Graphite oxide–iron oxide nanocomposites as a new class of catalyst for the thermal decomposition of ammonium perchlorate

Sanoop Paulose*, Rajeev Raghavan* and Benny K. George
Analytical and Spectroscopy Division, Analytical, Spectroscopy and Ceramics Group, Vikram Sarabhai Space Centre, Trivandrum-695022, India. E-mail: r_rajeev@vssc.gov.in; sanoop_ap@vssc.gov.in; Tel: +91 9447107553

Received 15th March 2016 , Accepted 3rd May 2016

First published on 4th May 2016


Abstract

Graphite oxide (GO) is receiving increased attention due to its special surface properties and layered structure for the synthesis of GO containing nanocomposites. It is possible that integration of GO sheets and iron oxide nanoparticles may result in enhanced properties and enlarge the application range. Herein, we report the effect of Fe2O3–GO nanocomposite as a new class of catalyst for the decomposition of ammonium perchlorate (AP), a rocket propellant oxidizer, and study the effect of Fe2O3[thin space (1/6-em)]:[thin space (1/6-em)]GO ratio on the catalytic activity. The material was characterized by X-ray diffraction and Raman spectroscopy and the formation of Fe2O3 and GO were confirmed. FESEM analysis showed that the Fe2O3 nanoparticles are highly dispersed between and on the graphene layers. With the addition of 3% of the composite with 1[thin space (1/6-em)]:[thin space (1/6-em)]1 Fe2O3–GO ratio, the decomposition temperature of AP was reduced by 45 °C, showing a high catalytic activity for the new composite. The high catalytic activity of the in situ synthesized Fe2O3–GO composite may be attributed to the uniform distribution of iron oxide nanoparticles which in turn provide a number of active sites on the surface due to the presence of GO.


1. Introduction

In the development of space vehicles and missiles composite solid propellants (CSP) are the major source of chemical energy. CSP are heterogeneous mixtures consisting of a large proportion of oxidizer, usually ammonium perchlorate (AP), a metallic fuel like aluminium powder and a fuel/binder, generally hydroxyl terminated polybutadiene. A specific feature of the thermal decomposition of AP is its extremely high sensitivity to the action of various additives, either entering the lattice (homophase) or forming their own phase (heterophase).1,2 These additives can accelerate or decelerate the processes of low-temperature and high-temperature thermal decompositions, which is important for the storage of AP and mix compositions based on it. It has been assumed that there exists a correlation between the effect of the additives on the rate of thermal decomposition and their influence on the combustion rates of mix compositions incorporating AP as the major component. This has stimulated the attention of many research groups, especially those dealing with the development of solid propellants, to the problem.3–5

Graphite oxide (GO) is receiving increased attention due to its special surface properties and layered structure for the synthesis of GO-containing nanocomposites. Specifically, owing to the introduction of oxygen-containing functional groups (hydroxyl, carboxyl and epoxy groups) on carbon nanosheets, GO became active and easily absorbs polar molecules and polymers. These materials often possess unusual properties as compared with their individual components, and can be used as precursors to produce conductive polymers, cathodic materials in lithium rechargeable batteries, and other functional nanomaterials like hybrid catalysts for the thermal decomposition of ammonium perchlorate, the major oxidizer used in composite solid propellants.6–12

To broaden the horizons for the use of GO-based composites, an idea of using nanoparticles (NPs) anchored onto GO sheets was examined. It is known that GO can be exfoliated under appropriate treatment forming quasi-two-dimensional carbon nanosheets. These exfoliated GO sheets possess large surface area and thus may be potential support materials to load NPs. In addition, the aforementioned oxygenated functional groups have been utilized as nucleation centers to anchor NPs onto some support materials (e.g. carbon nanotubes), forming NP-containing composites.13 Therefore, it is feasible to synthesize graphite oxide-nanoparticle composite (GONP) by depositing the NPs onto GO sheets. Meanwhile, just like other materials, we hope that GONP can lead to a possible concerted effect or an integration of the properties of the two components (GO and NPs) in the new materials that will present special features for catalysis and nanotechnology.14–16 Even though it has these special features, comparatively few investigations have been made with regard to GONP so far.17

Iron oxides and GO-based sheets have long been treated as promising materials for catalysis and energy storage such as in ultracapacitors due to their high electrical conductivity and surface area. Iron oxide (Fe2O3) is an important transition metal oxide that has been widely used as a catalyst in various industrial applications. Such a broad range of use has made the preparation of Fe2O3 nanostructures attract much attention.18,19 However, when used Fe2O3 individually, it is prone to aggregation that will greatly limit their accessible surface area, which prevents the full realization of their high catalytic activity. This problem can be solved by co-assembling Fe2O3 to GO—nanoparticles and sheets—to form Fe2O3-intercalated GO stacks. It is possible that integration of GO sheets and Fe2O3 NPs may result in enhanced properties and enlarge the application range, especially in the field of catalysis.20–23

Herein, we report a simple, efficient and scalable procedure for the synthesis of Fe2O3–GO sheets by in situ depositing Fe2O3 NPs between and on the surface of GO sheets from thermochemical oxidation of ferric nitrate. The assemblies of GO sheets are intercalated with iron oxides using solvothermal approach, and the structure is characterized by means of microscopy techniques (scanning electron microscopy). The chemical and physical properties of the assemblies are investigated by various analytical techniques. The catalytic activity of the composites was analyzed on the thermal decomposition of ammonium perchlorate by thermogravimetry analysis. More importantly, the optimum Fe2O3–GO ratio was investigated which may open up a whole new field for high energy application of carbon-based materials as support for catalytic systems.

2. Materials and methods

2.1 Chemicals

All chemicals used in this synthesis were of analytical grade and used without further purification. Analytical grade reagents viz., ferric nitrate trihydrate (Qualigens fine chemical, India) graphite flakes (Sigma-Aldrich, batch no. 282863), potassium permanganate, hydrochloric acid, sulphuric acid, hydrogen peroxide, barium chloride, (Merck, India) were used for the synthesis of catalysts. Ammonium perchlorate made in house with purity >99% was used for studying the catalytic activity.

2.2 Synthesis of graphite oxide

GO used in this work was prepared from purified natural graphite flakes according to modified Hummers method.24,25 In a typical procedure, 10 g of graphite flakes was added to 230 ml of cooled (0 °C) concentrated H2SO4. 30 g of KMnO4 powder was gradually added with constant stirring, keeping the temperature of the mixture below 20 °C. The mixture was then stirred at 35 °C for 30 min using a magnetic stirrer at 3000 rpm. Then 470 ml of distilled water was added slowly and the temperature was increased to 98 °C. The solution was maintained at that temperature for another 15 min. To the solution 1.4 l of distilled water was added followed by 10 ml of 30% H2O2 solution to terminate the reaction. The solid product obtained was separated by centrifugation, washed repeatedly with 5% HCl solution until it was free from sulphate (tested with BaCl2). After complete removal of sulphate, the suspension was dried in a vacuum oven at 60 °C for 48 h to obtain GO.

2.3 Synthesis of Fe2O3–GO hybrids

A series of four Fe2O3–GO were prepared with Fe2O3[thin space (1/6-em)]:[thin space (1/6-em)]GO weight percentage of 2[thin space (1/6-em)]:[thin space (1/6-em)]1, 1[thin space (1/6-em)]:[thin space (1/6-em)]1, 0.5[thin space (1/6-em)]:[thin space (1/6-em)]1, and 0.2[thin space (1/6-em)]:[thin space (1/6-em)]1. In a typical synthesis (Fe2O3[thin space (1/6-em)]:[thin space (1/6-em)]GO, 1[thin space (1/6-em)]:[thin space (1/6-em)]1) 500 mg of GO and 1.25 mmol of ferric nitrate was added to 15 and 20 ml of ethanol solution and ultrasonicated for 5 and 30 minutes respectively. The solutions were then mixed and magnetically stirred for another 30 min. The resulting mixture was transferred and sealed into a 50 ml Teflon-lined stainless steel autoclave, heated to 140 °C in an electric oven for 24 h. After attaining room temperature, the autoclave was opened and product obtained was rinsed extensively with absolute alcohol. Finally, the product was dried in a vacuum oven at 60 °C for 6 h. The resulting Fe2O3–GO powder was then heated to 200 °C in nitrogen atmosphere and kept at that temperature for 2 minutes. The other composites were also prepared by the same procedure, by changing the concentration of the ferric nitrate. Products thus obtained with Fe2O3[thin space (1/6-em)]:[thin space (1/6-em)]GO weight percentage of 2[thin space (1/6-em)]:[thin space (1/6-em)]1, 1[thin space (1/6-em)]:[thin space (1/6-em)]1, 0.5[thin space (1/6-em)]:[thin space (1/6-em)]1, and 0.2[thin space (1/6-em)]:[thin space (1/6-em)]1 are represented as FeGO1, FeGO2, FeGO3 and FeGO4 respectively. For comparison, Fe2O3 NPs without GO were prepared following the same procedure above without adding GO.

2.4 Characterization

Powder X-ray diffraction data of samples was collected on a Bruker D8-Discover powder X-ray diffractometer in a Bragg–Brentano configuration with a CuKα radiation (1.5418 Å) at a scan rate of 2.5 deg min−1. Crystalline phases were identified by comparing the experimental diffraction patterns to Joint Committee on Powder Diffraction Standards (JCPDS). Raman spectra of samples were recorded using a Witec Alpha 300R confocal microscope using an excitation wavelength of 532 nm. Perkin-Elmer GX FTIR spectrometer was used for FTIR analysis. Field emission scanning electron microscopy (FESEM) observations were performed to examine the morphology of the samples using Carl Zeiss, Supra 55 model field emission scanning electron microscope equipped with an energy-dispersive X-ray spectrometer (EDX). Simultaneous thermogravimetry-differential scanning calorimetry (TG-DSC), TA Instruments Q600, was employed for thermal characterization. In all the thermal analysis experiments a sample mass of 5 ± 1 mg was used under a nitrogen atmosphere in platinum sample cups at a heating rate of 5 °C min−1. For the evaluation of catalytic activity of synthesized Fe2O3–GO composites, fine AP (average particle, 50 μm) was homogeneously mixed with catalysts in the ratio 97[thin space (1/6-em)]:[thin space (1/6-em)]3 and subjected to thermal decomposition studies using TG-DSC techniques.

3. Results and discussion

GO, prepared by oxidation of graphite with strong oxidizing agents consists of distorted graphene layers bearing carbonyl, hydroxyl, and epoxy groups on the basal planes as well as carboxylic groups on the edges of the carbon sheets.20,21 All of these factors make the material acidic as well as highly hydrophilic and explain its easy composite formation in alkaline or alcohol solutions. Mechanism of formation of GO from graphite was already reported and hence it is not worthy to mention again.26 We are going to discuss the mechanism of formation of Fe2O3–GO system which is not reported elsewhere.

3.1 Driving force for the exfoliation of graphite and intercalation with Fe2O3

The intercalation process in GO is chemical as well as physical in nature.18 Even though it easily disperses in water due to the ionizable edge acid (–COOH) groups, a closer look at its structure reveals that it may actually be amphiphilic.26 Intercalation in GO can occur by reactive adsorption of the guest species (iron oxide in this case), where attractive forces among the functional groups of GO and the guest species are essentially ionic.16 However, the intercalation of certain species, mainly polar, is thought to be controlled by hydrogen bonding.14 Thus, The intercalant occupies and thereby expands the interplanar spacing of GO along its c-axis. It is already reported that intercalation of solvents from liquid phase showed that common solvents such as alcohols and both chlorine and aromatic compounds readily penetrate into the GO interspacing.27 Such molecules remained trapped in the GO structure after drying and caused irreversible changes in the GO interlayer distribution.

3.2 Raman spectra

Oxidations of graphite to produce GO introduces several chemical and structural changes in the parent graphite: increase in both the oxygen content and the interlayer distance and the formation of sp3-hybridized carbons which reduces the planar structure of the graphene layers. The extent of these changes depends not only on the synthetic methods but also on the graphite sources used. Therefore, our GO was first of all characterized by suitable and available techniques. Raman spectroscopy is a widely used tool for the characterization of carbon products, especially considering the fact that conjugated and double carbon–carbon bonds lead to high Raman intensities. Highly ordered graphite has only a couple of Raman-active bands visible in the spectra (Fig. 1), the in-phase vibration of the graphite lattice (G band) at 1575 cm−1 as well as the (weak) disorder band caused by the graphite edges (D band) at approximately 1355 cm−1.
image file: c6ra06860j-f1.tif
Fig. 1 Raman spectra of graphite after oxidation and exfoliation processes. The position of D, G and 2D band in graphite and GO is represented by a vertical, dotted line.

Both the G and the D bands in graphite undergo significant changes during the transformation of graphite to GO. Specifically, the G band broadens significantly and shift to higher frequencies (blue-shift), and the D band grows in intensity. A notable fact is that the G band peak is located at a higher frequency in GO than that in graphite (1590 vs. 1575 cm−1). Since in all measurements the same laser excitation frequency (532 nm) was used, we can exclude spurious shifts which are known to affect the D band of graphite. A literature survey points to several explanations for this blue shift, but the most plausible explanation is the presence of isolated double bonds produce another band, the DI band, resonate at higher frequencies than the G band of graphite, located at 1620 cm−1 which can partially merge with the G band.28–30

From the spectra, it is evident that presence of iron oxide (confirmed by the peaks in the range 200–300 cm−1) didn't produce any significant changes in the Raman spectra of the GO. D and G bands are well distinguishable and the 2D (even though it is weak) band is observable even in the presence of iron oxide. This gives an indication that the iron oxide particles were highly dispersed between and on the graphene layers (supported by SEM analysis discussed later in the paper).20 As the ratio of iron oxide in the composite increases the peaks intensity in the range 200–300 cm−1 increase.

3.3 IR spectra

FTIR spectra of pristine GO and Fe2O3–GO (Fig. 2) was recorded within the absorption range 400 to 4000 cm−1. The following functional groups were identified in pristine GO and Fe2O3–GO systems: O–H stretching vibrations (3420 cm−1), C–O stretching vibration (1720–1740 cm−1), C–C vibrations from unoxidized sp2 C–C bonds (1590–1620 cm−1), and C–O vibrations (1250 cm−1). The FTIR spectrum of GO (Fig. 2) shows a broad peak between 3000 and 3700 cm−1 in the high-frequency area corresponding to the stretching vibration of OH groups of water molecules adsorbed on graphite oxide. This shows the strong hydrophilicity of the material. The presence of absorption peak in the medium frequency area, at 1630 cm−1 can be attributed to the stretching vibration of C[double bond, length as m-dash]C.
image file: c6ra06860j-f2.tif
Fig. 2 FTIR spectra of GO and Fe2O3–GO composite.

The stretching vibration of carboxyl groups on the edges of the layer planes or conjugated carbonyl groups is observed at 1715 cm−1. Finally, the absorption peaks at 1385 cm−1 and 1110 cm−1 correspond to the stretching vibration of C–O of carboxylic acid and C–OH of alcohol, respectively. Even though these peaks are observed, there is an additional peak at 2930 cm−1 and 2850 cm−1 (weak) which correspond to the symmetric and antisymmetric stretching vibrations of unoxidized CH2, showing that the complete oxidation of graphite is not taking place during conversion. For the IR spectra of Fe2O3–GO composites, along with these peaks an additional peak at 530 cm−1 is observed corresponds to the stretching vibration of Fe–O bond. It is interesting to note that there is no change in the absorption frequencies of GO even in the presence of Fe2O3 nanoparticles. It is also to be noticed here that the peak corresponding to Fe–O stretching is grown in intensity as the concentration of Fe is increasing.

3.4 XRD

A series of characteristic peaks were observed in the XRD pattern of Fe2O3–GO (Fig. 3b). The positions and relative intensities of the reflection peak of all composites agree with the diffraction peaks of standard α-Fe2O3, according to standard data (JCPDS 33-0664).18,19
image file: c6ra06860j-f3.tif
Fig. 3 XRD of graphite and GO (a), Fe2O3 and Fe2O3–GO composites (b).

Oxidation of graphene sheets results in an increase of the interlayer distance in GOs compared to graphite. The expansion of the lattice is considered as one of the main indicators for the purity of the material and the degree of its oxidation. The high oxidation state of the GO samples in this study is confirmed by analysis of XRD patterns recorded from pristine powders at ambient conditions (Fig. 3a). As expected, GO sample exhibited a significant increase of interlayer distance compared to graphite (deduced from the position of (001) reflection), up to 7.18 Å. These results indicate that the interlayer space of graphite became mostly occupied by oxygen-containing functional groups upon oxidation. The reduction of the average size of coherent diffraction domains in GO as compared to its parent graphite indicates that severe disruption of graphite layers took place during the oxidation process.30,31 It should be noted that graphene oxide layers in GO are packed turbostratically and there is no ordering for various functional groups in the structure. Also, GO samples absorb some water from air at ambient humidity, and complete drying of samples seems to be very difficult. Therefore, the values of d-spacings cited above might reflect different abilities of samples to become hydrated by air at ambient humidity.

3.5 Electron microscopy and EDX

Field emission scanning electron microscopy (FESEM) observations were performed to examine the morphology of the samples. Fig. 4 shows the FESEM images of the pristine Fe2O3 and Fe2O3–GO composites. These figures (Fig. 4C–F) show that the graphite oxide layers are well separated due to thermal exfoliation and Fe2O3 particles are occupied between and on the surface these layers.
image file: c6ra06860j-f4.tif
Fig. 4 (A and B) FESEM images of Fe2O3 nanoparticles (C–F) high-magnification SEM images of Fe2O3–GO nanocomposites. (C) FeGO1 (D) FeGO2 (E) FeGO3 (F) FeGO4.

From Fig. 4A and B it can be seen that the pristine Fe2O3 NPs were polydisperse and seriously aggregated. After an introduction to GO, the particles maintained their original shape with a good monodispersity. Fig. 4C shows that, in comparing with pure Fe2O3, the tendency for aggregation is reduced for the FeGO1 sample. When the ratio is changed to 1[thin space (1/6-em)]:[thin space (1/6-em)]1 (FeGO2), the tendency for agglomeration is again reduced and the number of intercalated Fe2O3 particles is increased (Fig. 4D). The average particle size of the pristine Fe2O3 NPs was about 17 nm. In the presence of GO, the particle size is reduced to 7 nm which shows the effect of GO support on the size of Fe2O3 NPs. It has been reported that during the thermal exfoliation, GO actually undergoes disproportionation reactions, in which some of the partially oxidised sp3 carbon atoms become fully oxidised to carbonaceous gases such as CO2 and the rest reduced to sp2.32,33 The rapid evolution of gaseous species such as H2O and CO2 during the deoxygenation process fragmented the GO and results in a black plume of GO. Deoxygenation was triggered on the spot and then rapidly propagated across the entire film. The evolution of CO2 and H2O caused a large apparent volume expansion of ∼100–300 times, thus producing very low-bulk density.32 Fig. 4C–F shows the cross-sectional view of a GO film, showing much more loosely packed GO sheets after exfoliation. For the composite with other two combinations, since the Fe2O3–GO ratio is very less, a number of intercalated Fe2O3 particles is lesser than the other two samples. Hence, from these observations, it is concluded that composite with Fe2O3–GO ratio of 1[thin space (1/6-em)]:[thin space (1/6-em)]1 was the optimum concentration to obtain a well dispersed and intercalated Fe2O3 particles with lesser aggregation.

Fig. 5A shows the compositional analysis of the materials using EDX. The EDX technique can be used to determine the composition of a specimen as a whole as well as the composition of individual components. The areas under selected peaks can also be used to provide semi-quantitative elemental composition information. The compositional analysis results shown in Fig. 5A reveal that Fe, C, and O are the main elements present within the inspection field, with varying concentrations. From elemental mapping images shown in Fig. 5B it is confirmed that the Fe2O3 particle are well dispersed between and on the graphene layers.


image file: c6ra06860j-f5.tif
Fig. 5 (A) EDX spectrum of Fe2O3–GO composites at different compositions. EDX spectra confirm the regular increase in Fe concentration. (B) Elemental mapping images of Fe2O3–GO composites. Red – oxygen, green – carbon and white – iron. The regular decrease in Fe concentration was confirmed from these mapping images.

3.6 Surface area

Surface area for all the samples was measured using BET method and is tabulated in Table 1. From Table 1, it can be seen that surface area of all samples shows a direct dependence on the amount of Fe2O3 used during the synthesis. Accordingly, the surface area shows a significant increase with an increase in the GO content. For pristine GO, the surface area was about 205 m2 g−1. On addition of 0.2% of Fe2O3 surface area is reduced to 145 m2 g−1. As the concentration of Fe2O3 is increased, the surface area is still reduced and finally reached a value of 90 m2 g−1 for the sample with Fe2O3–GO ratio of 2[thin space (1/6-em)]:[thin space (1/6-em)]1.
Table 1 Surface area of samples measured using BET method
Sample Surface area (m2 g−1)
Fe2O3 45
FeGO1 90
FeGO2 100
FeGO3 114
FeGO4 145
GO 205


3.7 Catalytic activity on the thermal decomposition of AP

AP is the most common oxidant in composite solid propellants since its thermal decomposition characteristics directly influence the combustion behaviour of the propellant. More specifically, the activation energy, reaction rate and kinetics of thermal decomposition of AP are closely related to the performance of solid propellants. A lot has been said in the literature about the mechanism of decomposition of AP, but still it a matter of debate.8,33 According to electron transfer mechanism of decomposition of AP, the rate determining step for the Low-Temperature Decomposition (LTD) is the transfer of an electron from ClO4 to NH4+, while for High-Temperature Decomposition (HTD) rate determining step is the transformation of oxygen to superoxide. In the presence of burn rate modifiers, the rate of these LTD and HTD are accelerated and thus, the decomposition reaction is completed at low temperature. Unique properties of metal oxides like a large number of acid sites; ability to accept and release electrons makes them a good conductor of electrons thereby accelerating the decomposition reactions, especially redox reactions.

We have investigated the as-synthesized Fe2O3–GO composite as an additive to the thermal decomposition of AP, together with its individual component (Fe2O3) for comparison. Thermogravimetry-differential scanning calorimetry (TG-DSC) measurements were used to examine this catalytic process. The TG, DTG and DSC curves for pure AP and AP with catalysts are shown in Fig. 6 and 7. From Fig. 7 it can be seen that three peaks centered at 242, 293, and 360 °C are observed, corresponding to the endothermic phase transition, the exothermic low-temperature decomposition (LTD) and the exothermic high-temperature decomposition (HTD), in agreement with those reported earlier.34,35 The endothermic transformation happens from the orthorhombic phase to the cubic phase (240–250 °C).


image file: c6ra06860j-f6.tif
Fig. 6 TG and DTG curves for the thermal decomposition of AP with and without catalysts. High catalytic activity of the new hybrid composites was confirmed from these diagrams.

image file: c6ra06860j-f7.tif
Fig. 7 DSC curves for the thermal decomposition of AP with and without catalysts.

On addition of 3 wt% catalysts, the two stage decomposition of pure AP becomes almost a single stage with a lowering of decomposition temperature by 40–50 °C. A closer look at DSC curves (Fig. 7) revealed that the LTD of AP is not much affected by the catalyst whereas HTD is actively catalyzed, reducing its initiation temperature. Decrease in temperature is more significant by the addition of FeGO2 compared to all other catalysts which is attributed to the well dispersed and intercalated Fe2O3 particles as revealed by the FESEM analysis.

The decomposition kinetics also supporting the high catalytic activity of FeGO2. Kinetic parameters via activation energy (Ea) and rate constants (k) for the thermal decomposition of pure AP and AP in presence of catalysts were calculated using isoconversional Kissinger–Akahira–Sunose (KAS) method which is based on the following equation.36

 
image file: c6ra06860j-t1.tif(1)
where β is the heating rate, Tα is the temperature in kelvin corresponding to a fixed degree of conversion, α, A is the pre-exponential factor, R is the gas constant, Eα is the activation energy at a given degree of conversion and g(α) is the integral form of kinetic model function. Eα for a given degree of conversion is obtained from the slope of the linear fit of the plot image file: c6ra06860j-t2.tif versus 1/Tα. The average of Eα value is reported as activation energy (Ea) of the decomposition reactions. The rate constants (k) for the reactions were calculated using Arrhenius equation as shown in eqn 2.
 
image file: c6ra06860j-t3.tif(2)

TG analysis of pure AP, AP in presence of Fe2O3 and Fe2O3–GO (FeGO2) catalysts were carried out at heating rates of 2, 3 and 5 °C min−1. And the derived kinetic parameters are tabulated in Table 2. From the table it can be see that pure AP has Ea and k value of 90 kJ mol−1 and 5.5 × 103 min−1 respectively. Addition of Fe2O3 and FeGO2 reduce the Ea values to 60 and 55 kJ mol−1 while k values increase to 8.2 and 9.8 × 103 min−1 respectively. This reflects that FeGO2 catalyst has superior activity than Fe2O3.

Table 2 Activation energy and rate constant for the thermal decomposition of pure AP, AP in presence of Fe2O3 and FeGO2 catalysts
Sample Kinetic parameter
Activation energy, Ea (kJ mol−1) Rate constant k, (min−1)
Pure AP 90 5.5 × 103
AP + Fe2O3 60 8.2 × 103
AP + FeGO2 55 9.8 × 103


It can be seen from the above experimental results that Fe2O3–GO hybrids, especially FeGO2, significantly promote both the low-temperature and high-temperature exothermic process of AP (Fig. 6 and 7). It has been well addressed that GO exhibits a good conductivity and electrons in GO move a lot faster than they do among metal atoms. Due to its exceptional electronic characteristics, electrons can travel long distances in GO without being scattered.37 Thus, it can be inferred that Fe2O3–GO hybrids used here could offer accelerated electron flow from ClO4 to NH4+ and transforming to NH3 and HClO4. The O2 formed from HClO4 is transformed to superoxide ion (O2) at a faster speed due to the presence of GO as a perfect bed for the flow of electrons. The superoxide ions together with other products of HClO4 could then help the decomposition of NH3 and finally complete the decomposition of AP.

The ion current versus temperature curves of ion fragments during the thermal decomposition of AP, AP with pure Fe2O3 and AP with FeGO2 are shown in Fig. 8a–c. It was reported that during the LTD of AP, one of the decomposition product, ammonia, is not completely oxidised due to the prevailing low temperature. This ammonia will accumulate/adsorbed on the reactive surface of residual AP preventing it from further decomposition. However, as the temperature increases, adsorbed ammonia get oxidised, initiating the HTD. Most of the transition metal oxides catalyze the decomposition of perchlorate ion and oxidation of ammonia.33,34 The TG-MS studies of decomposition of AP with and without catalysts showed that in the LTD of pure AP the concentration of oxidized products like H2O and HCl are very low compared to that in HTD. However, the concentration of N2O and O2 in LTD and HTD are almost comparable indicating incomplete oxidation during LTD.


image file: c6ra06860j-f8.tif
Fig. 8 (a) Ion current versus temperature curves of ion fragments during the thermal decomposition of AP. (b) Ion current versus temperature curves of ion fragments during the thermal decomposition of AP with pure Fe2O3. (c) Ion current versus temperature curves of ion fragments during the thermal decomposition of AP with FeGO2.

It can be seen that the decrease in decomposition temperature is more significant by the addition of FeGO2 compared to other composites and pure Fe2O3. For a heterogeneous catalytic reaction like AP decomposition, where the rate determining step is the oxidation of gaseous ammonia, a catalyst (FeGO2) with high surface area and active sites will perform better than one with the lower surface area by providing a large platform for catalytic oxidation. In addition, the presence of GO, a good conductor of electrons in the system will enhance the redox reaction taking place during the decomposition of AP by acting as better carrier/conductor of electrons.13 Evolution of more amounts of oxidized products viz. HCl, N2O and H2O during the early stages of decomposition confirms the high exothermicity of the reaction in the presence of FeGO2 as a catalyst.

4. Conclusion

Fe2O3–GO composites with different Fe2O3[thin space (1/6-em)]:[thin space (1/6-em)]GO ratio and excellent catalytic properties have been synthesized successfully by solvothermal synthesis. Fe2O3 nanoparticles with a size of about 17 nm are homogeneously dispersed between and on the graphene layers that could effectively prevent them from aggregating. Raman spectroscopy and XRD studies confirm the formation of GO from graphite. FESEM analysis shows that the Fe2O3 nanoparticles are highly dispersed between and on the graphene layers. With the addition of 3% Fe2O3–GO composites the low-temperature decomposition and the high-temperature decomposition temperatures of AP were reduced. Catalytic activity was high for the FeGO2 composite with a Fe2O3[thin space (1/6-em)]:[thin space (1/6-em)]GO ratio of 1[thin space (1/6-em)]:[thin space (1/6-em)]1. The high catalytic activity of the in situ synthesized FeGO2 composite may be attributed to uniform distribution of iron oxide nanoparticles which in turn provide a number of active sites on the surface due to the presence of GO.

Acknowledgements

The authors thank Director, VSSC and colleagues in Analytical and Spectroscopy Division, VSSC for their support.

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