Yunxiang
Qiao
ab,
Nils
Theyssen
*a,
Bernd
Spliethoff
a,
Jan
Folke
b,
Claudia
Weidenthaler
a,
Wolfgang
Schmidt
a,
Gonzalo
Prieto
ac,
Cristina
Ochoa-Hernández
a,
Eckhard
Bill
ab,
Shengfa
Ye
abd,
Holger
Ruland
b,
Ferdi
Schüth
a and
Walter
Leitner
*be
aMax-Planck-Institut für Kohlenforschung, Kaiser-Wilhelm-Platz 1, 45470 Mülheim an der Ruhr, Germany. E-mail: theyssen@kofo.mpg.de
bMax Planck Institute for Chemical Energy Conversion, Stiftstr. 34-36, 45470 Mülheim an der Ruhr, Germany. E-mail: walter.leitner@cec.mpg.de
cITQ Instituto de Tecnología Química, Universitat Politècnica de València-Consejo Superior de Investigaciones Científicas (UPV-CSIC), Avenida de los Naranjos s/n, 46022 Valencia, Spain
dDalian Institute of Chemical Physics, Chinese Academy of Sciences, 457 Zhongshan Road, 116023 Dalian, PR China
eInstitut für Technische und Makromolekulare Chemie, RWTH Aachen University, Worringerweg 1, 52074 Aachen, Germany
First published on 12th January 2021
Sheet silicates, also known as phyllosilicates, contain parallel sheets of tetrahedral silicate built up by [Si2O5]2− entities connected through intermediate metal–oxygen octahedral layers. The well-known minerals talc and pyrophyllite are belonging to this group based on magnesium and aluminium, respectively. Surprisingly, the ferric analogue rarely occurs in nature and is found in mixtures and conglomerates with other materials only. While partial incorporation of iron into pyrophyllites has been achieved, no synthetic protocol for purely iron-based pyrophyllite has been published yet. Here we report about the first artificial synthesis of ferripyrophyllite under exceptional mild conditions. A similar ultrathin two-dimensional (2D) nanosheet morphology is obtained as in talc or pyrophyllite but with iron(III) as a central metal. The high surface material exhibits a remarkably high thermostability. It shows some catalytic activity in ammonia synthesis and can serve as catalyst support material for noble metal nanoparticles.
Minerals of the latter group contain three layers: silicate tetrahedral layers are located on the top and on the bottom (indicated by [Si4O10] in the formula), which are connected via a metal–oxygen octahedral layer. Materials with such etrahedral/ctrahedral/etrahderal arrangements are classified as TOT sheet silicates.4,5 Pyrophyllite is aluminum-based (Al2[Si4O10](OH)2) and talc is magnesium-based (Mg3[Si4O10](OH)2). The ferric analogue of pyrophyllite, known as ferripyrophyllite, has the idealized formula Fe2[Si4O10](OH)2 and was first reported by F.V. Chukhrov et al. in 1978.6,7 It is found as a natural mineral only in mixtures or conglomerates with lots of impurities. The structure of ferripyrophyllite is shown in Fig. 2.1,5,8,9 It is a dioctahedral TOT sheet silicate in which two-thirds of the octahedra are occupied with iron(III) centers, with hydroxyl groups attached.
Fig. 2 Two unit cells of Ferripyrophyllite – the proposed structure of the iron silicate described herein (side view). |
Although the hydrothermal formation of transition metal phyllosilicates is known for cobalt,11 nickel,12 cobalt–nickel mixtures13 and copper,14 no synthetic protocol for iron-based pyrophyllite has been reported to the best of our knowledge yet.10 Prominent iron silicate minerals are fayalite (Fe2SiO4),15 ferrosilite (FeSiO3 or Fe2Si2O6),16–18 iscorite (Fe(II)5Fe(III)2SiO10)19,20 and greenalite ([Fe(II), Fe(III)]2-3 Si2O5(OH)4).21,22 They are either formed under rather severe reaction conditions (>1000 °C, high pressure) or only found in nature.
Herein, we describe the discovery of Ferripyrophyllite formation at mild temperatures and almost ambient pressure. The initial isolation resulted from serendipitous observations carrying out catalytic reactions with SBA-15 material in aqueous media in steel reactors. Based on this initial finding, a reproducible synthetic protocol was developed that allows the usage of different silica sources (including for example also MCM-41, AlSBA-15, and aerosil) in combination with simple Fe powder in water. The preparation is typically performed at 100 °C in sealed stainless steel autoclaves (with glass inlet) under initial ambient pressure of air (see ESI for experimental details and S1–S11 for TEM and EDX analyses†).
Fig. 3 TEM image of iron silicate nanosheets synthesized from iron powder and SBA-15 at 100 °C in water. |
According to TEM analysis, the apparent thickness of the nanosheets were in a range between 0.5 and 0.8 nm, which is consistent with the theoretical value of 0.7 nm (Fig. S12†). While parallel formation of a thinner TO sheet silicate cannot be ruled out completely, we have no evidence from any of our analytical techniques.
The oxidation of metallic iron to Fe(III) centers during the synthesis is accompanied by proton reduction according to eqn (1). The evolution of hydrogen is indicated by a distinct pressure increase during the reaction and was confirmed via GC analysis of the gas phase. The presence of about 4.89 mmol g−1 hydroxyl groups in the iron silicate (8.31 wt%, after drying at 100 °C for 12 h to remove physisorbed water) as determined by titration24,25 also accounts for the OH− formation.
2 Fe0 + 6 H2O → 2 Fe3+ + 6 OH− + 3 H2 | (1) |
X-ray photoelectron spectroscopy (XPS) revealed an atomic ratio of Fe to Si of exactly 1:2 on the surface of the material. The XPS spectrum of Si 2p shows a single peak at 103.1 eV (Fig. S14†), which is well within the reported values for silicates (101.6–103.8 eV).26,27 The spectra of Fe 2p1/2 and Fe 2p3/2 show characteristic peaks at 725.6 and 712.0 eV, together with associated satellite peaks (Fig. S15†). Combined with the single peak of Fe 3p at 56.9 eV, a clear dominance of Fe(III) centers can be deduced from these data.28,29
The Fe(III) oxidation state is further confirmed by 57Fe Mössbauer spectroscopy (Fig. S16†).30–34 The small isomer shift of about 0.36 mms−1 at room temperature indicates Fe(III) high spin centers with six hard ligands, which are expected to be oxygen. A defined coordination environment is difficult to deduce, however, because the quadrupole splitting is quite large (about 0.79 mm s−1), showing deviations from cubic symmetry. Furthermore, the high experimental line width of about 0.74 mm s−1, which could be fitted with a Gaussian distribution of Lorentzian lines, points to heterogeneities and an overlap of several similar lattice sites. Almost 100% Fe(III) species were found to be present, a minor subspectrum (max. 7%) indicates the presence of only traces of Fe(II) species. A broad peak in the EPR spectrum (Fig. S17†) is typical of ferromagnetic resonances of small magnetic domains.35 Magnetization curves under zero-field-cooled (ZFC) and field-cooled (FC) conditions confirm that this iron silicate is paramagnetic or superparamagnetic (Fig. S18†).
Composition analysis with a combination of Energy-Dispersive X-ray spectroscopy (EDX) and Scanning Transmission Electron Microscopy (STEM) revealed a very uniform distribution of the elements Fe, Si and O in the nanosheets (Fig. 4), measuring an average composition of FeSi2.0O8.0 for the specific sample. EDX bulk analysis of iron silicates from five different batches gave an average composition of FeSi2.0O6.4. Another 76 EDX-analyses in combination with high resolution TEM allowed sampling directly at the nanosheet structures. These measurements resulted in an average composition of FeSi1.7±0.2 O5.2±0.4 (confidence level P = 95%).
The silicon-to-iron ratio of 2:1, together with clearly dominating Fe(III) centers are consistent with double chain silicates of the amphibole subgroup such as Fe2[Si4O11] as well as with sheet silicates of the serpentine subgroup of phyllosilicates such as Fe2[Si4O10](OH)2.
The already mentioned content of hydroxyl groups (8.31 wt%) measured via titration fits well with the chemical formula Fe2[Si4O10](OH)2, corresponding to 8.13 wt% hydroxyl groups theoretically. Further evidence for this composition results from the hydrogenative decomposition of the material in a temperature window between room temperature and 500 °C over 13 h. A total amount of 6.1 mmol water was formed from a sample of 1.458 mmol iron silicate as measured via integration of a calibrated online IR-detector signal (Fig. S19†), matching the stoichiometry for a sheet silicate in eqn (3) more closely than for eqn (2).
Fe2[Si4O11] + 3H2 → 2 Fe + 4 SiO2 + 3H2O | (2) |
Fe2[Si4O10](OH)2 + 3H2 → 2 Fe + 4SiO2 + 4H2O | (3) |
The absence of characteristic features of FeSiO4 and Fe2O3 in pair distribution function (PDF) analysis further confirms a unique structure rather than a mixture of these two known materials (Fig. S20†).36,37 Comparing the main atom distances as derived from the peak maxima in the iron silicate with other known materials indicates a coordination of iron with bridged oxygen atoms and hydroxyl groups (labelled as FeO(OH)). Such entities are in fact also present in Ferripyrophylite (Fig. 2), and the measured data correlates nicely with simulated data of this structure (Fig. 5).
Fig. 5 Pair distribution function (PDF) analysis of the iron silicate compared to simulated PDFs for Ferripyrophylite and FeO(OH). |
The existence of Fe–O–Si units in the material was evidenced by ATR-IR spectroscopy.38–43 While physical mixtures of Fe2O3 and SBA-15 showed only the additive signals of the two components (Fig. S21†), distinct differences are evident for the new material (Fig. 6 and also Fig. S22†). The characteristic absorbance of silica at 1057 cm−1 (asymmetric Si–O–Si stretching) was shifted to the lower frequency at 1023 cm−1, with concomitant inversion of the transmission ratio to the absorbance at 445 cm−1 (O–Si–O bending). Together with the shoulder at 678 cm−1 (Si–O–Fe symmetric stretching mode), this provides strong evidence for the extensive incorporation of iron atoms in the silica framework. The absorbance at 1443 cm−1 can be assigned to FeOOH units,44,45 correlating with its presence from PDF analysis. The broad band around 3350 cm−1 and the peak at 1635 cm−1 are assigned to O–H stretching (involving hydrogen bond interactions) and bending modes of adsorbed water, respectively.46
Upon heating the material at 450 °C for 4 h under vacuum to initiate dehydration, the OH stretching vibration region showed a sharp band at 3745 cm−1 (in the absorbance mode only) ascribed to the presence of the terminal silanol groups (Si–OH) (Fig. S23a†) The acidity of this material was assessed by pyridine adsorption/desorption. After pyridine desorption at 150 °C (Fig. S23b†), the iron silicate exhibits two bands at 1610 and 1450 cm−1 associated with pyridine coordinated Lewis acid sites. Very weak bands at 1637 and 1545 cm−1 characteristic of pyridinium ions (PyH+) indicate the presence of low amounts of Brønsted acid sites.47,48 When desorption temperature increases up to 250 °C, the band intensities drop, indicating the presence of acid sites with different strengths.
A series of NH3-TPD measurements have been performed in order to evaluate the surface acidity of the iron silicate material relative to standard silica–alumina solid acids (Fig. S24–S27†). The acid site density (per mass of the sample) and acid strength were found to be comparable with that of amorphous SiO2–Al2O3 materials.
The iron(III) silicate is chemically quite stable in weak bases. In fact, it was purified from a 6 M NH3 solution. However, it is not stable towards strong bases like diluted NaOH solutions. Moreover, it decomposes in acidic media, like diluted mineral acids such as HCl, H2SO4, and HF (1 M).
Thermostability of the iron silicate is very high, as evidenced by temperature-dependent X-ray diffraction (XRD) measurements (Fig. S28†). Only broad peaks were detected due to the thin sheet structutre. Interestingly, the pattern is not reported in any of the screened databases. Slight peak shifts were observed after calcination under synthetic air at 300 °C (Fig. S29†), consistent with reported dehydration temperatures of FeO(OH) units between 250 and 300 °C.49–52 This interpretation is supported by in situ diffuse reflectance infrared Fourier transform spectroscopy (DRIFT) indicating concomitant disappearance of the absorbance at 1440 cm−1 (Fig. S30†). 57Fe Mössbauer spectroscopy suggests the preservation of the Fe-silicate structure at this stage (Fig. S31 and S32†).
No further changes were observed in the XRD pattern upon heating up to 800 °C in synthetic air (Fig. S28†). The BET surface area remained high at about 182 m2 g−1 (Fig. S33†). TEM investigations showed that the ultrathin iron silicate sheets remained intact even after three hours at 600 °C (Fig. 7). EDX analysis on seven different locations revealed an average composition of FeSi2.0O5.6 fully in line with the native material.
Only at temperatures around 1000 °C, the material converts to SiO2 and Fe2O3 according to TEM and XRD analyses (Fig. S34 and S35†). Exchanging the oxidative atmosphere with pure nitrogen, temperature-dependent XRD measurements show phase transitions already between 550 and 600 °C. The new phases remain stable up to 850 °C and prevail also after cooling to room temperature (Fig. S36†). The new reflections could be assigned to Fayalite and Fe3O4 (Fig. S37†). Under inert atmosphere, the reduction is accompanied with oxygen evolution. TG-DSC-MS analysis under argon revealed the loss of molecular O2 in addition to water. In contrast, only water was detected under air, explaining the higher temperature stability of the iron silicate under air as compared to inert atmospheres (Fig. S38 and S39†).
Ultrathin 2D-nanostructures are finding great attention due to a broad spectrum of interesting properties related to their chemical, electrochemical, catalytic, electronic, optical, magnetic or thermal characteristics.53 A variety of applications has emerged, covering the areas of catalysis54–56 as well as energy storage devices, sensors, gas storage materials and others.57
Due to the good thermal stability and high surface area, the iron silicate was used as a support material for Pd catalysts synthesized by chemical fluid reactive deposition.58 The Pd-decorated material was tested for hydrogenation of unsaturated compounds, and high conversions and yields were obtained under standard screening conditions (Table 1). In comparison with 3 wt% Pd/SBA-15 and Pd/C under otherwise identical reaction conditions (not shown here), deoxyfunctionalization is much less pronounced. Instead, the formation of benzylic alcohols is preferred (entries 2–5). Interesting is also the relatively high selectivity for hydrogenation of the aromatic ring in entry 6, while the benzene ring of benzylidene acetone remained intact (entry 7). Furthermore, 3% Pd/iron silicate showed good stability and reusability in the hydrogenation of this substrate as shown in the ESI in Table S1.† The reduced conversion from run 5 onwards seems to be caused mainly by incomplete catalyst recovery rather than deactivation. So further studies in particular for hydrogenation of multifunctional compounds seem promising.59,60
Finally, the iron silicate was also tested as a catalyst precursor in ammonia synthesis (Fig. S40†).61–66 The comparison of the activity with a model catalyst (MgFe2O4),61 and a state-of-the-art industrial catalyst at different temperatures is shown in Fig. 8. The iron silicate shows indeed activity for ammonia synthesis with very similar activities as the model catalyst in the kinetic regime between 325 and 425 °C. STEM analysis of the iron silicate (Fig. S41†) shows the expected decomposition of the structure, resulting in a mixture of elemental Fe and SiO2. Accordingly, the BET surface area decreased to ca. 76 m2 g−1. It is noteworthy that the resulting iron shows a distinct activity already with SiO2 as the only additional component.
Fig. 8 Catalytic activity of the iron silicate in ammonia synthesis in comparison with an industrial catalyst and a model catalyst. |
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/d0dt03125a |
This journal is © The Royal Society of Chemistry 2021 |