The effect of initial salt composition on the formation of zero-valent bimetallic FeCo was investigated in this work. Pure crystalline zero-valent FeCo nanoparticles (NPs) were obtained using either chloride or nitrate salts of both metals. Smaller NPs can be obtained using nitrate salts. Comparing the features of the FeCo prepared at room temperature and the solvothermal method revealed that both materials are almost identical. However, the room-temperature method is simpler, quicker, and saves energy. Energy-dispersive X-ray (EDX) analysis of the FeCo NPs prepared using nitrate salts at room temperature demonstrated the absence of oxygen and the presence and uniform distribution of Fe and Co within the structure with the atomic ratio very close to the initially planned one. The particles were sphere-like with a mean particle size of 7 nm, saturation magnetization of 173.32 emu/g, and surface area of 30 m2/g. The removal of Cu2+ and reactive blue 5 (RB5) by FeCo in a single-component system was conformed to the pseudo-first-order and pseudo-second-order models, respectively. The isotherm study confirmed the ability of FeCo for the simultaneous removal of Cu2+ and RB5 with more selectivity toward Cu2+. The RB5 has a synergistic effect on Cu2+ removal, while Cu2+ has an antagonistic effect on RB5 removal.
The effect of initial salt composition on the formation of zero-valent bimetallic FeCo was investigated in this work. Pure crystalline zero-valent FeCo nanoparticles (NPs) were obtained using either chloride or nitrate salts of both metals. Smaller NPs can be obtained using nitrate salts. Comparing the features of the FeCo prepared at room temperature and the solvothermal method revealed that both materials are almost identical. However, the room-temperature method is simpler, quicker, and saves energy. Energy-dispersive X-ray (EDX) analysis of the FeCo NPs prepared using nitrate salts at room temperature demonstrated the absence of oxygen and the presence and uniform distribution of Fe and Co within the structure with the atomic ratio very close to the initially planned one. The particles were sphere-like with a mean particle size of 7 nm, saturation magnetization of 173.32 emu/g, and surface area of 30 m2/g. The removal of Cu2+ and reactive blue 5 (RB5) by FeCo in a single-component system was conformed to the pseudo-first-order and pseudo-second-order models, respectively. The isotherm study confirmed the ability of FeCo for the simultaneous removal of Cu2+ and RB5 with more selectivity toward Cu2+. The RB5 has a synergistic effect on Cu2+ removal, while Cu2+ has an antagonistic effect on RB5 removal.
Water quality is the main
affair that occupies humankind as it
is the source of life on Earth. Since our main goal is developing
a sustainable ecological environment, reuse of wastewater is vital.
The daily drainage of domestic and industrial wastewaters introduces
different contaminants to the aquatic environment, which reduces water
quality.[1] Treatment of textile wastewaters
is a worldwide concern since their release to the aquatic environment
is fatal to aquatic and human life due to their complex nature that
is composed of toxic trace metals and hazardous synthetic organic
dyes.[2] Among >10000 synthetic organic
dyes,
the reactive azo dyes are the most frequently used in the textile
industry because of the simple dyeing procedure and covalent binding
with cellulose fibers.[3,4] These dyes cause an aesthetic
problem, affect the photosynthesis process, form carcinogenic/mutagenic
intermediates, and can harm the liver and kidney.[5,6] On
the other hand, knowledge about the harmful impact and the toxicity
of trace metals has increased in the last two decades.[7] Of the trace metals, copper is a very toxic abundant and
naturally occurring element that has been detected in municipal wastewaters.
It causes vomiting, cramps, convulsion, and even death if it enters
the human body.[8]Several treatment
methods such as flocculation, ultrafiltration,
and the biological method have been used in textile wastewater treatment
and have been shown to be inefficient.[9−12] On the contrary, the adsorption
process, which is widely used, has been shown to be highly effective
and more economical.[13,14] Numerous materials have been
used as adsorbents. Among them, magnetic zero-valent-based bimetallic
nanoparticles (NPs) have attracted growing interest owing to their
promising features. For instance, magnetic FeCo alloys are characterized
by magnetic anisotropy energies, low magnetostriction, high resistivity,
great coercivity, large saturation magnetization, obvious Snoek’s
limit, and high Curie temperature.[15,16] However, the
preparation method determines the adsorption properties of FeCo alloys.Both sodium borohydride and hydrazine hydrate are used as reducing
agents in the preparation of zero-valent iron-based materials. However,
hydrazine hydrate outperforms sodium borohydride because it produces
high-purity Fe0 nanoparticles with good crystallinity and
higher magnetization. From the environmental point of view, hydrazine
hydrate produces harmless byproducts (nitrogen, hydrogen, and water)
upon complete decomposition, and the waste stream of the hydrazine
hydrate reduction process can be easily treated compared to that of
sodium borohydride.[17−19] Several methods based on hydrazine reduction have
been reported to prepare the FeCo alloy such as the texture-controlled
technique,[20] the polyol process,[21] hydrothermal synthesis,[22] electrodeposition,[23] mechanical alloying,[24] reductive salt-matrix annealing,[25] spray pyrolysis with hydrogen reduction,[26] organometallic route,[27] self-catalyzed coreduction method,[28] ultrasonic
wave-assisted solution method,[29] solution
phase method,[30] and coprecipitation.[31] However, some of these methods are complex,
energy-intensive, and/or result in low-crystalline and impure FeCo
alloys. In addition, the effect of the initial salt composition on
the features of the formed FeCo has not been investigated yet. This
work is devoted to filling this literature gap by studying, for the
first time, the effect of initial salt composition on the features
of the FeCo alloy. Furthermore, this work reports for the first time
the simultaneous removal of anionic and cationic contaminants from
contaminated water using FeCo alloys. More specifically, we report
an investigation on the effect of iron and cobalt salts on the formation
of nanosized zero-valent FeCo alloys using a simple one-step room-temperature
quick method. In this method, the salts of iron and cobalt are reduced
by hydrazine in an alkaline medium. In addition, the features of FeCo
prepared by this method were compared to those prepared by the solvothermal
method. The qualities of the prepared materials were investigated
using X-ray diffraction (XRD), field emission scanning electron microscopy
(FESEM), energy-dispersive X-ray (EDX), high-resolution transmission
electron microscopy (HRTEM), a vibrating sample magnetometer (VSM),
N2 adsorption at 77 K, and an X-ray photoelectron spectrometer
(XPS).The efficiency of the FeCo prepared at room temperature
and solvothermal
methods for the removal of reactive black 5 (RB5) dye and Cu2+ was compared. Finally, detailed parametric, kinetics, and isotherm
studies were executed on the removal of RB5 and Cu2+ by
the FeCo prepared at room temperature in single- and bicomponent systems.
Materials and Methods
Ferric nitrate
nonahydrate, (Fe(NO3)3·9H2O),
ferric chloride hexahydrate (FeCl3·6H2O),
cobalt nitrate hexahydrate (Co(NO3)2·6H2O), cobalt chloride heptahydrate (CoCl2·6H2O), cobalt sulfate heptahydrate (CoSO4·7H2O), sodium hydroxide (NaOH), hydrazine hydrate
(N2H4·7H2O), sodium chloride
(NaCl), and copper sulfate pentahydrate (CuSO4·5H2O) were purchased from Sigma–Aldrich and used as received.
Reactive blue 5 was obtained from a local dyeing factory.
Preparation Methods
Room-Temperature Method
First,
precise amounts of iron and cobalt salts were weighed to obtain a
theoretical Fe0:Co0 mass ratio of 1:1 and then
dissolved in 20 mL of ethanol. Then, 5.0 g of NaOH was added to the
solution under stirring followed by 10 mL of hydrazine hydrate. Stirring
was continued until homogeneity. The resulting magnetic product was
collected by magnetic separation and washed with hot distilled water
and then absolute ethanol several times. Finally, the products were
dried in a vacuum oven at 40 °C. Table gives the codes of the prepared samples
and the salts used in their preparation.
Table 1
Salts Used in the Preparation of FeCo
Alloy and the Code of Resulting Samples
sample code
1
salt
Fe(NO3)3·9H2O
Co(NO3)2·6H2O
weight
1.5390 g
0.9876 g
2
salt
Fe(NO3)3·9H2O
CoCl2·6H2O
weight
1.5390 g
0.8075 g
3
salt
Fe(NO3)3·9H2O
CoSO4·7H2O
weight
1.5390 g
0.9540 g
4
salt
FeCl3·6H2O
Co(NO3)2·6H2O
weight
0.9680 g
0.9876 g
5
salt
FeCl3·6H2O
CoCl2·6H2O
weight
0.9680 g
0.8075 g
6
salt
FeCl3·6H2O
CoSO4·7H2O
weight
0.9680 g
0.9540 g
Solvothermal Method
A typical solvothermal
method using chloride salts of iron and cobalt (sample 5 in Table ) was followed. The
sample preparation followed the same steps as previously, but, after
homogeneity, the mixture was transferred into a Teflon-lined stainless-steel
autoclave and kept at 80 °C for 12 h. Afterward, the autoclave
was left to cool down to room temperature, and the product was washed
and separated as illustrated above. The resulting sample was coded
as 7.
Characterization Methods
The crystal
structure of the prepared materials was characterized by an X-ray
diffractometer (Bruker AXS D8 advance instrument) between 5 and 80°
(2θ). The morphology, composition, and metal distribution were
obtained by JEOL 6400 F field emission scanning electron microscopy
(FESEM) with energy-dispersive X-ray analysis (EDX). Transmission
electron microscopy (JEOL TEM-2100) was used to characterize the internal
structure of the materials. The magnetic properties were investigated
through a vibrating sample magnetometer (LakeShore 7410). A BELSORP-max
surface analyzer was used to obtain the N2 adsorption–desorption
isotherms at 77 K. The Brunauer–Emmett–Teller specific
surface area (SBET) and the nonlocal density
functional theory (NLDFT) pore size distribution were determined from
the obtained N2 adsorption–desorption isotherms.
The surface elemental composition and states of the materials were
investigated by an X-ray photoelectron spectrometer (XPS) (K-Alpha
system, Thermo Fisher Scientific) with an X-ray Al K-Alpha monochromator
source and an X-ray spot size of 50–400 μm. Full-spectrum
range was acquired using a pass energy of 200 eV at a narrow spectrum
of 50 eV.The salt addition method was used to determine the
pH of the point of zero charge (pHpzc) of the FeCo alloy.[32] A series of sodium chloride solutions of concentration
0.01 mol/L was adjusted to initial pH (pHo) values of 2,
4, 6, 8, and 10 using 1 mol/L NaOH or HCl solutions. Afterward, 0.25
g of both FeCo alloys was added to 50 mL of each salt solution and
shaken for 24 h at room temperature. The final pH was measured, and
the changes in the solution pH values (ΔpH), calculated as the
difference between the final and initial pHs, were plotted versus
pHo. The pHpzc was identified through the intersection
of the curve with the x-axis (pHo).
Adsorption Study
First, the efficiency
of the FeCo prepared by solvothermal and room-temperature methods
toward Cu2+ and RB5 was compared. Then, the best sample
was used to investigate the effects of the adsorbent dosage and initial
pH (pHo) as a function of contact time on the adsorption
process. The aforementioned experiments were performed in a single-component
adsorption system. Finally, two types of adsorption isotherms were
performed: isotherm with a single adsorptive (Cu2+ or RB5)
and isotherm with binary mixtures of both Cu2+ and RB5.
In the binary mixture, two sets of experiments were performed: one
with a constant initial concentration of RB5 (30 mg/L) and a variable
initial concentration of Cu2+ (10–250 mg/L), and
the second with a constant initial concentration of Cu2+ (100 mg/L) and a variable initial concentration of RB5 (10–50
mg/L). All of the experiments were conducted in 250 mL conical flasks
at room temperature using a speed-adjustable Orbital shaker. Samples
were withdrawn at different time intervals; then, FeCo was magnetically
separated and the remaining concentration of RB5 or Cu2+ was determined. A Jasco V730 was used to determine the concentration
of the RB5 dye. Six different initial concentrations of the dye were
measured to construct a calibration curve. The maximum wavelength
was found at 598 nm. Figure S1 gives the
UV–vis spectra of the RB5 dye and the calibration curve. Copper
ion concentrations were determined using inductively coupled plasma
optical emission spectrometry (ICP-OES, Agilent 5100) in the prepared
samples. Details about the experimental conditions are given in the
caption of figures, and details about the analysis of adsorption data,
including kinetic and isotherm models and the criteria of selecting
the best fitting model, are given in the Supporting Information.
Results and Discussion
Characteristics of the Prepared Materials
Hydrazine hydrate (N2H4·H2O) is a low-cost and low-impurity potent reducing agent; therefore,
it has been widely used for the synthesis of several nanosized materials.
In this work, the FeCo alloy was prepared by the reduction of Fe and
Co salts using N2H4·H2O in an
alkaline medium according to the following reactionsIn these reactions, NaOH acts as a
precipitant that converts the Fe and Co salts to their hydroxides
(eq ) and also enhances
and maintains the reducing ability of N2H4·H2O (eq ).The formation of FeCo at ambient conditions starts by the reduction
of Co2+ to Co0 (eq ), which subsequently catalyzes the reduction of Fe3+ to Fe0 (eq ). Thus, Co0 enters the lattice of Fe0 particles, forming the FeCo alloy.[30] This
sequence of reaction is due to the fact that the Co2+/Co0 reduction potential (−0.73 V) is higher than that
of Fe+3/Fe0 (−0.77 V); therefore, N2H4·H2O can reduce Co2+ at ambient temperature and pressure, but the reduction of Fe3+ requires surface catalysis or high pressure.[29,30] Noteworthy, the N2 generated during the reaction could
protect the formed FeCo against oxidization.[33]Figure a shows
the XRD patterns of the samples prepared according to Table . All of the prepared samples
show two diffraction peaks at 2θ = 44 and 65° characteristic
of the crystal planes of (1 1 0) and (2 0 0) of the body-centered
cubic (bcc) phase of the FeCo alloy (JCPDS card No: 49-1567). However,
the purity of the samples is different. Relatively weak diffraction
peaks could be observed in the patterns of sample no. 2 at 2θ
= 31 and 38° and sample no. 3 at 2θ = 38 and 51°.
These peaks indicate the presence of cobalt oxide (JCPDS card No:
02-0770), which implies a slight oxidation in these samples. In sample
no. 6, diffraction peaks can be observed at 2θ = 51 and 75°
and 2θ = 41 and 47°, which can be assigned to the face-centered
cubic phase of Co0 (JCPDS card Nos: 15-0806 and 01-1277,
respectively). Contrariwise, no impurity peaks can be noticed in samples
no. 1, 4, 5, and 7, indicating the successful coreduction of Fe and
Co salts and the formation of a highly crystalline pure single bcc-FeCo
phase. Obviously, the intensity of the diffraction peaks of samples
no. 1 and 7 is relatively low, which could be ascribed to the smaller
particle size of these samples. To verify this assumption, the particle
shape and size of these samples were determined by HRTEM and are displayed
in Figure b–e.
Figure 1
XRD (a)
and HRTEM and particle size distribution histogram (b,
c, d, and e) of FeCo sample nos. 1, 4, 5, and 7, respectively.
XRD (a)
and HRTEM and particle size distribution histogram (b,
c, d, and e) of FeCo sample nos. 1, 4, 5, and 7, respectively.Figure b–e
reveals that sample nos. 1, 4, 5, and 7 are composed of sphere-like
nanoparticles (NPs); however, the samples have different particle
sizes and degrees of agglomeration. Sample nos. 4, 5, and 7 (Figure c–e) agglomerate
into large clusters, while sample no. 1 is well dispersed. The aggregation
of NPs creates several interparticle voids, which could result in
high surface area.It is known that the reactivity of Fe0-based bimetals
increases as their particle size decreases.[34] Therefore, the particle size of sample nos. 1, 4, 5, and 7 was compared
to select the most reactive sample. The particle size of sample nos.
1 and 7 ranged between 2–16 and 4–13 nm with a mean
of 7 and 8 nm, respectively. However, sample nos. 4 and 5 have particles
with sizes ranging between 15–59 and 13–41 nm and a
mean of 35 and 26 nm, respectively. Thus, it can be concluded that
sample nos. 1 and 7 have similar particle sizes, which is significantly
smaller than those of sample nos. 4 and 5.Overall, the results
of XRD and HRTEM indicate that the initial
salt composition has a paramount effect on the purity and particle
size of the produced FeCo. Although the anions of Fe and Co salts
do not take part directly in the reactions of FeCo formation (eqs –3), they play a key role by constituting the ionic atmosphere,
which affect the reaction rate. Increasing the ionic strength of the
reaction solution causes a decrease in the reaction rate and favors
the formation of smaller particles.[35] Herein,
the ionic strength of the solutions used for the preparation of sample
no. 1 was calculated to be 3.30 mol/L, while that of sample nos. 4,
5, and 7 was 3.18 mol/L. Therefore, sample no. 1 has the smallest
particle size and sample nos. 4 and 5 have comparable particle sizes.
Subjecting sample no. 5 to a solvothermal treatment step to get sample
no. 7 decreased the particle size considerably; the mean particle
size decreased from 26 to 8 nm.In a nutshell, the XRD and particle
size results reflect that both
solvothermal and room-temperature methods using Fe and Co nitrate
salt methods can efficiently prepare pure highly crystalline nanoscale
zero-valent bimetallic FeCo alloys with almost the same particle size.
Therefore, the characteristics of both sample nos. 1 and 7 were further
explored. Henceforward, sample nos. 1 and 7 were referred to as room-temperature
and solvothermal methods, respectively.Figure compares
the structure characteristics of FeCo prepared by solvothermal and
room-temperature methods. The FESEM images (Figure a,b) show that FeCo produced by both methods
forms large aggregates with interparticle voids. The attractive magnetic
forces between the particles cause the formation of such aggregates.[36] A higher degree of aggregation can be observed
for the sample prepared by solvothermal methods (Figure a); consequently, this sample
has more interparticle voids. Figure a shows that the sample prepared by the solvothermal
method has a three-dimensional structure with spicate branches, which
aggregate in an irregular shape. While the sample prepared at room
temperature (Figure b) is mainly quasi-spherical with an irregular salient. Stacking
of the initial particles results in the appearance of conelike and
double-conelike structures as minor morphologies. The difference between
the HRTEM and FESEM of the sample prepared at room temperature is
due to the different pretreatment of the sample for each characterization
technique.
Figure 2
FESEM (a, b) and EDX and elemental mapping (c, d) of FeCo prepared
by solvothermal and room-temperature methods, respectively.
FESEM (a, b) and EDX and elemental mapping (c, d) of FeCo prepared
by solvothermal and room-temperature methods, respectively.The coexistence of Fe and Co elements, their atomic
ratio, and
their distribution were evaluated by EDX and EDX mappings. Figure c,d proves the presence
of both Fe and Co in the samples prepared by both methods. Also, it
can be noticed that the Fe and Co are uniformly distributed within
the structure. The EDX spectra (Figure c,d) clarify that the presence of two peaks only corresponds
to Fe and Co. Importantly, the EDX analysis shows the absence of an
oxygen signal in the prepared samples, which further confirms the
successful preparation of zero-valent FeCo. The atomic ratios of Fe/Co
calculated from the EDX analysis were 54/46 and 55/45 for the sample
prepared by solvothermal and room-temperature methods, respectively.
Therefore, it can be concluded that both methods give almost the same
elemental composition of the FeCo alloy. These ratios also indicate
the closeness of the practical ratio to the initially designed composition.Figure a displays
the room-temperature magnetization curves of the prepared samples,
and Table lists the
values of magnetic parameters. The magnetization curves are S-shaped
with a hysteresis loop, which is characteristic of ferromagnetic materials.
The saturation magnetization of the sample prepared at room temperature
(173.32 emu/g) is insignificantly lower than that of the sample prepared
by the solvothermal method (182.02 emu/g). These values reflect the
high capability of magnetic separation and the consequent high removal
efficiency of the dispersed product from the aqueous medium, which
encourages its application in water treatment. Table also shows that both samples have almost
the same coercivity and retentivity. Specifically, the coercivity
values were 201.86 and 202.71 G for the samples prepared by solvothermal
and room-temperature methods, respectively. However, the value of
retentivity reached 12.92 emu/g for the sample prepared by the solvothermal
method and 12.38 emu/g for the sample prepared at room temperature.
Again, the results of the magnetic properties prove the close similarity
between the two preparation methods.
Figure 3
Magnetization curves (a), N2 adsorption–desorption
isotherm (b), NLDFT pore size distribution curve (c), and pHPZC (d) of bimetallic zero-valent FeCo nanoparticles prepared by solvothermal
and room-temperature methods.
Table 2
Magnetic and Textural Properties of
FeCo NPs Prepared by Solvothermal and Room-Temperature Methods
solvothermal method
room-temperature method
magnetization (emu/g)
182.08
173.32
coercivity (G)
201.86
202.71
retentivity (emu/g)
12.92
12.38
SBET (m2/g)
32.59
29.76
pore size (nm)
7.25
6.75
Magnetization curves (a), N2 adsorption–desorption
isotherm (b), NLDFT pore size distribution curve (c), and pHPZC (d) of bimetallic zero-valent FeCo nanoparticles prepared by solvothermal
and room-temperature methods.The N2 adsorption–desorption isotherms
of the
two FeCo samples are shown in Figure b. The isotherms of both samples belong to the type
II isotherm, while the hysteresis loops belong to type H3 of the IUPAC
classification. The type II isotherm is typical for nonporous and
macroporous materials, and the type H3 loop is common for nonrigid
aggregates of particles and macroporous materials partially filled
with pore condensate.[37] Thus, the N2 adsorption–desorption isotherms suggest nonporous
or macroporous materials. On the other hand, according to the NLDFT
pore size distribution curve (Figure c and Table ), mesopores dominate the porous structures of both samples,
implying that both samples are mainly mesoporous. These results seem
contradictory, but correlating the results of N2 adsorption,
FESEM, and HRTEM could reveal the nature of the materials. The results
of SEM and TEM illustrated that the materials are composed of aggregation
of NPs. Thus, the suggested mesoporosity of the materials by NLDFT
is a result of the interparticle voids of the aggregates, while the
suggested nonporosity by the N2 adsorption–desorption
can be attributed to the nature of FeCo NPs. In other words, the FeCo
NPs are nonporous and their aggregation gives rise to mesopores. The
specific surface area calculated by the multipoint Brunauer–Emmett–Teller
method (SBET, Table ) of the sample prepared by the solvothermal
method (32.59 m2/g) was slightly higher than that of the
sample prepared at room temperature (29.76 m2/g). This
result agrees with the results of FESEM and HRTEM, which illustrated
that the sample prepared by the solvothermal method has relatively
larger aggregates with more interparticle voids than the sample prepared
at room temperature.The point of zero charge (pHPZC) pHPZC is
the pH value at which the material surface charge becomes neutral.
It is of paramount importance for materials that are used as adsorbents
as it gives an indication about the surface charges of the material
at different pH values. Figure d displays the plot of ΔpH vs pHo. It can
be observed that the pHPZC of both samples is nearly identical
and its value is 8.3. Thus, at pH > 8.3, the surface of FeCo NPs
is
negatively charged, whereas at pH < 8.3, the surface of FeCo NPs
is positively charged.Conclusively, the results of the characterization
of the FeCo alloy
prepared by both solvothermal and room-temperature methods using Fe
and Co nitrate salts are almost identical; however, the preparation
at room temperature is advantageous as it is simple and saves energy
and time.
Contaminants’ Removal Properties
Zero-valent iron-based bimetallic nanoparticles can remove trace
metals, oxyanions, and different types of organic contaminants. The
mechanism of removal can be one or more of adsorption, coprecipitation,
reduction, oxidation, hydrodehalogenation, hydrogenation, or hydrodeoxygenation
based on the type of contaminant and experimental conditions.[38]The performance of both FeCo samples for
the removal of Cu2+ and RB5 was evaluated for comparison
purposes, and the results are graphed in Figure . Around 90% of Cu2+ was removed
by both samples after 45 min of contact time (Figure a). Thus, it can be concluded that both samples
have identical performance for the removal of Cu2+. These
results are logical and in line with the conclusion that the characteristics
of both materials are almost identical based on the discussion in
the characteristics of materials section.
Figure 4
Comparing the efficiency
of the FeCo alloy prepared at room temperature
and the solvothermal method for the removal of (a) Cu2+ (C 10 mg/L, pHo 5.5, dosage
0.10 g/L) and (b) RB5 (C 10 mg/L, pHo 5, dosage 1.00 g/L). Change of R % of (c)
Cu2+ (C 10 mg/L, dosage 0.10
g/L) and (d) RB5 (C 10 mg/L, dosage 1.00
g/L) at different pHo and (e) Cu2+ (C 10 mg/L, pHo 5.5) and (f) RB5 (C 10 mg/L, pHo 7) by different dosages
of the FeCo alloy prepared at room temperature.
Comparing the efficiency
of the FeCo alloy prepared at room temperature
and the solvothermal method for the removal of (a) Cu2+ (C 10 mg/L, pHo 5.5, dosage
0.10 g/L) and (b) RB5 (C 10 mg/L, pHo 5, dosage 1.00 g/L). Change of R % of (c)
Cu2+ (C 10 mg/L, dosage 0.10
g/L) and (d) RB5 (C 10 mg/L, dosage 1.00
g/L) at different pHo and (e) Cu2+ (C 10 mg/L, pHo 5.5) and (f) RB5 (C 10 mg/L, pHo 7) by different dosages
of the FeCo alloy prepared at room temperature.On the other hand, after 120 min of contact time,
the sample prepared
at room temperature removes 71% of the RB5, while the sample prepared
by the solvothermal method removes only 54% (Figure b). These results look odd since the characteristics
of both materials are very similar, as illustrated above. However,
a probable reason for the observed results can be deduced from the
SEM and TEM results. The results of SEM and TEM proved that the sample
prepared by the solvothermal method is more aggregated than the sample
prepared at room temperature. The aggregation blocks some adsorption
sites and increases the diffusion path length, which result in decreasing
the removal.[39,40] Thus, RB5 removal is lower by
the sample prepared by the solvothermal method.The difference
in the behavior of RB5 and Cu2+ can be
attributed to the difference in their sizes and removal mechanism.
The RB5 dye has a molecular size of 29.9 × 8.75 Å,[41] while Cu2+ has a hydrated atomic
radius of 4.19 Å.[42] Thus, contrary
to RB5, aggregation has no effect on Cu2+ removal as it
has a small atomic radius. Based on these results, the sample prepared
at room temperature was selected for further investigation.The solution’s initial pH affects the speciation and form
of the adsorptive and the composition of the adsorbent. Copper precipitates
as Cu(OH)2 starting from pH 6.0;[43] thus, we limited the study of the pH effect to pHo 5.5.
On the other hand, acidic pH accelerates the dissolution of the zero-valent
bimetallic nanoparticles,[44] causing an
undesirable increase in the concentration of the metals in the aqueous
solution. Therefore, we limited the study of pH effect to pHo 4.Figure c shows
that the Cu2+ removal increased from 70 to 93% by increasing
the pHo from 4 to 5.5. As illustrated above, the surface
of FeCo is positively charged up to pH 8.3. Therefore, repulsion between
Cu2+ and FeCo dominates under experimental conditions.
Thus, the probability of Cu2+ adsorption onto FeCo via
electrostatic forces can be precluded. It is well known that Fe0 is a powerful reductant in water. The standard reduction
potential of Cu2+ is much more positive than Fe0, so it can rapidly reduce to Cu0 and/or Cu2O and the reduction process is thermodynamically preferred over precipitation
and sorption processes.[45,46] Thus, herein, Cu2+ reduction is the most probable removal mechanism. To verify
this assumption, XPS analysis was performed before and after contact
of the FeCo alloy with a Cu2+ solution. Figure shows the obtained XPS survey
and narrow-scan spectra. The survey scan (Figure a) revealed that the curve shape and peak
position of the two samples are very similar. Also, the survey scan
exposed the presence of Fe, Co, O, and C elements in both samples
and the appearance of a new Cu peak in the sample exposed to the Cu2+ solution. The appearance of a Cu peak demonstrates the uptake
of Cu by the FeCo alloy. The presence of C might be due to the usage
of carbon as the standard XPS correction, while the presence of O
indicated the surface oxidation of both samples. The emergence of
O in the fresh FeCo alloy does not contradict the above-discussed
XRD and EDX results, which revealed the absence of oxides because
XPS gives information about the surface elements with a photoelectron
probing depth of a few angstroms.[33] Similar
trends of XRD, EDX, and XPS have been reported before.[33,34,47,48] Based on the results of XRD, EDX, and XPS, it can be concluded that
a thin passive oxide layer is formed over the FeCo nanoparticles.
This layer protects the FeCo alloy against further air oxidation.[49,50] The narrow-scan analysis of Fe 2p (Figure b) disclosed the presence of Fe0 (peaks at around 706 and 719 eV), Fe2O3 (peaks
at 710 and 724 eV), and Fe3O4 (peaks at 712
and 725 eV). On the other hand, the narrow-scan spectrum of Co 2p
(Figure c) revealed
the presence of peaks at Co0 (peak at 793 eV), Co3O4 (peak at 780 eV), and Co(OH)2 (peak at 796
eV). The peak at 785 eV is the satellite peak of the Co 2p3/2 main line.[33,34,47,48]
Figure 5
XPS analysis of bimetallic zero-valent FeCo
nanoparticles prepared
by the room-temperature method. (a) Survey scan before (spectrum i)
and after (spectrum ii) contact with Cu2+ solution (10
mg/L, pHo 5.5), and narrow-scan spectra of (b) Fe 2p, (c)
Co 2p, and (d) Cu 2p.
XPS analysis of bimetallic zero-valent FeCo
nanoparticles prepared
by the room-temperature method. (a) Survey scan before (spectrum i)
and after (spectrum ii) contact with Cu2+ solution (10
mg/L, pHo 5.5), and narrow-scan spectra of (b) Fe 2p, (c)
Co 2p, and (d) Cu 2p.Finally, the narrow-scan spectrum of Cu 2p (Figure c) showed a peak
at 933.5 eV corresponding
to CuO;[51,52] doublet peaks at 935.8 and 955.5 eV, which
are characteristic for Cu(OH)2;[51,53] satellite peaks at 940, 943, and 962 eV; and a peak at 952.9, which
could be due to Cu0 or Cu2O.[51,54] The differentiation between Cu0 and Cu2O from
the Cu 2p XPS spectra is difficult because they have identical binding
energies (±0.1 eV).[52,55] However, the difference
in binding energy between the Cu 2p3/2 and Cu 2p1/2 peaks is about 20 eV, which supports the presence of Cu0 or Cu+ on the FeCo alloy surface.[52]The presence of Cu0 or Cu2O
on the surface
of the FeCo alloy corroborates the reduction of Cu2+ by
the FeCo alloy. Similar results have been reported frequently for
the removal of Cu2+ by Fe0.[45,46] The appearance of CuO and Cu(OH)2 on the surface of FeCo
is likely due to the reoxidation of the deposited Cu0 or
Cu2O. The ease of reoxidation of Cu0 deposited
on Fe0 to CuO and Cu(OH)2(s) has been reported
previously.[46,56] Therefore, the XPS analysis supports
the assumption that Cu2+ removal by the FeCo alloy occurs
via the reduction mechanism.In aqueous solutions, a passive
layer of oxides is formed on the
surface of the FeCo alloy, as illustrated by XPS analysis (Figure ). Acidic pH dissolves
this passive layer and exposes the reactive sites and therefore is
expected to improve the reduction efficiency of the bimetallic nanoparticles.
Thus, the removal of Cu2+ is expected to be higher at pHo 4. However, this is not the observed case herein: the Cu2+ removal was higher at pHo 5.5. A probable reason
is that at pHo 4 a proportion of the removed Cu2+ undergoes dissolution again, causing an overall decrease in Cu2+ removal. A similar effect of pH on copper reduction by Fe0 has been observed by Crane et al.[57]The effect of pHo on RB5 removal displayed in Figure d indicates that
FeCo can remove RB5 at the different studied pHo. However,
the highest removal was observed at pHo 7. RB5 is an anionic
reactive dye of the vinyl sulfone type that contains an amino, a hydroxyl,
and four sulfonate groups (see Figure S1). The sulfonate groups have a very low pKa that can reach a negative
value,[58] so they remain in the anionic
form under the experimental conditions. The RB5 dye has pKa at 3.9
(corresponding to the −NH2 group) and 6.9 (corresponding
to the −OH group).[58] Thus, at pHo 5, the surface of FeCo is positively charged, and the hydroxyl
group of the RB5 dye becomes protonated, while the sulfonate groups
are negatively charged and the amino group has its lone pair of electrons
free. Thus, attraction between the opposite charges drives the removal
process.[59] At pHo 7, the lone
pair of electrons of the hydroxyl groups participates in the interactions
with the positively charged surface of FeCo, which results in increasing
the removal percentage. At pHo 9, the surface of FeCo is
negatively charged and repulsion with the anionic RB5 occurs, which
results in a lower removal.[59] Noteworthy,
the observed removal at pHo 9 suggests that electrostatic
interactions are not the sole mechanism for the removal of RB5. According
to the obtained results, pHo values of 5.5 and 7.0 were
used for Cu2+ and RB5, respectively, in further studies.Figure e,f shows
the change in the percentages of Cu2+ and RB5, respectively,
removed by different amounts of FeCo prepared at room temperature.
The typical trend of increasing the removal percentage with increasing
the dosage of a material can be observed for both adsorptives. This
trend is an axiomatical result of increasing the number of active
sites on increasing the amount of material. Figure e shows that Cu2+ removal percentages
after 120 min. were 81.3, 93.0, and 99.5% for 0.05, 0.10, and 0.30
g/L, respectively. Therefore, a considerable increase in the removal
was achieved by increasing the dosage from 0.05 to 0.10 g/L, but a
further increase to 0.30 g/L had an insignificant effect on Cu2+ removal likely due to approaching complete removal.[39] On the other hand, an invariably significant
increase in the removal of RB5 can be observed by increasing the dosage
over the whole studied contact time (Figure f). After 120 min., the removal percentages
were 17.6, 47.0, 65.1, and 96.9% for 0.25, 0.50, 0.75, and 1.00 g/L,
respectively. Therefore, further studies were conducted using dosages
of 0.10 g/L for Cu2+ and 1.00 g/L for RB5.The kinetic
of removal of Cu2+ and RB5 was investigated
to get insights into the removal mechanism. Fitting of three kinetic
models, pseudo-first order (PFO), pseudo-second order (PSO), and Elovich,
to the experimental kinetic data was evaluated. Figure S2 displays the experimental kinetic data and the fitted
models. The calculated kinetic parameters and error values are presented
in Table . The PFO
can describe the removal of Cu2+ better than the other
investigated models as it has a higher correlation coefficient (R2) and a lower chi-square (χ2) and root-mean-square error (RMSE). In addition, the value of qe calculated from the PFO was closer to the
experimental value. This result matches the previous reports that
Cu2+ reduction by Fe0 follows the PFO kinetic.[60,61]
Table 3
Calculated Kinetic Parameters and
Error Functions
Cu2+
RB5
experimental qe (mg/g)
93.00
3.28
PFO
R2
0.955
0.969
χ2
62.86
0.038
RMSE
7.93
0.196
k
0.06 ± 0.01
0.11 ± 0.02
qe
91.83 ± 4.90
3.02 ± 0.09
PSO
R2
0.928
0.995
χ2
99.59
0.006
RMSE
9.98
0.077
k
5.78 × 104 ± 2.76 × 104
0.05 ± 0.00
qe
109.13 ± 11.27
3.36 ± 0.05
Elovich
R2
0.892
0.994
χ2
149.60
0.007
RMSE
12.23
0.083
α
13.40 ± 10.54
2.31 ± 0.55
β
0.04 ± 0.01
1.85 ± 0.11
On the other hand, the experimental kinetic data of
RB5 was best
described by the PSO model because it demonstrated the highest R2 and lowest χ2 and RMSE values
among the tested models. The close match between the qe calculated from the PSO and the experimental one further
proved the best fitting of the PSO to the experimental data. The PSO
assumes that (i) the rate of adsorption depends on both the adsorptive
and the adsorbent; (ii) the adsorption step, not the mass transfer,
is the rate-determining step; and (iii) adsorption is due to physiochemical
interactions between the adsorptive and adsorbent.[62] Noteworthy, the Elovich model also gives a good fit to
the kinetic data. Typically, the Elovich model is applicable to chemisorption
onto a heterogeneous surface.[63] Thus, the
results of RB5 adsorption kinetic modeling suggest the chemisorption
process and heterogenous surface of FeCo. This suggestion will further
be confirmed by the isotherm study.The practical isotherm data
and the nonlinear fit of different
isotherm models are given in Figure . The shape of the practical isotherm of Cu2+ in single- and bicomponent systems (Figure a) can be classified as C1 and L1 curves
of the Giles classification, respectively,[64] while the adsorption isotherm of RB5 in both single- and bicomponent
systems (Figure b)
can be classified as L1. The C1 curve indicates (i) probable penetration
of Cu2+ into the FeCo alloy and (ii) the creation of more
reactive sites as long as Cu2+ is removed. On the other
hand, the L1 curve indicates that as more adsorptive is adsorbed,
finding a vacant adsorption site becomes difficult.[64]
Figure 6
Adsorption isotherm and fitted models for the adsorption of (a)
Cu2+ and (b) RB5 onto the FeCo alloy prepared at room temperature
in single- and bicomponent systems. Single-component system Cu2+ (pHo 5, dosage 0.10 g/L) and RB5 (pHo 5, dosage 1.00 g/L). Bicomponent system pHo 5, dosage
1.00 g/L.
Adsorption isotherm and fitted models for the adsorption of (a)
Cu2+ and (b) RB5 onto the FeCo alloy prepared at room temperature
in single- and bicomponent systems. Single-component system Cu2+ (pHo 5, dosage 0.10 g/L) and RB5 (pHo 5, dosage 1.00 g/L). Bicomponent system pHo 5, dosage
1.00 g/L.Comparing the adsorption isotherms of Cu2+ in the single-
and bicomponent systems (Figure a) reveals that Cu2+ removal in the bicomponent
system is much higher than in the single-component system. It seems
that the adsorbed RB5 adds negatively charged functional groups on
the surface of FeCo, which enhances the adsorption of Cu2+ through electrostatic interactions. As illustrated above, at pHo 5, RB5 is adsorbed onto FeCo through the electrostatic interactions
between the positively charged surface of FeCo from one side and negatively
charged sulfonate groups and electron-rich amino groups from the other
side. The unbonded negatively charged and electron-rich functional
groups of the RB5 adsorbed on the surface of FeCo act as adsorption
sites for Cu2+. This synergistic effect is known as “anion-synergism”
and has been reported frequently for the simultaneous adsorption of
anionic dyes and cationic trace metals.[65−68]Inversely, comparing the
adsorption isotherms of the single- and
bicomponent systems of the RB5 dye (Figure b) reveals that the FeCo alloy can remove
10 mg/L RB5 in both systems with the same efficiency. However, when
the initial concentration of RB5 increases, the removal in the bicomponent
system becomes lower than those in the single-component system. This
trend might be ascribed to (i) exhaustion of some active sites of
FeCo by Cu2+ and/or (ii) altering the adsorption characteristics
of FeCo as a consequence of the reduction and probable diffusion of
Cu2+ into the FeCo alloy. The latter reason can be verified
from the isotherm models as below.The parameters of the tested
isotherm models are given in Table . The analysis of R2 indicates
that the Cu2+ removal
in single- and bicomponent systems can be described by both Freundlich
and Langmuir models. The values of error functions decisively indicate
that Freundlich is the best model that fit the isotherm data of Cu2+. Additionally, the calculated parameters of the Langmuir
model in the single-component system look unrealistic. The value of
the Freundlich parameter n in the single-component
system was almost 1, indicating a linear process. However, in the
bicomponent system, the value of n was increased
to 1.56, indicating the favorability of the adsorption process and
increasing the heterogeneity of the FeCo surface.
Table 4
Calculated Isotherm Parameters and
Error Functions
Cu2+
RB5
single-component
bicomponent
single-component
bicomponent
Freundlich
R2
0.99
0.99
0.98
0.99
χ2
3923
15201
2.27
0.47
RMSE
62.63
123.29
1.51
0.69
kF
9.52 ± 4.87
14.21 ± 44.31
5.00 ± 0.91
5.67 ± 0.61
N
0.97 ± 0.11
1.56 ± 0.17
1.84 ± 0.23
3.33 ± 0.40
Langmuir
R2
0.99
0.98
0.98
0.97
χ2
3975
31703
2.27
1.17
RMSE
63.05
178.05
1.51
1.08
kL
1.82 × 10–6 ± 0.00
0.01 ± 0.006
0.09 ±0.03
0.26 ± 0.08
qL
5.89 × 106 ± 4.83 × 109
5563 ± 1894
39.72 ± 5.22
17.02 ± 1.25
Temkin
R2
0.70
0.83
0.98
0.99
χ2
95634
271065
1.92
0.65
RMSE
309.25
520.64
1.39
0.81
bT
12.87 ± 5.03
6.08 ± 1.64
272.01 ± 25.42
748.03 ± 93.42
AT
0.91 ± 1.24
2.41 ± 2.56
0.77 ± 0.15
3.44 ± 1.66
On the other hand, according to the values of R2, the Freundlich, Langmuir, and Temkin models
can describe
the adsorption isotherm of RB5 in single- and bicomponent systems.
Once again, the values of error functions show that the Temkin model
is the best model that fits the isotherm data of RB5 in the single-component
system. However, in the bicomponent system, a better fit can be observed
in the case of the Freundlich model. Both Freundlich and Temkin models
are nonideal models that suppose a multilayer adsorption. They differ
in their assumptions of (i) the relation between the heat of adsorption
and surface coverage: Freundlich assumes a logarithmic relationship,
while Temkin assumes a linear relationship; and (ii) the binding energy
of adsorption sites: Freundlich assumes energetically nonuniform adsorption
sites, while Temkin assumes uniform adsorption sites.[69,70]A comparison of the value of Langmuir qm of the
single-
and bicomponent systems (Table ) indicates that the coexistence of RB5 and Cu2+ in solution decreased the adsorption of RB5. The values of the Freundlich
parameter n are greater than 1 in both single- and
bicomponent systems, indicating a favorable adsorption process. In
addition, the value of the Freundlich heterogeneity factor (n) in the bicomponent system is significantly higher than
in the single-component system, suggesting an increase in the surface
heterogeneity likely due to the reduction and probable diffusion of
Cu2+ into the FeCo alloy. Thus, the isotherm study elucidated
that (i) the adsorption of RB5 and Cu2+ onto FeCo is a
complicated process that has a multilayer character, (ii) FeCo can
simultaneously remove RB5 and Cu2+ with more selectivity
toward Cu2+, and (iii) the simultaneous adsorption of RB5
and Cu2+ slightly changes the surface characteristics of
the FeCo alloy. In addition, this change was, obviously, associated
with a considerable decrease in the adsorption efficiency of FeCo
toward RB5.Usually, the Langmuir monolayer saturation capacity
is used to
compare the adsorption efficiency of different materials toward a
specific contaminant.[71] Unfortunately,
the value of qL in the case of Cu2+ looks unrealistic, so it cannot be reliably used for comparison
with other adsorbents. On the other hand, as the Langmuir model can
describe the adsorption isotherm of RB5 onto the FeCo alloy well,
the value of qL can be used for such a
comparison. Table lists the values of qL of different
reported adsorbents along with that of the FeCo alloy prepared in
this work toward the RB5 dye in a single-component system.
Table 5
Values of Langmuir Monolayer Adsorption
Capacity of Different Adsorbents toward the RB5 Dye
It can be seen from Table that the prepared FeCo alloy has a higher qL than several reported adsorbents. However,
there are
still some materials that have higher qL values. For example, Tanyildizi[72] and
Kumar et al.[73] have reported a higher qL for RB5 adsorption onto peanut hull and the
coral-like hierarchical magnesium oxide-incorporated fly ash composite,
respectively. However, the FeCo alloy is more practicable than these
adsorbents owing to its ease of separation by applying a magnetic
field after the treatment of contaminated water. Overall, the comparison
in Table shows that
the prepared FeCo alloy is a good choice for practical application
for the removal of RB5 and similar anionic dyes from contaminated
water.
Conclusions
A simple and quick preparation
method for FeCo preparation based
on hydrazine reduction at room temperature was revisited with the
aim of evaluating the effect of initial salt composition on the purity
and particle size of the product and comparing it with the solvothermal
method. The results indicated the dependency of the purity and particle
size of the produced FeCo on the initial salt composition used. Using
nitrate salts or chloride salts of both of iron and cobalt produces
a pure crystalline bimetallic zero-valent FeCo alloy. The particle
size of FeCo prepared using chloride salts was larger than that prepared
using nitrate salts. Solvothermal treatment of the sample prepared
using chloride salts reduces the particle size to be comparable to
that prepared using nitrate salts at room temperature. Furthermore,
the characteristics of FeCo prepared by solvothermal and room-temperature
methods using nitrate salts were almost the same. Thus, it can be
concluded that room-temperature reduction of iron and cobalt nitrate
salts is more advantageous than the solvothermal method. The advantages
of the room-temperature method include its fast speed, simplicity,
minimal energy consumption, and not requiring protection against oxidation
by an inert gas or any agent.Studies on the efficiency of the
prepared FeCo for the removal
of Cu2+ and RB5 dye in the single-component system illustrated
that 0.3 g/L FeCo can completely remove 10 mg/L Cu2+ at
pHo 5.5 in 10 min. However, the complete removal of 10
mg/L RB5 requires 90 min of contact with 1.0 g/L FeCo at pHo 7. The pseudo-first-order and pseudo-second-order models were best
suited to the removal kinetics of Cu2+ and RB5, respectively.
The FeCo can simultaneously remove Cu2+ and RB5 dye. However,
a considerable decrease in the removal of RB5 was observed in the
bicomponent system, especially at RB5 concentrations higher than 10
mg/L. Contrarily, a considerable increase in the removal of Cu2+ was observed in the bicomponent system. A Langmuir monolayer
saturation capacity of 5563 mg/g for Cu2+ in the bicomponent
system demonstrated the high efficiency of the prepared FeCo for water
decontamination.