2. out in inert gas (N2). Fe3O4 nanoparticles were synthesized by
co-precipitation of ferric and ferrous salts. The amount 6.4795 g of
FeCl3·6H2O and 3.3339 g of FeSO4·7H2O were dissolved into 150 mL
of deoxygenated distilled water. After stirring for 30 min, chemical pre-
cipitation was achieved at 30 °C under vigorous stirring by adding
20 mL of NH3·H2O solution (28%, v/v). During the reaction process, pH
was maintained at about 10. The reaction system was kept at 70 °C for
1 h. 1 g chitosan flake was dissolved in a 150 mL CH3COOH solution
2% (w/v). The chitosan solution was then dropped into the obtained
magnetic fluid in the flask through a dropper. Afterwards, 2 mL of
pure epichlorohydrin was added into reaction flask and stirred at
85 °C for 3 h, before the flask was cooled down to room temperature.
The precipitate was washed with distilled water to remove all existing
in the effluents. Silver nitrate (AgNO3) was used to detect residue of
Cl−
. The precipitate was then washed with ethanol and dried at 50 °C,
in the vacuum oven.
2.3. Adsorption experiments
The sorption experiments were performed by batch method. Sam-
ples of 0.1 g of magnetic chitosan nanoparticles were equilibrated with
50 mL of solution containing various amount of Cr(VI). The pH value
of solutions was adjusted by using diluted solution of NaOH and HCl.
The temperature of the solutions (25 °C, 35 °C, 45 °C) was controlled
with the thermostatic bath. The adsorbed amount of Cr(VI) per unit
weight of magnetic chitosan nanoparticles, qt (mg·g−1
), was calculated
from the mass balance equation as:
qt ¼
C0−Ctð Þ⋅V
m
ð1Þ
where C0 and Ct (mg/L) are the initial Cr(VI) concentration and the Cr(VI)
concentrations at any time t, respectively; V (L) is the volume of the
Cr(VI) solution; and m (g) is the mass of the magnetic chitosan
nanoparticles. Samples of the Cr(VI) solution were collected at pre-
determined time intervals and analyzed using a UV–Vis Spectrophotom-
eter (model UV-PC1600, Shimadzu), at λmax=540 nm, according to the
1,5-diphenyl-carbazide method [21]. All measurements were conducted
triplicate.
2.4. Characterization methods
X-ray diffraction (XRD) patterns were obtained at room tempera-
ture by D8 Advance, Bruker ASX, using CuKα radiation (λ=1.5406 Å)
Fig. 1. Camera pictures (a, b); FE-SEM images (c, d) and TEM images (e, f) of magnetic chitosan nanoparticles.
1215N.N. Thinh et al. / Materials Science and Engineering C 33 (2013) 1214–1218
3. in the range of 2θ=10°–60°, and a scanning rate of 0.02°·s−1
. Mor-
phology of magnetic chitosan nanoparticles was analyzed by Field
Emission Hitachi S-4500 Scanning Electron Microscope (FE-SEM) and
Transmission Electron Microscope (TEM, JEOL, Voltage: 80 kV). Absor-
bance measurements were carried out using Shimadzu UV-PC1600
spectrophotometer in the range of 400–800 nm.
The magnetic properties were measured with home-made vibrat-
ing sample magnetometer (VSM) and evaluated in terms of satura-
tion magnetization and coercivity. Chemical composition of samples
was determined by JEOL Scanning Electron Microscope and Energy
Dispersive Spectroscopy (SEM/EDS) JSM-5410 Spectrometer.
3. Results and discussion
3.1. Characterization of magnetic chitosan nanoparticles
TEM and SEM micrograph of magnetic chitosan particles provides in-
formation on their size and morphology. It can be observed from Fig. 1
that the magnetic particles have a spherical shape with a diameter of
about 30 nm.
XRD pattern of magnetic chitosan nanoparticles shows six charac-
teristic peaks for Fe3O4 corresponding to (220), (311), (400), (422),
(511) and (440) (JCPDS file, PDF No. 65-3107) (Fig. 2). Quite weak dif-
fraction lines of composite indicated that Fe3O4 particles have been coat-
ed by amorphous chitosan, which did not affect the phase and structure
of Fe3O4. Particle size of magnetic chitosan nanoparticles can be estimat-
ed approximately as 30 nm, via line broadening in the pattern, using
Debye–Scherrer equation (d=kλ/βcos θ).
Typical magnetization loops were recorded by VSM and shown on
Fig. S1 (supporting information). From the plot of magnetization vs.
magnetic field and its enlargement near the origin, the saturation
magnetization, remanence magnetization, coercivity and squareness
could be calculated. Because of no remanence and coercivity, it can be
suggested that the beads are superparamagnetic. It can also be observed
from this figure that magnetization moment of Fe3O4 nanoparticles
decreases very little after chitosan surface coating, meaning that chito-
san does not affect magnetic properties of these magnetic chitosan
nanoparticles. Therefore, maintaining such a high saturation magnetiza-
tion value (Ms) after coating these nanoparticles is advantageous and
susceptible to the external magnetic field for magnetic separation.
3.2. Effect of initial pH on the adsorption process
It is well known that some metals are preferentially adsorbed in acid-
ic media while chitosan can dissolve under this acidic condition. In this
regard, the chemical modification of chitosan by using crosslinking reac-
tion offers an important pathway for producing chemically more stable
chitosan derivatives, extending the potential applications of this bio-
polymer. In our study, the crosslinking approach with epichlorohydrin
to block/crosslink via hydroxyl (OH) group is expected to improve
chemical stability, mechanical resistance and adsorption/desorption
properties, compared to that with glutaraldehyde (to block amino
(NH2) group respectively), when keeping reactive amino groups intact
for complexing reaction with heavy metal ions [14,16,19].
Next, selecting an optimum pH is very important for the adsorp-
tion process, since pH affects not only the surface charge of adsorbent,
but also the degree of ionization and the speciation of the adsorbate
during the reaction. The effect of pH on the adsorption process was
investigated over the range from 2 to 6. As indicated in Fig. 3, the
maximum capacity of Cr(VI) absorption occurred at pH of 3. The ex-
planation would be addressed as the pH of the aqueous solution af-
fects to stability of chromium speciation and the surface charge of
the adsorbent. At pH 1, the chromium ions exists in the form of
H2CrO4, while in the pH range of 1–6, different forms of chromium
such as Cr2O7
2−
, HCrO4
−
, and Cr3O10
2−
coexist while HCrO4
−
predominates.
As the pH increases, those form shifts to Cr2O4
2−
and Cr2O7
2−
[11]. Cr(VI)
exists predominantly as HCrO4
−
in aqueous solution below pH 4 and the
amino groups (–NH2) of magnetic chitosan nanoparticles would be in
protonated cationic form (–NH3
+
) to a higher extent in acidic solution.
This results in the stronger attraction for negatively charged ions.
Electrostatic interaction between the sorbent and HCrO4
−
ions also con-
tributes to the high chromium removal. However, at the pH lower than
3, decrease in uptake capacity is observed as the predomination of
H2CrO4 and the strong competition for adsorption sites between
H2CrO4 and protons. The decreasing of the adsorption capacity at higher
pH values may be explained by the dual competition of CrO4
2−
and OH−
for adsorption [11]. Thus, pH 3 was selected as the optimum pH value for
the following adsorption experiment.
3.3. Adsorption isotherms
Equilibrium experimental data were successfully fitted to the
Langmuir isotherm whose equation can be expressed as
q ¼
qm⋅KL⋅Ce
1 þ KL⋅Ce
ð2Þ
where qm (mg·g−1
) is the maximum sorption capacity (corresponding
to complete monolayer coverage), Ce is the equilibrium concentration
in the solution (mg/L), qe is the equilibrium Cr(VI) concentration in
20 30 40 50 60 70
(440)
(511)
(422)
(400)
(311)
(220)
Intensity
2θ
Fig. 2. XRD pattern of magnetic chitosan nanoparticles.
2 3 4 5 6
50
55
60
65
70
75
80
85
R(%)
pH
Fig. 3. The influence of initial pH value on the adsorption of the Cr(VI) on magnetic
chitosan nanoparticles.
1216 N.N. Thinh et al. / Materials Science and Engineering C 33 (2013) 1214–1218
4. the sorbent (mg·g−1
), and KL is the sorption affinity constant related to
the binding energy of sorption (L·mg−1
). The experimental data
(Table 1) fitted well with Langmuir model (R2
>0.99), confirming that
the adsorption process is monolayer adsorption. The results of adsorp-
tion studies by Langmuir model, indicating improved Cr(VI) uptake
properties of magnetic chitosan nanoparticles (55.80 mg·g−1
, pH 3,
room temperature, compared to the other adsorbents (Table 2)), proba-
bly relates to the smaller loss of amine groups of chitosan, involved in
the cross-linking reaction when using epichlorohydrin as a cross-linker.
Cr(VI) removal by adsorbent as a function of contact time with
different initial concentrations (40, 80 and 180 mg·L−1
) of Cr(VI) is
shown in Fig. 4, where the adsorption rate of metal uptake was
quite slow and the maximum uptake was observed within 100 min.
3.4. Thermodynamic and kinetic studies
In this section, thermodynamic and kinetic aspects of the adsorp-
tion process will be considered. The experimental data obtained at
different temperatures were used in calculating the thermodynamic
parameters such as Gibbs free energy (ΔG), enthalpy (ΔH) and entro-
py (ΔS) according to the following equations:
ΔG ¼ ΔH−T Â ΔS ð3Þ
lnK ¼ ln qe=Ceð Þ ¼ −ΔH=RT þ ΔS=R: ð4Þ
Where K is the equilibrium constant, obtained from Langmuir iso-
therms at different temperature and R is the universal gas constant.
ΔH and ΔS were obtained from the slope and intercept of the plot
log (qe/Ce) vs. 1/T (Fig. 5), namely:
ΔH ¼ −0:6853 kJ⋅mol
−1
and ΔS ¼ −115:7366 J⋅mol
−1
⋅K
−1
:
Table 1
Adsorption equilibrium constants obtained from Langmuir isotherm in the adsorption
of Cr(VI) onto magnetic chitosan nanoparticles (volume: 50 mL; absorbent dose: 0.1 g;
initial concentrations: 60, 80 and 180 mg·L−1
; pH value: 3.0; temperature: 298,308,
318 K).
Temperature (K) qmax (mg·g−1
) KL R2
298 55.80 0.366 0.993
308 46.71 0.119 0.997
318 43.29 0.138 0.994
Table 2
Comparison of adsorption capacities of Cr(VI) with other adsorbents.
Adsorbents Adsorption capacity
(mg·g−1
)
pH Ref.
Tires activated carbon 58.50 2.0 [23]
Rubberwood activated carbon 44.05 2.0 [3]
Coconut shell activated carbon 20.00 2.0 [24]
Hazelnut shell activated carbon 17.70 2.0 [25]
Beech sawdust 16.10 1.0 [26]
Sugarcane bagasse 13.40 2.0 [27]
Coconut shell charcoal 10.88 4.0 [28]
Coconut tree sawdust 3.60 3.0 [29]
Chitosan 22.09 3.0 [30]
Non-cross linked chitosan 78.00 5 [31]
Cross linked chitosan 50.00 5 [31]
Magnetic chitosan nanoparticles (this
study)
55.80 3
0 50 100 150 200 250 300 350 400
10
15
20
25
30
35
40
45
50
55
60
65
70
q(mg/g)
t(min)
40mg/L
80mg/L
180mg/L
Fig. 4. Effect of contact time on Cr(VI) adsorption (volume: 50 mL; absorbent dose: 0.1 g;
initial concentrations: 40, 80 and 180 mg·L−1
; pH value: 3.0; temperature: 298 K).
3.20 3.22 3.24 3.26 3.28 3.30 3.32 3.34 3.36
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
y=-13.92069+4.38115x,R=0.99017
Ln(qe/Ce)
1/T*10-3
(1/K)
C=80 mg/L
Fig. 5. Thermodynamic plot of ln (qe/Ce) vs. 1/T.
Table 3
Thermodynamic data of Cr(VI) adsorption process.
T (K) ΔG (kJ·mol−1
) ΔH (kJ·mol−1
) ΔS (J·mol−1
·K−1
)
298 −35.164 −0.6853 −115.7366
303 −35.742
307 −36.205
312 −36.784
-50 0 50 100 150 200 250 300 350
-7
-6
-5
-4
-3
-2
-1
0
1
2
3
4
t(min)
40mg/L
80mg/L
180mg/L
ln(qe-qt)
Fig. 6. Kinetic pseudo-first order sorption kinetics of Cr(VI) (volume: 50 mL; absorbent dose:
0.1 g; initial concentrations: 40, 80 and 180 mg·L−1
; pH value: 3.0; temperature: 298 K).
1217N.N. Thinh et al. / Materials Science and Engineering C 33 (2013) 1214–1218
5. The negative value of ΔG obtained from Eq. (3) reflects a spontane-
ous (favorable) adsorption process of Cr(VI) (Table 3), while the nega-
tive value of ΔH indicates that the adsorption reaction is exothermic
and the adsorption of Cr(VI) is more effective at lower temperatures.
Kinetically, in order to understand the behavior of the adsorbent and
to examine the controlling mechanism of the adsorption process, the
pseudo-first-order and the pseudo-second-order were applied to the ex-
perimental data (Figs. 6 and 7). The pseudo-first-order rate expression of
Lagergren is given as: ln(qe−qt)=ln(qe)−k1⋅t where qe and qt are the
amounts of Cr(VI) (mg·g−1
) adsorbed on the adsorbent at equilibrium
and at time t, respectively and k1 is the rate constant of first-order adsorp-
tion (min−1
). The slopes and intercepts of plots of ln(qe−qt) vs. t were
used to determine the first-order rate constant k1. The pseudo-
second-order kinetic model is expressed as: t
qt
¼ 1
k2⋅qe
2 þ 1
qe
 t where k2
(g·mg−1
·min−1
) is the rate constant of second order adsorption. The
slopes and intercepts of plots of t/qt vs. t were used to calculate the
second-order rate constant k2 and qe [22]. Adsorption rate constants
were summarized in Table 4. The values of regression coefficient for
pseudo-second-order model were close to 1 for all initial Cr(VI) concen-
trations. The calculated values qe,cal were very close to obtained qe,exp
values. Hence, the adsorption of Cr(VI) onto magnetic chitosan nano-
particles could obey the pseudo-second-order kinetic model.
4. Conclusion
In this work, cross-linked with epichlorohydrin magnetic chitosan
nanoparticles were prepared and characterized. The Cr(VI) adsorption
behavior on the prepared magnetic chitosan nanoparticles has been
studied under various conditions of different solution pH values and ad-
sorption contact times. Optimal adsorption conditions of Cr(VI) were
found at pH 3, and contact time of 100 min, with maximum adsorption
capacity of 55.80 mg·g−1
. The Langmuir model was found to fit
well with the experimental data (correlation coefficient R2
0.99),
indicating the occurrence of monolayer adsorption process. Ther-
modynamically, the adsorption of Cr(VI) is spontaneous (in term
of ΔG) and exothermic (in term of ΔH) process. Kinetically, the
adsorption of Cr(VI) onto magnetic chitosan nanoparticles obeyed
the pseudo-second-order model. Compared to the other adsor-
bents, magnetic chitosan nanoparticles shows greatly improved
uptake properties of Cr(VI), probably due to high concentration of
remaining active sites on the surface of magnetic chitosan nano-
particles. The improved magnetic and adsorption uptake properties
are two main features of the synthesized nanoparticles that can be
advantageously used in water treatment.
Acknowledgments
Funding of this work was provided by Vietnam Ministry of Science
and Technology (grant 08/2011/HÐ-NÐT).
Appendix A. Supplementary data
Supplementary data to this article can be found online at http://
dx.doi.org/10.1016/j.msec.2012.12.013.
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0 50 100 150 200 250 300 350
0
2
4
6
8
10
12
14
16
18
40mg/L
80mg/L
180mg/L
t/qt(min.g/mg)
t(min)
Fig. 7. Kinetic pseudo-second order sorption kinetics of Cr(VI) (volume: 50 mL; absor-
bent dose: 0.1 g; initial concentrations: 40, 80 and 180 mg·L−1
; pH value: 3.0;
temperature: 298 K).
Table 4
Comparison of the first-order and second-order adsorption rate constants, calculated qe,cal and experimental qe,exp values for different initial Cr(VI) concentrations.
C0 (mg·L−1
) qe,exp (mg/g) First-order kinetic model Second-order kinetic model
k1 (min−1
) qe,cal (mg·g−1
) R2
k2(g·mg−1
·min−1
) qe,cal (mg·g−1
) R2
40 19.42 0.029 5.59 0.946 8.38×10−3
19.94 0.994
80 37.05 0.030 25.43 0.876 2.08×10−3
38.46 0.992
180 53.8 0.025 22.04 0.956 2.16×10−3
55.55 0.996
1218 N.N. Thinh et al. / Materials Science and Engineering C 33 (2013) 1214–1218