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Studies on Arsenic (III) biosorption from aqueous solution by glutaraldehyde cross-linked chitosan beads
Madala Suguna1* and Nadavala Siva Kumar
2
1. Biopolymers and Thermo physical Laboratories, Department of Chemistry, Sri Venkateswara University, Tirupati – 517 502, A.P., INDIA
2. Department of Biological and Agricultural Engineering Faculty of Engineering, University Putra Malaysia, Serdang,
Selangor Darul Ehsan, MALAYSIA
*[email protected]
Abstract In the present work, the ability of glutaraldehyde
cross-linked chitosan beads (GCC beads) as synthetic
adsorbent for adsorptive removal of As(III) from
aqueous solutions is reported. GCC beads are
synthesized by homogenous reaction of medium
molecular weight chitosan in aqueous acetic acid
solution with glutaraldehyde as cross linking agent.
The biosorbent has been characterized by BET and
FTIR techniques. The effects of experimental variable
parameters such as pH, concentration of metal ion,
amount of adsorbent, contact time and temperature on
adsorption have been investigated. The optimum
solution pH for adsorption of As(III) from aqueous
solutions has been found to be pH 7.0.
Based on R2 and error function values, it is observed
that the kinetic data are better fitted to pseudo-
second-order kinetic and chemisorption models. The
experimental data have been analyzed using
Langmuir and Freundlich adsorption isotherm
models. The monolayer biosorption capacity of GCC
beads as obtained from Langmuir isotherm at 350C is
found to be 68.5 mg/g. The thermodynamic process is
endothermic in nature and spontaneous. These studies
consider the possibility of using GCC beads as cost
effective adsorbent for the removal of As(III) from
aqueous medium. So GCC beads could be an
alternative for more costly adsorbents used for As(III)
removal.
Keywords: Biosorption, Arsenic(III), GCC beads,
Kinetics, Isotherms, Thermodynamics.
Introduction Heavy metals, due to their non-degradable, persistent and
accumulative nature are toxic when present in trace
amounts. Some heavy metals like As, Pb, Cd and Hg are
more toxic even at trace quantities also1. Arsenic is present
in water as a result of both natural and anthropogenic
activities. Arsenic occurs in ground and surface waters in
organic and inorganic forms, though the organic form is
uncommon. Inorganic arsenic can occur in the environment
in several forms2. Arsenic may exist in groundwater both in
+3 and +5 oxidation states depending upon the prevalent
redox conditions. The toxicity of arsenic depends on its
binding form. Inorganic forms of arsenic are more toxic
than organic species. As(III) is more toxic in biological
systems than As(V)3. As(V) can replace phosphate in
several biochemical reactions whereas As(III) may react
with critical thiols in proteins and may inhibit their
activity4,5
.
Arsenic is mobilized through a combination of natural
processes such as weathering reactions, biological activity
and volcanic emissions as well as through a range of
anthropogenic activities such as gold mining, non-ferrous
smelting, petroleum-refining, combustion of fossil fuel in
power plants and the use of arsenical pesticides and
herbicides6.
In recent years arsenic contamination of water and ground
water has become a major concern on a global scale. In
India many districts of West Bengal are facing the problem
of arsenic contamination of ground water7. Usually arsenic
reaches the body through drinking water and contaminated
food with arsenic and causes increased risk of cancer on the
skin, in lungs, liver, kidney and bladder. Consumption of
arsenic also leads to disturbance of the cardiovascular and
nervous system functioning and eventually leading to life
threat8. Arsenic contamination has been acknowledged as a
major public health issue. These serious health effects of
arsenic have alerted the World Health Organization (WHO)
and the United States Environmental Protection Agency
(USEPA) to reduce the drinking water arsenic standard
from 0.05 to 0.01 mg/L9. Drinking water arsenic
concentrations greater than 10 ppb pose a significant health
problem across the World10
.
The conventional removal methods for arsenic and other
heavy metals from drinking water and waste waters include
reverse osmosis, chemical precipitation, solvent extraction,
filtration, ion-exchange, phytoremediation, electro dialysis,
electro flotation, chemical oxidation or reduction,
coagulation and adsorption. The methods available for the
removal of arsenic have adequately been reviewed by
Mohan and Pittman11
. Although flotation12
, precipitation
with sulfide13
, coagulation14
and filtration and ion
exchange15
have been used for arsenic removal, there exist
certain disadvantages as those could produce large amounts
of toxic sludge which requires further treatment before
disposal in to the environment.
Among the various waste water treatment techniques,
biosorption of heavy metals is a promising alternative
method due to its high selectivity and easy handling. The
major advantages of the biosorption technology are its
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effectiveness in reducing the concentration of heavy metal
ions to very low levels and the use of inexpensive
biosorbent materials16
. A number of researchers have
studied the adsorption of As(III) on different sorbents such
as iron hydroxide coated alumina17
, activated alumina18
,
iron oxide coated cement19
, granular ferric hydroxide20
,
iron (III) loaded chelating resin21
, Zr (IV) - loaded
chelating resin22
, chitosan coated biosorbent8 and iron-
chitosan composite23
are used as adsorbents for the removal
of arsenic from aqueous environment.
Over the past couple of decades, biosorption has drawn
more attention of the scientists due to the diversity of the
available sorbent material such as fungal or bacterial
biomass and alginate or chitosan biopolymers. Chitosan is
an alkaline deacetylated product of chitin. The amine
groups on chitosan are much more reactive than the
acetamide groups on chitin24
. Yang and Zall25
have
reported that chitosan has the highest chelating ability in
comparison with other natural polymers obtained from
seafood wastes and natural substances like bark, activated
sludge and the synthetic polymers. But in natural form it is
soft and has a tendency in aqueous solution to agglomerate
or to form a gel. In addition, the active binding sites are not
readily available for sorption in its natural form thereby
reducing sorption capacity. Therefore chitosan is
chemically crosslinked with glutaraldehyde to improve
chemical and mechanical resistance and to improve metal
sorption capacity.
The main objectives of this study are to prepare
glutaraldehyde cross-linked chitosan beads to remove
As(III) ions from aqueous solution. The effects of contact
time, solution pH, concentration of metal ions, temperature
and amount of biomass on the extent of adsorption are also
studied. The kinetic data are checked for the pseudo-first-
order, pseudo-second-order, chemisorption, Weber-Morris
model, Boyd model, fractionary order reaction kinetic
models and the rate constants are evaluated. The
equilibrium data are fitted to Langmuir, Freundlich and
Sips isotherm models. In addition, the biosorbent is
characterized by BET and FTIR analysis to examine the
metal accumulation due to the presence of different
functional groups on biosorbent. The obtained results may
provide useful data for future scale up using this material as
a low cost and promising adsorbent for the removal of
As(III) from aqueous solutions.
Material and Methods Chemicals and equipment: All the chemicals used in the
study were of analytical grade and used without further
purification. Chitosan with molecular weight 9.9 ×105
g/mol was purchased from Sigma-Aldrich, St. Louis, MO,
U.S.A. Deionized double-distilled water was used for the
preparation of standard solutions. An adsorbate stock
solution of 1000 mg/L of arsenic (III) was prepared by
dissolving As2O3 (Sigma–Aldrich) in deionized double-
distilled water. The range of concentrations prepared from
stock solution varied from 100 to 400 mg/L. The pH of the
solution was measured with a Digisun electronics digital
pH meter (Model: 2001, Hyderabad, India) using solid
electrode calibrated with a standard buffer solutions of pH
4.0, 7.0 and 9.2. FTIR spectrometer (Thermo-Nicolet FTIR,
Nicolet IR-200, USA) was used for the IR spectral studies
(4000–400 cm−1
) of adsorbent. The metal As(III)
concentrations in the samples were determined using
atomic absorption spectrophotometer (AAS; Model AA
6300, Shimadzu, Japan) with arsenic hollow cathode lamp.
Absorbance was measured at wavelength of 193.7 nm
using 12 mA lamp current and a spectral slit width of 0.7
nm. The signals were registered using a Canon LBP-2900B
Laser Printer.
Preparation of glutaraldehyde cross-linked chitosan
beads: The glutaraldehyde cross-linked chitosan beads
(GCC beads) were prepared as follows:26
Chitosan solution
was prepared by dissolving 2.0 g of chitosan flakes in 60
ml of 5% (v/v) acetic acid solution. The chitosan solution
was sprayed into a precipitation bath containing 500 mL of
0.5 M NaOH which neutralizes the acetic acid within the
chitosan gel and thereby coagulates the chitosan gel to
spherical uniform chitosan gel beads. A magnetic stirrer
was used in stirring the aqueous NaOH solution. The wet
chitosan gel beads were extensively rinsed with distilled
water to remove any residual NaOH, filtered out and finally
air-dried in order to remove the water from the pore
structures.
Freshly prepared wet chitosan beads were suspended in
0.025 M glutaraldehyde solution to obtain a ratio of 1:1
with chitosan. The chitosan beads in resulting
glutaraldehyde solution are kept standing for 24 h at the
range of room temperature is 20-25oC. After 24 h the cross-
linked chitosan beads were intensively washed with
distilled water to remove excess glutaraldehyde, filtered
and air-dried at room temperature.
Batch studies: Batch adsorption studies were carried out
by adding 100 mg of GCC beads to 100 mL of metal
solution taken in a 125 mL Erlenmeyer flask. The
equilibration (shaking) time was 4 h at an agitation speed of
200 rpm on a Lab line rotatory shaker. The initial pH was
adjusted with solution of 0.1M HCl or 0.1M NaOH.
Equilibrium isotherm measurements were carried out by
keeping the solution volume (100 mL) and amount of GCC
beads was kept constant by varying the concentration of
As(III) ions. For kinetic studies, samples were withdrawn at
periodic time intervals and filtered by using Whatmann No.
42 filter paper.
Atomic absorption spectrophotometer was used for the
determination of As(III) before and after adsorption. The
effects of contact time, metal ion concentration, adsorbent
dose, effect of pH and effect of temperature are studied.
The adsorption on the glassware was found to be negligible
and was determined by running blank experiments. Each
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experiment was repeated at least three times and mean
values were taken. Based on mass balance, the amount
adsorbed per unit mass of adsorbent (Qe) is obtained using
the following equation:
i ee
C CQ v
m (1)
where Qe (mg/g) is the adsorption capacity at equilibrium,
Ci and Ce denote respectively the initial and equilibrium
concentrations of metal ion (mg/L), V is volume of the
solution (L) and m is the mass of the adsorbent (g). The
effect of pH on adsorption was studied by carrying out the
experiment at different pH values, keeping the
concentration, volume of adsorbate solution and amount of
adsorbent constant. The effects of adsorbent dose on
adsorption of metal ions were studied by agitating 100 mL
of 100 mg/L metal solution with different amounts of
adsorbent.
Statistical evaluation of the kinetic parameters 1. Marquardt’s percent standard déviation (MPSD): The MPSD error function
27 is employed in this study to
find out suitable kinetic model to represent the
experimental data. The MPSD error function has been used
previously by a number of researchers in the field26
.
2
mod exp
exp
1% 100х .
1
pi el i
error
i i
q qF
q p (2)
where qimodel is each value of q predicted by the fitted
model and qiexp is each value of q measured experimentally
and p is the number of experiments performed.
2. The sum of the squares of the errors (SSE): The SSE
is defined as:
SSE = 2
exp model
1
( )p
i i
i
q q (3)
3. The hybrid fractional error function (HYBRID): This
error function was developed in order to improve the fit of
the SSE method at low concentration values28
:
HYBRID = exp model
1 exp
( )100
p-n
pi i
i i
q q
q (4)
Adsorption kinetics Adsorption kinetic study is important in treatment of
aqueous solutions as it provides valuable information on
reaction path-ways and in the mechanism of adsorption
reactions. Many kinetic models were developed to find out
kinetic adsorption constants.
1. First-order kinetics: Regarding kinetic modeling of As
(III) biosorption, the pseudo first order rate expression is
given by
1log( ) log2.303
e t e
kQ Q Q t
(5)
where Qe and Qt are the amounts of metal ion adsorbed per
unit mass of adsorbent at equilibrium and at time t (min). k1
is the rate constant of adsorption.
2. Fractionary order: Pseudo-first and pseudo–second–
order kinetic models are being used for most adsorption
kinetic works, determination of kinetic parameters, possible
change of the adsorption rates as function of initial
concentration and adsorption time. An alternative
fractionary order kinetic equation proposed by Avrami29,30
is used to analyze the present data:
α 1 exp[ ( )]n
AVk t (6)
where α is adsorption fraction (qt /qe) at time t, kAV is the
Avrami kinetic constant (min-1
) and n is a fractionary
reaction order.
3. Second order kinetics: Experimental data are also
analyzed in terms of pseudo-second-order kinetic model
which is given by the following equation:
2
2
1 1
t e e
tt
Q k Q Q (7)
where k2 (g/mg/min) is the rate constant of the second-
order equation, Qt (mg/g) is the amount adsorbed at time t
(min) and Qe is the amount adsorbed at equilibrium (mg/g).
4. Chemisorption: The Elovich equation is commonly
used to determine the kinetics of chemisorption of gases
onto heterogeneous solids and in recent years, this equation
has been found to be valid to describe the sorption of
pollutants from aqueous solution31
. The equation has been
applied satisfactorily to some chemisorption processes and
has been found to cover a wide range of slow adsorption
rates. The Elovich equation could be written in the
following form:
1 1ln( ) ln( )
β βtQ t
(8)
where α is adsorption rate (mg/g/min) and β is related to
the extent of surface coverage and the active energy
involved in chemisorption (g/min).
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5. Weber-Morris method: In the case of batch mode
operation, there is a possibility of transport of sorbate
species into the pores of sorbent which denotes the rate
controlling step. An intra particle diffusion model proposed
by Weber-Morris could be written as follows:
1/ 2Q k t C
t id (9)
where Qt (mg/L) is the amount adsorbed at time t (min), kid
(mg/g min-1/2
) is the rate constant of intraparticle diffusion.
C is the value of intercept which gives an idea about the
boundary layer thickness i.e. larger is the intercept, greater
is the boundary layer effect.
6. Boyd model: Boyd model32
is applied to check that
sorption proceeds via film diffusion or intraparticle
diffusion mechanism and can be written in the following
form:
2(1 - ) exp(-6
)t
F B
(10)
where F = qt/qe; qe is the amount of metal ions adsorbed at
equilibrium (mg/g), qt represents the amount of ions
adsorbed at any time t (min) and Bt is a mathematical
function of F. Eq. 10 can be rearranged by taking the
natural logarithm to obtain the equation:
tB = -0.4977 - ln(1 - F)
(11)
Adsorption isotherms Langmuir isotherm: Langmuir model is generally used to
describe equilibrium adsorption data. This is valid for
monolayer sorption on to a surface with a finite number of
identical sites which is given by:
e
e
o
bC
bCQQ
1e
(12)
where Q0 is the maximum amount of the metal ion
adsorbed per unit weight of GCC beads to form a complete
monolayer on the surfaces at equilibrium concentration and
b is related to affinity of the binding site.
Freundlich isotherm: A widely used empirical Freudlich
equation, based on sorption on a heterogeneous surface is
given by:
nef CKQ1
e (13)
where Kf and n are Freundlich constants, Kf and 1/n
indicate the adsorption capacity and adsorption intensity
respectively.
At low sorbate concentration it effectively reduces to a
Freundlich isotherm while at high sorbate concentration it
predicts a monolayer adsorption capacity characteristic of
the Langmuir isotherm.
Thermodynamic parameters: Based on fundamental
thermodynamics concepts, it is assumed that in an isolated
system, energy cannot be gained or lost and the entropy
change is the only driving force. In environmental
engineering practice, both energy and entropy factors must
be considered to determine the process occurrence
spontaneously. The thermodynamic parameters such as the
enthalpy change (ΔH0), the entropy change (ΔS
0) and the
free energy changes of the sorption (ΔG0) are calculated
using the following well-known relations33
:
0Δ ln LG RT K
(14) 0 0 0Δ ΔH ΔSG T (15)
0 0Δ ΔL
S HlnK
R RT (16)
where R is gas constant and KL is Langmuir constant.
Results and Discussion Characterization of the biosorbent: FTIR spectra of GCC
beads, before and after adsorption of metal ions are shown
in fig. 1. The spectra display a number of peaks, indicating
the complex nature of the material examined. The broad
and intense absorption peaks around 3400 cm-1
were
indicative of the existence of bounded hydroxyl groups (-
OH) or amine (-NH) groups of the biomass (3400–3436
cm-1
). The peaks observed at 2920 cm-1
could be assigned
to the C-H group. The spectrum of glutaraldehyde cross
linked chitosan displayed the intense peak at 1642.9 cm-1
which can be due to the N=C stretching of the imine group.
This clearly indicates the cross linking reaction with
glutaraldehyde. The intense bands at 1070 cm-1
are
assigned to the C-O of alcohols and carboxylic acids. This
figure reveals that all functional groups are actually present
in chitosan that are intact even after cross linked with
glutaraldehyde and are available for interaction with the
metal ions. The intensity of transmittance of peaks is
relatively more in the case of metal-ions-loaded GCC beads
compared with unloaded GCC beads. This higher intensity
may be attributed to the presence of a lesser number of
functional groups in the loaded GCC beads i.e. some
functional groups are binded with metal ions.
Surface Area Analysis: Surface area, pore volume, pore
diameter and porosity of the GCC beads were determined
on the basis of the BET (Brunauer, Emmett and Teller)
instrument (Micromeritirics ASAP-2000, USA). Surface
area is measured by assuming that the adsorbed nitrogen
forms a monolayer and posses a molecular cross sectional
area of 16.2 A˚2/molecule. The isotherm plots were used to
calculate the specific surface area (N2/BET method) and
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average pore diameter of GCC beads while micropore
volume is calculated from the volume of nitrogen adsorbed
at p/po 1.2. The shape of the adsorbent is nearly spherical
with particle diameter ranging from 100–150 mm. The
sorbent material shows an average surface area of 121.6
m2/g, pore volume of 0.36 cm
3/g, pore diameter 32.8 nm
and porosity of 50.12%.
Effect of pH: The pH of the solution is an important
variable parameter which governs metal adsorption. The
effects of pH on metal biosorption have earlier been studied
by many researches and the results indicate that pH of the
solution can significantly influence the biosorption23,34
. The
variation of adsorption capacity of GCC beads with pH for
As(III) is graphically presented in fig. 2. In order to
evaluate the influence of this parameter on the adsorption
of As(III), the experiments were carried out in the pH range
of initial pH 2-9. The free amino groups (-NH2) in chitosan
(Ch-) exist in equilibrium with the protanated amino group
in presence of acidic aqueous solution.
Ch-NH2 + H2O ↔ Ch-NH3+ + OH
-
The removal of As (III) increases as the pH of the system
increases and reaches maximum at pH 7.0 followed by a
sharp decrease in the extent of adsorption up to pH 9.0. As
(III) exists in non-ionic (H3AsO3) and anionic (H2AsO3-)
forms in the pH range of 2.0-9.0 and 10-12 respectively35
.
In acidic conditions the surface of GCC beads is highly
protanated and such a situation is not favorable for the
removal of As(III). When pH increases, the degree of
protanation of the adsorbent surface decreases.
Therefore, the adsorption of As(III) would be less strongly
influenced by charge repulsive forces. Given adsorbing
species are uncharged, adsorption will occur most readily
on all surface sites36
. In alkaline medium the negative
charged adsorbate species start dominating and the surface
of the adsorbent also acquires negative charge. Hence
repulsive forces exist between adsorbent and adsorbate
resulting in a decrease of adsorption.
Effect of contact time: The effect of contact time on the
extent of adsorption of As(III) on GCC beads at different
concentrations was studied. The extent of adsorption
increased with time and attained equilibrium for all the
concentrations of As(III) studied (100, 200, 300, 400 mg/L)
at 180 min. After this equilibrium period, the amount of
metal adsorbed did not change significantly with time
indicating that this time is sufficient to attain equilibrium
for the maximum removal of As(III) from aqueous
solutions by GCC beads.
Effect of adsorbent dosage: One of the parameters that
strongly affect the biosorption capacity is the amount of the
biosorbent. Quantity of biomass can influence the extent of
metal uptake from solution. The dependence of metal
sorption on dose is studied by varying the amount of
adsorbents from 0.05 to 0.5g while keeping other
parameters (pH and contact time) constants. The effect of
adsorbent dose on the extent of adsorption is studied and it
is noticed that the extent of removal of metal ions increases
with an increase in the amount of adsorbent. The removal
efficiency increases up to an optimum dose, beyond which
the increase in removal efficiency becomes negligible for a
given initial concentration. This is to be expected because
for a given fixed initial solute concentration, increasing the
adsorbent dose provides a greater surface area or adsorption
sites. The results indicate that the GCC beads remove 89 %
of As(III) as shown in fig. 3.
Adsorption kinetics: For the pseudo-first-order rate
constant k1, fractionary order constant kav are obtained from
plots of ln(qe-qt) vs. t and ln[-ln(1-Qe/Qt)] against time (t)
for As(III) analyzed. Approximately, linear fits are
observed. The kinetic models are used to fit experimental
data by non linear regression, using three different error
functions. The correlation coefficient, rate constant k1
and error function values have been calculated and are
summarized in table 1.
The pseudo-second order sorption rate constants k2 of
As(III) are calculated from the slopes of the plots of t/Qt vs.
t (Figure not shown). Equilibrium adsorption capacity Qe
along with the correlation coefficients for As(III)
adsorption on GCC beads is shown in table 1. It may be
concluded that the data are well fitted to pseudo-second-
order kinetic model on the basis of higher R2 values, the
low error function values and the calculated Qe (cal) values
are closer to the experimental data than the calculated
values of pseudo-first-order kinetic model. The error
function evaluates the differences associated with each
individual point fitted by the model in relation to each
experimental point measured. This observation supports the
contention that the adsorption of As(III) on GCC beads
follows pseudo-second-order kinetic model.
Weber-Morris method: If the plots of Qe vs. t1/2
are linear
and pass through the origin, it indicates that intraparticle
diffusion alone determines the overall rate of adsorption.
The intraparticle diffusion rate constant kid, correlation
coefficient and error function values are given in table 1.
However, the linear plots could not pass through the origin,
indicating that the intra particle diffusion is not the only
rate determining factor. This indicates that the mechanism
of metal ions adsorption by GCC beads is complex and
both, the surface adsorption as well as intraparticle
diffusion contribute to the rate determining step.
Chemisorption: The plots of ln (t) vs. Qt are presented in
fig. 4. The values of α, β and error function values are
given in table 1. The plots are linear and with good
correlation coefficients and low error function values. The
equilibrium concentrations, calculated from this model are
closely related with experimental equilibrium concentration
values. This suggests that the sorption system studied
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67
belongs to the pseudo-second-order kinetic model based on
the assumption that the rate determining step may
bechemisorption, involving valence forces through sharing
or exchange of electrons between adsorbent and adsorbate.
Boyd model: The Boyd model plots of Bt vs. t at different
initial concentrations of As(III) are shown in fig. 5. The
plots showed that the adsorption process is controlled by
film diffusion that means adsorption mechanism was
governed by external mass transport. Adsorbate ions travel
towards the external surface of the adsorbent.
Adsorption isotherms: Q0 and b are determined from the
linear plots of 1/Ce vs. 1/Qe. The linearized Langmuir
adsorption isotherms of As(III) ions obtained at the
temperatures of 25, 30 and 350C are shown in fig. 6. The
values of the parameters and correlation coefficient (R2) of
As(III) are summarized in table 2.
It is noted that the Langmuir isotherm model exhibits better
fit to the sorption data of As(III) over the Freundlich
isotherm model. The value of Q0 determined from the
Langmuir model increases with increase in temperature,
thereby confirming that the process of adsorption is
endothermic. Comparing the monolayer adsorption
capacity of GCC for As(III) obtained in the present study
with those included in table 3 indicates that the GCC beads
show higher adsorption capacity compared with many of
the adsorbents reported in literature. This observation
clearly demonstrates the enhancement in the uptake of
As(III) as a result of chitosan cross linking with
glutaraldehyde.
Freundlich isotherm constants n and Kf for As(III) are
calculated at different temperatures (25, 30 and 350C) from
the slope and intercept as shown in fig. 7 and presented in
table 2. The R2 values of Freundlich isotherm from table 2
indicate that this model has not been able to adequately
describe the relationship between the amounts of As(III)
adsorbed by the biomass and its equilibrium concentration
in the solution. The adsorption capacity, Kf was found to
increase with an increase in temperature which suggests
that adsorption process is endothermic in nature.
Table 1
Values of the parameters of kinetic models for As(III) on GCC beads
Parameter Initial concentration of As(III) (mg L-1
)
100 200 300 400
Pseudo-first-order-kinetic model
k1 (min–1
) 0.007 0.005 0.003 0.003
R2 0.967 0.987 0.974 0.971
Qe,(cal) (mg g-1
) 19.98 17.90 19.01 27.35
Qe,(exp) (mg g-1
) 37.66 55.61 90.63 130.37
MPSD (%) 79.0 81.0 84.0 90.0
HYBRID 469.0 692.0 790.0 753.0
SSE 323.0 1483 5129 10606
Pseudo-second-order-kinetic model
k2 g mg-1
min-1
0.001 0.001 0.001 0.001
R2 0.999 0.997 0.995 0.995
Qe, (cal) (mg g-1
) 41.5 59.2 94.3 137.0
MPSD (%) 1.1 0.2 0.9 1.6
HYBRID 38.7 0.03 0.83 3.26
SSE 14.6 0.017 0.75 4.25
Weber-Morris
kid mg g-1
min-1
1.378 1.355 1.743 2.500
R2 0.912 0.982 0.933 0.912
Qe, (cal) (mg g-1
) 37.63 54.68 88.32 126.7
MPSD (%) 2.2×103 0.017 0.025 0.014
HYBRID 7.9 16.00 25.00 28.00
SSE 0.97 0.86 5.32 13.24
Chemisorption
α (mg g-1
min-1
) 10.4 186.8 3.4 × 103 5 × 10
3
β (g mg-1
) 0.15 0.15 0.13 0.11
R2 0.977 0.967 0.875 0.833
MPSD (%) 2.3 0.4 1.7 2.0
HYBRID 1.9 0.1 2.7 5.4
SSE 0.7 0.05 2.4 7.1
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Table 2
Langmuir and Freundlich isotherms constants for adsorption of As(III) on GCC beads at different temperatures.
Temperature K Langmuir Freundlich
Q0 b R
2 Kf n R
2
298 55.9 0.045 0.994 1.12 1.42 0.966
303 60.6 0.034 0.997 3.32 1.55 0.976
308 68.5 0.022 0.993 4.22 1.71 0.936
Table 3
Comparison of maximum adsorption capacity (mg g-1
) of GCC beads for As(III) on different adsorbents
* Present study
Table 4
Values of thermodynamic parameters for the adsorption of As(III) on GCC beads.
Δ H0
(kJ mol-1
)
Δ S0
(J mol-1
K-1
)
Temperature
(K) -ΔG
0 (kJ mol
-1) R
2
39.09 0.135
298 2.36
0.998 303 1.82
308 1.02
Wave numbers (cm
-1)
Fig. 1: FTIR spectra of GCC beads (a) Pure GCC beads (b) loaded with As(III).
Biosorbent Adsorption capacity (mg g-1
) pH
Iron oxide coated sand7
28.57 μg g-1
7.5
Alumina Coated chitosan8
56.50 4.0
Iron hydroxide coated Alumina17
7.64 6.6-6.7
Granular Ferric hydroxide20
2.30 8.0-9.0
Iron(III)-loaded chelating resin21
62.93 9.0
Zr(IV)-loaded chelating resin22
49.15 9.0
Iron coated chitosan23
22.47 7.0
FeS-coated sand37
10.7 7.0
Iron doped phenolic resin38
13.0 6.5
Chitosan Coated Sand39
17.0 7.0
Macrofungus (Inonotus hispidus)40
51.9 6.0
Algae (Maugeotia genuflexa) biomass41
57.48 6.0
Lichen (Xanthoria parietina) biomass42
63.8 6.0
Green algae(Ulothrix cylindricum) biomass43
67.2 6.0
Glutaraldehyde cross-linked chitosan beads*
68.5 7.0
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69
1 2 3 4 5 6 7 8 9 100
5
10
15
20
25
30
35
40
Ad
sorp
tion
cap
acit
y (m
g/g)
pH Fig. 2: Effect of pH for adsorption of As(III) on GCC
beads. Experimental conditions: initial concentration
= 100 mg/L; contact time = 4h;
agitation rate = 200 rpm.
As
0
10
20
30
40
50
60
70
80
90
100
0 0.1 0.2 0.3 0.4 0.5 0.6
Amount of adsorbent (g/L)
Percen
t rem
ov
al
Fig. 3: Effect of adsorbent dose on percent removal of
As(III) on GCC beads. Experimental conditions: for
As(III): initial concentration = 100 mg/L;
contact time = 4h; pH 7.0.
Elovich
0
20
40
60
80
100
120
140
2 3 4 5 6
Ln (t)
Ad
sorp
tio
n c
ap
acit
y (
mg
/g)
100 mg/L
200 mg/L
300 mg/L
400 mg/L
Fig. 4: Elovich model for adsorption of As(III) on
GCC beads. Experimental conditions: for As(III): pH
7.0; initial concentration = 100 mg/L;
biosorbent dosage = 0.1g/0.1L.
0
0.5
1
1.5
2
2.5
3
0 50 100 150 200
Time (min)
Bt
100 mg/L
200 mg/L
300 mg/L
400 mg/L
Fig. 5: Boyd model for adsorption As(III) on GCC
beads. Experimental conditions: for As(III): pH 7.0;
initial concentration = 100 mg/L;
biosorbent dosage = 0.1g/0.1L.
0
0.02
0.04
0.06
0.08
0.1
0.12
0.14
0.16
0.18
0.2
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35
1/Ce
1/Q
e
As-308 K
As-303 K
As-298 K
Fig. 6: Langmuir isotherms for adsorption of As(III)
on GCC beads. Experimental conditions: for As(III):
pH 7.0; initial concentration = 100 mg/L;
biosorbent dosage =0.1g/0.1L.
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
0 0.5 1 1.5 2
Log Ce
Lo
g Q
e
As-308 K
As-303 K
As-298 K
Fig. 7: Freundlich isotherms for adsorption of As(III)
on GCC beads. Experimental conditions: for As(III):
pH 7.0; initial concentration = 100 mg/L;
biosorbent dosage = 0.1g/0.1L.
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70
The values of n between 1 and 10 (i.e. 1/n less than
1) represent a favorable sorption37
. For the present study
the values of n also follows the same trend. Higher is the
value of 1/n, higher will be the affinity between the
adsorbate and adsorbent to reveal heterogeneity of the
adsorbent sites.
Thermodynamics: The values of ΔG
0 for sorption of As
(III) on GCC beads at different temperatures are given in
table 4. The negative values of ΔG0 indicate feasibility and
spontaneity of the process of removal of metal ions by
adsorption on the GCC beads. The values of ΔH0 and ΔS
0
are determined from the slope and intercept of the plot of ln
KL vs. 1/T (Figure not shown). From table 4 it is clear that
the positive value of enthalpy indicates that the process of
removal of As(III) is endothermic in nature.
Conclusion
In this study, the use of GCC beads as a biosorbent has
been successfully examined in the removal of As (III) ions
from aqueous solution. The following conclusions are made
based on the results of the present study:
The kinetics of As(III) ions biosorption on glutaraldehyde
cross-linked chitosan beads depends on the experimental
conditions particularly medium pH, initial metal ion
concentration, biosorbent dosage, contact time and
temperature. As the pH increased, the metal biosorption
capacity increased significantly up to pH 7.0. The
equilibrium data were fitted very well to the Langmuir
isotherm model. The maximum monolayer biosorption
capacity of GCC beads was found to be 68.5 mg/g.
Comparing the equilibrium capacities of the kinetic models
with the experimental and calculated equilibrium capacities
of the biosorbent, second order equation seems to give a
best fit of the experimental data. The rate determining step
may be chemisorption, involving valence forces through
sharing or exchange of electrons between adsorbent and
adsorbate. This suggests that rate limiting step is a chemical
adsorption phenomenon. Based on the thermodynamic
constants ΔG0, ΔH
0 and ΔS
0, biosorption of As(III) on
GCC beads is an endothermic and spontaneous process.
Studies conducted using synthetic metal ion solutions
revealed the practical application of the glutaraldehyde
cross-linked chitosan as a potential biosorbent for the
removal of As(III) from aqueous medium.
Acknowledgement
Madala Suguna is thankful to DST, New Delhi, India for
the award of Women Scientist and the financial support of
this research project, SR/WOS-A/CS-76/2011/.
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(Received 19th December 2013, accepted 12
th February
2014)