CLOSED-SHELL ION-PAIR STRUCTURE AND DYNAMICS - STEADY-STATE H-1(H-1),B-10(H-1, AND B-11(H-1) NUCLEAR OVERHAUSER EFFECTS AND B-10, B-11 NUCLEAR-RELAXATION OF TETRAALKYLAMMONIUM TETRAHYDRIDOBORATES IN ION-PAIRING AND DISSOCIATIVE SOLVENTS
Tc. Pochapsky et al., CLOSED-SHELL ION-PAIR STRUCTURE AND DYNAMICS - STEADY-STATE H-1(H-1),B-10(H-1, AND B-11(H-1) NUCLEAR OVERHAUSER EFFECTS AND B-10, B-11 NUCLEAR-RELAXATION OF TETRAALKYLAMMONIUM TETRAHYDRIDOBORATES IN ION-PAIRING AND DISSOCIATIVE SOLVENTS, Journal of the American Chemical Society, 115(24), 1993, pp. 11084-11091
The magnitudes of selective steady-state H-1{H-1} interionic nuclear O
verhauser effects (NOEs) and nonselective B-10{H-1} and B-11{H-1} NOEs
as well as B-10 and B-11 spin-lattice relaxation times were measured
for solutions of (butyl)4N+,BH4- 1a in (HCCl3)-H-2, (H2O)-H-2, and [H-
2(6)]dimethyl sulfoxide. Interionic NOEs resulting from the selective
saturation of cationic alkyl resonances were used to evaluate the time
average structure of the ion pair la in various solvents. The largest
NOEs are observed in (HCCl3)-H-2, while smaller specific interionic N
OEs were observed in [H-2(6)]-dimethyl sulfoxide and [H-2(6)]benzene.
Only small nonspecific interionic NOEs were observed in (H2O)-H-2 Solu
tions of 1a. B-10 and B-11 T1 relaxation times and nonselective steady
-state B-10{H-1} and B-11{H-1} NOEs were also measured for solutions o
f NaBH4 2 in 2H2O and [H-2(6)]dimethyl sulfoxide in order to determine
the effect of counterion on observed relaxation behavior for BH4-. Di
polar and quadrupolar contributions to observed spin-lattice relaxatio
n of both boron nuclei were calculated. B-10{H-1} and B-11{H-1} NOEs o
btained upon broad-band presaturation of H-1 resonances were in all ca
ses similar to the values predicted from dipolar contributions to B-10
and B-11 relaxation. Quadrupolar coupling constants of 5.2 x 10(5) Hz
for B-10 and 2.5 x 10(5) Hz for B-11 in the BH4- anion were calculate
d. Quadrupolar contributions to boron relaxation in ion pair la correl
ate with measured solution viscosity as a function of temperature unde
r ion pairing conditions, but interionic H-1{H-1} NOEs do not, showing
a negative deviation from intensity expected as a result of viscosity
. Increasing the size of the cation increases the deviation. It is con
cluded that magnitude and sign of interionic NOEs reflect the motion o
f the ion pair as a unit, and hence the effects of multiion aggregatio
n, while the relaxation of the boron nucleus reflects more rapid motio
n independent of the ion pair. The correlation time of the interionic
vector is used to predict a lower limit on the mean lifetime of a disc
rete ion binding mode.