105 (2018) 287–297
February
Desalination and Water Treatment
www.deswater.com
doi:10.5004/dwt.2018.22132
Aminofunctionalized silica monolith for Pb2+ removal:
synthesis and adsorption experiments
Hakimeh Sharififarda,c, Paolo Apreab,*, Domenico Caputob, Francesco Pepec,*
a
Department of Chemical Engineering, Amirkabir University of Technology, No.424, Hafez Ave., Tehran, Iran,
email: hakimeh.sharifi@gmail.com
b
ACLabs – Applied Chemistry Laboratories, Department of Chemical, Materials and Industrial Production Engineering, Università
Federico II, P.le Tecchio 80, 80125, Napoli, Italy, email: paolo.aprea@unina.it (P. Aprea), domenico.caputo@unina.it (D. Caputo)
c
Department of Engineering, Università del Sannio, Piazza Roma 21, 82100 Benevento, Italy, email: francesco.pepe@unisannio.it
Received 15 February 2017; Accepted 31 January 2018
ABST R AC T
Lead(II) removal from aqueous solutions by adsorption on APTMS-functionalized silica monolith
(APTMS-Monosil) was investigated. Functionalized silica monolith was selected as adsorbent due to
its ease of synthesis and versatility. Adsorption experiments were performed in a batch system, and
the effects of various operating parameters, such as solution pH, initial concentration and solid to
liquid ratio were evaluated. According to the Response Surface Methodology results, the optimum
operating conditions for Pb2+ removal by APTMS-Monosil were pH = 6.24, initial Pb2+ concentration
of 89.5 mg L–1 and solid to liquid ratio of 1.84 g·L–1. The kinetic data suggested that chemical adsorption, rather than mass transfer, was the controlling step for lead capture. Equilibrium isotherms were
analyzed using different models, and data were well fitted to the Langmuir isotherm. The thermodynamic parameters of the adsorption process (∆H° = 30.9 kJ·mol–1, ∆S° = 0.187 kJ·mol–1 K–1, and ∆G°
= –24.826 kJ·mol–1 at T = 298 K), calculated from three isotherms at T = 30– 60°C, revealed a spontaneous, endothermic process, with a strong chemical nature. The maximum adsorption capacity of
APTMS-Monosil for lead was 450 mg·g–1, which is a high value if compared with other materials
presented in the literature.
Keywords: Silica monolith; Amine functionalization; Lead adsorption; Response surface method
1. Introduction
Heavy metal contamination of water resources is one
of the greatest environmental concerns because of the toxic
effects that these substances have for human beings and
other animals and plants in the environment, and because
of their tendency to bioaccumulate. One of the most ubiquitous heavy metals is lead, that is released to environment
through a number of industrials activities such as refineries, printing, production of pigments etc. [1–5]. The presence of lead in water, even at very low concentrations, is
extremely harmful to the aquatic environment and human
health. Lead can damage, among others, the nervous
system, kidney, and reproductive system [6]. The World
Health Organization (WHO) and US Environmental Protection Agency (US EPA) have set a maximum guideline
concentration of 0.01 and 0.015 mg·L–1 for Pb in drinking
water, respectively [7].
Several technologies, such as chemical precipitation,
electrocoagulation, ion exchange, membrane processes
and adsorption have been tested for heavy metal removal
from industrial wastewater [8–17]. Among them, adsorption seems to be the most suitable method in case of low
concentration of contaminant, due to its relatively low
cost and high efficiency [18,19]. With the increase in global
awareness for environmental pollution, there is a growing
*Corresponding author.
1944-3994 / 1944-3986 © 2018 Desalination Publications. All rights reserved.
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H. Sharififard et al. / Desalination and Water Treatment 105 (2018) 287–297
demand for novel adsorbents characterized by high performances and efficiency for removal of heavy metals from
aqueous systems, and quite recently several adsorbents
have been tested, such as metal oxides/hydroxides [20,21],
zero valent iron composites [22,23], and surfactant modified
materials [24,25].
Among the materials of interest for adsorption applications are ordered mesoporous silicas (OMS). OMS constitute a large class of mainly amorphous materials, whose
greatest advantages are their relatively large, yet uniform
pore size, large surface area, and easily controllable surface chemistry [26,27]. However, since OMS have no strong
affinity towards heavy metals, it is necessary to modify
them by insertion of appropriate functional groups, such as
amino groups, in order to increase their adsorption performances [13,28–31].
OMS are typically synthesized as powders, and their
textural properties are subject to degradation during
aggregation/shaping processes. An interesting alternative to powder functionalization followed by aggregation is the use of substrates directly obtained as aggregate
materials, such as macro/mesoporous silica monoliths
that can be subjected to a post synthesis functionalization
process [32]. Silica monoliths, which can be produced by
different synthesis routes [32–34], feature high chemical
and mechanical stability, and their surface can be readily
functionalized via grafting of organic and inorganic moieties [35]. According to published literature, there are few
research works regarding the application of silica monoliths for heavy metal removal. For example, Sugrue and
coworkers [36] modified a commercially available chromatographic silica column with iminodiacetic acid, reporting some encouraging results about its ion-exchange
properties. Awual and coworkers [37,38], on the contrary,
performed a direct synthesis of silica monoliths followed
by a direct immobilization of functional acids, in order to
perform an efficient removal of copper and cobalt from
aqueous solutions.
The goal of the present investigation is the evaluation of
a silica monolith, named Monosil [35], functionalized with
3-aminopropyl-trimethoxysilane for the removal of Pb2+
ions from aqueous solutions. The effect of several operating parameters, such as initial pH, lead concentration and
solid to liquid ratio on removal efficiency is investigated in
batch conditions using Central Composite Method (CCD)
with response surface methodology (RSM), and kinetic and
equilibrium data are thoroughly analyzed in order to better
clarify the lead adsorption mechanisms.
2. Materials and methods
2.1. Synthesis and characterization of APTMS-Monosil
Monosil silica monoliths were synthesized following
the approach adopted in [35]. 23.15 g of deionized water
and 2.3 g of HNO3 (68%) were mixed for 15 min at 0°C.
Afterwards, 2.4 g of polyethylene oxide (PEO, 20 kDa) was
added, and the mixture was stirred for 1 h. After that, 18.9
g of tetra-ethyl-ortho-silicate (TEOS) was added, and the
new mixture was further stirred for 1 h. The solution was
then poured into plastic tubes of 10 cm length and 8 mm
internal diameter, and was kept at 40°C for 24 h to allow
complete solidification. The monoliths, of cylindrical shape,
were extracted from the tubes, washed in water, and then
treated in an ammonia solution (0.1 M) at 40°C for 24 h.
Finally, they were dried at 40°C overnight and calcined at
550°C for 8 h.
In order to perform adsorption experiments, the monoliths were crushed and sieved to select 2–3 mm particles.
The selected particles were functionalized with 3-aminopropyl-trimethoxysilane (APTMS) using a wet impregnation
method. Initially, they were dried at 100°C for 24 h; then,
grafting of aminic groups was carried out by refluxing 0.1 g
of Monosil in a 50 mL dry toluene solution containing 0.25
mL of 97% pure APTMS at 110°C for 24 h. The APTMS functionalized particles were then collected and washed with
toluene, and then dried at room temperature for 24 h. All
reagents for the synthesis procedure were purchased from
Sigma Aldrich Co., while deionized water (s≤0.055 mS/cm)
was prepared in house.
The surface area (SBET) and pore size distribution of
both raw Monosil and APTMS–Monosil were determined
from adsorption–desorption isotherms of N2 at 77 K. A
Quantachrome NOVA 1000 surface area analyzer was used
to determine the isotherms. Furthermore, pHZPC (point of
zero charge) of APTMS–Monosil was measured using the
following technique: 0.3 g of adsorbent was added to 50
mL of a 0.1 N NaCl solution, the pH of which was adjusted
using aqueous HCl or NaOH solutions. The pHZPC of the
adsorbent was assumed to coincide with the initial solution pH if this remained constant after addition of the
adsorbent and thorough mixing [15]. Fourier Transform
Infrared (FT-IR) spectra of the samples were recorded
between 4000 and 400 cm−1 using the KBr method, with a
resolution of 4 cm−1 with a Nicolet FT-IR spectrophotometer (NEXUS 670).
2.2. Effect of adsorption parameters
The effects of three operating parameters, namely
solution pH, solid to liquid ratio and initial concentration, were investigated. Batch Pb2+ adsorption experiments were performed by adding a measured weight
of APTMS-Monosil in 50 mL of Pb2+ solutions with an
assigned initial Pb2+ concentration and pH. Reagent grade
Pb(NO3)2 from Sigma-Aldrich Co. and deionized water
were used to prepare the solutions. The initial pH of the
solutions was adjusted with HCl and NaOH solutions.
The mixtures, kept in 100 mL Erlenmeyer flasks, were
shaken at 30°C using an orbital shaker (FINEPCR-SH30)
at 150 rpm for 3 h. At the end of the experiment, the adsorbent was separated from liquid phase by filtration on filter
paper (Whatman No. 40). The residual Pb2+ concentration
in solution was determined using Inductively Coupled
Plasma Optical Emission Spectrometry (ICP OES, Perkin
Elmer Optima 2100 DV), and the comparison between initial and final Pb2+ concentrations allowed to evaluate the
removal percentage.
With the purpose of assessing the role of the three operating parameters mentioned above, CCD was used. Since
the number of independent parameters is three, 20 experiments consisting of 8 factorial points, 6 axial points and 6
replicates at the center points were carried out [39–43]. The
range of variables investigated is given in Table 1.
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Table 2
Porosity parameters of Monosil and APTMS-Monosil
Table 1
Experimental ranges and levels of independent variables
Independent parameter
X1
X2
X3
pH
Solid to liquid ratio
Initial Pb2+ concentration
Actual form of coded levels
Parameter
–1
0
+1
2
0.5
10
4.35
1.75
55
6.7
3
100
BET Sp. Surf. area (m g )
Mesopore volume (mL g–1),
BJH method
Micropore volume (mL g–1),
HK method
Average pore radius (Å)
2
–1
Monosil
APTMS-Monosil
543
0.844
163
0.327
0.032
0.042
32.3
43.3
2.3. Kinetic studies
The kinetics of adsorption were studied by placing 0.05
g of adsorbent in flasks containing 50 mL of 100 mg·L–1 Pb2+
solution at pH 6.0. The flasks were agitated in the orbital
shaker at 150 rpm for a time ranging between 2–360 min at
30°C. After that, the suspension was filtered, and the solution concentration was analyzed. The metal uptake was calculated as:
q=
V
(C0 − C f )
m
(1)
where q is the amount of solute adsorbed per unit weight of
adsorbent (mg·g–1), V and m are solution volume (L) and dry
weight of adsorbent (g), respectively, and Coand Cf are the initial and final metal ion concentration (mg·L–1), respectively.
2.4. Equilibrium studies
The adsorption isotherms for Pb2+ on APTMS-Monosil
were determined by placing 0.025 g of adsorbent in a series of
flasks containing 50 mL of metal ion solutions at different initial concentrations (10–220 mg L–1). Initial pH was adjusted at
6.0 in all experiments. The flasks were agitated in an orbital
shaker at 150 rpm for 24 h at various temperatures (30°, 45°C
and 60°C). After this period, the suspension was filtered and
the residual Pb2+ concentration was determined. The amount
of lead adsorbed, q, was calculated using Eq. (1).
Fig. 1. BJH differential pore size distribution of: (a): Monosil,
(b): APTMS-Monosil.
3. Results and discussion
was determined by HK (Horvath−Kawazoe) and BJH (Barrett, Joyner, and Halenda) methods, respectively [45,46].
BJH differential pore size distribution (Fig. 1) shows
that both Monosil and APTMS-Monosil have a mesoporous
structure. It can be seen that functionalization of Monosil
with APTMS causes a reduction in surface area and pore
volume: this can be interpreted by assuming that the molecules of APTMS diffuse into the mesoporous structure
of Monosil, limiting the accessibility of N2 molecules to
smaller pores. As a result, the average pore radius of the
APTMS-Monosil is higher compared to that of Monosil. The
pHZPC of APTMS-Monosil is 4.9.
The FT–IR spectra of Monosil and APTMS-Monosil are
shown in Fig. 2. In both spectra, the two peaks located at
around 3450 cm−1 and 1630 cm−1 can be attributed to the
stretching and bending modes of adsorbed water molecules, while the peak at around 950 cm−1 is due to asymmetric vibrations of (Si–OH), thus revealing the presence of
hydroxyl groups. The asymmetric, stretching and bending
vibrations of (Si–O–Si) are responsible for the peaks at 1090
cm−1, 800 cm–1 and 460 cm–1, respectively [47]. After modification of Monosil with APTMS, new peaks are detected
between 1610 cm–1 and 1715 cm–1. These new peaks represent
the vibration of different amine groups such as NH2 [26].
3.1. Characterization of the adsorbents
3.2. Effect of separation parameters
2.5. Regeneration and reuse of APTMS-Monosil
The regeneration tests of APTMS-Monosil were carried
out as follows: 0.05 g of adsorbent, previously saturated
with Pb2+ ions by contacting it with a 100 mg L–1 Pb2+ solution at pH 6.0 for 48 h, was treated with 5 ml of 0.1 M EDTA
solution under vigorous stirring at 50°C for 1 h, followed by
washing with deionized water for several times and drying
at 80°C for 2 h. The regenerated adsorbent was then used
for the next adsorption test. Five consecutive adsorption–
regeneration cycles were performed to check the reusability
of the APTMS-Monosil for capturing Pb2+ [44].
The porosity parameters of Monosil and APTMS-Monosil are presented in Table 2. The surface area was calculated
by applying the 3-point BET (Brunauer−Emmett−Teller)
method. The volume (mL·g–1) of micropore and mesopore
3.2.1. Regression model equation development
The complete design matrix and the response values
obtained from the experimental works are reported in
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Table 3, together with a comparison with the prediction of
Eq. (2). Eq. (2) represents the empirical quadratic model that
was used to fit the experimental data, with the coefficients
of this model obtained by multiple regression analysis technique using Design-Expert® 7.0 software:
Removalpercentage = −95.56 + 53.59X1 + 52.32X 2 − 0.45X 3
−5.69X1X 2 + 7.44 ⋅ 10 −3 X1X 3 + 7.77 ⋅ 10 −3 X 2 X 3 (2)
−3.74 X12 − 4.26 X 22 + 3.47 ⋅ 10 −3 X 32
As indicated in Table 1, in this equation X1, X2 and X3 are
solution pH, solid to liquid ratio (g L–1) and initial concentration of Pb2+ (mg L–1), respectively.
The analysis of variance (ANOVA) was applied in order
to critically evaluate the role played by the different variables considered. The ANOVA results are shown in Table 4.
According to the rule, the best regression model is deter-
mined by highest Fisher’s F values and lowest p-values
[43,48]. Data in Table 4 indicate that the quadratic model
was significant at the 90% confidence level. As it can be seen
from inspection of Table 4, the F value for the model is 77.1,
and correspondingly the p–value is lower than 0.0001 and
SS is quite high (SS = 1.81·104). This implies that the model
is significant, and that it can appropriately explain the relationship between response and variables individuated as
independent. This conclusion is also confirmed by the fact
that both R2 and R2adj approached unity. Furthermore, p-values that are lower than 0.05 allow to individuate the model
terms which are significant, while values greater than 0.1
allow to individuate model terms are not significant, and
can be omitted [49]. According to the results reported in the
ANOVA table, the linear, quadratic and combined effects of
pH (X1) and solid to liquid ratio (X2) are the most significant
variables, while Pb2+concentration plays a less relevant role,
at least in the concentration range explored here.
The fact that Pb2+ concentration is practically irrelevant probably depends on the fact that the adsorbent is far
from saturation. Eliminating the less significant terms from
Eq. (2) and refining the model, Eq. (2) may be simplified to:
Removalpercentage = −95.56 + 53.59X1 + 52.32X 2 − 5.69X1X 2
−3.74 X12 − 4.26 X 22
Fig. 2. FT–IR spectra of Monosil and APTMS-Monosil.
(3)
A further confirmation of the validity of the analysis
now presented comes from the diagnostic plot of Fig. 3, in
which the values predicted by Eq. (3) are reported vs. experimental data, with a very satisfactory comparison.
The different roles played by the three independent
variables under consideration are graphically described in
Table 3
Experimental conditions and results for lead removal
Run
pH
Solid to liquid ratio (g L–1)
Initial concentration (mg L–1)
Actual removal (%)
Predicted removal (Eq. (2), %)
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
1.49
4.35
4.35
2.00
7.21
6.70
4.35
4.35
6.70
6.70
4.35
2.00
4.35
2.00
4.35
6.70
2.00
4.35
4.35
4.35
1.75
1.75
1.75
3.00
1.75
0.50
3.27
1.75
0.50
3.00
1.75
0.50
1.75
0.50
0.23
3.00
3.00
1.75
1.75
1.75
55.00
55.00
55.00
10.00
55.00
10.00
55.00
55.00
100.00
10.00
55.00
10.00
0.28
100.00
55.00
100.00
100.00
55.00
109.72
55.00
30.1
89.9
90.4
76.1
83
100
96
92
100
100
92.6
11
100
6.1
58.5
100
74.7
91.6
95.2
93.6
27.42
90.26
90.26
77.23
92.57
98.30
97.31
90.26
96.72
96.44
90.26
12.10
101.88
7.65
60.53
96.88
74.66
90.26
99.43
90.26
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H. Sharififard et al. / Desalination and Water Treatment 105 (2018) 287–297
Table 4
ANOVA table for lead removal using APTMS-Monosil
Source
Sum of squares (SS)
df
Mean square
F–Value
p–value
Model
X1
X2
X3
X1 X 2
X1 X 3
X2 X3
X12
X 22
18145.067
8206.843
3459.752
0.114
2947.968
7.430
6.319
1109.030
9
1
1
1
1
1
1
1
2016.118
8206.843
3459.752
0.114
2947.968
7.430
6.319
1109.031
77.143
314.021
132.381
0.004
112.799
0.284
0.242
42.435
< 0.0001
< 0.0001
< 0.0001
0.9486
<0.0001
0.6055
0.6335
<0.0001
517.404
5.989
261.346
0.00
1
1
10
517.404
5.989
26.134
19.797
0.229
0.0012
0.6424
X32
Residual
Pure Error
R2
R 2adj
Fig. 3. Predicted versus experimental values plot for Pb2+ removal using APTMS-Monosil (predicted values: Eq. (3)).
the perturbation plot of Fig. 4. As expected from the analysis of the ANOVA table, Fig. 4 indicates that the effect of pH
(X1) on removal efficiency is quite strong, followed by the
effect of solid to liquid ratio (X2), with a weak dependence
on Pb2+ initial concentration (X3).
3.2.2. Response surface plots
Three-dimensional response surface plots were generated to further investigate the effects of the three process
parameters considered, i.e. solution pH, solid to liquid ratio
and initial concentration on Pb2+ removal.
3.2.3. Effect of pH
Figs. 5a and 5b show the effect of solution pH on the
removal efficiency. According to these figures, the removal
0.986
0.973
Fig. 4. Perturbation plot for Pb2+ removal at central point of design parameters. X1: pH; X2: solid to liquid ratio; X3: Pb2+ initial
concentration. See Table 1 for the actual values of each parameter.
efficiency of Pb2+ increases with pH ranging from 2 to 6.5
at any fixed initial concentration and solid to liquid ratio,
even though this effect is smaller when solid to liquid ratio
increases. Presumably, the importance of solution pH in the
removal process derives from its effect on the surface functional groups and the speciation of lead in solution. Indeed,
the fact that pHZPC for APTMS-Monosil is 4.9 means that
the surface charge of the adsorbent is positive when pH <
4.9 and negative when pH > 4.9. Since the dominant forms
of lead at initial pH < 6–6.5 is Pb2+ cations [50,51], at pH <
pHZPC the surface of APTMS-Monosil is positively charged,
and mainly an electrostatic repulsion occurs between Pb2+
cations and positive adsorption sites of APTMS-Monosil,
while at pH > pHZPC, the adsorbent surface is negatively
charged and it can more easily adsorb Pb2+.
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H. Sharififard et al. / Desalination and Water Treatment 105 (2018) 287–297
3.2.4. Effect of initial concentration
The effect of initial concentration is shown in Figs. 5b
and 5c. The results indicate that this variable does not have
a significant effect on removal efficiency regardless of pH
and solid to liquid ratio, confirming the indications deriving from ANOVA table (p value = 0.9486).
3.2.5. Effect of solid to liquid ratio
According to Figs. 5a and 5c, the removal efficiency
increases with increasing solid to liquid ratio. This tendency
was expected because, as the ratio increases, so does the
number of adsorbent active sites, and thus more Pb2+ ions
can be removed.
Based on the optimum conditions, complete Pb2+
removal was predicted by the model under operating conditions of pH = 6.24, solid to liquid ratio 1.84 g L–1 and initial concentration of 89.5 mg L–1 for APTMS-Monosil. This
result was validated experimentally (99.5% Pb2+ removal).
3.3. Adsorption kinetics
The adsorption kinetics were investigated in order to
analyze the mechanism of adsorption and the potential
rate controlling phenomena, such as mass transfer and
chemical reaction. The adsorption kinetics of Pb2+ onto
APTMS-Monosil were investigated by three common models, namely pseudo-first-order model, pseudo-second-order
model and intraparticle diffusion model.
The pseudo-first-order model assumes that the limiting
step of the adsorption process is the interaction between
adsorbate molecules (here Pb2+ ions) and adsorbent active
sites, and that this interaction can be kinetically described
by a first order kinetic equation, with no role played by liquid–solid and intraparticle diffusion. If this model is appropriate, then the adsorption kinetics can be described by the
following equation:
(
qt = qe 1 − e k1t
)
(4)
where t (min) is time, qe and qt (mg g–1) are the amount of
Pb2+ adsorbed at equilibrium and at time t, respectively,
and k1 (min–1) is the rate constant for the adsorption
(pseudo) reaction.
The experimental data were also analyzed by the
pseudo–second–order model, which once again assumes
that the overall process is limited by the adsorbent–adsorbate interaction, but then assumes that this can be described
by a second order kinetic equation. In this case the adsorption kinetics can be described by the following equation:
t
1
t
=
+
qt k 2 qe2 qe
(5)
in which k2 (g mg–1min–1) is the rate constant for the adsorption (pseudo) reaction.
Eventually, the possibility that adsorption process is
controlled by intraparticle diffusion was considered. If this
is the case, then the adsorption kinetics can be described by
the Morris–Weber model [52], according to which it is:
qt = kidt1/2 + θ
Fig. 5. Response surfaces plots for Pb2+ removal using
APTMS-Monosil. (a): Effects of X1 and X 2; (b): effects of X1 and
X3; (c): effects of X 2 and X3 (X1: pH; X 2: solid to liquid ratio; X3:
Pb2+ initial concentration).
(6)
in which kid (mg·g–1min1/2) is the intraparticle diffusion rate
constant, and θ (mg g–1) is a constant, the value of which
depends on the role played by external (fluid–solid) mass
transfer.
In order to compare the three models, the kinetic data relative to Pb2+ adsorption with solid to liquid ratio of 1 g·L–1,
initial Pb2+ concentration of 100 mg L–1 and initial pH of 6.0
have been reported in Fig. 6. In particular, Fig. 6a refers to
the pseudo-first-order model, and is a plot of ln(qt) vs. t;
H. Sharififard et al. / Desalination and Water Treatment 105 (2018) 287–297
293
confirmed by the fact that the R2 value for the pseudo-second-order model is significantly closer to 1 than those relative to the two other models considered. This suggests
that adsorption of Pb2+ on APTMS functionalised Monosil
is controlled by a pseudo–chemical reaction, which can be
described by a second order kinetic equation. In particular,
the fact that the Weber–Morris model fails to describe the
available kinetic data (see Fig. 6c) appears to indicate that
intraparticle diffusion plays a secondary role in the overall
adsorption process, at least in the experimental conditions
considered.
3.4. Equilibrium and thermodynamic of adsorption
The equilibrium data relative to Pb2+ adsorption on
APTMS-Monosil at 30°, 45° and 60°C are reported in Fig. 7.
The most striking feature of Fig. 7 is that adsorption capacity increases with temperature, rather than decreasing, as
is the case of most adsorption phenomena. In particular,
the highest Pb2+ adsorption capacity, about 450 mg·g–1, was
observed at the highest temperature explored, i.e. T = 60°C,
with a behavior similar to the one exhibited by a number of
amine–functionalized silicas toward gas–phase adsorption,
in particular of CO2 [27].
In order to have a clearer understanding of the
adsorption process, the available data were fitted using
the Langmuir, Freundlich and Dubinin-Raduskevich isotherms. The Langmuir isotherm is based on the assumptions that all the adsorption sites are equivalent for what
concerns adsorbent–adsorbate interactions, that each site
only interacts with a single adsorbate molecule/ion and
that adsorbate–adsorbate interactions are negligible. The
Langmuir isotherm equation is described by the following equation:
qe = qmax
K LCe
1 + K LCe
(7)
where Ce (mg g–1) is the liquid phase concentration of adsorbate at equilibrium and KL (L·mg–1) and qmax (mg·g–1) are the
model parameters: qmax represents the maximum amount
of adsorbate which can be theoretically adsorbed per unit
mass of adsorbent when the monolayer coverage is complete, while KL is a measure of adsorbent–adsorbate affinity.
The Freundlich isotherm is an essentially empirical
equation, which assumes that the adsorption process takes
place on a heterogeneous surface, and is described by the
following equation:
Fig. 6. (a) Pseudo-first-order model; (b) Pseudo-second-order
model; (c) Intraparticle diffusion model for Pb2+ removal.
Fig. 6b refers to the pseudo-second-order model, and is a
plot of 1/qt vs. t; eventually, Fig. 6c refers to the intraparticle
diffusion model, and is a plot of qt vs. t1/2. Parameters and R2
values for the three models are reported in Table 5. Inspection of Fig. 6 clearly indicates that experimental results are
much better interpreted by the pseudo-second-order model
than by the other models taken into account. This is also
qe = K f (Ce )
1
n
(8)
where Kf and n are the model parameters: Kf (mg g–1 L1/n
mg–1/n) is an indicator of the adsorption capacity of adsorbent and n is a measure of favorability of adsorption.
The Dubinin–Radushkevich (D-R) isotherm is a model
originally proposed to describe gas–phase adsorption of
subcritical vapors on porous sorbents, and can in general
be used to describe adsorption on a heterogeneous surface
characterized by a Gaussian distribution of adsorbent–
adsorbate interaction energy [53]. The D–R equation is
described by Eq. (9):
294
H. Sharififard et al. / Desalination and Water Treatment 105 (2018) 287–297
Table 5
Constants and regression coefficient for kinetic models
Pseudo-first-order
k1 (min–1)
qe (mg g–1)
0.034
46.54
R2
0.92
Pseudo-second-order
k2 (g mg–1·min–1)
0.0009
qe (mg g–1)
104.16
R2
0.998
Intra-particle diffusion
kid (mg g–1·min–1/2)
5.32
θ
31.63
R2
0.778
Table 6
Langmuir, Freundlich and D-R isotherm constant parameters.
Isotherm
Parameters
30ºC
45ºC
60ºC
Langmuir
qmax (mg g )
337.3
413.6
448.1
KL (L mg–1)
R2
Kf (mg g–1 L1/n mg1/n)
n (–)
R2
E (kJ mol–1)
qmax (mol g–1)
R2
0.232
0.964
85.81
3.396
0.874
0.543
313.1
0.828
0.248
0.981
101.17
3.286
0.926
0.459
364.0
0.918
0.383
0.973
130.33
3.636
0.840
0.743
423.3
0.964
Freundlich
D-R
Fig. 7. Adsorption isotherms of Pb2+ on APTMS-Monosil T = 30°,
45° and 60°C (points: experimental data; continuous curves:
Langmuir isotherms with parameters taken from Table 6).
1 ε 2
qe = qmax exp −
2 E
1
ε = RT ln 1 + C
e
–1
(9)
where R and T are the gas constant (kJ mol–1 K–1) and absolute temperature (K), respectively, and qmax (mg·g) and E (kJ
mol–1) are the model parameters. As indicated above, qmax
represents the maximum possible amount of adsorbate; E,
on the other hand, is the mean free energy of adsorption per
mole of adsorbate when it is transferred to the surface of
solid from infinity in the solution.
In order to compare the three isotherms considered,
the optimal values of the parameters were estimated starting from the linearized forms of Eqs. (7–9). The results of
the regressions, together with the regression coefficients
R2, are presented in Table 6. The comparison among the
different regressions indicates that the Langmuir isotherm
consistently gives the best fit to experimental data, and
for this reason the curves relative to the Langmuir isotherms using the parameters taken from Table 6 have been
reported in Fig. 7.
The results of Table 6 and the very good agreement between Langmuir isotherms and experimental
data shown in Fig. 7 suggest that Pb2+ adsorption on
APTMS-Monosil takes place as a monolayer or, in other
words, that all the adsorbing sites are equivalent, and
capable of capturing a single Pb2+ ion each. In particular,
the amino groups available on the silica surface can form
complexes with Pb2+ ions [13], and it can be assumed that
each couple of amino groups adsorbs a Pb2+ ion according
to the scheme of Fig. 8.
Fig. 8. Schematic of adsorption mechanism of Pb2+ by
APTMS-Monosil nanocomposite.
Furthermore, it is interesting to observe that both the
maximum adsorption capacity qmax and the affinity constant KL significantly increase with temperature: qmax has an
almost fivefold increase between 30° and 60°C: this could be
due to a more active chelating effect of amino groups with
increasing temperature. For what concerns KL, its dependence on temperature was used to determine the thermodynamic parameters of the adsorption process according to
the following equations:
∆G o = − RT ln K L
− ∆H o ∆So
+
ln K L =
RT
R
o
o
o
T ∆S = ∆H − ∆G
(10)
where ∆Go, ∆Ho and DSo are the standard changes in Gibbs
free energy, enthalpy and entropy, respectively. ∆Ho and ∆So
H. Sharififard et al. / Desalination and Water Treatment 105 (2018) 287–297
295
can be obtained as the slope and intercept of a plot of ln (KL)
vs. 1/T (Fig. 9). Calculated thermodynamic parameters are
reported in Table 7.
The positive value of ∆H° confirms that the Pb2+ adsorption on APTMS-Monosil has an endothermic nature. Furthermore, its relatively high value is in good agreement
with the adsorption mechanism devised above, which has a
strong chemical (rather than purely physical) nature. Eventually, it must be pointed out that the high value of DSo
counterbalances the value of ∆Ho, leading to a negative ∆Go
(spontaneous process).
The maximum adsorption capacity of APTMS-Monosil for Pb2+ (about 450 mg·g–1 at T = 60°C.) was also compared with the adsorption capacity of other adsorbents
proposed for Pb2+ removal [50,51,54–67]. The results of this
comparison, reported in Fig. 10 and in Table 8, indicate that
APTMS-Monosil has very interesting performances.
Fig. 9. Relationship between ln (KL) and 1/T for Pb2+ adsorption
on APTMS-Monosil.
3.5. Regenerability tests
Table 7
Thermodynamic parameters at T = 298 K for Pb2+ adsorption on
APTMS-Monosil
∆H°, kJ·mol–1
30.9
DS° , kJ·mol–1 K–1
∆G°, kJ·mol–1
0.187
–24.826
In order to verify the capacity of APTS–Monosil to withstand a number of repeated adsorption–desorption cycles, a
series of experiments in which the same sample was used
to remove Pb2+ from a solution having a Pb2+ concentration
of 100 mg/l was carried out. As mentioned above, between
two removal experiments the sample was regenerated by
treatment with 0.1 M EDTA. The results for adsorption-desorption cycles of Pb2+ are presented in Fig. 11. As the results
show, the adsorption percentage of lead decreased from
Table 8
Comparison of Pb2+ adsorption capacity (mg g–1) of different
adsorbents [45,46,49–62]
Adsorbent
Pb2+ adsorption
capacity (mg g–1)
Reference
Goethite nanoparticles
HAp/Fe3O4 microspheres
Modified mesoporous
carbon
APTMS-Monosil
Chitosan nanoparticles
Hydrated maganes oxide
(HMO)
Polymer-based hybrid
Zeolite (Clinoptilolite)pretreated
Iron-activated carbon
(IAC) nanocomposite
MHC/OMCNTs
Co0.6Fe2.4O4 micro-particles
Activated carbon/Fe3O4
nanocomposite
Activated carbon
Pine cone activated carbon
Fe3O4 nanospheres
Fe3O4/SiO2 nanocomposite
Nanometer titanium
dioxide/silica gel
820.5
540
500
49
62
50
450
400
325
(This work)
51
52
181.4
122
53
58
121.9
61
116.3
80.32
71.42
54
59
60
51.81
27.53
18.47
17.65
3.16
46
45
55
56
57
Fig. 10. Comparison of Pb2+ adsorption capacity (mg g–1) of different adsorbents [45,46,49–62].
Fig.11. Removal efficiency of Pb2+ on APTMS-Monosil as a function of regeneration cycles of the adsorbent.
296
H. Sharififard et al. / Desalination and Water Treatment 105 (2018) 287–297
100% to 86.4%. The limited extent of decrease in adsorption
indicates a very high regenerability of the proposed material.
[9]
[10]
4. Conclusions
Amino-functionalized silica monolith (APTMS-Monosil) was synthesized and tested in several batch experiments
as a highly porous adsorbent for Pb2+ removal from aqueous
solution. The RSM results indicated that solution pH and
solid to liquid ratio are the most significant removal parameters, and that the optimum operating conditions are pH of
5.9, solid to liquid ratio of 1.74 g L–1 and initial Pb2+ concentration of 84 mg L–1. In these conditions, practically 100% of
Pb2+ present in solution can be removed by APTMS-Monosil. The kinetics of Pb2+ removal is controlled by the adsorption pseudo–reaction rather than intraparticle diffusion,
and this reaction can be described by a second order kinetic
equation. The Langmiur isotherm satisfactorily describes
equilibrium adsorption of Pb2+ on APTMS-Monosil. Results
show that this process has a markedly chemical nature, and
that the maximum adsorption capacity of APTMS-Monosil
is about 450 mg·g–1 at 60°C. The comparison between the
adsorption capacity exhibited by APTMSMonosil and the
capacities reported in the literature for other adsorbing
materials is very favorable. Furthermore, APTMS-Monosil
exhibits a good capacity of withstanding several adsorption-regeneration cycles.
Based on this analysis, APTM-functionalized Monosil adsorbent could be an excellent candidate for practical applications in the removal of Pb2+ from wastewater,
and continuous removal experiments in columns systems
should be carried out in order to better evaluate it. Last
but by now way least, preparation and application costs of
APTMS-Monosil will have to be taken into account to fully
ascertain its practical applicability.
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