Open Access Article
Yoseph Kim‡
a,
Kang Mun Lee‡
b,
So Han Kim‡a,
Jung Hee Moona and
Youngjo Kim
*a
aDepartment of Chemistry, BK21+ Program Research Team, Chungbuk National University, Cheongju, Chungbuk 28644, Republic of Korea. E-mail: ykim@chungbuk.ac.kr
bDepartment of Chemistry, Institute for Molecular Science and Fusion Technology, Kangwon National University, Chuncheon, Gangwon 24341, Republic of Korea
First published on 13th October 2017
The solid-state structures of dimeric alumatranes with three five-membered rings chelated by [(OCMe2CH2)nN(CH2CH2O)3−n]3− (n = 1, L1; n = 2, L2; n = 3, L3), which vary by the number of CMe2 groups adjacent to the OH functionality [1 (L1H3), 2 (L2H3), and 3 (L3H3)], were determined by single-crystal X-ray diffraction. The X-ray structures revealed that the aluminum geometries were slightly distorted trigonal bipyramids. The obtained aluminum complexes are the first structurally characterized dimeric alumatranes with tricyclic five-membered rings. Quite unexpectedly, the sterically bulky side arms with dimethyl substituents were always located in the bridging sites, as determined by density functional theory calculations. Their solution-state structures were analyzed by 1H, 13C, and 27Al NMR techniques, and their gas-phase structures were determined by mass spectrometry. Unlike Al(OCH2CH2)3N, complexes 1–3 were all dimeric in the solid state, solution phase, and gas phase. In addition, they were found to promote the reaction of aryl, heteroaryl, and alkyl aldehydes with trimethylsilylcyanide to provide the corresponding products in excellent yields under mild conditions of room temperature, a short reaction time of 1 h, and a very low catalyst loading of 0.5 mol%.
As shown in Chart 1, alumatranes with tricyclic five-19–33 and six-membered17,18,34–38 rings are well known. Like other atranes,39–41 all alumatranes with tricyclic five- or six-membered ring systems also have a transannular N → Al interaction from the bridgehead N atom in the tetradentate ligand to the Al atom. Although alumatranes with tricyclic six-membered rings (Chart 1(b)) are monomeric or dimeric in solution and in the solid state, Al(OCH2CH2)3N (Chart 1(a)) has been described as a dimer28 in the gas phase, a hexamer29 and octamer30 in solution, and a tetramer31 in the solid state.
Even though some examples of structurally characterized alumatranes with tricyclic six-membered rings have been reported,17,34–38 few examples of five-membered alumatranes and their derivatives20,31–33 have been identified.
Thus, to the best our knowledge, no studies on a structurally characterized dimeric alumatrane with a tricyclic five-membered ring have appeared in the literature. In addition, examples of five-membered alumatranes having the same structure in the gas phase, solution phase, and solid state have, to our knowledge, not been reported. Herein, we report the logical synthesis, characterization, X-ray structures, theoretical density functional theory (DFT) studies, and catalytic application of dimeric alumatranes.
The alcoholysis of AlMe3 has proven to be a useful synthetic route for alumatranes.17–38 As shown in Scheme 1, the addition of AlMe3 to a solution of (HOCMe2CH2)nN(CH2CH2OH)3−n (n = 1, L1H3; n = 2, L2H3; n = 3, L3H3) in toluene gave novel alumatranes 1–3 as colorless crystals after workup. These reactions proceeded readily at ambient temperature, resulting in good isolated yields of 62–79%. The crude compounds were purified by washing with n-hexane and were recrystallized in toluene. Importantly, in contrast to aluminum complexes with Al–Me bonds,47 complexes 1–3 are very stable at room temperature for more than 1 week, even in chloroform-d1 and benzene-d6 solutions. They are soluble in various solvents, including toluene, chloroform, methanol, and acetone.
![]() | ||
| Fig. 1 X-ray crystal structures of 1 (left), 2 (center), and 3 (right) (50% thermal ellipsoids). All H atoms and toluene molecules (for 1 and 2) are omitted for clarity. | ||
| 1 | 2 | 3 | |
|---|---|---|---|
| Al–O1 | 1.841(2) | 1.8540(10) | 1.8593(11) |
| Al–O1′ | 1.848(2) | 1.8565(10) | 1.8515(11) |
| Al–O2 | 1.753(3) | 1.7604(11) | 1.7436(11) |
| Al–O3 | 1.755(3) | 1.7539(11) | 1.7601(12) |
| Al–N | 2.074(3) | 2.1055(12) | 2.1158(14) |
| O1–Al–O2 | 121.41(14) | 120.52(6) | 116.65(6) |
| O1–Al–O3 | 117.23(14) | 120.08(5) | 120.85(5) |
| O2–Al–O3 | 119.88(15) | 117.56(6) | 120.75(6) |
| O1–Al–O1′ | 78.18(11) | 77.85(4) | 78.54(5) |
| O2–Al–O1′ | 101.37(12) | 102.72(5) | 101.46(5) |
| O3–Al–O1′ | 102.11(13) | 102.94(5) | 102.45(5) |
| O1–Al–N | 83.53(11) | 82.68(5) | 82.71(5) |
| O2–Al–N | 86.95(12) | 86.90(5) | 87.30(5) |
| O3–Al–N | 87.39(13) | 86.99(5) | 86.75(5) |
| O1′–Al–N | 161.66(12) | 160.53(5) | 161.25(5) |
| Al–O1–Al′ | 101.81(11) | 102.14(4) | 101.46(5) |
In the solid state, complexes 1–3 exist as dimers with pseudo-Ci symmetry. Each is composed of two alumatrane units with a four-membered Al2O2 ring linked by two Al–O bonds. To our knowledge, compounds 1–3 represent the only structurally characterized examples of an alumatrane dimer with all five-membered rings reported thus far. The aluminum atoms in 1–3 adopt a slightly distorted trigonal bipyramid geometry with Oax–Al–Nax angles (∠O1′–Al–N in Table 1) of 161.66(12)° in 1, 160.53(5)° in 2, and 161.25(5)° in 3. Trigonal bipyramidal and square pyramidal are two possible coordination geometries around the metal center in five-coordinate systems. They could also be determined by the trigonality parameter τ (τ = [α − β]/60, where α and β are the largest and next-largest interligand bond angles, respectively).48,49 The largest and next-largest interligand bond angles are ∠O1′–Al–N [161.66(12)° in 1, 160.53(5)° in 2, and 161.25(5)° in 3] and ∠O2–Al–O3 [119.88(15)° in 1, 117.56(6)° in 2, and 120.75(6)° in 3], respectively. Thus, the τ values of 0.71 for 1, 0.72 for 2, and 0.68 for 3 means that complexes 1–3 have distorted trigonal bipyramidal structures; the trigonality parameter τ for regular trigonal bipyramidal complexes is 1.0, and τ for perfect square pyramidal complexes is zero.
All Al–O bond distances of dimeric compounds 1–3 were observed as ca. 1.74–1.86 Å, which are similar to those found in typical pentacoordinate aluminum complexes.50,51 Moreover, two equatorial bonds, Al–O2 and Al–O3 [1.753(3) and 1.755(3) Å in 1, 1.7604(11) and 1.7539(11) Å in 2, and 1.7436(11) and 1.7601(12) Å in 3], are substantially shorter than those between the aluminum and bridging oxygen atoms in the other equatorial Al–O1 bond and in one axial Al–O1′ bond [1.841(2) and 1.848(2) Å in 1, 1.8540(10) and 1.8565(10) Å in 2, and 1.8593(11) and 1.8515(11) Å in 3]. The longer bridging Al–O1 and Al–O1′ distances are also observed in dimeric alumatranes with tricyclic six-membered rings.17,33
The transannular Al–Nax interaction distances of 2.074(3) Å in 1, 2.1055(12) Å in 2, and 2.1158(14) Å in 3 are slightly longer than the sum of the ionic radii of Al3+ and N3− (2.00 Å)52 and that of the covalent radii of Al and N (2.05 Å).53 This means that all dative N → Al coordinating bonds in 1–3 have a substantial degree of single bond character. All Al–N bond distances in 1–3 are among the longest of those observed for other structurally characterized alumatranes with tricyclic five-membered (2.003–2.094 Å)20,31–33 or six-membered rings (2.026–2.083 Å).17,34–38
The sum of the Oeq–Al–Oeq angles (∠O1–Al–O2 + ∠O1–Al–O3 + ∠O2–Al–O3) are 358.52° in 1, 358.16° in 2, and 358.25° in 3. Interestingly, the obtuse Oeq–Al–Oax angle [av = 93.89° for 1, 94.50° for 2, and 94.15° for 3; (∠O1–Al–O1′ + ∠O2–Al–O1′ + ∠O3–Al–O1′)/3] and acute Oeq–Al–Nax angle [av = 85.96° for 1, 85.52° for 2, and 85.59° for 3; (∠O1–Al–N + ∠O2–Al–N + ∠O3–Al–N)/3] reflect a displacement of the aluminum atoms toward the bridging oxygen atoms. No direct Al–Al′ interactions occur in 1–3.
Even though boron and aluminum, which are in the same group of the periodic table, have similar chemical properties, boratranes42 and alumatranes chelated by L1–L3 are monomeric and dimeric, respectively. In addition, titanatranes showed dramatic dimer-to-monomer structural changes induced by an increase of steric hindrance in the side arm of the tetradentate ligands.45 However, alumatranes are insensitive to the effects of ligand change. Unexpectedly, the sterically bulky side arm with dimethyl substituents in dimeric 1–3 is always located in the bridging sites; however, the less hindered side arms with no substituents in the dimeric titanatranes45 are placed in the same positions.
The presence of dimethyl-substituted bridging arms in alumatrane isomers could play a significant role in determining their thermodynamic stability. To obtain the thermodynamic stabilities for each isomers shown in Chart 3, the relative free energy (ΔG/kcal mol−1) of the ground-state optimized structures in the gas phase was calculated using the B3LYP functional and 6-31G(d) basis set. The structural geometries used for the calculations were optimized on the basis of the X-ray structures of 1 and 2, and the energy states of the isomers were given relative to 1 or 2 because 1 and 2 were assigned to zero ΔG (kcal mol−1). Computed free energy diagram for 1, 2, and their possible isomers is shown in Fig. 2. Since enantiomers exhibit identical thermodynamic stabilities, data for only one enantiomer was given.
According to Fig. 2, the ΔG values of 1a–1c were 1.09, 3.68 and 3.85 kcal mol−1, respectively, higher than that of 1 (Fig. 2, left), distinctly indicating that the structure of 1 is the most thermodynamically stable isomer among six possible ones. The thermodynamic stability was proportional to the number of dimethyl-substituted bridging arms in the order of 1 > a pair of enantiomers 1a/1d > a pair of enantiomers 1b/1e > 1c. The ΔG values of 2a–2c were calculated to be 0.46, 1.63 and 3.46 kcal mol−1 higher than that of 2. Like 1 and its isomers, the similar stability order of 2 > a pair of enantiomers 2a/2d > a pair of enantiomers 2b/2e > 2c was also observed. In particular, the energy states for 1b and 1c (>3.6 kcal mol−1), which have no dimethyl-substituted bridging arms, are conspicuously enhanced compared to those for 1 and 1a. Whereas the ΔG values of 2 and 2a, bearing two dimethyl-substituted bridging arms each, differ slightly (by 0.46 kcal mol−1), those of 2b and 2c, which having one and no dimethyl-substituted bridging arms, respectively, linearly increase.
A key factor of the association between the structural features and thermodynamic stabilities of the isomers was found from the angle (φN) between the two unbridged arms of each structure optimized by theoretical calculations (Table S1 in ESI†). The φN is defined as the angle of CH2–N–CH2 (CH2 from the unbridged arm, see the inset figure of Table S1†), indicating the angle strain between the two unbridged arms centered at the N atom. These dimeric structures have two φN values (φN1 and φN2), and each value is dictated by the number of CH3 pairs substituted onto the unbridged arms. Whereas the φN between the two unbridged arms without CH3 substituents was observed to be ∼114° (φN1 and φN2 for 1 and φN1 for 1a, Table S1†), this angle between the unbridged arm with CH3 substituents and the unbridged arm without CH3 substituents was increased to ∼116° (φN2 for 1a and φN1 − φN2 for 1b–c, Table S1†). These φN values are the same for 2 and 2a. Furthermore, the φN between both unbridged arms with CH3 substituents (in 2b or 2c) was observed as >118°. These results distinctly indicate that the CH3 substituents on the unbridged arms increase the φN values and that CH3 substituents evoke angle strain centered at the N atom in the structure of each isomer. Consequently, we found that 1 and 2 are the most thermodynamically stable structures in comparison to the other isomers because these structures have the smallest angle strain among the isomer structures.
Unlike dimeric alumatranes 1 and 2, we recently found that the corresponding titanatranes chelated by L1 and L2 always had the less hindered side arms with no substituents in the bridging sites.45 Even though titanatranes have different site preference, such the correlation between the angle strains and thermodynamic stabilities were exhibited once again from the calculation results of dimeric titanatrane complexes45 (see Ti1–Ti3 in Table S2 in ESI†). The more increasing the substituted methyl groups on unbridged arms, the larger φN values are (Ti1: ∼106°, Ti2: ∼105° and Ti3: ∼104.6° in Table S2†) and simultaneously, these complexes become thermodynamically unstable (ΔG of Ti1: 0.48 kcal mol−1 and ΔG of Ti2: 0.22 kcal mol−1 in comparison of ΔG of Ti3, Table S2†). These results distinctly indicate that the angle strain between unbridged arms in dimeric complexes can evoke those thermodynamical unstability.
:
2
:
1 (Fig. S1 and S4 in ESI†). In addition, the 1H NMR for compound 2 shows four singlets for the methyl protons with the integration ratio of 1
:
1
:
1
:
1 (Fig. S10 and S13 in ESI†). These data support only structures 1 and 2 among all possible structural isomers shown in Chart 3. The 1H and 13C NMR spectra support dimeric structures in solution; NMR separations for the bridging and terminal side arms were observed.
The coordination number and geometry around aluminum correlate well with the 27Al NMR chemical shift. The 27Al NMR spectra of 1–3 were collected with the samples dissolved in CDCl3, and two broad peaks at approximately 6 ppm and 65 ppm were observed (Fig. S7, S16 and S28 in ESI†).54 Low-field signals in their 27Al NMR spectra could be definitely assigned to the aluminosilicate peak of the NMR tube. The both pentacoordinate alumatranes N(C6H4O)3Al–NH2CH2Ph19 and Al(OCH2CH2)3N21 showed similar signals at 66 ppm in their 27Al NMR spectra. Although the 27Al NMR signal for the pentacoordinate six-membered system34 was shifted downfield to 37.2 ppm, which is within the expected region from 33 to 61 ppm for monomeric five-coordinate aluminum alkoxides,55 the 27Al NMR signal at approximately 6 ppm for 1–3 is very similar to those for other reported pentacoordinate alumatranes with tricyclic five-membered rings.19,21 Thus, 1H, 13C, and 27Al NMR data support that alumatranes 1–3 in the solution phase exist as pentacoordinate dimeric structures. Especially, 2D NMR (COSY, HSQC, and HMBC) spectra for compounds 2 and 3 made the proper assignment of NMR peaks (see ESI†).
The electron impact mass spectra (70 eV) of 1–3 show that the molecular peaks of compounds 1–3 appeared at 402, 458, and 514 m/z, respectively (Fig. S8, S20 and S32 in ESI†). In addition, the absence of other peaks between 500 and 1000 m/z excludes the existence of oligomeric species other than dimers. Similar data have been reported in the literature,28 and the mass spectra data indicate that 1–3 exist as dimeric structures in the gas phase.
| Entry | Catalyst | Mol% | Solvent | t (h) | Yieldb,c (%) |
|---|---|---|---|---|---|
| a Reaction conditions: 2 mmol benzaldehyde, 3.5 mmol TMSCN, and 5 mL solvent.b Isolated yields after silica-gel column chromatography based on benzaldehyde.c Average of two runs.d [AlL]2 = [Al(OC6H2-2,4-Me2-6-CH2)3N]2. | |||||
| 1 | 1 | 0.5 | CH3CN | 1 | 95 |
| 2 | 2 | 0.5 | CH3CN | 1 | 90 |
| 3 | 3 | 0.5 | CH3CN | 1 | 84 |
| 4 | [AlL]2d | 0.5 | CH3CN | 1 | 15 |
| 5 | — | — | CH3CN | 1 | 0 |
| 6 | 1 | 0.1 | CH3CN | 6 | 93 |
| 7 | 2 | 0.1 | CH3CN | 6 | 87 |
| 8 | 3 | 0.1 | CH3CN | 6 | 83 |
| 9 | [AlL]2d | 0.1 | CH3CN | 6 | 13 |
| 10 | 1 | 0.05 | CH3CN | 6 | 39 |
| 11 | 2 | 0.05 | CH3CN | 6 | 31 |
| 12 | 3 | 0.05 | CH3CN | 6 | 26 |
| 13 | [AlL]2d | 0.05 | CH3CN | 6 | 5 |
| 14 | 1 | 0.1 | Toluene | 6 | 67 |
| 15 | 2 | 0.1 | Toluene | 6 | 59 |
| 16 | 3 | 0.1 | Toluene | 6 | 54 |
Such an order of the catalytic activities for 1–3 is significantly correlated with the dissociation free energy barrier of each bond between Al and bridged O atom. In order to exhibit efficiently catalytic behaviors of these alumatrane complexes, the dissociation of Al–O bond have to be especially well occurred for the insertion of substrates to Al center. These energy barriers could be calculated as the thermal stabilities between before and after dissociation of Al–O bonds in gas phase. The values of 1–3 were estimated as 1740 kcal mol−1 for 1, 1766 kcal mol−1 for 2 and 1780 kcal mol−1 for 3, indicating that the more decreasing the dissociation energy barrier of Al–O bond are, the more increasing the catalytic activities show. Consequently, the reason why the high catalytic activity in 1 could be shown compared to 2 or 3 is the weakest bond strength between Al and bridged O atom in 1 among those of alumatrane complexes. For the trimethylsilylcyanation reaction, a polar solvent such as acetonitrile is normally used to attain a high yield. As expected, changing the solvent from polar acetonitrile to nonpolar toluene caused a decrease of catalytic activity (entries 14–16). Since our systems 1–3 have higher solubility in CH3CN and toluene than [AlL]2,18 they showed higher catalytic activity than [AlL]2. However, the maintained homogeneity after completion of the reaction prevents the recycling of catalysts 1–3 for this reaction.
With the optimized conditions of 0.5 mol% 1, 5 mL CH3CN, rt and 1 h in hand, we examined the effect of various aryl aldehydes (instead of benzaldehyde) on the trimethylsilylcyanation reaction (Table 3). The coupling of benzaldehyde (entry 1) with TMSCN efficiently generated the desired product in 95% isolated yield. Electron-donating aldehydes such as p-tolualdehyde (entry 2) and p-anisaldehyde (entry 3), electron-withdrawing aldehydes such as α,α,α-trifluorotolualdehyde (entry 4), 4-nitrobenzaldehyde (entry 5), 4-cyanobenzaldehyde (entry 6), methyl 4-formylbenzoate (entry 7), and 4-chlorobenzaldehyde (entry 8) and electron-neutral aldehydes such as 1-naphthaldehyde (entry 9) and 2-naphthaldehde (entry 10) were also effective in the trimethylsilylcyanation reaction. When 0.5 mol% 1 was employed in this reaction, three aryl aldehydes—the highly electron-withdrawing α,α,α-trifluorotolualdehyde (entry 4) and 4-chlorobenzaldehyde (entry 8) and the sterically hindered electron-neutral 1-naphthaldehyde (entry 9)—resulted in only 83–85% isolated yields. Other aryl aldehydes showed activities similar to that of benzaldehyde.
| Entry | ArC( O)H |
Yieldb,c (%) |
|---|---|---|
a Reaction conditions: 2 mmol ArC( O)H, 3.5 mmol TMSCN, 5 mL CH3CN, 0.5 mol% 1, rt, and 1 h.b Isolated yields after silica-gel column chromatography based on aryl aldehyde.c Average of two runs. |
||
| 1 | Benzaldehyde | 95 |
| 2 | p-Tolualdehyde | 90 |
| 3 | p-Anisaldehyde | 94 |
| 4 | α,α,α-Trifluoro-p-tolualdehyde | 85 |
| 5 | 4-Nitrobenzaldehyde | 91 |
| 6 | 4-Cyanobenzaldehyde | 92 |
| 7 | Methyl 4-formylbenzoate | 90 |
| 8 | 4-Chlorobenzaldehyde | 83 |
| 9 | 1-Naphthaldehyde | 85 |
| 10 | 2-Naphthaldehde | 91 |
We also screened various heterocyclic and alkyl aldehydes using the optimized trimethylsilylcyanation conditions of 0.5 mol% 1, 5 mL CH3CN, rt and 1 h (Table 4). With 2- and 3-pyridine-carboxaldehyde and 6-methyl-2-pyridine-carboxaldehyde, good product yields of 91%, 86%, and 93%, respectively, were obtained (entries 1–3). As shown in Table 4 (entries 4–6), 6,2- and 3-thiopenecarboxaldehyde and 4-methyl-2-thiazolecarboxaldehyde also worked well in this reaction, giving 90%, 83%, and 91% yields of the corresponding products, respectively. Straight-chain alkyl aldehydes (entries 7 and 8), a conjugated aldehyde (entry 9), and an aldehyde with a sterically hindered cyclic ring (entry 10) also provided the corresponding products in reasonably good yields of 80–87%.
A possible mechanism for alumatrane catalyzed trimethylsilylcyanation reaction is proposed in Scheme 2. The catalytic cycle starts with the coordination of aldehyde to the Lewis acidic Al center in alumatrane 1, generating neutral monomeric alumatrane 1′. Generally, dimeric alumatranes in the presence of aldehyde could be easily converted to monomeric specie, which was supported by structurally characterized monomeric alumatrane adduct with benzaldehyde obtained from the reaction between dimeric alumatrane and benzaldehyde.17 In addition, we also calculated the dissociation free energy barrier of Al–O bond as 1740 kcal mol−1 for 1, 1766 kcal mol−1 for 2 and 1780 kcal mol−1 for 3, indicating that monomeric alumatrane containing aldehyde could be easily generated. Then, a cyanide anion as a nucleophile attacks the electron-deficient carbonyl carbon on the activated aldehyde to make new ionic species 1′′. Finally, the production of the desired product facilitates the regeneration of the catalyst 1.
| 1 | 2 | 3 | |
|---|---|---|---|
| a R1 = ∑||Fo| − |Fc||/∑|Fo|.b wR2 = {∑[w(Fo2 − Fc2)2]/∑[w(Fo2)2]}1/2. | |||
| Chemical formula | C15H24AlNO3 | C68H112Al4N4O12 | C12H24AlNO3 |
| Formula weight | 293.33 | 1285.53 | 257.30 |
| Crystal system | Monoclinic | Monoclinic | Monoclinic |
| Space group | P21/c | P21/n | P21/n |
| a (Å) | 10.3390(5) | 13.6533(6) | 9.4843(5) |
| b (Å) | 9.2969(4) | 14.1939(6) | 10.5629(6) |
| c (Å) | 17.3082(8) | 18.8530(8) | 14.1175(7) |
| α (deg) | 90.00 | 90.00 | 90.00 |
| β (deg) | 107.191(3) | 98.997(2) | 91.340(3) |
| γ (deg) | 90.00 | 90.00 | 90.00 |
| V (Å3) | 1589.35(13) | 3608.6(3) | 1413.93(13) |
| Z | 4 | 2 | 4 |
| dcalcd (g cm−3) | 1.226 | 1.183 | 1.209 |
| F(000) | 632 | 1392 | 560 |
| Reflections collected | 19 264 |
79 871 |
24 117 |
| # of independent reflections | 3343 [R(int) = 0.0340] | 13 281 [R(int) = 0.0668] |
4377 [R(int) = 0.0571] |
| # of parameters | 184 | 407 | 160 |
| R1 (I > 2σ(I))a | 0.0903 | 0.0579 | 0.0513 |
| wR2 (I > 2σ(I))b | 0.2667 | 0.1526 | 0.1350 |
| GOF (I > 2σ(I)) | 1.082 | 1.017 | 1.060 |
Footnotes |
| † Electronic supplementary information (ESI) available: NMR, IR, EI mass spectra and computational details. CCDC 1494116–1494118. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c7ra09851k |
| ‡ The first, second, and third authors contributed equally to this work. |
| This journal is © The Royal Society of Chemistry 2017 |