Open Access Article
Carlos
Marquez
a,
Arkadiy
Simonov
b,
Michael T.
Wharmby
c,
Cédric
Van Goethem
a,
Ivo
Vankelecom
a,
Bart
Bueken
a,
Andraž
Krajnc
d,
Gregor
Mali
d,
Dirk
De Vos
*a and
Trees
De Baerdemaeker
*a
aCentre for Surface Chemistry and Catalysis, KU Leuven, Celestijnenlaan 200F, 3001 Leuven, Belgium. E-mail: dirk.devos@kuleuven.be; trees.debaerdemaeker@kuleuven.be
bInorganic Chemistry Laboratory, University of Oxford, South Parks Road, Oxford OX1 3QR, UK
cDeutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany
dDepartment of Inorganic Chemistry and Technology, National Institute of Chemistry, Hajdrihova 19, 1001 Ljubljana, Slovenia
First published on 4th April 2019
Double metal cyanides (DMCs) are well known, industrially applied catalysts for ring opening polymerization reactions. In recent years, they have been studied for a variety of catalytic reactions, as well as other applications, such as energy storage and Cs sorption. Herein, a new, layered DMC phase (L-DMC), Zn2[Co(CN)6](CH3COO)·4H2O, was synthesized. The structure, which crystallizes in the monoclinic space group P21/m, consists of positively charged {Zn2Co(CN)6}+ DMC layers linked through acetate groups and presents a new layered structure to the family of double metal cyanides. L-DMC proved to be a reusable and stable catalyst that exhibited a higher activity than the benchmark DMC catalyst in two important applications: hydroamination of phenylacetylene with 4-isopropylaniline and polymerization of 1,2-epoxyhexane.
In all the aforementioned phases, however, the pores are too narrow to allow the diffusion of the majority of aromatic compounds, which for DMC-catalyzed reactions of these molecules signifies that the reaction takes place on the outer surface.7 In the light of this, many strategies have been suggested in order to increase the accessibility and availability of the catalytically active sites. For example, we recently showed that by dispersing the catalytically active Zn3[Co(CN)6]2 DMC on silica, its activity can be vastly improved in hydroamination and epoxide polymerization reactions because of the increased accessibility of the active sites.8 Furthermore, Robertson et al.18 proposed layered Co(H2O)2[M′(CN)4] DMCs (M′ = Ni, Pd or Pt) as high surface area catalysts for the propylene oxide (PO) homopolymerization and PO/CO2 copolymerization. In this case, the activity of the Co[M′(CN)4] system still remained lower than that of the Zn3[Co(CN)6]2 DMCs. Layered materials, such as layered double hydroxides (LDHs), layered metal–organic frameworks (MOFs) and clay minerals, are generally of wide interest because of their highly tunable properties and wide range of potential applications, including in catalysis,19–22 energy storage,23,24 and CO2 capture.25,26 Additionally, their potential for modification through, for instance, exfoliation has been extensively investigated in the case of clays, layered zeolite precursors or layered double hydroxides.27–35
During our investigation of Zn3[Co(CN)6]2 DMCs, we discovered single crystals of a phase that was not cubic, but instead, consisted of positively charged DMC layers linked by acetate anions. To the best of our knowledge, such a cationic, layered DMC structure has not yet been reported in the literature. Given the known catalytic activity of other Zn3[Co(CN)6]2 DMCs – cubic,36 monoclinic,16 or (partially) amorphous37–39 – we were motivated to synthesize this layered DMC phase as a powder to investigate its catalytic properties. Herein, we report the synthesis, structure, physicochemical characterization and catalytic activity of this layered DMC (L-DMC). Moreover, the advantages of L-DMC over the benchmark DMC catalyst will be demonstrated for two important catalytic applications of DMCs: hydroamination of phenylacetylene and 4-isopropylaniline, and epoxide polymerization of 1,2-epoxyhexane.
:
50 mixture of water
:
tBuOH, and then dried at 60 °C overnight.
:
3 (v
:
v) solution of HNO3–HCl and heated to 200 °C in a microwave oven for 2 h, as reported by Lee et al.52 Fourier-transform infrared (FTIR) spectra of KBr wafers (1 wt% of DMC) were collected on a Bruker IFS 66 v/S Vacuum FTIR spectrometer (resolution 4 cm−1). Solid state nuclear magnetic resonance experiments (SSNMR) were performed on a 600 MHz Varian spectrometer, equipped with a 1.6 mm triple-resonance magic-angle spinning (MAS) probe. Larmor frequencies were 599.44 MHz for 1H and 150.74 MHz for 13C nuclei, and the spectral axes of the recorded spectra were referenced with respect to the signals of tetramethylsilane. The sample was spun at MAS rate of 40 kHz. The 1H MAS NMR spectrum was collected using Hahn-echo sequence with 90° and 180° pulses of 1.5 μs and 3.0 μs, respectively, and inter-pulse delay of 25 μs. 16 scans were accumulated with a recycle delay of 5 s. The 1H–13C cross-polarization (CP) MAS NMR spectrum was recorded by first exciting protons and transferring polarization to carbon nuclei using the ramped-amplitude CP block with a duration of 5 ms. 10
000 scans were accumulated with the recycle delay of 1 s. During the acquisition, high-power XiX heteronuclear decoupling was applied. N2 physisorption isotherms were collected on a Micromeritics 3Flex Surface Analyzer at −196 °C. Before the measurements, the samples were evacuated at 150 °C for 16 h. The specific surface area (SBET) was determined using the BET method in a p/p0 range from 0.004 to 0.03. The specific external surface area (Sext) and the micropore volume (Vmicro) were obtained using t-plot analysis. In order to estimate the micropore size distribution (MPSD), Ar physisorption isotherms were collected under similar conditions and the MPSD was estimated using the Horvath–Kawazoe (HK) method. Scanning electron microscopy (SEM) images were taken using a JEOL-6010LV SEM. Prior to imaging, samples were coated with a Pd/Au layer using a JEOL JFC-1300 autofine coater under Ar plasma for 10 s. Transmission electron microscopy (TEM; high angle annular dark field, HAADF) images and energy-dispersive X-ray spectroscopy (EDX) maps were recorded with a JEOL ARM-200F TEM with a probe Cs corrector operated at 200 kV. Before imaging, the samples were suspended in ethanol and dropped onto a Cu grid (300 Mesh, Pacific Grid Tech, USA) coated with a Lacey carbon layer. Thermogravimetric mass spectrometry (TG-MS) analysis measurements were carried out on a NETZSCH STA 449 F3 Jupiter® thermal analyzer coupled with a Hiden HPR-20 EGA gas analysis system with a heating rate of 10 °C min−1 under air atmosphere.
| Composition | Co(CN)6Zn2(CH3COO)·4H2O |
| Space group (crystal system) | P21/m (monoclinic) |
| a/Å | 12.3804(3) |
| b/Å | 7.50396(16) |
| c/Å | 8.4883(2) |
| β/° | 85.3299(19) |
| Cell volume/Å3 | 785.97(4) |
| R wp/RBragg | 2.36/1.31 |
| χ 2 | 0.652 |
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| Fig. 1 Final Rietveld plot for the refinement of L-DMC. Data collected at beamline P02.1, PETRA III (DESY, Hamburg, Germany); λ = 0.20738 Å. | ||
The structure crystallizes in the monoclinic space group P21/m and is shown in Fig. 2. The asymmetric unit consists of two symmetry independent Zn atoms and one Co atom, four cyanide groups (labelled CN20 to 23, with each C and N atom numbered accordingly), acetate and three water molecules (represented as isolated O atoms Ow1, Ow11 and Ow12). Zn1 is tetrahedrally coordinated to three N atoms from two symmetry independent cyanide groups (twice to CN20 and once to CN21) and one O atom of the acetate (O10). By contrast, Zn2 has an octahedral coordination environment consisting of three N atoms of two independent cyanide groups (twice CN22, once CN23), one O atom from an acetate group (O11) and two water molecules (Ow1). Co1 is also octahedrally coordinated by six C atoms, two from CN20 and CN22 and one from each of the other cyanide groups. The metal polyhedra are linked together through cyanide groups to form a puckered-layered structure in the ab-plane, in which two octahedrally coordinated Zn2 sites and one tetrahedral Zn1 site define a pocket, into which an octahedrally coordinated Zn2 from the underlying layer projects. The layers are coordinatively bonded together through an acetate group in the apical position of the tetrahedral Zn1, which bridges to the octahedral Zn2 in the layer below. Two capping water molecules (Ow1) project from this octahedral Zn2 site into the interstitial region where they form a H-bonding network with two further water molecules (Ow11 and Ow12), with O⋯O distances in the range 2.827(19)–3.054(16) Å.
It should be noted that the powder pattern reported by Zhang et al.53 of a DMC obtained by ball milling K3[Fe(CN)6] and zinc acetate (complex 2 in ref. 53) is qualitatively similar to the diffraction pattern of L-DMC. We therefore suggest that the structure they observed during ball milling is an Fe(CN)6 analogue of our layered phase. Furthermore, from the FTIR spectrum of their complex 2, they found that acetate should be coordinated to Zn, which is in agreement with our structure and FTIR analysis (vide infra).
m) and the layered phase (monoclinic, P21/m). In an attempt to ensure the incorporation of acetate ions, the synthesis was repeated with Zn(CH3COO)2·2H2O dissolved in a 2 M solution of acetic acid instead. This yielded a solid, DMC-2, that also consisted of a mixture of phases, as evidenced by its PXRD pattern and SEM images (Fig. S1 and S3†). When the concentration of the acetic acid solution was increased from 2 M to 4 M, we obtained a solid (DMC-3) with a PXRD pattern very similar to that of L-DMC. Nevertheless, TEM images revealed that the synthesized solid was not phase pure (Fig. S4†), as two different morphologies (with two different metal ratios) were discerned. Only after increasing the crystallization temperature to 80 °C, phase pure L-DMC was finally obtained. This synthesis temperature has also been used to crystallize a rhombohedral Zn3[Co(CN)6]2 phase, in which all Zn atoms adopt a tetrahedral coordination.36,54 Additionally, we studied the effect of the presence of acetate ions during the synthesis. To that end, we replaced Zn(CH3COO)2·2H2O by other zinc salts, such as ZnCl2 and Zn(CF3COO)2 while keeping the acetic acid concentration at 4 M (DMC-4 and DMC-5, respectively). The pattern of DMC-4 exhibits reflections that are readily assigned to the rhombohedral phase, while the pattern of DMC-5 shows reflections typical of both a rhombohedral and a cubic structure. Substitution of acetic acid by trifluoroacetic acid (DMC-6) also produced a cubic DMC. These results indicate the importance of both the presence of acetic acid in the synthesis solution and the use of Zn(CH3COO)2·2H2O as Zn source to form the desired layered structure, since the acetate ions are needed to balance the positive charge of the {Zn2[Co(CN)6]}+ layers and ensure their linkage. The other studied anions most likely do not have the appropriate geometry to form the desired 2D structure and incomplete hydrolysis of Zn acetate might be necessary to avoid formation of the cubic structure. Furthermore, the electronic properties of the anions, in all likelihood, also play a crucial role in the synthesis of the layered phase. In this sense, CF3COO− may bind too poorly to Zn, as it offers low electron density, and thus it can be easily displaced by water, forming a cubic structure.
| Sample name | Synthesis conditions | ||
|---|---|---|---|
| Zn source | Crystallization temperature | Acid concentration | |
| a Acetic acid. b Trifluoroacetic acid. | |||
| L-DMC | Zn(CH3COO)2·2H2O | 80 °C | 4 Ma |
| DMC-1 | Zn(CH3COO)2·2H2O | Ice bath | — |
| DMC-2 | Zn(CH3COO)2·2H2O | Ice bath | 2 Ma |
| DMC-3 | Zn(CH3COO)2·2H2O | Ice bath | 4 Ma |
| DMC-4 | ZnCl2 | 80 °C | 4 Ma |
| DMC-5 | Zn(CF3COO)2 | 80 °C | 4 Ma |
| DMC-6 | Zn(CH3COO)2·2H2O | Ice bath | 4 Mb |
In an attempt to delaminate the layered structure, the optimized synthesis of L-DMC was slightly modified. Before final isolation (final washing step), the solid was dispersed in an aqueous miscible organic solvent (AMOS) for 16 h.55 The structural changes that occurred during the AMOS dispersion procedure were followed by high throughput powder X-ray diffraction (Fig. S5†). No significant changes were observed in the patterns of L-DMC after washing with the solvents (acetone, methanol, ethanol, acetonitrile and acetaldehyde). This suggests that no exfoliation took place and that the L-DMC structure was maintain, confirming its chemical stability.
:
Co molar ratio of 2.0 was obtained, which corresponds with the theoretical composition of L-DMC - Zn2[Co(CN)6](CH3COO)·4H2O. TEM images were collected at different regions to corroborate the phase purity of L-DMC (Fig. 3). All images show a flake-like morphology, typical of a two-dimensional (2D) geometry, with many of the flakes randomly aggregated. Moreover, HAADF-STEM images and EDX mapping of L-DMC (Fig. S6†) confirm a homogeneous distribution of Zn and Co throughout the structure with a Zn
:
Co molar ratio of 2.0. The FTIR spectra of L-DMC (Fig. S7†) exhibits all the bands associated with DMCs,54 as well as two additional bands around 1550 cm−1 and 1450 cm−1 attributed to the asymmetric and symmetric vibrations of –COO−, respectively.56–58 The presence of such bands in the FTIR spectra is in agreement with the solved crystal structure. Moreover, the band attributed to the stretching vibrations of the C
N bond is observed at 2190 cm−1, a red shift compared to the ν(C
N) frequency in the spectrum of cubic Zn3[Co(CN)6]2 DMC complexes (2200 cm−1), indicating the influence of the acetate anions on the electronic environment of Zn. 1H–13C CPMAS NMR spectrum of L-DMC (Fig. 4) exhibits two well resolved signals of acetate at about 184 and 22 ppm (belonging to carboxyl and methyl groups, respectively), and four partly overlapped signals between 125 and 140 ppm, which can be assigned to carbon nuclei of the four crystallographically distinct cyanide groups. This is in excellent agreement with the proposed structure of L-DMC. Note that signal intensities in the 1H–13C CPMAS NMR spectrum do not properly reflect the abundancies of individual species in the crystals, because the efficiency of polarization transfer from protons is very different to carbon nuclei within –CH3, –COO− or –CN− groups. 1H MAS NMR measurement (Fig. S8†) resolves a stronger signal of water molecules at 4.2 ppm and a weaker signal of the –CH3 groups of acetate at 1.7 ppm, and thus additionally confirms that L-DMC comprises coordinating water molecules. TG-MS analysis of L-DMC (Fig. S9†) showed two marked mass decays: a first decay before 100 °C (∼10% mass loss) attributed to the elimination of water, and a second decay between 320 and 390 °C (∼35% mass loss) corresponding to the decomposition of CN. Since the TG-MS analysis was performed under air flow, the cyanide ligands were removed as (CN)2, and the observed CO2 evolution indicates the decomposition of acetate as no acetic acid desorption was observed before this temperature. After the analysis, the recovered powder exhibited an intense green color, which is indicative of the formation of Zn1−xCoxO oxides (cobalt green). The N2 adsorption isotherm at −196 °C of cubic Zn3[Co(CN)6]2 DMCs is a Type I isotherm with no hysteresis loop, typical of purely microporous materials. In contrast, the isotherm of L-DMC, presented in Fig. S10,† shows a small hysteresis loop.59,60 The high initial N2 uptake at low p/p0 is attributed to the filling of micropores, while the slope in the 0.25 to 0.35 range indicates the presence of a considerable external surface area (Sext) in agreement with the small crystallite size and plate-like morphology.61 Analysis of the N2 sorption isotherm of L-DMC results in a BET surface area (SBET) of 784 m2 g−1 and a Sext of 123 m2 g−1, which are both higher than those obtained for DMC-PTMEG (Table S1†). Furthermore, the MPSD was estimated from the Ar adsorption–desorption isotherms. Horvath–Kawazoe (HK) pore size analyses disclose differences in the microporous nature of both materials (Fig. S11†). While DMC-PTMEG exhibits a relatively narrow MPSD, centered around 6.7 Å, the MPSD of L-DMC shows the presence of three micropore systems with maxima around 6, 10 and 11 Å. This evidences the different geometries between L-DMC and the common, cubic DMC structure.
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| Fig. 4 1H–13C CPMAS NMR spectrum of L-DMC (thick black line – measured; thin red line – decomposition into individual contributions). | ||
The second application, the hydroamination reaction, is a 100% atom efficient route towards the production of fine chemicals,64,65 thus representing a greener alternative over other important C–N bond forming reactions, like the Buchwald–Hartwig amination. Furthermore, the formation of undesired products is limited, as only acetophenone was formed as a side product under these reaction conditions. Zn-based Lewis acid DMCs have been found to be superior catalysts for this reaction, showing a higher selectivity to the hydroamination product than materials that contain Brønsted acid sites.6,7,65,66Fig. 5 (bottom) shows the conversion of phenylacetylene and the yield of the desired hydroamination product obtained with DMC-PTMEG and L-DMC, and the kinetic data for L-DMC are presented in Fig. S12.† The higher catalytic activity of L-DMC (TOFL-DMC = 0.87 compared to TOFDMC-PTMEG = 0.23) can be attributed to a combination of the easier accessibility of the catalytic sites and the changed coordination environment of the Zn atoms in the structure. Additionally, the effect of the presence of acetate ions in the structure of L-DMC on its high catalytic activity cannot be disregarded, since it has been found to enhance the performance of DMC catalysts for other organic reactions.11 Nevertheless, in order to fully disclose their involvement in the reaction mechanism, further studies are required.
As observed in both catalytic activity tests, the differences in activity exhibited by the DMCs highlight the advantages of L-DMC. The catalyst L-DMC also exhibits a higher hydroamination activity than the other synthesized DMCs and other Lewis acid catalysts (Tables S2 and S3†). Furthermore, recycling tests, PXRD and FTIR characterization after three hydroamination runs show the high stability and reusability of L-DMC as a solid catalyst (Fig. S13–S15†). The leaching of active species from the solid catalysts was studied by a hot filtration test (Fig. S16†). To this end, the catalyst was removed from the hot reaction mixture after 0.5 h reaction time (phenylacetylene conversion, ∼24%). The clear supernatant (in the absence of solid catalysts) was allowed to react for an additional 19.5 h reaction time, after which no increase in phenylacetylene conversion was detected. This indicates that no leaching of catalytically active species from the solid occurs during the reaction under the studied conditions.
Footnote |
| † Electronic supplementary information (ESI) available: Characterization (XRD patterns, SEM and TEM images, N2 sorption isotherms, FTIR spectra, 1H MAS NMR spectra, TG-MS profiles) of the synthesized DMCs and L-DMC and catalytic data of the synthesized DMCs. Stability, recycling and hot filtration test of L-DMC. CCDC 1894386. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c9sc00527g |
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