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Me3SiNHBn (16) with Ph2SiH2 to afford Me3SiN(Bn)SiHPh2 (17),
followed by coupling with BnNH2.[42]
one THF for an amine molecule and evolves through a meta-
thesis-type transition-state (TS) structure to deliver intermedi-
ate CI2·(T)2·RSi featuring a barium-bound H2C(SiMe3)2 moiety.
Its rapid displacement by another amine molecule prepares for
protonolytic cleavage of the second BaꢀC alkyl bond through
a similar metathesis-type TS structure that decays thereafter
into C2 with the rapid release of H2C(SiMe3)2 and THF. The Baꢀ
C alkyl bond protonolysis has an affordable barrier of 16.7 kcal
molꢀ1 (for aminolysis of the first BaꢀC bond, see Figure S18) to
overcome and is driven by a huge thermodynamic force that
amounts to 35.3 kcalmolꢀ1. Thus, one can safely conclude that
barium bis-alkyl C1·(T)3 is likely converted irreversibly in a quan-
titative fashion by 4Me into the competent barium bis-silazanyl
amido compound C2.
It has been shown above that 4 exhibits a distinct reactivity
pattern under varying experimental conditions, on the one
hand, when generated under conditions of CDC catalysis
(hence in the presence of benzylamine), or alternatively in the
absence of any amine substrate other than 4. Thus, we
deemed it instructive to study the aminolysis of C1·(T)3 by
NH2Bn and the conversion of the thus formed barium bis-ben-
zylamido C3 into C2 as well. The sequential protonolytic dis-
placement of a hydrocarbyl with an amido group by either 4Me
or NH2Bn, share structural features and similar energy profiles.
For the less encumbered primary NH2Bn, the most accessible
pathway (see Figure S22, but also Figures S21, S23, S24 in the
Supporting Information) proceeds after the initial displacement
of all three THF molecules by amine with a moderate overall
barrier of 7.5 kcalmolꢀ1 to engage thereafter in the cleavage of
the remaining BaꢀC bond. This affords the NH2Bn adduct
C3·(Am)3 of the barium bis-benzylamido compound. Overall,
the conversion of starting material C1·(T)3 in the presence of
The benzene-releasing cyclisation from 4 to 5 is not specific
to barium precatalysts; it is also catalysed by, for instance,
Ca[CH(SiMe3)2]2·(THF)2 (B), the calcium analogue of A. In a con-
trol experiment performed under otherwise identical experi-
mental conditions ([4]0/[precatalyst]0 =20:1, 608C in benzene,
[precatalyst]0 =10 mm), B catalyses the reaction at a rate very
comparable to that of A, kobs =9.16ꢁ0.3ꢂ10ꢀ6 sꢀ1 and 1.98ꢁ
0.1ꢂ10ꢀ5 sꢀ1, respectively. Eyring analyses in the temperature
range 328–353 K (five data points) allowed for the calculation
of the activation parameters for B, DH° =16.8ꢁ0.1 kcalmolꢀ1
and DS° =ꢀ22.3ꢁ0.1 calmolꢀ1 Kꢀ1, with DG° =23.4ꢁ0.1 kcal
molꢀ1 at 298 K. This final value replicates that for A, but the re-
spective enthalpic and entropic contributions are very differ-
ent. Due to its much smaller size compared to barium (effec-
tive rionic for C.N.=6: Ca2+, 1.00 ꢃ; Ba2+, 1.38 ꢃ), calcium has
a greater entropic factor that becomes unfavourable as the
temperature of the reaction is increased. The energy of activa-
tion determined by Arrhenius analysis is actually lower for the
calcium precatalyst B (Ea =17.5ꢁ0.1 kcalmolꢀ1; R2 =0.9938)
than for the barium A (Ea =21.3ꢁ0.2 kcalmolꢀ1; R2 =0.9928).
Computational investigations
A reliable state-of-the-art density functional theory (DFT)
method has been employed to complement the mechanistic
studies reported above with an aim to further enhance our un-
derstanding of mechanistic intricacies behind the generation
of cyclodisilazanes. We have examined various mechanistic
pathways conceivable for the conversion of disilazane 4 into
the 4-membered cyclodisilazane 5 by the barium precatalyst A
(denoted C1·(T)3 hereafter). For the disilazane, the two silicon-
bound phenyl spectator groups have been replaced by methyl
ones (4Me) for the sole purpose of expediting computations,
but no further simplifications of any kind have been imposed
for any of the key species involved. The computational meth-
odology employed (dispersion-corrected B97-D3 in conjunc-
tion with triple-z basis sets and a sound treatment of bulk sol-
vent effects; see the computational methodology in the Sup-
porting Information) adequately simulated the authentic reac-
tion conditions and has been demonstrated before to reliably
map the free-energy landscape of alkaline earth-mediated hy-
droelementation reactions.[15,43] This has allowed mechanistic
conclusions with substantial predictive value to be drawn.
We started with an examination of the BaꢀC alkyl bond ami-
nolysis at starting material C1·(T)3 (ꢂA) by 4Me, thereby trans-
forming C1·(T)3 into the related [Ba{N(Bn)SiMe2N(Bn)SiMe2Ph}2]
barium bis-amido compound C2, which is likely competent to
trigger the 4Me!5Me conversion. The activation of C1·(T)3 en-
tails that amine binds initially at barium. Several pathways,
which are distinguished by the number of THF molecules to
remain bound at barium, have been examined. The most ac-
cessible case (Figure S18) together with the complete account
of all the studied pathways (Figure S17–S20) can be found in
the Supporting Information. The energetically prevalent path-
way for BaꢀC alkyl bond aminolysis sees the first exchange of
4
Me or NH2Bn into the respective barium bis-amido compounds
is found affordable kinetically and strongly downhill, driven by
a thermodynamic force of comparable substantial amount.
For the experimental setup of CDC catalysis to be applied,
the barium bis-benzylamido, which is predominantly present
as amine adduct C3·(Am)3, is likely representing the catalyst
resting state.[15] Hence, under such conditions, C3 needs first to
be converted into C2 to proceed along the various conceivable
avenues that lead to the formation of the cyclodisilazane. In-
terestingly, the sequential exchange of benzylamido by silazan-
yl amido appears to be equally kinetically viable, featuring an
overall activation energy of 11.3 kcalmolꢀ1. This barrier is
linked to aminolysis of the first BaꢀN amido bond, along the
energetically prevalent pathway (see Figure S26 but also Figur-
es S25, S27, S28 in the Supporting Information) that proceeds
from the bis-silazane adduct C3·(4Me)2. However, the thermody-
namic force associated with the overall transformation of C3
into C2 is found strikingly different to the findings for starting
material C1·(T)3. The huge negative reaction free energy pre-
dicted there is indicative of an irreversible and essentially
quantitative conversion of C1·(T)3 into the respective barium
bis-amido compounds. This is in sharp contrast to the process
here, which does not benefit from a massive thermodynamic
driving force, but is rather thermoneutral with C3·(Am)3QC2
likely in a mobile equilibrium that does not favour C2 over C3.
Chem. Eur. J. 2016, 22, 1 – 12
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