Influence of the temperature-dependent dielectric constant on the H/D isotope effects on the NMR chemical shifts and the hydrogen bond geometry of the collidine-HF complex in CDF3/CDClF2 solution
Ig. Shenderovich et al., Influence of the temperature-dependent dielectric constant on the H/D isotope effects on the NMR chemical shifts and the hydrogen bond geometry of the collidine-HF complex in CDF3/CDClF2 solution, MAGN RES CH, 39, 2001, pp. S91-S99
The influence of solvent polarity on the properties of hydrogen-bonded 1:1
complexes of 2,4,6-trimethylpyridine-N-15 with HF and DF, labeled below as
FHN and FDN, has been studied by multinuclear magnetic resonance spectrosco
py in the slow hydrogen bond exchange regime reached below 190 K. Mixtures
of CDF3/CDClF2 were employed as solvent, which is liquid down to 90 K. In o
rder to evaluate their polarity, the static dielectric constants so of the
CHF3, CHClF2 and of the binary 1: 1 mixture were measured from 160 K down t
o 90 K. A strong increase of so from 14 at 190 K to 38 at 103 K is observed
for the mixtures used in the NMR measurements. Upon cooling, i.e. increase
of the dielectric constant, the NMR spectra indicate a gradual transformat
ion of an asymmetric molecular complex F-H . . .N to a quasi-symmetric comp
lex Fdelta-. . .H . . .Ndelta+ and eventually to a more or less zwitterioni
c species F-. . .H-N+. These changes are not only manifested in the scalar
couplings J(H-1, F-19) and J(H-1, N-15) but also lead to characteristic pri
mary and secondary H/D isotope effects on the chemical shifts of the hydrog
en bonded nuclei. Whereas the primary isotope chemical shift effect (p)Delt
a (D/H) equivalent to delta ((FHN)-H-2) - delta ((FHN)-H-1) = -0.2 ppm is n
egative at 190 K and in agreement with an asymmetric hydrogen bond in the m
olecular complex, it changes its sign when the temperature is lowered, goes
through a maximum of +0.27 ppm at epsilon (o) approximate to 22 and finall
y decreases again. The positive value of PA(D/H) is in agreement with D mor
e confined to the hydrogen bond center compared with H, which constitutes a
fingerprint of a quasi-symmetric hydrogen bond involving a single well pot
ential for the proton motion. The quasi-symmetric complex is further charac
terized by the following NMR parameters, J(H-1, F-19) = 30 Hz, J(H-1,N-15)
= -50 Hz, J(F-19, N-15) = -96 Hz, delta ((FHN)-H-1) = 20.0 ppm, delta((FHN)
-F-19) = -114.2 ppm, delta ((FHN)-N-15) = -63.5 ppm, and the one-bond H/D-i
sotope effects delta ((FHN)-H-2) - delta ((FHN)-H-1) = +0.27 ppm, delta((FD
N)-F-19) - delta((FHN)-F-19) = 1.4 ppm and delta ((FDN)-N-15) - delta ((FHN
)-N-15) = -3.4 ppm. Copyright (C) 2001 John Wiley & Sons, Ltd.