Molecular reorientation and shear viscosity in dense liquids

Probing transport and microheterogeneous solvent structure in acetonitrile-water mixtures and reversed-phase chromatographic media by NMR quadrupole relaxation

Mixtures of CH(3)CN and H(2)O are the predominant solvent systems used in reversed-phase liquid chromatographic (RPLC) separations, as well as in a multitude of other applications. In addition, acetonitrile is the simplest model for an amphiphilic molecule possessing both organic and polar functional groups. Although many studies have focused on this solvent system, the general nature of the intermolecular interactions are not fully understood, and a microscopic description of the proposed microheterogeneity that exists is still not clearly established. In the present study, we measure the spin-lattice relaxation times (T(1)) of (14)N to determine reorientational correlation times (tau(c)) of CH(3)CN-H(2)O solvent mixtures over the entire binary composition range and at temperatures ranging from 25.0 to 80.0 degrees C. At all compositions, the microscopic observable, tau(c), is found to be directly proportional to the macroscopic solution viscosity when scaled for temperature (eta/T). This indicates that for a constant composition, this system's dynamics are well described by hydrodynamic theory on a microscopic level. These results suggest that under appropriate conditions, the measurement of changes in quadrupolar relaxation times is a reliable means of determining changes in solution viscosity. We stress the importance of this approach in systems not amenable to traditional viscosity measurements, such as those having species in interfacial regions. This approach is used to examine the changes in the interfacial solution viscosity of CH(3)CN-H(2)O mixtures in contact with a commercially available C(18)-bonded stationary phase. The measurements indicate that CH(3)CN is motionally hindered at the stationary phase surface. The surface affected CH(3)CN has a larger dependence of tau(c) on temperature than the bulk CH(3)CN, indicating greater changes in the interfacial viscosity as a function of temperature. Additionally, the bulk relaxation data show direct correlations to existing models of proposed regions of structure for CH(3)CN-H(2)O mixtures. Using a microscopic hydrodynamic approach, we show that, quite unexpectedly, each of the experimentally determined parameters in the viscosity correlation plots change simultaneously, and we propose that these are indicative of changes in the distribution of species for this microheterogeneous liquid system. Although distinct regions for the onset of microheterogeneity have previously been proposed, within the framework of a microscopic hydrodynamic model and the recently proposed model of Reimers and Hall,(1) the present data support the existence of a microheterogeneous solvent structure that varies continuously over the full range of temperatures and compositions examined.

Structural, computational, and (59)Co NMR studies of primary and secondary amine complexes of Co(III) porphyrins

Four novel low-spin bis(amine) Co(III) porphyrins [Co(TPP)(BzNH(2))(2)](SbF(6)), 1, [Co(TPP)(1-BuNH(2))(2)](SbF(6)), 2, [Co(TPP)(PhCH(2)CH(2)NH(2))(2)](SbF(6)), 3, and [Co(TPP)(1-MePipz)(2)](SbF(6)), 4, have been synthesized and characterized by low-temperature X-ray crystallography, IR, electronic, and NMR ((1)H, (13)C, and (59)Co) spectroscopy. The mean Co-N(p) distance for the four structures is 1.986(1) A. The Co-N(ax) distances for the 1 degrees amine derivatives average to 1.980(5) A; the axial bonds of the 2 degrees amine derivative are significantly longer, averaging 2.040(1) A. The porphyrin core conformation of 4 is significantly nonplanar (mixture of S(4)-ruf and D(2d)-sad distortions) due to a staggered arrangement of the axial ligands over the porphyrin core and meso-phenyl group orientations < 90 degrees. The X-ray structures have been used with the coordinates for [Co(TPP)(Pip)(2)](NO(3)) (Scheidt et al. J. Am. Chem. Soc. 1973, 95, 8289-8294.) to parametrize a molecular mechanics (MM) force field for bis(amine) complexes of Co(III) porphyrins. The calculations show that two types of crystal packing interactions (van der Waals and hydrogen bonding) largely control the crystallographically observed conformations. Gas phase conformational energy surfaces have been computed for these complexes by dihedral angle driving methods and augmented with population distributions calculated by MD simulations at 298 K; the calculations demonstrate that the bis(1 degrees amine) complexes are significantly more flexible than the bis(2 degrees amine) analogues. (59)Co NMR spectra have been acquired for a range of [Co(TPP)(amine)(2)]Cl derivatives as a function of temperature. The (59)Co chemical shifts increase linearly with increasing temperature due to population of thermally excited vibrational levels of the (1)A(1) ground state. Activation energies for molecular reorientation (tumbling) have been determined from an analysis of the (59)Co NMR line widths as a function of 1/T; lower barriers exist for the conformationally rigid 2 degrees amine derivatives (2.6-3.8 kJ mol(-1)). The (59)Co chemical shifts vary linearly with the DFT-calculated radial expectation values <r(-3)>(3d) for the Co(III) ion. The correlation leads to the following order for the sigma-donor strengths of the axial ligands: BzNH(2) > or = Cl(-) > 1-BuNH(2) > PhCH(2)CH(2)NH(2) > 1-Bu(2)NH > Et(2)NH. The (59)Co NMR line widths are proportional to the square of the DFT-calculated valence electric field gradient at the Co nucleus. Importantly, this is the first computational rationalization of the (59)Co NMR spectra of Co(III) porphyrins.