
0896-8446/$ – see front matter © 2010 Published by Elsevier B.V.
doi:10.1016/j.supflu.2010.04.005