Pendaranahalli Nadikeraiah Anantharamaiah1, Hadonahalli Munegowda Shashanka1, Sujoy Saha2, Keerthi Haritha3, C V Ramana4,5. 1. Department of Chemistry, Faculty of Mathematical and Physical Sciences, M. S. Ramaiah University of Applied Sciences, Bangalore 560058, India. 2. Department of Materials Engineering, Indian Institute of Science, Bangalore 560012, India. 3. Environmental Science and Engineering, University of Texas at El Paso, 500 W. University Avenue, El Paso, Texas 79968, United States. 4. Center for Advanced Materials Research, University of Texas at El Paso, 500 W. University Avenue, El Paso, Texas 79968, United States. 5. Department of Mechanical Engineering, University of Texas at El Paso, 500 W. University Avenue, El Paso, Texas 79968, United States.
Abstract
We demonstrate an approach based on substituting a magnetic cation with a carefully chosen isovalent non-magnetic cation to derive catalytic activity from otherwise catalytically inactive magnetic materials. Using the model system considered, the results illustratively present that the catalytically inactive but highly magnetic strontium hexaferrite (SrFe12O19; SFO) system can be transformed into a catalytically active system by simply replacing some of the magnetic cation Fe3+ by a non-magnetic cation Al3+ in the octahedral coordination environment in the SFO nanocrystals. The intrinsic SFO and Al-doped SrFe12O19 (SrFe11.5Al0.5O19; Al-SFO) nanomaterials were synthesized using a simple, eco-friendly tartrate-gel technique, followed by thermal annealing at 850 °C for 2 h. The SFO and Al-SFO were thoroughly characterized for their structure, phase, morphology, chemical bonding, and magnetic characteristics using X-ray diffraction, Fourier-transform infrared spectroscopy, and vibrating sample magnetometry techniques. Catalytic performance evaluated toward 4-nitrophenol, which is the toxic contaminant at pharmaceutical industries, reduction reaction using NaBH4 (mild reducing agent), the Al-doped SFO samples exhibit a reasonably good performance compared to intrinsic SFO. The results indicate that the catalytic activity of Al-SFO is due to Al-ions occupying the octahedral sites of the hexaferrite lattice; as these sites are on the surface of the catalyst, they facilitate electron transfer. Furthermore, surface/interface characteristics of nanocrystalline Al-SFO coupled with magnetic properties facilitate the catalyst recovery by simple, inexpensive methods while readily allowing the reusability. Moreover, the activity remains the same even after five successive cycles of experiments. Deriving the catalytic activity from otherwise inactive compounds as demonstrated in the optimized, engineered nanoarchitecture of Al-doped-Sr-hexaferrite may be useful in adopting the approach in exploring further options and designing inexpensive and recyclable catalytic materials for future energy and environmental technologies.
We demonstrate an approach based on substituting a magnetic cation with a carefully chosen isovalent non-magnetic cation to derive catalytic activity from otherwise catalytically inactive magnetic materials. Using the model system considered, the results illustratively present that the catalytically inactive but highly magnetic strontium hexaferrite (SrFe12O19; SFO) system can be transformed into a catalytically active system by simply replacing some of the magnetic cation Fe3+ by a non-magnetic cation Al3+ in the octahedral coordination environment in the SFO nanocrystals. The intrinsic SFO and Al-doped SrFe12O19 (SrFe11.5Al0.5O19; Al-SFO) nanomaterials were synthesized using a simple, eco-friendly tartrate-gel technique, followed by thermal annealing at 850 °C for 2 h. The SFO and Al-SFO were thoroughly characterized for their structure, phase, morphology, chemical bonding, and magnetic characteristics using X-ray diffraction, Fourier-transform infrared spectroscopy, and vibrating sample magnetometry techniques. Catalytic performance evaluated toward 4-nitrophenol, which is the toxic contaminant at pharmaceutical industries, reduction reaction using NaBH4 (mild reducing agent), the Al-doped SFO samples exhibit a reasonably good performance compared to intrinsic SFO. The results indicate that the catalytic activity of Al-SFO is due to Al-ions occupying the octahedral sites of the hexaferrite lattice; as these sites are on the surface of the catalyst, they facilitate electron transfer. Furthermore, surface/interface characteristics of nanocrystalline Al-SFO coupled with magnetic properties facilitate the catalyst recovery by simple, inexpensive methods while readily allowing the reusability. Moreover, the activity remains the same even after five successive cycles of experiments. Deriving the catalytic activity from otherwise inactive compounds as demonstrated in the optimized, engineered nanoarchitecture of Al-doped-Sr-hexaferrite may be useful in adopting the approach in exploring further options and designing inexpensive and recyclable catalytic materials for future energy and environmental technologies.
Strontium hexaferrite
(SrFe12O19), which
is one among the metal-oxide-based hard magnetic materials, has been
widely used in numerous scientific and technological applications.[1−10] SrFe12O19 (referred to as SFO hereafter),
which belongs to the crystal group of magnetoplumbite, exhibits attractive
electromagnetic properties such as a high coercivity (∼7000
Oe), a moderate saturation magnetization (∼60 emu/g), a high
Curie temperature (TC), and a high remanence
(35 emu/g).[1,3,7,11,12] Due to its superior
magnetic parameters, high permeability, and low conductivity loss,
SFO has been widely used in numerous technological applications, which
include permanent magnet designs, microwave absorbers, magnetic recording
media and sensors, high-frequency electromagnetic (EM) devices, EM
shielding devices, and so forth.[1,3−7,10]Current interest in SFO
and SFO-based hybrids or composite materials
at the nanoscale dimensions has been driven by a challenging goal
of further enhancing their performance in addition to expanding their
potential applicability into other fields, most importantly in energy,
health, bio-, and environment-related technologies. In fact, recently,
numerous attempts were made to further enhance/improve the magnetic
properties of the SFO by metal ion doping, adopting suitable synthesis
methods, and optimizing the processing conditions.[2−15] Also, composites of SFO with soft magnetic phases and improved magnetic
properties achieved through the exchange-spin mechanism have been
reported in the literature.[3,10,16,17] For instance, using a conducting
polymer and a SFO content for tunability, polypyrrole/SFO composites
were designed and tested for efficient EM-shielding purposes.[10] It was demonstrated that the electrical and
magnetic properties of such composites can be controlled simply by
tuning the SFO content. Based on the results obtained using polypyrrole/SFO
composites, the authors concluded that the incorporation of magnetic
constituents and conducting polymeric materials into multifunctional
composites opens new possibilities for the achievement of good shielding
effectiveness for various electromagnetic sources.[10] Most recently, magnetic hybrid films containing diblock
copolymers (DBCs) and magnetic NPs of SFO were also considered for
sensor applications.[2] Spray deposition
was applied to prepare perpendicular anisotropic magnetic hybrid films
by controlling the orientation of SFO nanoplatelets inside ultra-high-molecular-weight
DBC polystyrene-block-poly(methyl methacrylate) (PS-b-PMMA) films.[2] Using the superconducting
quantum interference device data, authors demonstrated that the ferromagnetic
hybrid polymer films with high coercivity can be achieved via spray
deposition. The spray-deposited hybrid films were reported to be highly
promising for potential applications in magnetic data storage and
sensing.[2] Similarly, nanostructuring of
SFO is shown to enhance the property and performance effectively.[3−7] SFO nanomaterials with highly aligned nanocrystallites combined
with crystal growth during spark plasma sintering (SPS) exhibit enormous
enhancement of the magnetic properties compared to the as-synthesized
powders, leading to high-performance bulk magnets with high-energy
products (26 kJ m–3).[4,5] Based on the
extensive work, Christensen and team proposed a complete bottomup
nanostructuring protocol for preparation of magnetically aligned,
high-performance hexaferrite permanent magnets with a record-high
(BH)max for dry-processed ferrites.[3,4] Supercritical
hydrothermal flow synthesis of anisotropic magnetic-single-domain
SFO nanocrystallites of various sizes, and their subsequent compaction
into bulk magnets by SPS, followed by thermal treatments enabled design
of magnets, energy ratings of which even exceed those of the highest
grade commercial magnets produced according to the European, Japanese,
and American standards.[4] These considerations
of “nanostructuring and composites” are very appealing
to combine the nanoscale features and SFO materials’ characteristics
to design advanced materials for modern technologies. However, while
a wealth of information available in the literature toward various
approaches to utilize and/or design materials for electromagnetic
and electronic applications, designing catalytic materials based on
SFO is seldom explored. Therefore, the impetus for the present work
is to combine the advantages of nanostructuring, surface/interface
engineering, and doping aspects into SFO to design catalytically active
materials from an otherwise inactive catalytic system and demonstrate
their potential applications in modern pharmaceutical industries.
The approach employed in this work to derive catalytic activity from
SFO by means of Al-doping and surface/interface engineering is schematically
presented in Figure . The motivation to design SFO-based catalytic materials for chemical
industries is derived from the following considerations.
Figure 1
Schematic diagram
of the key technical approach employed in this
work to derive catalytic activity in SFO by means of Al-doping and
surface/interface engineering.
Schematic diagram
of the key technical approach employed in this
work to derive catalytic activity in SFO by means of Al-doping and
surface/interface engineering.Magnetically recoverable and recyclable materials, more specifically
the magnetic oxide-based nanocomposite materials, have been receiving
significant attention for the design and development of novel catalysts
due to their applications in numerous chemical industries, including
production of bidiesel.[18−21] In fact, in recent years, considerable efforts were
directed toward magnetically recyclable solid catalyst design for
energy application to meet the demand of green and clean production.[18−20] For instance, Xie et al. have developed magnetically recyclable
solid catalysts for the production of biodiesel.[18] The magnetically susceptible Fe3O4/MCM-41 composites with a core–shell structure exhibited a
strong magnetic response and displayed extraordinary catalytic activities
in the transesterification of soybean oil for the production of biodiesel,
with the oil conversion reaching 99.2% by using a methanol-to-oil
molar ratio of 25:1 and a catalyst loading of 3 wt % at reflux of
methanol after 8 h of the reaction.[18] Moreover,
the separation of the solid catalyst from the reaction mixture can
be readily achieved by simple magnetic decantation without obvious
mass loss, and the solid catalyst can be reused for the heterogeneous
transesterification.[18] Similarly, efficient
solid hybrid base catalysts based on Fe3O4@HKUST-1
composites were reported for clean production.[19] The hybrid catalysts consist of core–shell-structured
Fe3O4@HKUST-1 composites with a magnetic core
and a porous metal–organic framework shell fabricated using
a versatile layer-by-layer assembly method, then basic ionic liquids
were encapsulated within the core–shell magnetically responsive
material.[19] These catalysts exhibited superparamagnetic
behavior allowing them for easy separation from the reaction mixture
by using an external magnetic field.[19] The
solid base catalyst appeared to be an efficient and environmentally
benign catalyst for the transesterification of soybean oil with methanol
for the production of biodiesel, giving 92.3% oil conversion.[19] Such a catalyst can be readily recovered by
simple magnetic decantation and reused several times without significant
degradation in its catalytic activity. Additionally, magnetic nanostructured
materials containing Fe and Ca synthesized using a simple coprecipitation
method were demonstrated to be highly efficient catalysts.[21] Based on these considerations, it is imperative
to investigate SFO, which is a widely adopted permanent magnetic material,
for catalyst design.SrFe12O19 is a n-type
semiconducting material
and it has been used as a magnetic component to make composites with
various metal oxide-based photocatalysts such as BiOBr and Bi4O5Br2.[9,22,23] Therefore, the composites act as catalysts as well
as they are magnetic in nature that helps to recover the catalysts
from the reaction mixture with a simple, inexpensive method of using
a magnet. Thus, catalysts based on such a widely utilized permanent
magnetic material may open up the new possibilities for integration
into chemical and pharmaceutical industries, where the demand is continuously
evolving for catalysts to eliminate or convert toxic and harmful chemical
emissions into useful products. Especially, catalysts with possible
easy recovery and reusability along with recyclability are highly
beneficial in chemical and health sectors,[24,25] and more specifically in pharmaceutical industries. In this context,
the present work was performed on designing catalysts based on SFO
for utilization in pharmaceutical industries for efficient conversion
of toxic pollutants into useful products. To illustratively demonstrate
the applicability of doped SFO as a catalyst for pharmaceutical industries,
efforts were directed toward the efficient conversion of para-nitrophenol chemicals. Para-nitrophenol is one
of the toxic pollutants being released by pharmaceutical industries.
Additionally, nitrophenols are some of the recalcitrant substances,
which are considered as high-priority toxic pollutants.[24−30] These are most refractory substances present in industrial wastewaters
because of their high stability and solubility in water. The detection,
determination, and catalytic conversion of the nitrophenols are, therefore,
extremely important. Catalytic conversion of a toxic chemical into
a useful and value-added product is the simple and key approach,[24−27] which can be readily integrated to achieve an efficient wastewater
treatment technology in both chemical and pharmaceutical industries.
Therefore, conversion of nitrophenol into other chemicals such as para-aminophenol is highly beneficial as these chemicals
can be used as starting materials for industrial dyes, photography
development agents, rubber chemicals, and so forth.[24,31−35] While there are recent attempts to design and develop catalysts
for the purpose based on environmental friendly, cost-effective, and
high-performance materials, catalysts based on noble metals, such
as Au, Pd, Pt, Ag, and so forth, have been studied for a long time
to convert para-nitrophenol to para-aminophenol.[25−30,33,36−39] Realizing that the noble metals are expensive, which exhibit sintering
and related problems at the nanoscale dimensions, many researchers
directed their recent efforts to design and develop various other
catalysts, which are based on inexpensive, green, and highly stable
metal oxides and/or composites, for the para-nitrophenol
reduction reaction.[24,28,35,40−44] However, the catalytic studies on the hard magnetic
materials such as barium- and strontium-hexaferrites and their derivatives
are yet to be explored. On the other hand, based on our previous work
on magnetic and electronic materials,[45,46] we recognize
that tailoring the materials’ structure and controlled phase
in nanostructured materials can provide opportunities to design inexpensive
nanomaterials for the desired applications. Furthermore, most recently,
we demonstrated that the surface/interface magnetic properties can
be tailored[46] and have made successful
attempts to derive catalytic properties in Cu-substituted strontium
hexaferrites synthesized using a tartrate-gel method.[47,48] Therefore, in the present study, Al is chosen for the substitution
in place of Fe in SrFe12O19 and evaluated its
activity toward the nitrophenol reduction reaction. Al3+ is a non-magnetic trivalent cation that can be used for substituting
isovalent Fe3+ in SFO. It has been inferred from our previous
studies reported in ref (47) that the catalytic activity more or less remains the same
irrespective of dopant concentrations. Hence, we have considered a
specific composition of Al-substituted strontium hexaferrite (SrFe11.5Al0.5O19). However, we considered
a reasonable amount of Al for doping, so that no doping-induced perturbation
in the overall magnetic properties of SFO occurs. Also, other non-magnetic
trivalent cations such as Ga3+ and In3+, although
they are isovalent in nature compared to Fe3+, are not
suitable as dopants due to their tetrahedral site preference, and
these sites are not exposed to the surface of the particles. Interestingly,
as presented and discussed in this paper, Al-substituted SFO samples
combine the advantages of magnetic and catalytic properties to render
economically viable and environmental friendly catalytic nanomaterials.
Materials and Methods
Synthesis
Nanocrystalline
materials
of SFO and SrFe11.5Al0.5O19 (Al–SFO)
were synthesized using high-purity Sr(NO3)2,
Fe(NO3)3·9H2O, and Al(NO3)3 salts as starting materials. We adopted a previously
established experimental procedure,[47,48] which is based
on the tartrate-gel method, to synthesize the SFO and Al–SFO
materials. Briefly, calculated amounts of metal nitrates, which correspond
to the SrFe12O19 and SrFe11.5Al0.5O19 compositions, were weighted into a beaker
and dissolved completely with a minimum volume of distilled water.
The crystals of tartaric acid (1.5 M/metal ion) were weighed into
a 200 mL crystallizing dish and made into a solution with distilled
water of the same volume taken for the preparation of metal nitrate
solution. Subsequently, metal nitrates and tartaric acid solutions
were mixed homogeneously using a magnetic stirrer at 50 °C. In
the next step, 2 mL of the ethylene glycol (acts as a polymerizing
agent) was transferred to the above reaction mixture and the temperature
of the solution was increased to 80 °C under the same stirring
conditions. A brown colored thick viscous gel was found after all
the solvent molecules evaporated from the reaction mixture. The viscous
gel was dried at 80 °C and crushed into a form of fine powers
using a mortar and pestle, followed by calcination at 850 °C
for 2 h.
Characterization
X-ray
Diffraction
A powder X-ray
diffractometer (XRD) [SmartLab, Rigaku X-ray diffractometer (Cu Kα
radiation)] was used to probe phase formation and structural aspects
of the synthesized materials.
Scanning
Electron Microscopy
The
scanning electron microscopy (SEM) measurements were carried out on
both SFO and Al-doped SFO samples to understand their surface morphology.
The measurements were made using a scanning electron microscope (TESCAN
VEGA 3LMU). In order to compare and understand the effect of Al-substitution,
the samples were imaged under the identical conditions.
Fourier Transform Infrared Spectroscopy
A Fourier transform
infrared (FTIR) spectrometer (Bruker, Alpha-P,
Diamond ATR cell) was employed to record the FTIR spectra of the samples.
Catalytic Properties and Performance
Catalytic Performance
To investigate
the catalytic activity of the synthesized hexaferrite materials, the
conversion reaction of para-nitrophenol to para-aminophenol is chosen as a model chemical reaction.
The detailed procedure employed for the purpose of evaluating catalytic
property and performance is as follows. Initially, a large volume
of 0.2 mM of 4-nitrophenol (4-NP) solution was prepared. 100 mL of
0.2 mM 4-NP solution was transferred into a 250 mL beaker. Later,
NaBH4 crystals (equivalent to a concentration of 0.2 M),
a mild reducing agent, were mixed with the 4-NP solution and stirred
vigorously to make the solution more uniform. After mixing NaBH4 with the 4-NP solution, it is noticed that the pale yellow
color of the 4-NP solution turned into a dark yellow color solution
due to the formation of a phenolate anion, which exhibits a resonance
effect. The UV–visible spectrum of the solution containing
the phenolate anion was recorded, and an absorption band was found
at a wavelength of 400 nm. 10 mg of the prepared catalyst was mixed
with the para-nitrophenolate solution and time-dependent
UV–visible spectra of the reaction were recoded to examine
the catalytic performance of the prepared catalysts. Furthermore,
using standard practices, the reaction kinetics also evaluated.
UV–vis–NIR Spectroscopy
The catalytic activity and the extent of chemical reaction and/or
progress have been measured by means of the optical absorption measurements.
The optical absorption measurements were performed using a UV–visible
spectrophotometer (Shimadzu UV-2600). The time-dependent UV–visible
optical spectra of the catalytic reaction of 4-nitrophenol were recorded.
Catalyst Recovery and Magnetism
Catalyst
recovery measurements were carried out based on the testing
and confirmation of samples that showed catalytic properties. The
coexistence of catalytic and magnetic activity is believed to help
in faster recovery of the catalyst that too using a simple and inexpensive
method. Therefore, room-temperature magnetic characteristics of the
calcined SFO and Al–SFO samples were investigated using a vibrating
sample magnetometer (VSM) (EG&G PAR 4500), After confirmation
of magnetic property, the catalyst recovery was attempted by using
a simple magnet.
Results and Discussion
Crystal Structure and Phase
The XRD
data of SFO and Al-doped SFO are shown in Figure . Both the samples exhibit prominent peaks
that correspond to the strontium hexaferrite phase. However, comparison
of the XRD patterns of the samples with the simulated powder pattern
of SrFe12O19 reveals that both samples show
a small quantity of the hematite (α-Fe2O3) impurity phase along with the prominent peaks corresponding to
SFO (see, Figure ).
The formation of an α-Fe2O3 impurity phase
can be expected when the SrFe12O19 sample is
heat treated at lower temperatures.[14] As
suggested in the literature, the temperature required to form a single
phase of SrFe12O19 would be ≥1000 °C.
Extra line broadening associated with the diffraction peaks of the
samples signifies that the materials are nanocrystalline in nature.
The average crystallite size estimated using the Scherrer relation
is ∼40 nm for SFO. The average crystallite size of the Al–SFO
sample is ∼35 nm, which is slightly lower than that of intrinsic
SFO. The size reduction, although not very significant, is due to
the effect of dopant Al ions, which increases the overall surface
energy and, thereby, causes a size reduction. It is well documented
in the literature that whenever a foreign element/ion is substituted
into the spinel/hexagonal ferrite lattice structure, the local strain
will be developed due to size mismatch.[49,50] Here, the
ionic size of Al3+ is considerably smaller than that of
Fe3+ and therefore local lattice strain will be generated
that is reflected in the peak broadening. Peak broadening indicates
a decrease in the particle size and an increase in the surface area.
As the surface area of the hexaferrite particles is proportional to
the surface energy, there is an increase in the surface energy due
to Al-incorporation into the lattice structure of strontium hexaferrite.
Also, the surface energy is directly proportional to the number of
broken bonds present on the surface of the nanoparticles. When the
size of the particles is decreased, one can find a more number of
broken bonds on the surface of the particles.
Figure 2
XRD patterns of the SFO
and Al-SFO samples. The data compared with
the indexed SrFe12O19 pattern (generated using
the PCW program).
XRD patterns of the SFO
and Al-SFO samples. The data compared with
the indexed SrFe12O19 pattern (generated using
the PCW program).The effect of Al-doping
is reflected in the diffraction peaks,
where the peak position of Al-doped SFO indicates a positive shift.
Such a peak shift to a higher 2θ angle compared to intrinsic
SFO is due to a decrease in the unit cell parameters. The decrease
in the lattice parameters is primarily due to the size difference
of Al substituted for Fe in SFO. Thus, the lattice reduction is mainly
due to the replacement of a bigger cation (Fe3+) of size
0.645 Å for 6-fold coordination by a smaller cation (Al3+) of size 0.55 Å for 6-fold coordination.[51]To extract further information about the lattice
parameter values
and percentage of the impurity phase in both intrinsic and Al-doped
SFO samples, the Rietveld refinement analysis was performed. The results
of the refined patterns are presented in Figure . A good fit is obtained for both samples
as revealed from the fitting parameters such as Rp, Rwp, Rexp, and χ2. The values of structural
parameters and percentage of the strontium hexaferrite phase and impurity
phases are tabulated in Table . As revealed from the refinement analysis, the percentage
of the impurity phase also decreases from 9.2 to 2.2% after replacing
a small fraction of Fe by Al in the hexaferrite lattice structure.
Figure 3
Rietveld
fit XRD patterns of the SFO and Al–SFO samples.
Table 1
Structural and Rietveld Refined Parameters
of the SFO and Al–SFO Samples
SrFe12O19
SrFe12O19 hexagonal (P63/mmc)
lattice
parameters: a = b = 5.87985 Å, c = 23.05185 Å, vol. = 690.191 Å3, α = β = 90°, γ = 120°
B (Å2)
phase fraction (vol.)
Sr
2/3
1/3
1/4
0.167
90.80
Fe1
0
0
0
0.949
Fe2
0
0
1/4
0.680
Fe3
1/3
2/3
0.02847
0.802
Fe4
1/3
2/3
0.19142
0.166
Fe5
0.16257
0.32512
0.89031
0.843
O1
0
0
0.15581
1.0
O2
1/3
2/3
0.94881
1.0
O3
0.18309
0.36618
1/4
1.0
O4
0.16451
0.32903
0.05303
1.0
O5
0.50519
0.98962
0.15458
1.0
Rietveld
fit XRD patterns of the SFO and Al–SFO samples.
Surface Morphology
The surface
morphology of the SFO and Al–SFO samples is shown in Figure . As is evident from
the SEM images, no significant changes in the morphology of ferrite
particles are observed even after replacing a larger-sized magnetic
cation (Fe3+) by a smaller-sized non-magnetic cation (Al3+) in the lattice structure of SFO. Although the samples were
heat-treated (calcined) relatively at a high temperature (850 °C),
the hexaferrite particles are nanocrystalline in nature with an average
size of ∼40 nm, which is in agreement with the crystallite
size computed from the XRD data. The majority of the particles exhibit
a plate-like morphology and this is due to the fact that the samples
tend to crystallize in the hexagonal structure.
Figure 4
SEM images of the calcined
SFO and Al–SFO samples. Images
are on the same scale and magnified for better correlation.
SEM images of the calcined
SFO and Al–SFO samples. Images
are on the same scale and magnified for better correlation.
Chemical Bonding
Chemical bonding
analyses using spectroscopic methods provide direct information on
the chemical bonding and dopant-induced changes (if any).[52,53] We found that the FTIR measurements were useful to understand the
effect of metal-ion-substitution on the magnetic ion site in simple
and complex metal oxides.[42,49] Therefore, in the present
work, we relied on FTIR measurement to probe the Al-substitution-induced
changes in the chemical bonding in SFO nanomaterials. Figure shows the FTIR spectra of
SFO and Al–SFO samples. The data shown are spectra recorded
at room temperature in the wavenumber range of 300 to 1600 cm–1. The FTIR spectra show the characteristic absorption
bands of vibrations of a typical hexaferrite system. In the FTIR spectrum
of intrinsic SFO, the bands appearing at the wavenumbers of 583.3
and 423.2 cm–1 are attributed to stretching vibrations
of tetrahedral metal–oxygen (Mtetra–O) and
octahedral metal–oxygen (Mocta–O) bonds,
respectively. Interestingly, these bands are accompanied by shoulders
at lower wavenumbers due to the contribution of neighboring cations
and anions.[49] As expected, the effect of
Al-substitution is the resulting positive shift of tertrahedral and
octahedral bands of SFO. It should be noted that these two bands shifted
considerably toward higher wavenumbers after incorporating Al ions
into the lattice structure of parent SFO. This can be interpreted
based on the changes in the bond length and atomic weight. As the
size and atomic weight of Al3+ are relatively smaller than
those of Fe3+, the Al–O bond length is shorter than
the Fe–O bond length. As a result, a higher energy is required
to stretch the chemical bonds formed in Al–SFO. Hence, a blue
shift is observed for the Al-substituted SFO. Thus, corroborated with
XRD measurements and structure refinement analyses, the FTIR data
reveal the chemical quality of SFO and Al–SFO compounds in
addition to confirming the presence of Al- and Al-substitution-induced
changes in the chemical bonding in SFO.
Figure 5
FTIR spectra of the SFO
and Al–SFO samples. The effect of
Al-substitution is evident in the absorption band shifts.
FTIR spectra of the SFO
and Al–SFO samples. The effect of
Al-substitution is evident in the absorption band shifts.
Catalytic Performance
To assess the
catalytic properties and evaluate the performance, the SFO and Al–SFO
samples were tested as catalysts to drive the 4-nitrophenol reduction
reaction under the influence of a weak reducing agent, NaBH4. The para-nitrophenol solution is pale yellow in
color and changes into a dark yellow color after the addition of NaBH4 due to the formation of a phenolate anion. The absorption
band of the para-nitrophenolate anion appears at
a wavelength of ∼400 nm in the UV–visible spectrum.[24,26] Although NaBH4 is a reducing chemical agent, it cannot
convert para-nitrophenol to para-aminophenol due to a high energy barrier between phenolate and borate
anions.[24,26] It is possible to drive the same reaction
in the presence of a catalyst, provided if it is active. The time-dependent
UV–visible spectra of the SFO and Al–SFO samples, taken
at different time intervals, are shown in Figure . It is evident that the intensity of the
absorption band located at ∼400 nm (para-nitrophenolate
anion band) remains unaffected even after 25–30 min, indicating
that the parent compound is catalytically inactive toward nitrophenol
reduction. However, on the other hand, the remarkable effect of Al-doping
into SFO toward catalytic activity is clearly visible in the optical
data. Unlike the intrinsic SFO, the Al-substituted strontium hexaferrite
is catalytically active as manifested in the intensity of the ∼400
nm band, due to the phenolate anion, decreasing with a simultaneous
increase in the intensity of the ∼303 nm band, due to para-aminophenol, with an increase in the reaction time.
At the end of 50 min, the para-nitrophenol is completely
converted into a para-aminophenol. The presence of
Al3+ ions at the octahedral coordination sites of the hexaferrite
is the prime reason for the observed catalytic activity. As the octahedral
sites are exposed to the surface of the catalyst, the presence of
Al3+ ions in octahedral sites facilitates rapid electron,
proton, and hydride (electron-rich species) transfer and hence the
reduction chemical reaction.
Figure 6
Optical absorption (UV–visible) spectra
of para-nitrophenol conversion using (a) intrinsic
SFO and (b) Al-doped
SFO catalysts. The data shown are as a function of time. Intrinsic
SFO shows no catalytic activity even for an extended period of time.
The Al-substitution-induced catalytic activity in Al-doped SFO is
clearly evident.
Optical absorption (UV–visible) spectra
of para-nitrophenol conversion using (a) intrinsic
SFO and (b) Al-doped
SFO catalysts. The data shown are as a function of time. Intrinsic
SFO shows no catalytic activity even for an extended period of time.
The Al-substitution-induced catalytic activity in Al-doped SFO is
clearly evident.The possible mechanistic
pathway for the nitrophenol reduction
reaction using the Al–SFO nanocatalyst is illustrated in Figure . The hydrogens of
the borohydride [BH4]− ion form a complex
with Al ions, present in the octahedral sites and exposed to the surface,
to result in aluminum hydride. Along with hydrogen, the nitrophenolate
anion also gets adsorbed over the surface of the catalyst. Now, the
hydrogens of the aluminum hydrides could interact electrostatically
with oxygen of nitro groups adsorbed on the surface of the Al–SFO
catalyst, enabling the elimination of oxygen and reduction of nitro
(NO2) groups. Due to a large electronegativity difference
between the residual nitrogen of the NO2 group and the
carbon of the benzene ring, the H atoms of the H2O molecules,
present in the reaction medium, could effortlessly combine with the
residual nitrogen (negatively charged species) of the nitrophenol
leading to the formation of aminophenol as a final product. Once the
nitrophenol is transformed completely into aminophenol, the final
product will be detached from the surface of the catalyst and the
catalyst will be regenerated. In addition to the proton transfer and
deoxygenation processes, electron transport must take place simultaneously
from the hydride to para-nitrophenol through the
Al–SFO catalyst substrate to compensate for the charge balance
and achieve the reduction process.[54,55]
Figure 7
Possible mechanistic
pathway for the para-nitrophenol
reduction reaction using the synthesized Al-doped SrFe12O19 nanocatalyst.
Possible mechanistic
pathway for the para-nitrophenol
reduction reaction using the synthesized Al-doped SrFe12O19 nanocatalyst.The kinetics (rates) of a chemical reaction helps us to understand
whether the reaction is progressing slower, moderate, or faster. For
most of the reactions, the catalyst will be added into the reaction
medium in order to achieve a final product of the reaction in a less
period of time. If a chemical reaction is driven by a catalyst, the
catalyst will be regarded as a best catalyst when the rate of the
reaction is relatively faster. Determination of the rate constant
of the reaction is one of the best ways to assess the performance
of the catalyst. In the present study, the concentration of NaBH4 is relatively higher than the nitrophenol concentration and
therefore the reaction is considered as the pseudo-first-order reaction,
which can be written aswhere k1 is the
reaction rate constant, t is the reaction time, Co is the relative concentration at time zero
(initial concentration), and C is the concentration at time “t”
(which is the time interval during the catalytic reaction).The SFO sample is found to be catalytically inactive and, hence,
its rate constant is negligible. On the other hand, the rate constant
for the nitrophenol reduction reaction under the influence of Al–SFO
catalysts is found to be 0.05 min–1 (see Figure ). While the first
attempt to derive catalytic activity from SFO by Al-doping is successful,
we believe that there may be further options that allow us to further
tune the surface/interface properties and further reduce the nanocrystal
size improving the surface sites to promote the catalytic reaction.
Figure 8
Plot of
ln (Co/Ct)
vs time for the catalytic reduction of nitrophenol using
the Al–SFO catalyst. The data points are fitted with a linear
function to obtain the reaction rate constant.
Plot of
ln (Co/Ct)
vs time for the catalytic reduction of nitrophenol using
the Al–SFO catalyst. The data points are fitted with a linear
function to obtain the reaction rate constant.
Catalyst Recovery and Reusability
Our approach
to recovery and reusability is relied on the combined
magnetic and catalytic activities, which coexist in the Al-doped sample.
Therefore, for the purpose of catalyst recovery, we first consider
the magnetic properties of Al-doped SFO compared to SFO. The magnetic
field-dependent magnetization of the SFO and Al–SFO samples
is presented in Figure . These magnetic data were recorded under ambient conditions. It
is evident (Figure ) that both samples exhibit well-defined hysteresis loops with high
magnetic parameters (saturation magnetization, remanence, and coercivity)
indicating hard magnetic nature of SFO and Al-SFO samples. The values
of Ms, Hc,
and Mr of the samples, obtained from the
magnetization loops, are tabulated in Table . It is interesting note that, after replacing
a magnetic cation (Fe3+) by a non-magnetic cation (Al3+) with similar ionic charges from the lattice structure of
hexaferrite, the Ms value decreases from
59.4 to 50.5 emu/g. However, the value of Hc was found to be increased considerably from 5482 to 6888 Oe. A similar
feature of increase in Hc has been reported
for the Al-doped strontium hexaferrite in the literature.[7,15] The decrease in Ms and the increase
in Hc for the Al-substituted SFO can be
understood based on the two primary considerations. The crystallite
size of Al-doped SFO smaller than that of the parent counterpart (SFO)
is the first. Note that the smaller the crystallite size the lower
will be Ms and higher will be Hc.[15] The later consideration
or reason for the observed variation in Ms and Hc values is based on the dopant
site occupation effect. The dopant ion (Al3+) is a non-magnetic
cation and occupies 4f2, 4f1, 2a, and 12k crystallographic
sites of the hexaferrite. As a result, the dopant cation affects the
anisotropy constant weakly but strongly affects Ms and hence a strong decrease in Ms and an increase in Hc for the
Al-doped SFO compared to intrinsic SFO.
Figure 9
Field-dependent magnetization
curves of the SFO and Al–SFO
samples.
Table 2
Magnetic Parameters
of the Calcined
SrFe12O19 and SrFe11.5Al0.5O19 Samples
sample
MS (emu/g)
HC (Oe)
Mr (emu/g)
SrFe12O19
59.4
5482
33
SrFe11.5Al0.5O19
50.5
6888
28
Field-dependent magnetization
curves of the SFO and Al–SFO
samples.Thus,
as revealed from the magnetic property measurements and characterization,
similar to intrinsic SFO, Al-substituted SFO is also magnetic in nature.
Therefore, magnetic properties of the catalyst should facilitate the
easy recovery of the catalyst from the heterogeneous reaction mixture
using a simple magnet. To test the validity of this hypothesis, we
used a magnet to recover the Al-doped SFO catalyst. As demonstrated
in Figure , the
Al-doped SFO catalyst was easily recovered by simple means. Therefore,
clearly and as demonstrated in this work, advantage of developing
magnetic based catalysts is one can get rid of tedious filtration
and centrifugation methods for the recovery of the catalysts.
Figure 10
Recovery
of the catalyst using a magnet, after the catalytic reaction.
The photographs are taken by the authors during experiments in the
laboratory.
Recovery
of the catalyst using a magnet, after the catalytic reaction.
The photographs are taken by the authors during experiments in the
laboratory.In order to investigate repeatability
and reusability of the Al–SFO
catalyst toward nitrophenol reduction, we have performed five consecutive
cycles under the identical conditions. After completion of each cycle,
the catalyst was recovered from the reaction mixture using a magnet
(as demonstrated in Figure ) and washed several times with distilled water, followed
by ethanol and dried thoroughly. The dried catalyst was used for the
next cycle. After each cycle, there was a loss of a small amount of
the catalyst and volume of the nitrophenol solution was taken according
to the weight of the catalyst for the successive cycles. The time-dependent
optical absorbance spectra of fifth cycle are presented in Figure a and the corresponding
residual activity percentage of the catalysts as a function of number
of cycles is given in Figure b. Even after five successive cycles, the activity was found
to remain the same signifying the robustness of the designed Al–SFO
catalyst.
Figure 11
(a) Fifth cycle time-dependent optical absorption (UV–visible)
spectra of para-nitrophenol conversion using the
Al-doped SFO catalyst and (b) percentage of residual catalytic activity
as a function of number of cycles.
(a) Fifth cycle time-dependent optical absorption (UV–visible)
spectra of para-nitrophenol conversion using the
Al-doped SFO catalyst and (b) percentage of residual catalytic activity
as a function of number of cycles.Finally, to shed some light toward the merit and future applications,
the Al-SFO nanocatalysts prepared in this work exhibit all the features
of a catalyst. These Al–SFO nanomaterials characterized by
the presence of nanocrystalline particles present a high surface area
and appreciable catalytic activity while no catalytic activity exists
in intrinsic SFO, with an excellent magnetic behavior that is high
enough for simple separation by means of a magnet. Furthermore, as
revealed from the repeatability and reusability measurements of the
Al–SFO catalyst for nitrophenol reduction, these magnetic Al–SFO
nanomaterial-based catalysts can be reused several times without significant
loss of their catalytic activity. Thus, all these features, such as
catalytic activity toward nitrophenol reduction, good stability, easy
recovery, and no loss in catalytic activity after several cycles,
which are particularly desirable for industrial applications, make
Al–SFO interesting for further studies to employ them in conjunction
with other potential candidates so as to design and develop efficient
catalysts for energy and environmental applications.
Summary and Conclusions
In conclusion, we have synthesized
Al-doped strontium hexaferrite
nanocrystals and demonstrated their catalytic properties and performance
while such characteristics were fully absent in intrinsic strontium
hexaferrite. The Al–SFO nanomaterials were synthesized using
a simple approach, which can facilitate further tuning of the materials’
structure and properties. XRD and FTIR analyses indicated that Al
ions are successfully assimilated into the lattice structure of strontium
hexaferrite. Due to the non-magnetic nature of Al3+ and
its octahedral site preference, a considerable decrease in the magnetization
and increase in the coercivity have been observed for the Al–SFO
samples. The Al–SFO nanomaterials can be employed as a catalyst
for the para-nitrophenol reduction reaction under
mild reaction conditions. The Al–SFO samples exhibit good catalytic
activity compared to the parent compound due to the presence of Al3+ ions at the octahedral sites, and these sites are exposed
to the surface of the strontium hexaferrite catalyst. Furthermore,
magnetic properties similar to parent SFO makes recovery of the Al–SFO
catalyst readily possible as tested and validated in this work. Furthermore,
as revealed from the repeatability and reusability measurements of
the Al–SFO catalyst for nitrophenol reduction, these magnetic
Al–SFO nanomaterial-based catalysts demonstrate that they can
be reused several times without significant loss of their catalytic
activity. The physical and chemical properties, such as a large surface
area, inexpensiveness of raw materials, relatively low preparation
cost and toxicity, excellent stability, good coercivity, low Curie
temperature, and recovery and reusability coupled with recyclability,
make the nanomaterials with combined magnetic and catalytic properties
highly useful for industrial applications. Therefore, our future efforts
will be directed to further refine the size and morphology and/or
other dopants to explore possible options to further enhance the catalytic
efficiency.