PROTEIN ROTATIONAL RELAXATION AS STUDIED BY SOLVENT H-1 AND H-2 MAGNETIC-RELAXATION
PROTEIN ROTATIONAL RELAXATION AS STUDIED BY SOLVENT H-1 AND H-2 MAGNETIC-RELAXATION
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DOI:
10.1021/bi00664a019
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发表时间:
1976-01-01
期刊:
影响因子:
2.9
通讯作者:
KOENIG, SH
中科院分区:
文献类型:
--
作者:
HALLENGA, K;KOENIG, SH
Earlier studies of the magnetic field dependence of the nuclear spin magnetic relaxation rate of solvent protons in solutions of diamagnetic proteins have indicated that this dependence (called relaxation dispersion) is related to the rotational Brownian motion of solute proteins. In essence the dispersion is such that 1/T1 (the proton spin-lattice relaxation rate) decreases monotonically as the magnetic field is increased from a very low value (.apprx. 10 Oe [oerstedt]); the dispersion has a point of inflection at a value of magnetic field which depends on protein size, shape, concentration, temperature and solvent composition. The value of the proton Larmor precession frequency .nu.c at the inflection field appears to relate to .tau.R, the rotational relaxation time of the protein molecules. Proton relaxation dispersions were measured for solutions of various proteins that span a three-decade range of molecular weights, and for 1 sample of tRNA. Deuteron relaxation dispersions were also measured for solutions of 3 proteins: lysozyme, carbonmonoxyhemoglobin and Helix pomatia hemocyanin with MW 900,000. A quantitative relationship between both proton and deuteron disperson data and protein rotational relaxation is confirmed, and the point is made that magnetic disperson measurements are of very general applicability for measuring the rotational relaxation rate of macromolecules in solution. It has been previously shown that the influence of proton motion on the relaxation behavior of the solvent is not due to exchange of solvent molecules between the bulk solvent and a hydration region of the protein. The present paper suggests that the interaction results from a long range hydrodynamic effect fundamental to the situation of large Brownian particles in an essentially continuum fluid. The general features of the proposed mechanism are indicated, but no theoretical computations are presented.