Abstract
The new ansa-phosphinoborane (dicyclohexyl(2-(dimesitylboryl)phenyl)phosphine was synthesized via an one-pot protocol in 67% yield. The compound has been characterized by 1H, 13C, 11B and 31P NMR, and its solid-state structure determined by a single crystal X-ray diffraction analysis. The ansa-phosphinoborane does not react with molecular hydrogen or water at room or elevated temperature. According to performed DFT studies, heterolytic splitting of water or hydrogen by the phosphinoborane are both endergonic but close in thermodynamics. In polar solvents, such as in methanol or acetonitrile, addition of hydrogen is energetically more favorable than of water.
1 Introduction
Frustrated Lewis pairs (FLPs) is a powerful yet simple concept to activate various chemical bonds through their heterolytic splitting. In order to achieve “frustration”, i.e. prevent formation of classical Lewis adducts, Lewis acids and the Lewis bases with sterically bulky substituents are needed. Various parameters such as acid and base strengths, and steric hindrance of the reactive centers can be varied to affect reactivity, catalytic activity, and selectivity of FLPs. FLP chemistry emerged as a powerful tool for activation of a broad range of small molecules, but, primarily, of molecular hydrogen (H2). Particularly, many breakthroughs have been accomplished in the hydrogenation of organic molecules catalyzed by FLPs [1], [2], [3], [4], [5], [6]. Parahydrogen-induced polarization (PHIP) represents another application of FLPs to activate H2. PHIP is a phenomenon of achieving nuclear magnetic polarization states well above the thermal level through interaction with molecular hydrogen that is enriched with parahydrogen, one of its spin isomers [7], [8], [9]. To achieve high PHIP levels, para-H2 should lose symmetry upon addition to a substrate or a catalyst and the mechanism of parahydrogen addition should be pairwise. Hyperpolarization can be observed with intensities increased by orders of magnitude of para-H2-originated 1H nuclei as well as other magnetically coupled nuclei, such as 13C, 15N, etc. In a typical protocol, parahydrogen is initially added to a heterogeneous or homogeneous metal center along with a substrate molecule. Then either parahydrogen is transferred to the substrate molecule, or magnetization can be transferred via reversible coordination of parahydrogen and a substrate molecule to the metal center (SABRE) [10].
We and others have recently demonstrated that PHIP can be observed in metal-free conditions upon addition of parahydrogen to ansa-aminoboranes, for example, 1 [11] (Fig. 1). In a later publication we conducted a detailed study of PHIP observed with other type of ansa-aminoboranes, compounds 2a–c, and concluded that the relatively low levels of achieved hyperpolarization (<20-fold signal intensity enhancements) were caused by the presence of quadrupole 14N (nuclear spin 1) and 11B (nuclear spin −3/2) nuclei that drastically diminish polarized signals intensities due to fast spin relaxation. To overcome this limitation, it was proposed to replace 14N nucleus with 15N or 31P both of which have spin 1/2 with longer typical relaxation times [12]. Herein we report synthesis of previously unknown (dicyclohexyl(2-(dimesitylboryl)phenyl)phosphine 6 and studies of its interaction with molecular hydrogen and water.

Ansa-amino- and ansa-phosphinoboranes reported to activate molecular hydrogen.
Phosphinoborane 3 was the first FLP reported to split H2 [13]. Since then, other types of phosphinoboranes, particularly, ansa-phosphinoboranes with saturated [14], [15], [16], [17] and unsaturated [18], [19] linkers between the P and B atoms have been demonstrated to react with H2. Among them, 2-phosphinophenylboranes 4a–c were prepared by a sequence of electrocyclic ring closure and oxidation reactions [18], [19]. Besides this, various 2-phosphinophenylboranes have previously been synthesized and used as ligands for transition metal complexes [20], [21], [22], [23], [24], [25].
2 Results and discussion
Ansa-phosphinoborane 6 was synthesized in 67% yield by a one-pot procedure from commercially available phosphine 5 (Fig. 2). Unlike in 4a–c, there is no dative bond between B and P atoms (3.1773 (17) Å distance) in 6 as established by the single crystal X-ray diffraction analysis (Fig. 3). In CD2Cl2, 11B and 31P NMR signals of 6 appear as singlets at 75.68 (broad) and −0.64 ppm, revealing that there is no P–B interaction [26]. Because 6 is structurally close to the previously reported ansa-aminoborane 2a and proton affinities of isostructural N,N-dimethylaniline and dimethylphenylphosphine are close [27], we expected to detect 7, the product of dihydrogen addition to 6. However, prolonged exposure of a solution of 5 to pressurized hydrogen (10 bar) in a gas-tight NMR tube revealed no evidence of the phosphonium borate 7. To our surprise, 6 did not react with water as well, neither at ambient not at elevated temperatures.

Synthesis of ansa-phosphinoborane 6, and its inertness to hydrogen or water.

(a) Structure of 6 in the solid state based on XRD data. Ortep drawing, thermal ellipsoids at the 50% probability level, P–B distance 3.1773(17) Å. (b) Optimized molecular geometry of 6in vacuo, DFT, ωB97X-D/6-311G(d,p), P–B distance 3.18179 Å.
To rationalize the observed failure of the addition, we examined thermodynamics of formation of 7 and 8via DFT calculations. The optimized geometry of 6 (Fig. 3b) is in good agreement with the one obtained from the single-crystal X-ray diffraction analysis (Fig. 3a). For both 7 and 8 we analysed endo and exo isomeric forms, with and without an intramolecular PH···XB (X=H or OH) bond, respectively (Fig. 4). Intramolecular H···H bonding appears to be crucial for observation of PHIP by ansa-aminoboranes. Therefore, our finding that, in terms of solution Gibbs free energies, endo-7 is by ca. 2 kcal mol−1 more stable than exo-7 shows that the chosen scaffold is a promising starting point for further studies. Previously reported H2 adducts of 4a and 4b also exist as endo-forms [18]. A very close analog of 6, (diisopropyl(2-(dimesitylboryl)phenyl)phosphine, was previously reported along with its HF adduct. Collected NMR data indicated the presence of an intramolecular H···F bond [28]. For the water adduct 8, however, we found that the exo-form is favored by 3–5 kcal mol−1 over the endo-form. In contrast to H2, adducts of H2O and P/B FLPs are much less studied, but available XRD data point to a preference of the PH···(OH)B bond formation [29] that can be outweighed by strong steric effects [30]. The thermodynamics of the formation of 7 and 8 were found to be endergonic, in agreement with experimental observations. It was most surprising, however, that, in benzene as a solvent, hydrogen addition to 6 is by only 2.6 kcal mol−1 more endergonic than water addition. Moreover, addition of hydrogen become energetically more favorable in more polar solvents such as methanol or acetonitrile. As is shown in Table 1, 7 gets progressively stabilized with increasing polarity of the solvent, an effect we have previously observed for a hydrogen adduct of an ansa-aminoborane [31]. At the same time, the Gibbs energy of the formation of 8 remains nearly unchanged.

Optimized geometries of 7 and 8in vacuo. DFT, ωB97X-D/6-311G(d,p).
Calculated solution Gibbs free energies (kcal mol−1) of the formation of 7 and 8 from 6.a
C6H6 | CH2Cl2 | MeOH | MeCN | |
---|---|---|---|---|
endo-7 | 8.0 | 4.5 | 3.2 | 3.0 |
exo-7 | 9.7 | 6.7 | 5.4 | 5.3 |
endo-8 | 10.0 | 9.5 | 10.5 | 9.1 |
exo-8 | 5.4 | 5.5 | 7.7 | 5.2 |
aThe energies correspond to the equilibria 6+H2⇌7 and 6+H2O⇌8.
The reported solution phase Gibbs free energies are based on ωB97X-D/6-311++G(3df,3pd) electronic energies, and all additional terms were obtained at the ωB97X-D/6-311G(d,p) level.
Sensitivity of FLPs to moisture is considered as one of the serious limiting factors in the widespread application of FLPs as hydrogenation catalysts [32]. The majority of FLP-based catalysts contain highly Lewis acidic organoboron compounds. Based on the bond dissociation energies, the reaction B–H+H–O→B–O+H–H is exothermic by 111 kcal mol−1 (standard state enthalpy at 298 K) [33]. It is not surprising then that water molecules are bound much stronger than H2 in FLPs structures, thus deactivating the catalysts. To cope with this problem, organoaluminium and silicon compounds were successfully utilized as scavengers of water [32]. Alternatively, the high oxophilicity of boron centers can be suppressed by hindrance its atom with sterically bulky substituents [34]. Both front and back strain allow strong steric discrimination of an OH substituent over a compact H atom [35]. Apparently, this scenario is realized in the case of 6 that contains sterically bulky 2-(dicyclohexylphospino)phenyl and mesityl groups around the Lewis acidic center. Although these and other approaches [36] were successfully used in catalysis, to the best of our knowledge, no FLP-H2 adduct formation in the presence of water have been reported.
Further experimental and computational studies on water-tolerant intramolecular FLPs are in progress, especially, with regard to PHIP applications in aqueous media such as for vivo magnetic resonance imaging.
3 Experimental section
Starting materials were purchased from Sigma-Aldrich and used as received. All solvents were dried using a Vac solvent purification system and stored over 3 Å molecular sieves. Deuterated solvents were dried by standing over 3 Å molecular sieves and used without additional purification. Synthesis was performed under argon atmosphere by a conventional Schlenk technique or in a glove box. Hydrogen addition at 10 bar was carried out in gas-tight NMR tubes (QPV tubes from Wilmad). Schlenk vessels were equipped with gas-tight Teflon valves and Glindemann PTFE sealing rings. NMR spectra were recorded at Varian Mercury 300 (31P, 13C) or Varian Inova 500 (1H, 11B) spectrometers at 27°C and referenced to the residual 1H/13C resonances of the deuterated solvent and reported as parts per million relative to tetramethylsilane. 31P and 11B NMR spectra were referenced externally to 85% H3PO4 at 0 ppm, and BF3·Et2O at 0 ppm, respectively.
3.1 Preparation of (dicyclohexyl(2-(dimesitylboryl)phenyl)phosphine (6)
A solution of 250 mg (0.71 mmol) of (2-bromophenyl)dicyclohexylphosphine in 6 mL of diethyl ether was prepared in a 25 mL Schlenk tube and cooled to −78°C. A solution of n-butyllithium (0.45 mL, 1.6 M in hexane, 0.72 mmol) was added dropwise during 10 min using a syringe. The mixture was allowed to warm to room temperature and was additionally stirred for 1 h. After recooling to −90°C, a solution of dimesitylboron fluoride (199 mg, 0.74 mmol) in 3 mL of diethyl ether precooled to −90°C was added at once. The mixture was allowed to warm to room temperature and left stirring overnight. The solvent was evaporated in vacuum of an oil pump and the residue was redissolved in 10 mL of n-hexane. The resulting suspension was filtered into another Schlenk tube and the solvent was evaporated to dryness. The resulting white powder was recrystallized from 5 mL of n-hexane and dried giving 247 mg (67%) of the colorless product. – 1H NMR (500 MHz, C6D6): δ=2.59–0.82 (br, 40H, Cy and MeMes), 6.82–6.49 (br, 4H, HMes), 7.02 (tm, J=7.3, 1H, C6H4), 7.11 (m, 1H, C6H4), 7.29 (dm, J=7.5, 1H, C6H4), 7.40 (dd, J=7.7, 2.7 Hz, 1H, C6H4). – 13C NMR (75 MHz, C6D6): δ=21.30 (CH3,para -Mes), 26.92 (CH3,ortho -Mes), 37.23–22.58 (brm, Cy), 128.32 (d, J=1.5 Hz), 128.63–129.22 (brm, Cortho ,Mes), 129.16 (C6H4), 131.88 (d, J=2.7 Hz), 133.37 (d, J=14.7 Hz), 139.18 (brm, Cortho ,Mes), 139.69–142.31 (brm, CMes-B), 141.21 (Cpara ,Mes). 141.32 (Cpara ,Mes), 143.53–145.72 (brm, CPh-B), 159.09 (d, J=41.8 Hz, CPh-P). – 11B NMR (160 MHz, C6D6,): δ=75.51 (brs). – 31P NMR (122 MHz, C6D6): δ=−0.78 (s). – 1H NMR (500 MHz, CD2Cl2): δ=2.37–0.71 (brm, 40H, Cy and MeMes), 6.77 (brs, 4H, HMes), 7.14 (dm, J=7.5, 1H, C6H4), 7.25 (tm, J=7.3 Hz, 1H, C6H4), 7.36 (td, J=7.5, 1.5 Hz, 1H, C6H4), 7.53 (dd, J=7.6, 2.7 Hz, 1H, C6H4). – 13C NMR (75 MHz, CD2Cl2): δ =21.48(CH3,para -Mes), 27.11 (CH3,ortho -Mes), 37.38–22.30 (brm, Cy), 128.30 (d, J=1.5 Hz, C6H4), 128.78 (brs, Cmeta, Mes), 129.19 (s, C6H4), 132.32 (d, J=2.9 Hz, C6H4), 133.15 (d, J=14.6 Hz, C6H4), 139.03 (brm, Cortho , Mes), 141.55 (Cpara, Mes), 141.66 (Cpara, Mes), 142.51–140.15 (brm, CMes-B), 145.69–143.65 (brm, CPh-B), 158.95 (d, J=41.3 Hz, CPh-P). – 11B NMR (160 MHz, CD2Cl2): δ=75.68 (brs). – 31P NMR (122 MHz, CD2Cl2): δ=−0.64 (s).
3.2 Hydrogen addition
A solution of 20 mg (0.034 mmol) of 6 in 0.3 mL of CD2Cl2 was placed into a Wilmad QPV NMR tube and the sample was pressurized with 10 bar of H2. The 1H, 13C, and 11B NMR spectra revealed no changes when compared to the reference spectra of 6. Further addition of two drops of water to the same NMR tube also did not reveal any changes in 1H and 11B NMR spectra neither at room temperature nor after gentle heating.
3.3 X-ray structure determination
Single crystal X-ray diffraction data were collected on a Bruker D8 Venture diffractometer with Photon100 detector using graphite-monochromatized CuKα radiation (λ=1.54178 Å) at T=−150°C. The structure was solved by direct methods [37] and refined by full-matrix least-squares on F2 [38], [39]. A semi-empirical absorption correction was applied. All non-hydrogen atoms were refined anisotropically, and hydrogen atoms were located from ∆F maps and refined at idealized positions using a riding model. The benzene solvent molecule is disordered about a center of symmetry. For details see Table 2.
Crystal structure data for 6.
Formula | C36H48BP·0.5 (C6H6) |
---|---|
Mr | 561.57 |
Cryst. size, mm3 | 0.32×0.24×0.22 |
Crystal system | Triclinic |
Space group | P1̅ (no.2) |
a, Å | 9.6700(4) |
b, Å | 12.0333(5) |
c, Å | 17.0173(7) |
α, deg. | 101.693(1) |
β, deg | 99.992(1) |
γ, deg. | 113.636(1 |
V, Å3 | 1703.27(12) |
Z | 2 |
Dcalcd, g cm−3 | 1.095 |
μ(MoKα ), mm−1 | 0.876 |
F(000), e | 610 |
hkl range | ±11, ±14, −20:21 |
2θmax., deg | 144.2 |
Refl. measured/unique/Rint | 39 395/6664/0.022 |
Param. refined/restraints | 391/36 |
R1 [for 6545 refl. with I>2 σ(I)] | 0.048 |
wR2 (all reflexions) | 0.140 |
GoF (I) | 1.03 |
Δρfin (max/min), e Å−3 | 1.65/−0.49 |
CCDC 1559790 contains the supplementary crystallographic data for this paper. These data can be obtained free of charge from The Cambridge Crystallographic Data Centre viawww.ccdc.cam.ac.uk/data_request/cif.
3.4 DFT calculations
DFT calculations were carried out using the dispersion-corrected range-separated hybrid functional ωB97X-D along with the 6-311G(d,p) basis set as implemented in Gaussian 09 [40]. The electronic energies were refined by single-point energy calculations using a larger basis set (6-311++G(3df,3pd)). The SMD continuum model was employed to account for solvation effects. The reported energies refer to solvent-phase Gibbs free energies.
4 Supporting information
NMR spectra of 6 and computational details (method description, total energy and geometry data) associated with this article can be found in the online version (DOI: https://doi.org/10.1515/znb-2017-0133).
Dedicated to: Professor Dietrich Gudat on the occasion of his 60th birthday.
Acknowledgments
This work was funded by the Academy of Finland (276586). The authors wish to acknowledge CSC – IT Center for Science, Finland, for computational resources (CSC project 2000358).
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- PCl bond length depression upon coordination of a diazaphosphasiletidine to a group 13 element Lewis acid or a transition metal carbonyl fragment – Synthesis and structural characterization of diazaphosphasiletidine adducts with P-coordination
- Iminopyridine ligand complexes of group 14 dihalides and ditriflates – neutral chelates and ion pair formation
- On the structure of the P-iodo-, bromo- and chloro-bis(imino)phosphoranes: A DFT study
- (Dicyclohexyl(2-(dimesitylboryl)phenyl)phosphine: en route to stable frustrated Lewis pairs-hydrogen adducts in water
- Insertion of phenyl isocyanate into mono- and diaminosilanes
Articles in the same Issue
- Frontmatter
- In this Issue
- Preface
- Congratulations to Dietrich Gudat
- On the dimorphism of Pr6Mo10O39
- Rhodium-rich silicides RERh6Si4 (RE=La, Nd, Tb, Dy, Er, Yb)
- Coordination of the ambiphilic phosphinoborane tBu2PCH2BPh2 to Cu(I)Cl
- N-Heterocyclic germylenes and stannylenes of the type [Fe{(η5-C5H4)NR}2E] with bulky alkyl substituents
- Die Europium(II)-Oxidhalogenide Eu2OBr2 und Eu2OI2
- Structure and spectroscopic properties of porphyrinato group 14 derivatives: Part I – Phenylacetylido ligands
- Synthesis, solid-state structures and reduction reactions of heteroleptic Ge(II) and Sn(II) β-ketoiminate complexes
- Reactions of Al/P, Ga/P and P–H functionalized frustrated Lewis pairs with azides and a diazomethane – formation of adducts and capture of nitrenes
- Metal carbonyl complexes of potentially ambidentate 2,1,3-benzothiadiazole and 2,1,3-benzoselenadiazole acceptors
- Lithium alkaline earth tetrelides of the type Li2AeTt (Ae=Ca, Ba, Tt=Si, Ge, Sn, Pb): synthesis, crystal structures and physical properties
- Magnetic properties of the germanides RE3Pt4Ge6 (RE=Y, Pr, Nd, Sm, Gd–Dy)
- Overcrowded aminophospanitrenes: a case study
- PCl bond length depression upon coordination of a diazaphosphasiletidine to a group 13 element Lewis acid or a transition metal carbonyl fragment – Synthesis and structural characterization of diazaphosphasiletidine adducts with P-coordination
- Iminopyridine ligand complexes of group 14 dihalides and ditriflates – neutral chelates and ion pair formation
- On the structure of the P-iodo-, bromo- and chloro-bis(imino)phosphoranes: A DFT study
- (Dicyclohexyl(2-(dimesitylboryl)phenyl)phosphine: en route to stable frustrated Lewis pairs-hydrogen adducts in water
- Insertion of phenyl isocyanate into mono- and diaminosilanes