Open Access Article
Lauren E.
Wenger
and
Timothy P.
Hanusa
*
Department of Chemistry, Vanderbilt University, Nashville, Tennessee 37235, USA. E-mail: t.hanusa@vanderbilt.edu
First published on 27th March 2024
The heavy Group 15 allyls
(E = As, Sb, Bi; [A′] = [1,3-(SiMe3)2C3H3]−) can be prepared either in solution or mechanochemically, and exist in two diastereomeric forms of C1 and C3 symmetry. For E = As and Sb, their ratio varies with the method of preparation: the C1 diastereomer is the major form by both methods, but the mechanochemical route increases the C1
:
C3 ratio compared to synthesis in hexanes solution. The difference in selectivity has previously been identified as a consequence of the layered crystal lattices of the EX3 reagents, which provide a templating effect through an anisotropic grinding environment. How this selectivity changes with other typical mechanochemical variables is explored here, including the use of different reagents and LAG solvents, pre-grinding the reagents, the use of different milling media (stainless steel, Teflon, etc.) and apparatus (mixer mill, planetary mill), and the number and size of balls. The extent to which the anisotropic environment is either maintained or modified during synthesis (especially by LAG and the choice of metal reagent) affects the diastereomeric ratio.
We have previously explored the formation of the heavy Group 15 allyls
(E = As, Sb, Bi; [A′] = [1,3-(SiMe3)2C3H3]−), which can be prepared either in solution or mechanochemically from EX3 and K[A′] (for As, Sb) or [AlA3] (for Bi).5 The
complexes are generated in two diastereomeric forms, one of C1 symmetry and the other of C3 symmetry (Fig. 1), and for E = As and Sb their ratio varies with the method of preparation (for E = Bi, the ratio is essentially the same for both reaction environments). The halide metathetical synthetic approach is not successful for all combinations of reagents. For example, AsI3 and K[A′] in THF solution, or BiCl3 and K[A′] in the solid state, initiate a redox reaction leading to allyl coupling and the formation of 1,3,4,6-tetrakis(trimethylsilyl)hexa-1,5-diene ({A′}2) as the major product.
![]() | ||
Fig. 1 Diastereomeric forms of . The C1 form is crystallographically characterized for E = As, Sb; the C3 forms have been identified from NMR spectroscopy and their structures studied computationally.5 | ||
The C1 diastereomer is the major form by both methods for both As and Sb, but the mechanochemical route increases the relative amount of C1 by 3.3 times for As and 1.5 times for Sb, compared to preparation in hexanes solution. This difference in selectivity has been attributed to the layered crystal lattice of each metal precursor (Fig. 2 and Table S1†).5 Density functional theory (DFT) calculations have been used to demonstrate that when arsenic is embedded in an AsI3 lattice (Fig. 2b), the first allyl to bind to As will preferentially be aligned parallel to the lattice planes of AsI3, thereby avoiding excessive steric interaction (Fig. 3a). The second allyl will then most easily bind perpendicularly to the first; calculations indicate that the lower energy isomer of the intermediate
contains allyls of opposite handedness, i.e. [As(R-A′)(S-A′)I] is lower in energy than [As(R-A′)2I] by 11.5 kJ mol−1.5 Setting the stereochemistry in this step leads to a preference for the C1 form in the solid state. In contrast, for a
unit in solution, the C3 backbone of the allyl is arranged roughly perpendicularly to a line connecting the iodides (i.e., 90° from the solid-state orientation). There is not a strong stereochemical preference for the subsequent orientations of the other allyl ligands, raising the probability of generating the C3 form in solution (Fig. 3b). The weaker preference for the C1 form in
is likely the result of the zig-zag layers of SbCl3 enforcing the stereochemically directed assembly less strictly than does the planar geometry of AsI3.
![]() | ||
| Fig. 2 Structures of MX3 (M = As, Sb; X = Cl, I): (a) AsCl3 (liquid at room temperature); (b) lattice of AsI3; (c) lattice of SbCl3; (d) lattice of SbI3. See Table S1† for details of the structures. | ||
![]() | ||
Fig. 3 (a) Preferred conformation of an unit when the [AsI2] fragment is part of the AsI3 lattice; (b) Lowest energy conformation of an unit in solution. TMS = trimethylsilyl. | ||
The original report of
synthesis found that the C1
:
C3 ratio of the mechanochemically prepared compounds was relatively constant over a range of grinding times in a planetary mill with stainless steel grinding balls (5 min to 2 h), although at very short reaction times (30 s), the C1
:
C3 ratio of
was somewhat higher, suggesting that C1 is the more rapidly formed diastereomer.5 We were interested in determining whether other mechanochemical reaction variables, including the mill type, jar and ball material, size of balls, operation of liquid assisted grinding (LAG),6 or changes in metal precursor (two different halides are now used for both As and Sb), could lead to alterations in the diastereomer selectivity.
The mechanochemical formation of diastereomeric
complexes serves as a valuable model system to investigate the potential amplification or suppression of the effects of an anisotropic reaction environment. Furthermore, it sheds light on how manipulating this environment might affect the balance between halide metathesis and redox behavior.
was prepared mechanochemically from AsI3 or AsCl3 and 3 equiv. of K[A′] under various milling conditions.
was prepared analogously from SbCl3 or SbI3 and 3 equiv. of K[A′]. Additional experimental details are provided in the ESI.† This section highlights the relevant changes from the literature procedure, which fall into four categories: LAG, pre-grinding, changes in metal precursor, and mechanochemical equipment variables.
For all conditions, each experiment was performed in at least duplicate and often triplicate. For each reaction, 1H NMR data was used to determine the C1
:
C3 ratio, yield of
, and the
ratio.
and other products (potassium iodide, {A′}2, elemental As), leading to decomposition of
to form more {A′}2. Therefore, decomposition studies were performed to better understand how reaction time affects the production of
and {A′}2. Specifically,
was milled alone or with 3 equiv. of potassium iodide in the mixer mill for 30–60 min with small or large stainless steel ball bearings (see Table S7†). For comparison, prepared
was dissolved in toluene-d8 in an NMR tube and heated in an oil bath at 90 °C for 7.5 h, and the outcome monitored with 1H NMR.
:
C3 ratio of
decreased with increasing amounts of solvent. The addition of a small volume of hexanes modifies the C1
:
C3 ratio quickly: mechanochemical enhancement compared to solution is cut in half by ca. 3.5 equiv. of hexanes (η = 0.41)6 (Fig. 4). Arsenic triiodide has low, but detectable solubility in hexanes;7 in contrast it has no measurable solubility in HMDSO. Nevertheless, HMDSO displays similar effects on the C1
:
C3 ratio (Fig. 4); 3 equiv. reduces the C1
:
C3 excess by half (η = 0.56). From dry grinding to solution conditions, the changes in C1
:
C3 ratios in the LAG reactions follow a simple power curve.
LAG with THF prevents formation of
. In the presence of THF, K[A′] can reversibly form the solvent adduct {K[A′](thf)3/2}.8 This might be the reason that the use of 4.5 equiv. (η = 0.33) of THF (and 3 K[A′]) completely blocks product formation, yielding only recovered starting material. Using more THF (10 or 13 equiv., η = 0.81 and 0.95, respectively), affords {A′}2 as the major product
with low C1
:
C3 ratios (3.5, 3.3), close to that found in the preparation from hexanes solution (see Table S5†). As noted above, the solution-based reaction in THF produces {A′}2 as the major identified product.5 Once prepared, however,
is stable in THF-d8 solution (1H NMR), indicating that the difficulty with THF is only in the formation of
, not with its subsequent reactivity.
For
, LAG was performed for reactions of SbCl3 and 3 equiv. of K[A′] with hexanes. As with the arsenic system, the C1
:
C3 ratio decreases with increasing solvent, but the trend is less pronounced, in part due to the lower magnitude of change between dry grinding and solution conditions (Fig. 4). Here, the reduction in the preference for C1
:
C3 by 50% requires the addition of 17 equiv. of hexanes (η = 2.4), which is firmly in the “slurry” region of the LAG range.6
For both
and
, trends in the yield of
or
ratio do not show clear correlations with increasing addition of solvent, so it remains uncertain what role the solvent plays in the competing reactions of metathesis and redox (see Fig. S6, S7, S15 and S16†).
does reveal a decrease in the C1
:
C3 ratio, but only when using the planetary mill. The C1
:
C3 ratio decreases ca. 27% over 45 min (linear equivalent = −0.053 min−1). However, the C1
:
C3 ratio does not approach that from a solution reaction during that time (Fig. 5). The yield and
ratio also trended downward with increased pre-grinding time (see Fig. S8 and S9†).
![]() | ||
| Fig. 5 Effect of pre-grinding AsI3 on diastereomer formation. PBM600 = planetary mill, 600 rpm; MM30 = mixer mill at 30 Hz; MM10 = mixer mill at 10 Hz. | ||
With a mixer mill, in contrast, the C1
:
C3 ratio was nearly constant at 30 Hz over all pre-grinding time points (Fig. 5). Visual inspection showed no significant change in the appearance of AsI3 with pre-grinding time. After 1 min, the solid was finely ground and appeared similar to that ground for 30 min (see Fig. S22†). The higher energy collisions from the larger ball bearings and faster speed in the mixer mill likely erased any trend in the C1
:
C3 ratio of
by reaching a small particle size more quickly than in the planetary mill. In order to determine whether an effect was obvious with lowered energy input, the energy of both pre-grinding and the reaction were reduced by pre-grinding at 10 Hz and performing the reaction for 5 min instead of 10 min. Although there is a visual change in particle size from the shortest to longer pre-grinds (see Fig. S19–S21†), there is again no obvious trend in the C1
:
C3 ratio (Fig. 5).
Pre-grinding of SbCl3 was performed at 300 rpm in a planetary mill for 1 to 60 min or in the mixer mill at 20 Hz for 1 to 45 min. (The decreased frequencies in the mills match those of the optimized reaction conditions for
.) SbI3 was pre-ground at 300 rpm in the planetary mill for 1 to 45 min.
In the planetary mill, extended pre-grinding led to a slight decrease in C1
:
C3 for both SbI3 and SbCl3 (Fig. 6). The decrease was less than that of AsI3 under the same conditions (ca. 7% decrease for SbI3 after 45 min and a 10% decrease for SbCl3 in 60 min). Similar to the case with AsI3, when SbCl3 was pre-ground in the mixer mill there was no significant decrease in the C1
:
C3 ratio over time. Instead, mixer mill pre-grinding led to a significant decrease in both yield (−36%) and the
ratio with increased pre-grinding time (see Fig. S17 and S18†). Pre-grinding in the planetary mill led to small increases in these values as pre-grinding time increased (e.g., the yield rose from 31% (no pre-grinding) to 42% (pre-grinding SbCl3 for 60 min)). This suggests that the type of mill impacts the competition between metathesis and redox pathways.
![]() | ||
| Fig. 6 Effect of pre-grinding SbX3 on diastereomer formation. SbCl3–MM = SbCl3 in mixer mill; SbCl3–PBM = SbCl3 in planetary mill; SbI3–PBM = SbI3 in planetary mill. | ||
Although not as extensively studied as the pre-grinding experiments, several trials were conducted to explore the effect of variable frequency on the formation of
. Grinding K[A′] and SbCl3 at 20 Hz in a mixer mill for 10 min produced the highest yield (70 ± 10%), with a C1
:
C3 ratio of 2.53(±0.05) and a
ratio of 6(±3). Raising the frequency to 30 Hz for the same length of time marginally improved the C1
:
C3 ratio (2.66), but the yield dropped to 49%, and the
ratio decreased to 3.6. At 15 Hz, not only was the C1
:
C3 ratio lowered to 2.31, but also the reaction was incomplete, as unreacted K[A′] could be detected among the reaction products (1H NMR). It seems that although there is a modest boost (5%) to the C1
:
C3 ratio on going from 20 to 30 Hz, there is actually only a narrow window of usable frequencies for the optimum yield and maximum
ratio.
:
C3 in the preparation of
, as seen in Table 1. AsCl3 is a liquid at room temperature9 and produces a relatively low C1
:
C3 ratio (<3.7
:
1) for both mechanochemical and solutions reactions, similar to AsI3 in toluene solution. Milling with the layered AsI3 more than doubles the C1
:
C3 ratio obtained from AsCl3 in the mixer mill. Reactions with AsCl3 strongly favor metathesis over the redox pathway, producing very little {A′}2 when compared to AsI3. Although there are individual exceptions, the yields from AsCl3 under mechanochemical reactions are generally comparable, and often somewhat better, than those from solution. The original report of
5 found that it was formed in 80% yield from a 5 min grind in a planetary ball mill, but 64% from a solution reaction in hexanes. Table 1 expands on this, comparing yields of
from a mixer mill reaction and solution. The yields from AsCl3 are marginally higher in solution than in a mixer mill, but as just noted, its liquid state brings its behavior closer to what would be expected from a solution reaction rather than one conducted under solvent-free conditions.
| Entry | As source | Reaction conditionsa | Yield (%) | C1 : C3 ratio |
ratio |
|---|---|---|---|---|---|
| a Toluene = 3 h reaction time, room temperature; MM (mixer mill) = 10 min, 30 Hz; 2 × 3.5 g stainless steel ball bearings. | |||||
| 1 | AsCl3 | Toluene | 80(±4) | 3.65(±0.03) | 14(±5) |
| 2 | AsCl3 | MM | 70(±1) | 3.19(±0.01) | 14(±5) |
| 3 | AsI3 | Toluene | 28(±8) | 2.60(±0.09) | 0.6(±0.2) |
| 4 | AsI3 | MM | 44(±1) | 6.7(±0.2) | 1.4(±0.2) |
The structure of the two antimony halides, SbCl3 and SbI3, are more similar than in the arsenic case, but significant distinctions remain between them. After examining differences through reactions in the planetary and mixer mills, pre-grinding experiments, and use of multiple jar materials, it is clear that compared to SbCl3, SbI3 yields
with a higher C1
:
C3 ratio, but also more {A′}2 and decreased yield. For example, a 60 min grind in the planetary mill in ZrO2 jars produced a C1
:
C3 ratio of 3.8 and a 25% yield with SbI3, but a 2.8 C1
:
C3 ratio and 60% yield with SbCl3. The parallel layers of solid SbI3 resemble those of AsI3 more than the zig-zag layers of SbCl3, evidently leading to a greater preference for the C1 form when SbI3 is used. As with the arsenic derivative, yields of
are favored somewhat under mechanochemical conditions. As one example, using SbCl3 for a 10 min grind in ZrO2 jars in a planetary mill provides a 72% yield of
; a 3 h reaction in hexanes provides 48%.
synthesis,5 there is little to no change in the C1
:
C3 ratio for
or
over extended reaction times when reactions are conducted in a planetary mill, using either stainless steel or zirconia jars. However, when
is prepared in a mixer mill, increased milling time led to a detectable decrease in C1
:
C3 with both stainless steel and Teflon jars (Table 2). The same was also true for reactions to form
(Fig. S12†).
:
C3 ratio of
a
| Entry | Milling environment | Time (min) | C1 : C3 ratio |
|---|---|---|---|
| a MM = mixer mill; PM = planetary mill. | |||
| 1 | Teflon, MM | 10 | 10.7(±0.4) |
| 2 | Teflon, MM | 60 | 8.5(±0.1) |
| 3 | Stainless, MM | 10 | 6.7(±0.2) |
| 4 | Stainless, MM | 60 | 6.0(±0.5) |
| 5 | ZrO2, PM | 10 | 6.46(±0.01) |
| 6 | ZrO2, PM | 60 | 6.7(±0.4) |
| 7 | Stainless, PM | 10 | 7.7(±0.8) |
| 8 | Stainless, PM | 60 | 8.5(±1.0) |
The trends in the
ratio and yield for
follow the same trend as C1
:
C3 (Fig. S1–S3†). For
, the
ratio decreased at longer reaction times under all conditions, but the rate of decrease was greatest for mixer mill reactions (Fig. S13 and S14†). The yields of
and
were consistent over time when using the planetary mill, but yields decreased at longer reaction times in the mixer mill.
The highest C1
:
C3 ratio
was found from short reaction times using Teflon mixer mill jars (Table 2, entries 1 and 2), notably higher (>30%) than comparable reactions using stainless steel (entries 3 and 4) (With a short grinding time of 5 min, the Teflon/MM environment yielded a C1
:
C3 ratio of 11.1, the highest C1 enrichment we have yet observed; it is 37% higher than the 8.1 ratio found with stainless steel/MM). In the planetary mill, reactions in zirconia jars (entries 5 and 6) yielded a lower C1
:
C3 ratio than in stainless steel (7 and 8).
The highest C1
:
C3 ratio for
was observed using antimony iodide and stainless-steel planetary jars at short reaction times or using zirconia planetary jars at long reaction times. In general, however, the C1
:
C3 ratio does not appear to be significantly dependent on the jar material for
(Fig. S12†).
Generally, the
yield and the
ratio is the lowest using stainless steel materials, owing to higher rates of redox activity, an effect similar to that previously observed in other mechanochemical syntheses.10,13 The effects were greater for the metal iodides than antimony chloride. Across the reactions, yields and the
ratio decreased with increasing reaction time (Fig. S2, S3, S13 and S14†).
. For each reaction, a total of 7 g of stainless-steel balls were used (2 large balls or 14 small balls). The change in the C1
:
C3 ratio is not statistically significant with the smaller balls; with the larger balls the decline was noticeable (Fig. 7). The smaller balls consistently give higher C1
:
C3 ratio than the larger balls.
![]() | ||
Fig. 7 Effect of ball size on the C1 : C3 ratio of (small ball = 4.8 mm, 0.5 g per ball; large ball = 9.5 mm, 3.5 g per ball). | ||
The yield and the
ratio were both higher for the small ball bearings than the large, and all saw a decrease as reaction times increased (Fig. S4 and S5†).
was milled alone or with 3 equiv. of potassium iodide (i.e., a reaction by-product) in a mixer mill for 30–60 min. The change in C1
:
C3 ratio (Fig. S10†) and
ratio (Fig. S11†) before and after milling were monitored. There is little difference in either ratio when KI is present or absent, so it appears that KI does not play a significant role in the decomposition of
, the formation of {A′}2, or in changing the C1
:
C3 ratio.
As the presence of KI does not affect decomposition, the data in Fig. 8 omits experiments where KI was added (Table S6†). In this case, the percent change of the C1
:
C3 ratio (blue) or
ratio (red) is shown both before and after milling/heating. The change from heating is negligible, which is consistent with the original report of the synthesis.5 All milling experiments saw a decrease in C1
:
C3 and a decrease of
relative to {A′}2. The percent change in
is about twice that of C1
:
C3. Consistent with other findings, increased time and larger balls lead to more decomposition and less formation of the C1 diastereomer.
![]() | ||
Fig. 8 Effect of grinding prepared with either large (9.5 mm) or small (4.8 mm) stainless steel ball bearings. The negligible effect of heating in solution is also evident. | ||
Examining only diastereomeric ratios alone leaves unanswered the question of whether more of the C3 diastereomer is produced with increased milling time or whether less of the C1 form is produced. That the latter is more important is indicated by the masses of the products in some representative reactions to form
(Table 3). For both small and large balls, the amounts of both diastereomers decreases, but less of the C1 form is isolated relative to the more symmetric C3. As discussed below, it is possible that the solid C1 form is degraded more rapidly than the oily/liquid C3.
:
C3 composition of
a
| Ball size | Time (min) | C1 : C3 ratio |
Mass C1 | Mass C3 | Mass {A′}2 | |
|---|---|---|---|---|---|---|
| a Small ball = 4.8 mm, 0.5 g per ball; large ball = 9.5 mm, 3.5 g per ball. Masses are in mg. | ||||||
| Small | 5 | 8.5 | 89.5 | 10.5 | 12.5 | 8 |
| Small | 60 | 7.9 | 64.8 | 8.2 | 5.6 | 13 |
| Large | 5 | 8.1 | 77.4 | 9.6 | 5.4 | 16 |
| Large | 60 | 6.0 | 36 | 6 | 1.2 | 35 |
complexes constitute a well-defined system in which two diastereomers are formed for each element, and whose ratio is affected by the anisotropic environment in which they are formed. Our working hypothesis has been that the extent to which that environment is maintained or modified during synthesis will affect the diastereomeric ratio. The question is then to determine how mechanochemical variables affect that ratio.
:
C3 or
ratios. Solid-state reactions are inherently heterogeneous; a major benefit of solution-phase reactions is the creation of homogeneous mixtures. The problem of mixing is exacerbated when running reactions on a small scale. Furthermore, the chosen metal halides were used in their crystalline form and not as powders. As such, even though there was an attempt to minimize this as much as possible, there was heterogeneity in starting particle size. Across our studies, the ratio of C1
:
C3 was more consistent across multiple experiments under the same conditions, whereas the
ratio and yield were more varied.
In this system, it seems that the solubility of the intermediates of product formation may play a substantial role modifying the C1
:
C3 ratio. Crystalline AsI3 is slightly soluble in hexanes, and insoluble in HMDSO, but their use in LAG equally affects the C1
:
C3 ratio. In contrast, the product
is highly soluble in either solvent. While not experimentally testable (as these species are not isolable), the proposed intermediates of metathesis,
and
, would each be more soluble in the LAG liquid than AsI3, with solubility increasing with each substitution with an allyl. Hence in the presence of hexanes/HMDSO, the metathesis intermediate
should be more soluble in hexanes and could diffuse away from the AsI3 lattice (and the anisotropic environment) before additional substitution occurs, producing less C1 and relatively more of the C3 diastereomer. The more solvent present in the system, the more diffusion/detachment can proceed. It should be noted that although the experiments were conducted well within the standard LAG region (η < 1), the η value only takes into account the mass and volume of solvent.6 On a molecular level, three or more molecules of the LAG solvent were present for every metal center, providing enough for molecular diffusion to occur.18 Although a structure-directing effect has been observed before with LAG in the formation of host–guest complexes, co-crystals, and polymorphs,19 in which liquid polarity, the η value, and interactions between the liquid and the reactants have been implicated, it is rare to observe the effect displayed by the
complexes, in which LAG affects organometallic reaction intermediates.4a
:
C3 ratio in the mixer mill evidently happens within the first few minutes, as there is no apparent change when grinding from 5–30 min. Grinding in the planetary mill for up to 45 min shows a modest decrease, which might be related to the greater shearing forces in a planetary mill.20 Such forces can induce lattice defects, such as vacancies, dislocations, stacking faults, and grain boundaries, and cause partial reordering of the crystalline lattice.21 These disruptions could serve to degrade the environment on the surface of AsI3 particles. The effect is muted with the antimony precursors, but the C1
:
C3 ratio is smaller than that with the arsenic counterparts to begin with, so there is less room for change.
:
C3 ratios are associated with lower
ratios).
:
C3 with jar milling material (i.e., reactions in zirconia jars yielded a lower C1
:
C3 ratio than stainless steel, and Teflon provided the highest of all (Table 2)) suggest that a softer jar material favors an increase of C1, while a harder material favors a relative increase of C3 (zirconia has a Mohs hardness of 8.0–8.5, stainless steel is ca. 6.5, and Teflon from 2.0–2.5).24 This appears to be more important than the density, as steel (density ≈ 7.5 g mL−1) is denser than zirconia (≈5.6 g mL−1).
Another possible contributor to the lower C1
:
C3 ratio with harder grinding media may be related to deformations that occur to the reagents under pressure. For example, in the layers of arsenic triiodide are identifiable AsI3 units. The iodine anions are arranged in an hexagonal close packed (hcp) lattice with arsenic cations filling two-thirds of the octahedral holes in every other layer (Fig. 2b).25 Each arsenic is covalently bonded to three iodine atoms (2.65 Å), with another set of three iodine atoms further away (3.62 Å) but within the sum of van der Waals radii (ca. 3.9 Å).26 Under high pressure (>1.7 GPa), it has been found that AsI3 undergoes a phase transformation from the anisotropic phase to a more centrosymmetric phase.27 The intermolecular separation of AsI3 units decreases, new bonds form, and the environment around arsenic becomes similar to that of bismuth in hcp BiI3.28 When the metal center is in this more symmetric (i.e., more solution-like) environment at the moment of impact, the C3 isomer would presumably form faster than when the metal center is in the more anisotropic form at atmospheric pressure.
That this is not an unrealistic scenario reflects the fact that in ball milling experiments the impacts between balls or a between ball and the jar create a small area of high pressure on the powder trapped within the collision; this pressure can be on the order of gigapascals (Maurice and Courtney reported 2–4 GPa in their experiments).29 Additionally, ball milling has been shown to induce phase transformations in particles at lower temperatures30 or pressures31 than reported for bulk materials. The high level of shear forces and structural defects that occur in ball milling experiments lead to these depressed transition conditions.31a A related phase transformation under pressure has been reported for SbI3 (>1.4 GPa).32
In the formation of
, small grinding balls regularly give higher C1
:
C3 ratios than the larger balls. This trend is consistent with that of the jar material, in that lower energy collisions (with smaller balls) lead to more of the C1 diastereomer than C3. Emmerling and coworkers have found a linear correlation between the mass of a single ball and the reaction rate, even when the total mass of the balls is the same.4c Our data are consistent with this trend.33
complexes is not currently known, although since {A′}2 is a major decomposition product, it is likely that the compounds undergo homolytic E–C bond cleavage to form ˙A′ radicals, which couple to form {A′}2. Similar decomposition does not occur in solution at temperatures up to 90 °C, a thermal environment comparable to the energetics reached in a mixer mill (Fig. 8).34 Hence it appears that this is a mechanochemically specific mode of decomposition, perhaps driven by transient build-up and relaxation of strain.35 The fact that the C1
:
C3 ratio decreases during decomposition suggests that the C1 form is decomposing more quickly than the more symmetric C3 diastereomer. Although this point is not certain, the fact that the C1 forms of both
and
are crystalline solids at room temperature, whereas the C3 isomer of
is a liquid at room temperature and that for
is a near-liquid/oil5 may mean that the C3 conformations are not subject to the same levels of compressive stress that the more rigid C1 forms are.
In addition to the use of layered solids, anisotropy could potentially be introduced into mechanochemical environments in other ways, such as with solid additives or liquid crystals in LAG.36 We are continuing to explore these possibilities.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d4mr00001c |
| This journal is © The Royal Society of Chemistry 2024 |