A. D. Vermaa,
R. K. Mandalb and
I. Sinha*a
aDepartment of Chemistry, Indian Institute of Technology (Banaras Hindu University), Varanasi 221005, India. E-mail: isinha.apc@iitbhu.ac.in
bDepartment of Metallurgical Engineering, Indian Institute of Technology (Banaras Hindu University), Varanasi 221005, India
First published on 25th October 2016
The search for nanomaterials for catalysis of transfer hydrogenation reactions with green hydrogen sources is an important topical issue. In this work we show that anisotropic silver nanoparticles act as efficient catalysts for p-nitrophenol (Nip) reduction with glycerol, a renewable biomass byproduct, as the green hydrogen source. Anisotropic silver nanoparticles (AgNPs) were prepared using polyol method in presence of Cu2+ salt as an etchant. These AgNPs are found to be a combination of mixture of anisotropic shapes and spherical faceted nanoparticles. The percentage of anisotropic shapes in the distribution changes with amount of etchant used. Effect of shape and size of AgNPs on the catalytic kinetics of Nip reduction using glycerol as a hydrogen source was investigated. The AgNPs sample having more nanoparticles with anisotropy and finer average particle size exhibits better kinetics, lower activation energy and better turnover frequency (TOF).
Among the available nitroarenes, the reduction of p-nitrophenol (Nip) using NaBH4 as the reductant has been studied extensively as a model pollutant and catalytic reduction reaction. Given its model behavior, this reaction has been used to compare the kinetics of catalytic reduction over various nanoparticles. In contrast to this conventional reaction, in which NaBH4 is used as a reductant, glycerol can work both as reductant as well as the solvent. In the present work we investigate the catalytic reduction of p-nitrophenol to p-aminophenol (AP) as a model representative of nitroarenes using glycerol as the reductant in a mixture of glycerol and water as the reaction medium. Current literature suggests that there are only few reports of nanomaterials used as catalysts in reduction of nitroarenes to aminoarenes using glycerol as the reductant. In most of these studies glycerol has been used to serve as solvent. A survey of recent literature shows that nanoparticles of Ru, Ni, Ir, Fe3O4–Ni have been used as catalysts for this class of reactions.3,18–20
In this communication we show that anisotropic silver nanoparticles (AgNPs) act as efficient catalysts for this reaction. It is well-known that shape, size and composition of nanoparticles affect their catalytic activities. One popular and simple route for preparation of anisotropic AgNPs, is by polyol route in presence of etchants like H2O2, chloride ion, bromide ion and Cu2+ ions.21,22 In the present study, first of all, we report the effect of amount of Cu2+ etchant on the type of anisotropic AgNPs formed. We then discuss the effect of shape and size of the prepared AgNPs on the kinetics of the transfer hydrogenation using glycerol as a hydrogen source. To the best of our knowledge this is a first report of silver nanoparticles being utilized as catalyst for the transfer hydrogenation reaction of Nip to AP using glycerol as a hydrogen donor. Effects of temperature on the reaction and thereby on activation energies are discussed.
As per XRD data reported for silver in JCPDS-ICDD (card no. 87-0720), these correspond to the [111], [200], [220], [311] and [222] planes of FCC silver. TEM micrographs of AgNPs samples C1, C2, C3 and C4 are shown in Fig. 2. The size distribution histograms of the respective AgNPs samples are displayed as inset in these figures. The average size of nanoparticles observed in samples C1, C2, C3 and C4 are ∼45, ∼58, ∼65 and ∼135 nm respectively. The crystallite sizes of AgNPs samples were calculated by the Scherrer formula. Crystallite sizes for samples C1, C2, C3 and C4 were found to be 13.9, 14.6, 16.9, 31.2 nm respectively. Since these sizes are smaller than the average nanoparticle sizes, therefore, we can conclude that the AgNPs samples prepared are made of multiple crystallites. The AgNPs size increases with the Cu2+ etchant concentration. Furthermore, the nature of shape anisotropy also changes with the etchant. We observe that at low etchant concentration (sample C1) various anisotropic shapes like rod, triangle, square and hexagon are present. However, the percentage of spherical faceted particles formed (in C1) is the largest. Table 1 gives the percentage distribution of various anisotropic shapes formed in various AgNPs samples. As the amount of Cu2+ salt was increased, the percentage of various anisotropic shapes decreased from C1 to C4. In all cases spherical faceted nanoparticles dominate the distribution. In C4, along with some of these shapes, nanowires were also formed.
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Fig. 2 TEM images of C1, C2, C3 and C4 AgNPs shown as (a), (b), (c) and (d) respectively (particle size distributions are shown as inset of their corresponding TEM micrograph). |
Fig. 3 shows LSPR absorbance spectra of aqueous dispersions of AgNPs samples. For samples C1, C2, C3 and C4 LSPR absorbance maxima are observed at 420, 445, 465 and 475 nm respectively. Ag nanostructures show different LSPR bands depending upon the size and shape of nanoparticles. Mock et al. reported that faceted spherical particles show a red shift in LSPR absorbance from ∼410 to ∼490 nm with the nanoparticle size variation from ∼40 to ∼90 nm.23 The gradual red shift in transverse LSPR with increase in the average particle size (from C1 to C4) is in agreement with observations in reference.23 As mentioned earlier, in all the four AgNPs samples faceted spherical shapes are in majority. AgNPs sample C1 exhibits maximum number of anisotropic shapes, whereas in other three samples the percentage of anisotropic shapes are less. The LSPR absorbance spectrum of sample C4, owing to the presence of nanowires, displays a longitudinal LSPR at 750 nm.24
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Fig. 4 UV-Vis absorption spectra of Nip versus time of the blank sample (without AgNPs catalyst) (a) and in presence of C1 AgNPs catalyst (b). |
The general form of the rate equation for reduction of Nip is given by the following equation.
![]() | (1) |
![]() | (2) |
![]() | (3) |
The slope of the linear fit of vs. ln
At plot gives the order n.26,27 The value of n is found to be ∼2 for all AgNPs catalyst samples prepared. Thus, the kinetics followed is second order kinetics with respect to Nip when glycerol is the hydrogen source. This is in contrast to the pseudo first order (or in some cases zero order) kinetics reported for reduction of Nip with NaBH4 in presence of different nanocatalysts.27–29
Consequently, in Fig. 5 we plot 1/At versus time integrated kinetics plots for C1, C2, C3 and C4 catalyzed reactions. As expected in all these plots 1/At changes linearly with time. The kapp values were determined from the slope of the linear fit of (1/At) with time. The kapp values are given in Table 2. It can be seen that the kapp for C1 is highest and then the values decrease as for C2, C3 and C4 AgNPs. This correlates well with the increase in nanoparticle size from C1 to C4. As the nanoparticle size increases, the surface area of the catalyst and thus the number of surface active sites decreases. The kapp value of C1 is relatively higher than the rest of the samples. This possibly is because C1 AgNPs has the smallest average nanoparticle size with larger number of anisotropic shapes. As we move from C1–C4, the sizes of catalysts increase and the percentage of anisotropic shapes decreases, hence kapp decreases from C1 to C4.
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Fig. 5 Variation of 1/At [absorbance (A) measured at λ = 406 nm] versus time (t) for C1, C2, C3 and C4 AgNPs. |
Sr. no. | Catalyst | Apparent reaction rate (kapp) (mol−1 l min−1) | Activation energy (Ea) (kJ mol−1) | ||
---|---|---|---|---|---|
kapp | R2 | Ea | R2 | ||
1 | C1-AgNPs | 0.0122 | 0.99342 | 24.98 | 0.99631 |
2 | C2-AgNPs | 0.0089 | 0.99201 | 41.96 | 0.99462 |
3 | C3-AgNPs | 0.0059 | 0.99403 | 47.56 | 0.99775 |
4 | C4-AgNPs | 0.0041 | 0.95319 | 60.95 | 0.99052 |
5 | C0-AgNPs | 0.00937 | 0.988 | 52.77 | 0.99399 |
To find the activation energies of catalyst for Nip reduction, the reactions were carried out at different temperatures. These experiments showed that kapp for all AgNPs catalyst increased with temperature. The classical Arrhenius equation was employed to find out the activation energies of catalyst. Fig. 6 shows lnkapp versus 1/T plots for all the samples C1, C2, C3 and C4. A linear fit was obtained in all the cases as per linearized Arrhenius eqn (4).
ln![]() ![]() | (4) |
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Fig. 6 Arrhenius plot for Nip reduction reaction catalyzed by C1, C2, C3 and C4 AgNPs. Please note that for most data points, error bars are smaller than the size of the symbol used. |
The activation energy (Ea) was obtained from the slope (−Ea/R) of the linear fits to the plots. The values computed are in agreement with the catalytic activity of AgNPs samples. The activation energy increases from C1 to C4. As mentioned in Section 2, for the sake of comparison AgNPs were also synthesized in absence of etchant. The average size of AgNPs formed without etchant is 60 nm (Fig. S2 ESI†). Almost spherical nanoparticles (but faceted) are formed. The activation energy for AgNPs without using Cu2+ etchant was found to be 52.77 kJ mol−1 (Fig. S4 ESI†). In contrast to this the average size of C3 AgNPs is ∼65 nm, while the activation energy is 47.56 kJ mol−1. Sample C2 has an average size of 58 nm and Ea ∼ 41.96 kJ mol−1. From this comparison, we can infer that the lesser Ea of C2 and C3 is due to the anisotropic shapes present in the sample. For instance, in the paper published by Xia et al.,30 the authors reported that the activation energy of hydrogenation of benzene for anisotropic nanocrystals was almost three times lower. Narayanan et al. also showed that activation energy changes with anisotropic shapes of the catalyst.31
Furthermore, the activation energy value of C1 is nearly half of the values found for other catalysts. This is possibly due to the larger percentage of smaller anisotropic particles in C1. From the trend of Ea values it appears as if activation energy values are correlated with the percentage of anisotropic nanoparticles in the AgNPs sample. To verify this, we plotted percentage of nanoparticles with anisotropic shapes (excluding long nanowires) against activation energy (Fig. 7a). There seems to be an approximately linear relation between percentage of nanoparticles with anisotropic shapes and their activation energies.
As mentioned in Section 3.1, a comparison of crystallite size from XRD and nanoparticle size from TEM analysis shows that the nanoparticles are composed of multiple crystallites. Therefore, change in Ea from sample C1 to C4 could also be due to change in grain boundary densities with increase in particles sizes.32,33 Grain boundaries are high energy regions, therefore, Ea could also change due to change in grain boundary density with increase in particle size. To explore whether grain boundaries affect the activation energy or not we have plotted the activation energy against average size of the nanoparticles. The plot is non-linear and agrees with a second order polynomial fit. The activation energy increases with size of the nanoparticles (Fig. 7b). This may be because of decrease in grain boundary density with increase in the size of the nanoparticles.
Rate constant alone is not sufficient to compare the catalytic activity due to various reasons. The actual amount of catalyst and products are not considered in determining the rate constants. Furthermore, the orders of the reactions may be different. Therefore, we calculated turnover frequency (TOF) to compare the activities of these catalysts. The comparisons of rates and TOF for all four systems are tabulated in Table 3. In ref. 1 and 10 glycerol was used as the solvent. On the hand, in ref. 3, 10% glycerol was used as the hydrogen source under inert gas atmosphere and solvothermal conditions. In contrast to these (ref. 1, 3 and 10), in the present study all reactions were carried out at ∼65 °C with only 16% glycerol as the reductant. More importantly, the TOF values for all AgNPs catalysts are much higher than the earlier three studies. As shown in Fig. 7, with decreasing percentage of anisotropic shapes the activation energy decreases. Moreover, as we go from C1 to C4 the AgNPs size also increases, which means that the overall nanoparticle surface area and consequently the number of active catalytic sites also decreases. Owing to a combination of these two factors, the TOF values decrease as we go from C1 to C4.
Sr. no. | Catalyst | Nitroarenes | Reaction conditions | TOF (min−1) | Reference |
---|---|---|---|---|---|
1 | Fe3O4–Ni | 4-Nitrophenol | In glycerol at 80 °C | 2.4 × 10−2 | 1 |
2 | Ru/MgLaO | Nitroarenes | In water–10% glycerol at 170 °C and inert gas pressure (N2 gas) 1 MPa in autoclave | ∼2.6 × 10−2 | 3 |
3 | RANEY® Ni | Nitrobenzene | In glycerol at 70 °C | ∼4.37 × 10−4 | 10 |
4 | C1-AgNPs | 4-Nitrophenol | In water–16% glycerol at 65 °C | 80 | This study |
5 | C2-AgNPs | 4-Nitrophenol | In water–16% glycerol at 65 °C | 42 | This study |
6 | C3-AgNPs | 4-Nitrophenol | In water–16% glycerol at 65 °C | 27 | This study |
7 | C4-AgNPs | 4-Nitrophenol | In water–16% glycerol at 65 °C | 19 | This study |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra23676f |
This journal is © The Royal Society of Chemistry 2016 |