Combinations of Ethers and B(C<sub>6</sub>F<sub>5</sub>)<sub>3</sub> Function as Hydrogenation Catalysts
Bibliographic record
Abstract
It works ether way: Labile adducts of dialkyl ethers with the electrophilic borane B(C6F5)3 are shown to scramble HD to H2 and D2 and catalyze the hydrogenation of 1,1-diphenylethylene. Since its discovery in the 1960s, the electrophilic borane B(C6F5)31, 2 has been used extensively in catalysis. Perhaps best-known as a co-catalyst or activator for ethylene polymerization,3–7 this highly electrophilic species has also found applications within a variety of Lewis acid-catalyzed transformations. For example, in the early 2000s, Piers, Gevorgyan, and co-workers pioneered its use in hydrosilylation chemistry.8–13 Since then, others have developed applications in hydrostannylation,14, 15 silane dehydrocoupling, and silicone production and derivatization.16–25 More recently, this electrophile has been exploited in “frustrated Lewis pair” (FLP) chemistry, acting as the Lewis acid partner in conjunction with bases to activate a wide variety of small molecules, including H2, CO2, olefins,26 alkynes,27 N2O,28, 29 and NO,30 among others.31 The application of this borane in FLP or “metal-free” hydrogenation catalysis32 has drawn much attention. Initially, the substrates were limited to imines, protected nitriles, and aziridines. Subsequently, enamines and silylenol ethers were also shown to be viable substrates for FLP reductions. More recently, combinations of B(C6F5)3 with weakly basic triaryl phosphines or triaryl amines were shown to be capable of catalyzing hydrogenations of olefins33 and polyaromatic systems.34 B(C6F5)3 was then shown to effect reductions of N-substituted anilines,35 pyridines, and N-heteroatomic species.36 At the same time, Nikonov et al.37 provided experimental and theoretical evidence that B(C6F5)3 alone does not activate H2. Interestingly, however, these authors and others38 showed that C4H8OBD3 undergoes H/D exchange under pressures of H2 to produce C4H8OBH3. In very recent work, we described the reaction of H2 with the epoxyborate salt, [tBu3PH] [(C6F5)2BCH(C6F5)OB(C6F5)3], affording the borane–borate salt, [tBu3PH][(C6F5)BCH2(C6F5)OB(C6F5)3].31 This observation suggested the possibility that simple oxygen donors might also act in concert with B(C6F5)3 to effect H2 activation, thereby affording a remarkably simple and inexpensive hydrogenation catalyst. Indeed, herein we describe such reactivity. Labile dialkyl ether/B(C6F5)3 combinations are shown to effect H2 activation to catalyze hydrogenations of 1,1-diphenylethylene and anthracene. The combination of B(C6F5)3 with 2 equiv of Et2O in CD2Cl2 exhibits two distinct chemical exchange processes by 1H NMR spectroscopy at reduced temperatures. Analysis of a 2:1 mixture of Et2O/B(C6F5)3 between 25 and −90 °C39 reveals coalescing Et2O methylene signals at −55 °C that are consistent with lone pair inversion at oxygen in the adduct Et2OB(C6F5)3 of ΔG≠=10.3 kcal mol−1. A similar coalescence is also observed at −30 °C, corresponding to the rapid exchange of free and coordinated Et2O with a ΔG≠=10.5 kcal mol−1.40 In a subsequent experiment, a 1:1 mixture of Et2O/B(C6F5)3 in CD2Cl2 (0.14 M) was exposed to 4 atm of HD gas in a J-Young tube at ambient temperature. 1H NMR analysis of the mixture after 15 min showed equal intensity signals for H2 and HD. Integrations were also consistent with the catalytic isotope equilibration of HD to a 2:1:1 statistical mixture of HD/H2/D2 (Figure 1 B). It is noteworthy that such equilibration was not observed employing solutions of B(C6F5)3 alone (Figure 1 A). 1H NMR spectra showing A) HD in the presence of B(C6F5)3 after 60 min and B) complete isotope scrambling of HD by 1:1 Et2O/B(C6F5)3 after 15 min in CD2Cl2. These observations clearly indicate the ability of Et2OB(C6F5)3 to activate dihydrogen, thus suggesting the ability of this species to act as a hydrogenation catalyst. To assess this inference, a 0.4 M solution of 1,1-diphenylethylene containing 20 mol % B(C6F5)3 and 30 mol % ether in CD2Cl2 was pressurized with 4 atm of H2. Heating to 50 °C for 48 h resulted in 95 % conversion of the olefin to the alkane, Ph2C(H)CH3 (Scheme 1; Table 1). Interestingly, the same reaction carried out in C6D5Br at 150 °C resulted in slower hydrogenation of the olefin, although increasing the concentration of Et2O to 160 mol % afforded faster and higher conversion. Increasing the pressure of H2 also enhances the reduction rate. Using 10 mol % B(C6F5)3 and 20 mol % Et2O under 100 atm of H2 pressure at 20 °C, the reduction of Ph2CCH2 is essentially quantitative in 24 h, whereas at 4 atm, heating to 50 °C for 96 h is required for complete reduction. Reaction of 1,1-diphenylethylene in presence of B(C6F5)3 with (right) and without (left) diethyl ether. Substrate B(C6F5)3 [mol %] Ether (mol %) T [°C] t [h] Conv. [%] Ph2CCH2 20 – 20 24 65[f] Ph2CCH2 20 Et2O (30) 50 48 95 Ph2CCH2[c] 20 Et2O (30) 150 24 35 Ph2CCH2[c] 20 Et2O (160) 120 18 60 Ph2CCH2 10 Et2O (30) 50 96 96 Ph2CCH2[b] 10 Et2O (20) 20 24 >99 Ph2CCH2 20 12C4 (20) 25 48 56 Ph2CCH2 20 12C4 (20) 50 72 >99 Ph2CCH2 20 DB24C8 (20) 25 48 57 Ph2CCH2 20 DB24C8 (20) 50 72 >99 C14H10[b] 10 Et2O (20) 20 24 34 C14H10[b,d] 20 DB24C8 (20) 80 24 59 Although somewhat less effective than Et2O, the crown ethers [12]crown-4 (12C4) or dibenzo[24]crown-8 (DB24C8) also enabled the hydrogenation of Ph2CCH2 in the presence of B(C6F5)3. Anthracene could also be hydrogenated to 9,10-dihydroanthracene using DB24C8/B(C6F5)3 in up to about 60 % yield, although more forcing conditions (heating to 80 °C under 100 atm of H2 in 1,2-dichloroethane) were required. Using (Me3Si)2O or Ph2O instead of Et2O only resulted in the previously reported Friedel–Crafts-type dimer of the olefin (Scheme 1).41 It is also noted that this same dimer is formed on treatment of Ph2CCH2 with 20 mol % B(C6F5)3 alone, under H2. Thus, it appears that the decreased basicity of (Me3Si)2O or Ph2O preclude H2 activation, thus permitting the dimerization pathway to prevail in the absence of a donor. An attempt to hydrogenate a series of olefins, including cis-stilbene, 1-hexene, cyclohexene, methylenecyclohexane, and tert-butylethylene as well as 1,2-diphenylacetylene using Et2O/B(C6F5)3 gave no reduction after 24 h. Efforts to reductively open cis/trans-1,2-diphenylcyclopropane was also ineffective. These observations are consistent with the lower Brønsted basicity of terminal olefins and suggest the formation of a relatively stable tertiary carbocation by protonation is required for reduction to proceed. In the case of α-methylstyrene, p-methoxy-α-methylstyrene, and α,p-dimethylstyrene, the reactions proceed to more than 99 % consumption of the olefin; however, the major products are the Friedel–Crafts dimers with a minor product being the hydrogenated alkane, demonstrating that Lewis acid catalyzed dimerization is kinetically favored over hydrogenation. The mechanism of hydrogenation (Scheme 2) is presumably analogous to that reported for FLP hydrogenations of olefins by phosphine/B(C6F5)3 combinations in which heterolytic cleavage of hydrogen allows for protonation of the olefin and hydride delivery to the resulting carbocation.33 Comparing the experimental rates of H/D-exchange and hydrogenation demonstrates that the activation of H2, and thus the equilibrium concentration of the ion pair, [Et2O⋅⋅⋅H⋅⋅⋅OEt2][HB(C6F5)3], is not rate-determining for the olefin reduction. The somewhat accelerated conversions observed when phosphines were employed as bases could be attributed to the simultaneous use of a J-Young NMR tube rotation technique (that we did not employ), which was found to increase the effective concentration of H2 in solution.33 Proposed mechanism of the hydrogenation of 1,1-diphenylethylene by Et2O/B(C6F5)3. (The addition and removal of Et2O molecules is not depicted.) It is indeed surprising that ether and borane act as an FLP to effect the activation of H2 with such ease. To understand the mechanism of this remarkably facile H2 activation process, a DFT study using state-of-the-art quantum chemical methods was conducted42–46 (see the Supporting Information for details). First, gas-phase structure optimizations at the dispersion-corrected DFT level, using large triple-zeta AO basis sets (TPSS-D3/def2-TZVP), followed by single-point energy calculations at the high double-hybrid level (B2PLYP-D3/def2-QZVP), were performed. On top of that, thermostatistical corrections from ZPVE-exclusive energy (ΔE) to free energy (at T=298.15 K, 1 atm pressure) and corrections for solvation free energy by the accurate (DFT-based) COSMO-RS model were applied.47–50 Various H2 activated structures were investigated and the most likely candidates selected (Figure 2). Consideration of all corrections from gas-phase energy to ΔG in solution (ΔGR) is essential for an understanding of the mechanism. Previous results51, 52 have showed that the barrier to H2-splitting is only a few kcal mol−1 higher than the zwitterionic intermediate. Thus, only the thermodynamics under equilibrium conditions were considered, and ΔGR values were given relative to the separated reactants (B(C6F5)3, Et2O, and H2). The Lewis acid–base adduct (Et2O)B(C6F5)3 forms with ΔG=−2.0 kcal mol−1 (ΔE=−14.7 kcal mol−1), indicating that a significant concentration of the FLP is present in solution. Splitting of H2 by B(C6F5)3 and one Et2O molecule is weakly exothermic (ΔE=−3.1 kcal mol−1) in the gas phase. The explicit “solvation” of the protonated ether by a second Et2O yields a strong hydrogen bond and lowers the energy considerably to −17.4 kcal mol−1. Adding a third molecule (not shown) lowers it further to −23.8 kcal mol−1. However, compared to the corresponding FLP activation with tBu3P/B(C6F5)3, and in agreement with its lower efficiency, the present reaction is clearly less exothermic (tBu3P/B(C6F5)3: ΔE=−30.2 kcal mol−1), reflecting the lower basicity of Et2O compared to the phosphine. Furthermore, the need of two or three molecules Et2O leads to a large entropic penalty. (Free) energy diagram with DFT-D3 optimized structures for hydrogen activation by B(C6F5)3 and Et2O (n=1, 2) leading to the ions [Et2OH⋅⋅⋅OEt2]+[HB(C6F5)3]− (ΔGR (kcal mol−1): black; ΔE (kcal mol−1): blue). The calculated free energies ΔGR were 10.3 and 9.0 kcal mol−1 for the computations involving one and two ether molecules, respectively, and thus such species are thermally accessible. Adding a third Et2O to the ion pair complex seems less likely (increase of ΔGR to 14.9 kcal mol−1). Values of around 10–15 kcal mol−1 are our estimates of the effective free energy barrier to the splitting of H2. The similar values for rather different structures indicate the flatness of the free energy hypersurface, and that the system is probably rather dynamic, an aspect that could not be treated adequately at present. Subsequently, the complex with two Et2O dissociates exergonically to give the solvated ions [Et2O⋅⋅⋅H⋅⋅⋅OEt2]+ and [HB(C6F5)3]−, which are only ΔGR=5.9 kcal mol−1 above the reactants. Keeping in mind the theoretical error bars (2–3 kcal mol−1 for ΔGR), this value is compatible with a significant equilibrium concentration of solvated proton and hydridoborate under ambient conditions. A large solvation energy and entropy release appear to be essential for formation of free ions, giving rise to the observed H/D exchange and hydrogenation catalysis. In conclusion, the remarkable ability of ether/B(C6F5)3 combinations to activate H2 and effect catalytic hydrogenations of 1,1-diphenylethylene and anthracene has been demonstrated. A detailed theoretical study is consistent with an accessible barrier to the “encounter complex” in which H2 is activated. Subsequent dissociation of this complex affords the ions [Et2O⋅⋅⋅H⋅⋅⋅OEt2]+ and [HB(C6F5)3]− in sufficient concentration to effect hydrogenation. The synthetic utility and variants of this remarkably simple hydrogenation catalyst are the subject of on-going efforts. As a service to our authors and readers, this journal provides supporting information supplied by the authors. Such materials are peer reviewed and may be re-organized for online delivery, but are not copy-edited or typeset. Technical support issues arising from supporting information (other than missing files) should be addressed to the authors. Please note: The publisher is not responsible for the content or functionality of any supporting information supplied by the authors. Any queries (other than missing content) should be directed to the corresponding author for the article.
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How this classification was reachedexpand
Full frame distilled prediction
Teacher imitationNot calibrated prevalence, not ground truth. Human validation pending. Learned from the 10,348 direct Codex labels and 10,348 direct Gemma labels. Candidate is the union of thresholded teacher heads; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels or direct frontier model labels.
Codex and Gemma teacher scores by category
| Category | Codex | Gemma |
|---|---|---|
| Metaresearch | 0.000 | 0.000 |
| Meta-epidemiology (narrow) | 0.001 | 0.001 |
| Meta-epidemiology (broad) | 0.000 | 0.000 |
| Bibliometrics | 0.000 | 0.000 |
| Science and technology studies | 0.000 | 0.000 |
| Scholarly communication | 0.000 | 0.001 |
| Open science | 0.000 | 0.000 |
| Research integrity | 0.001 | 0.001 |
| Insufficient payload (model declined to judge) | 0.000 | 0.000 |
Machine scores (provisional)
The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.
Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.
score_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from itClassification
machine, unvalidatedMachine predicted; a candidate call from one teacher head, not a consensus.
How this classification was reached, model by model and score by score, is at the end of the page under "How this classification was reached".