2.1. Bis(Trimethylsilyl)Methyllithium 1 and -Sodium 2 in Solution
The preparation of alkyl compounds of heavier alkali metal compounds often follows a similar protocol. By mixing an alkoxide of the corresponding alkali metal with an alkyllithium compound in
n-hexane, the immediately formed insoluble alkyl compound can be isolated by filtration [
8]. The preparation for
2 stands out, because no precipitate is formed, and the alkyl sodium compound is isolated by crystallization at −30 °C from hexane [
11]. This unusual high solubility in the non-coordinating solvent should be caused by breaking of the polymeric chain found in solid state into more mobile molecular units. To obtain information about the molecular weight and aggregation degree of these molecular units, we tested solutions of
1 and
2 by cryoscopic and NMR-DOSY methods. Cryoscopic measurements under inert gas conditions were performed in cyclohexane, which combines minimal to non-existent Lewis basicity (and therefore no coordinating abilities) and a considerable high cryoscopic constant with a freezing point at a convenient temperature (6.7 °C) [
20]. This allows measurements with higher concentrations with comparatively high depression of the observed melting points (
Table 1 and
Table S1). The freezing point depression of
1 was measured only at one concentration (0.04 mol/L) due to its low solubility in cyclohexane at this temperature. We observed a freezing point depression of 0.50 degrees, which corresponds to a molecular weight of 345 g/mol. This result points to the existence of dimeric units (open or ring-shaped dimers) in solution (2 × 166 g/mol = 332 g/mol, ∆M = +3.7%). The comparable high solubility of
2 at ~6 °C allowed us to study its solubility in cyclohexane in a range of concentrations (0.021, 0.041, and 0.087 mol/L, see
Table 1). The results at 0.021 and 0.041 mol/L point to the existence of tetrameric units, while measurements at the higher concentrations of 0.087 mol/L reveal higher molecular weights consistent with the presence of hexameric units. Cryoscopic measurements of trimethylsilylmethyllithium [LiCH
2SiMe
3] in cyclohexane revealed a very similar behavior; depending on the concentration, it was possible to identify tetrameric or hexameric oligomers [
15]. For geometric reasons, only even-numbered oligomers (dimer, tetramer, and hexamer) are considered. For tetramers and hexamers, the most likely arrangements are cages, such as face-capped tetra- or octahedrons. The basic elements of these cages are dimeric units, which can form higher oligomers following a principle called “ring-laddering” [
21,
22]. For this reason, the appearance of pentameric units is unlikely. However, the formation of ring-shaped trimers is possible but rarely observed for unsolvated organolithium compounds and more commonly for secondary lithium amides [
23].
Additionally, we studied solutions of
1 and
2 by NMR spectroscopy (
Figures S1–S21). Measurements in solvents with different coordinating abilities can reveal influences on the corresponding aggregation behavior [
24]. However, the results obtained by
1H,
13C,
29Si, and
7Li NMR spectroscopy in deuterated benzene [C
6D
6], deuterated tetrahydrofuran [D8]THF, and deuterated cyclohexane [C
6D
12] did not reveal significant differences such as changes in chemical shifts or splitting of signals (
Table 2).
To obtain additional information about the degree of aggregation in non-coordinating solvents parallel to the results obtained by cryoscopic measurements (see above), we carried out
1H diffusion ordered spectroscopy (DOSY) NMR [
25] at 21 °C to study the oligomer formation as a function of the concentration (
Table 3) in deuterated cyclohexane [C
6D
12] solutions of two organometallic compounds
1 [LiCH(SiMe
3)
2] and
2 [NaCH(SiMe
3)
2]. Considering the basic properties of the compounds, inert tetrakis(trimethylsilyl)silane [Si(SiMe
3)
4] at the same concentration as the investigated compounds for all samples was chosen as a reference. The
D values (m
2/s) were acquired from the diffusion analyses, and the respective hydrodynamic radii were calculated using the Stokes-Einstein equation:
D = (
kBT)/(6
πηrH) where
kB is the Boltzmann constant,
η [kg/(s·m)] is the viscosity of the solvent at the respective temperature
T (K) and
rH the hydrodynamic radius in nm (for a spherical particle).
Increasing the concentration of the solutions for both investigated compounds leads to a slight increase in the calculated value for the hydrodynamic radius of the reference Si(SiMe
3)
4 (on average 0.35 nm), which is related to a somewhat slower diffusion (
Figure 1). This variation is, however, minimal and probably due to more contact with other molecules in the solution at higher concentrations. In the solution of
2 with a 0.1 mol/L concentration, the hydrodynamic radius is determined to be approximately twice as high compared to Si(SiMe
3)
4 (0.72 nm versus ca. 0.35 nm). This fact most probably reflects the formation of a tetramer, especially considering the difference in the molecular masses (182.39 g/mol for the base compared to 320.84 g/mol for Si(SiMe
3)
4). Further stepwise increase of the solute concentration in 0.1 mol/L steps (until saturation) results in slower diffusion, resp. noticeably higher
rH values for
2. This we attribute to the formation of higher oligomers. It should be considered that the formation and dissociation of such complexes is fast on the NMR timescale, and the measured diffusion coefficients and the corresponding calculated hydrodynamic radii represent a weighted average of the present species in the mixture. Thus, we conclude that at a concentration of 0.2 mol/L of NaCH(SiMe
3)
2, the maximum in the distribution of the formed oligomeric complexes is around 5 aggregated monomer units (a mixture of tetramers and hexamers), which corresponds to an average hydrodynamic radius of 0.88 nm. A further increase in the concentration leads to a shift of this maximum to about 1.10 nm, which is related to a predominant hexamer formation.
In a parallel study, such a concentration-dependent complex growth was not detected for the solutions of
1. At all measured concentrations, comparable
D and
rH values for the organometallic base and the Si(SiMe
3)
4 reference were observed (
Table 3). Taking into account the molecular masses of both compounds (166.34 g/mol for the LiCH(SiMe
3)
2 and 320.84 g/mol for Si(SiMe
3)
4) as well as comparing with the hydrodynamic radii calculated for
2, we conclude that a dimer is predominantly stabilized in all solutions of
1 with a corresponding
rH of 0.34 nm. The slightly higher
rH value measured at saturation (0.39 nm) is most probably related to the sole amount of solute rather than with the formation of higher complexes, which, however, cannot be completely excluded. Thus, the NMR results are in good agreement with the cryoscopy measurements (
Figure 2). The discrepancy between the cryoscopy and DOSY results for the concentrations of
2 resulting in hexamers can be attributed to temperature-dependent tendencies to form higher aggregates. The formation of higher aggregates of
2 seems to be thermodynamically favored, but at higher temperatures the lower aggregates are favored by entropy.
2.2. Formation of Complexes of Compounds 1 and 2 with O- and N- Donors
In order to obtain more data about possible structural motifs of
1 and
2 existing in solution, we studied complexes of
1 and
2 with THF or TMEDA in the solid state (
Scheme 2). The metal atom of the alkali metal alkyl compound interacts with the carbon atoms through electron-deficient 2-electron-3-(or more)-center bonds. This makes the electrophile metal atom very susceptible to interactions with Lewis-basic ligands. The obtained structures may show structural motifs with relevance to monomeric, dimeric, or tetrameric units, due to the increased steric saturation of the coordination sphere of the metal atoms. At the same time, several possible coordination modes corresponding to metal atoms, such as linear bridging, angular bridging, or terminal coordination of the bis(trimethylsilyl)methyl groups (or metal atoms) can be studied.
Treatment of solutions of
1 or
2 in
n-hexane at RT with THF or TMEDA in equimolar amounts (
1b) or excess (
1a,
2a,
b) produces clear solutions, from which colorless crystals can be obtained (
1a at RT,
1b at 5 °C,
2a,
b at −20 °C) with moderate to low yields (
1a: 52%;
1b: 34%;
2a: 17%,
2b: <5%). The absence of decomposition (ether cleavage) in the case of the mixture of
1 and
2 with THF demonstrates the low reactivity of these bis(trimethylsilyl)methyl compounds towards THF in contrast to other lithium compounds such as neopentyllithium [
24] or
t-butyllithium [
26]. Crystals of compound
2b easily decomposed or melted at RT. Lappert et al. already described and characterized solutions of compound
1b in cyclohexane as monomeric units [
16]. However, a solid state structure was not reported.
2.4. X-ray Crystallographic Measurements of Compounds 1a,b and 2a,b
All four compounds
1a,
b and
2a,
b crystallized in the same monoclinic space group (
Table 5,
Figures S36–S39). The thermal instability of single crystals of compounds
1b and
2b required sample preparation for X-ray crystallography at low temperatures [
27]. The THF or TMEDA groups showed significant positional disorder in compounds
1a (0.53/0.47),
1b (0.68/0.32 and 0.75/0.25), and
2b (0.78/0.22) [
16]. In compound
1b, one trimethylsilyl group displayed rotational disorder (0.5/0.5). In all four compounds, it was possible to locate the hydrogen atom of the metal bound CH-group.
Compound
1a (
Figure 3) is a dimer formed by two THF-coordinated
1-units (
Table 6). The central motif is a planar Li
2C
2 ring with crystallographic inversion symmetry. This motif is similar to the THF-coordinated lithium bis(trimethylsilyl)amide, where the bis(trimethylsilyl)methyl group is replaced by the isoelectronic bis(trimethylsilyl)amide [
29]. The Li
2C
2 ring has one shorter (2.204(2) Å) and one longer (2.274(3) Å) Li–C bond, and the C‒Li‒C angle (115.36(10)°) is far wider than the corresponding Li‒C‒Li angle (64.64(10)°). The trigonal pyramidal bis(trimethylsilyl)methyl unit (sum of the Si‒C‒Si and two H‒C‒Si angles: 327.2°) leads to an orientation of both trimethylsilyl groups above and below, and the corresponding hydrogen atom roughly in the plane of the central Li
2C
2 ring. The lithium atom with a coordination number of CN = 3 shows an additional coordination of the oxygen atom of the THF group (Li‒O 1.953(8) Å), leading to an approximate trigonal planar arrangement (C‒Li‒O 137.4(7)° and 110.5(6)°).
X-ray crystallography as well as NMR spectroscopy revealed compound
1b (
Figure 4) as a monomeric TMEDA-coordinated bis(trimethylsilyl)methyllithium with one TMEDA molecule per lithium atom, similar to the corresponding monomeric complex
1-PMDETA [
16]. Two crystallographically independent units are found in the monoclinic cell. The distance between the lithium atoms (both with a coordination number of CN = 3) and the carbon of the central carbon atom of the bis(trimethylsilyl)methyl group Li‒C is 2.070(3)/2.083(3) Å shorter than the corresponding distances in polymeric
1 (2.14 to 2.22 Å) [
10] or dimeric
1a (2.204(2) Å). On the other hand, the Li‒C distance for evaporated
1 determined by gas-phase electron diffraction is with 2.03 Å shorter [
10]; in monomeric
1-PMDETA, the Li‒C distance is 2.14 Å [
16]. The similar results for both monomeric
1b (
1-TMEDA) and
1-PMDETA with a considerable difference in the steric demand of the corresponding ligand demonstrate the spacial flexibility of the bis(trimethylsilyl)methyl group, which makes it such a useful ligand in the formation of otherwise inaccessible metal compounds.
This difference between short Li–C distances for monomeric units and longer Li–C distances in oligomers can be explained by the existence of two-center two-electron bonds for the monomeric compounds, while the bonds in oligomeric and polymeric compounds should be based on three-center two-electron bonds (linear or bent). Due to the one-sided interaction of the lithium with the bis(trimethylsilyl)methyl group, the (Me3Si)2CH unit shows a trigonal pyramidal arrangement of the trimethylsilyl groups and the hydrogen atom (Si‒C‒Si 123.25(10)° and 122.48(11)°; the sum of the Si‒C‒Si and two H‒C‒Si angles: 341.1° and 341.0°). The two nitrogen atoms of the TMEDA coordinate the lithium atom (Li‒N 2.054(6) and 2.071(9) Å; 2.133(7) and 2.061(9) Å) with an N–Li–N bite angle of 88.8(2)° and 87.2(2)°.
According to X-ray crystallographic data the sodium compound
2a (
Figure 5) organizes in the solid state as a polymeric chain along the crystallographic
b-axis consisting of THF-coordinated
2 units with sodium oxygen–interactions (Na1‒O1 2.375(3) Å). The central carbon of the CH(SiMe
3)
2 group shows a roughly linear (Na‒C–Na 159.30(18)°) coordination by two sodium atoms with slightly different bond lengths (Na1‒C1 2.778(4) Å; Na1A‒C1 2.657(4) Å), leading to an approximately trigonal bipyramidal environment of the carbon atom. A very similar pattern of Na‒C distances was found in polymeric TMEDA-coordinated trimethylsilylmethylsodium with Na‒C 2.523 Å and 2.530 Å [
8]. Additionally, the sodium atoms with a coordination number of CN = 3 are coordinated by the oxygen of a THF group, leading to an approximately trigonal planar environment (C1‒Na1‒C1A 130.74(6)°; C1‒Na1‒O1 129.93(13)°; C1A‒Na1‒O1 99.33(13)°; sum of angles: 360.0°) of the sodium atom. Overall, this results in a zigzag shape of the polymeric chain very similar to the structure of bis(trimethylsilyl)methylpotassium coordinated by THF [
13] or the structure of parent
2. Compared to the latter, the additional interaction with the oxygen atom merely leads to the reduction of the Na‒C‒Na angle from 143° in
2 to 130.74(6)° in
2a, and the change from a screw axis with a periodicity of four to a simple zigzag chain.
The CH(SiMe3)2 moiety itself shows an approximate planar coordination of both SiMe3 groups and the hydrogen atom (Si11‒C1‒Si12 127.9(3)°, sum of the Si‒C‒Si and two H‒C‒Si angles: 359.3°). In addition, the methyl groups close to the Na atoms give rise to Na···Me contacts with short Na‒C distances (Na1‒C111 3.104(5) Å and Na1‒C123 2.961(5) Å). Compound 2a is characterized by unusually short Na‒H interactions with the hydrogen atom of the central C‒H unit (Na–H 2.66 Å/2.70 Å) which are in a similar range as the corresponding Na‒C distances.
In contrast to the composition found through
1H NMR spectroscopy with an equimolar ratio
2:TMEDA of 1:1, the crystals of compound
2b (
Figure 6) isolated for X-ray crystallography show a ratio
2:TMEDA of 2:3. The compound can be described as dimer of TMEDA-coordinated monomers of
2. The (symmetric) sodium atoms with a coordination number CN = 4 are in close contact with a CH(SiMe
3)
2 group (Na1‒C1 2.520(2) Å). The coordination sphere of the sodium is completed to a distorted tetrahedral environment by the three nitrogen atoms of two different TMEDA groups (Na1‒N21 2.559(2) Å; Na1‒N31 2.569(2) Å; Na1‒N32 2.635(2) Å) with one TMEDA group bridging between the two symmetric monomeric units. A similar arrangement was found for TMEDA-coordinated trimethylsilyllithium [
30]. The CH(SiMe
3)
2 unit shows a clear trigonal pyramidal arrangement of the SiMe
3 groups and the hydrogen atom (Si‒C‒Si 120.91(7)°; the sum of the Si‒C‒Si and two H‒C‒Si angles: 336.0°).