An
integrated thermodynamic and kinetic study was carried out to
clarify how the formation of ionic aggregates higher than ion pairs
affects the rate of olefin insertion into the Zr–C bond. To
this aim, the reaction with olefin of three-member zirconaziridium
metallacycles [Cp2Zr(η2-CH2-N(R)2)]+[X]− [R = C18H37; X– = MeB(C6F5)3
– (1BN) or B(C6F5)4
– (1BT)], models for tight (t-ISIP, 1BN) and loose (l-ISIP, 1BT) inner sphere ion pair (ISIPs), was studied at different
levels of concentration and thus self-aggregation. Both 1BN and 1BT undergo a regioselective insertion of a single
α-olefin molecule (1-hexene or 2-Me-1-heptene) into the Zr–C
bond to form the corresponding five-member metallacycles outer sphere
ion pairs (2BN, 2BT, 3BN, and 3BT), with no evidence for further olefin insertions. Under
comparable experimental conditions, where monomeric ion pairs dominate
(aggregation number N ≈ 1), the apparent rate
constant (k
app) of 1-hexene insertion
into 1BT is about 200 times higher than that in 1BN, in agreement with the weaker strength of cation–anion
interaction in the former. For 1BT, k
app is only marginally affected by the self-aggregation
level in all investigated experimental conditions. For example, k
app = 1.1 M–1 s–1 (N ≈ 1.1) and 1.3 (N ≈
4.8) for the insertion reaction of 1-hexene in toluene at 223 K and
range from 19 × 10–3 M–1 s–1 (N ≈ 1.5) to 10 × 10–3 (N ≈ 39) for the insertion
of 2-Me-1-heptene in methylcyclohexane at 258 K. On the contrary, k
app is markedly dependent on self-aggregation
in the case of 1BN. For instance, when 1BN is reacted with 1-hexene in methylcyclohexane at 258 K, k
app increases more than 1 order of magnitude,
from 6 × 10–3 to 93 × 10–3 M–1 s–1, upon increasing the
aggregation level from N ≈ 1 ([1BN] = 6 × 10–5 M) to N ≈
4.6 ([1BN] = 12.8 × 10–3 M). Although
the insertion of 1-hexene in 1BN is faster in the slightly
more polar solvent toluene (k
app = 39
× 10–5 M, N ≈ 1), the
relative reactivity difference between ion pairs and larger ionic
aggregates is similar in both solvents (about 4× and 3×
increment, on passing from N ≈ 1.0 to N ≈ 1.6, in methylcyclohexane and toluene, respectively).
The addition of an inert external salt with a common counterion (2BN) to solution of 1BN dramatically raises the
olefin insertion rate constant: at [1BN] = 6 × 10–5 M, k
app increases from
6 × 10–3 M–1 s–1, in the absence of 2BN, to 42 × 10–3, 90 × 10–3, and 166 × 10–3 M–1 s–1 in the presence of 1,
3, and 5 equiv of 2BN, respectively. All of the thermodynamic
and kinetic data can be rationalized by taking into account the strength
of cation–anion interaction in the two kinds of ion pairs.
In t-ISIPs, the cation–anion interaction energy is relatively
strong, resulting in a relatively small dipole moment and a little
thermodynamic tendency to self-aggregate. However, under conditions
where homo (or mixed) ion aggregates form, an additional weakening
of the cation–anion interaction occurs, causing a substantial
increase of the intrinsic reactivity of each t-ISIP within aggregates.
On th...