A. C. Sather et al. / Tetrahedron Letters 52 (2011) 2100–2103
2103
Figure 7. The thermal decomposition of N-benzylnitrosoamide 4 in the presence of 1. All starting material remains after 144 h at 35 °C. Free guest 4 is indicated by a red
circle.
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signals disappear as the guest is released to the bulk solution (see
Supplementary data). After heating at 35 °C for ꢀ63 h all of the
signals corresponding to the guest disappear from the 1H NMR
89, 165.
spectrum and signals corresponding to ester can be observed
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In conclusion, encapsulated N-nitrosoamides behave differently
than those in bulk solution. Inside the capsule, the host restricts
the elongation of the guests and prevents the rearrangement reac-
tion. Guest 2 does not react inside the capsule although there is
enough room to accommodate the longer (by two carbon atoms)
hexyl guest 3. The physical constraints of the capsule either pre-
vent the breakdown of the diazoester intermediate (I) or, more
likely, keep it from forming altogether. We were able to free encap-
sulated guests by the addition of methanol, restoring their reactiv-
ity. Guest 4 also shows no reactivity while encapsulated in 1, as
was the earlier case with dibenzoyl peroxide.14 By surrounding
N-nitrosoamides we were able to turn off their reactivity and sta-
bilize them at elevated temperatures.
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11. Usually, guests are added to a suspension of the capsule and heated to give a
solution. However in this case, the guests are sensitive to heat, so the
suspensions were sonicated for about 30 min and then placed in an oil bath
between 30 and 35 °C overnight. After this period of time the suspensions
became solutions and all of the guest was taken up by the host. During this
brief induction period, the guest that is in the bulk solution can react giving
rise to a small background reaction.
Acknowledgments
We are grateful to the Skaggs Institute for support. A.C.S. is a
Skaggs Pre-doctoral Fellow. O.B.B. thanks the NIGMS (GM 27953)
for financial support. A postdoctoral fellowship for O.B.B. was
provided by NIH (F32GM087068).
Supplementary data
Supplementary data associated with this article can be found, in
12. DFT calculations were performed with the Gaussian 09, Revision A.1 program
using Ab initio gas phase energy minimization at the Hartree–Fock (HF) level.
(HF/6-31G*) was carried out on each structure, with ‘tight’ convergence
optimization criterium.
References and notes
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14. Körner, S. K.; Tucci, F. C.; Rudkevich, D. M.; Heinz, T.; Rebek, J., Jr. Chem. Eur. J.
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