Amine-substituted [s]-triazines display hindered rotation
around
the triazine-N bond. While this barrier, ΔG
‡, has been measured to be between 15.1 and 17.7
kcal/mol for neutral triazines, the impacts that solvent and protonation
state have not been addressed. Using a dimethylamine substituent as
a reporter, ΔG
‡ was measured
to be 17.5–19.3 kcal/mol upon protonation across a range of
solvents (D2O, DMSO-d
6, MeCN-d
3, MeOD-d
4, tetrahydrofuran-d
8, trifluoroethanol-d
3). Furthermore, ΔG
‡ increases
as the solvent dielectric decreases (p < 0.01).
This trend is consistent with the role that solvent plays in stabilizing
the increased charge density on the triazine ring resulting from a
loss of conjugation with the dimethylamine substituent. Across these
solvents, ΔG
‡ for the neutral
molecule is smaller by ∼2–3 kcal/mol, ranging from 15.3–16.1
kcal/mol. In pyridine, ΔG
‡ does not correlate with the solvent dielectric for the “protonated”
model. The lower barrier is attributed to competitive protonation:
the pK
a of the protonated triazine (∼6)
is similar to that of protonated pyridine-d
5 (5.8). As additional acid is added, ΔG
‡ increases. Adding additional acid to the protonated
model in D2O or DMSO-d
6 does
not significantly affect ΔG
‡.