Intermolecular protein interactions in solutions of bovine lens beta L-crystallin. Results from 1/T1 nuclear magnetic relaxation dispersion profiles

Proton exchange as a relaxation mechanism for T1 in the rotating frame in native and immobilized protein solutions

T1 relaxation in the rotating frame (T1rho) is a sensitive magnetic resonance imaging (MRI) contrast for acute brain insults. Biophysical mechanisms affecting T1rho relaxation rate (R1rho) and R1rho dispersion (dependency of R1rho on the spin-lock field) were studied in protein solutions by varying their chemical environment and pH in native, heat-denatured, and glutaraldehyde (GA) cross-linked samples. Low pH strongly reduced R1rho in heat-denatured phantoms displaying proton resonances from a number of side-chain chemical groups in high-resolution 1H NMR spectra. At pH of 5.5, R1rho dispersion was completely absent. In contrast, in the GA-treated phantoms with very few NMR visible side chain groups, acidic pH showed virtually no effect on R1rho. The present data point to a crucial role of proton exchange on R1rho and R1rho dispersion in immobilized protein solution mimicking tissue relaxation properties.

1H-NMRD and 17O-NMR assessment of water exchange and rotational dynamics of two potential MRI agents: MP-1177 (an extracellular agent) and MP-2269 (a blood pool agent)

The parameters that govern water proton magnetic relaxation (e.g. water exchange rates, and rotational and electronic correlation times) of representatives of two classes of Gd(III) complexes have been estimated, using two different approaches and the results compared with those derived for known analogs. The complexes studied are: (i) the non-ionic GdDTPA-bis(-methoxyethyl-amide) [Gd(DTPA-BMEA)], a typical small-molecule extracellular MR agent, and (ii) the ionic Gd(III) complex of 4-pentylbicyclo[2.2.2]octane-1-carboxyl-di-L-aspartyl-lysine-deriv ed-DTPA [GdL]4-, a prototype MR blood pool agent, which binds to serum albumin in vivo through non-covalent hydrophobic interactions. An 17O-NMR study of [Gd(DTPA-BMEA)] gives a water exchange rate constant of k(ex)298 = (0.39 +/- 0.02) x 10(6) s(-1), identical to that for the bismethylamide analog [Gd(DTPA-BMA)]. Both approaches yield longer rotational correlation times for [Gd(DTPA-BMEA)], consistent with its higher molecular weight. An 17O-NMR study of [GdL]4- gives a water exchange rate constant of k(ex)298 = (4.2 +/- 0.1) x 10(6) s(-1), identical to that for [Gd(DTPA)]2-. The water exchange rate on [GdL]4- did not decrease considerably when bound to albumin, the lowest limit is k(ex,GdL-BSA) = k(ex,GdL)/2. Both approaches yield identical rotational correlation times for [GdL]4-, however, it was difficult to derive a consistent rotational constant for the albumin-bound [GdL]4- using the different approaches (values ranged between 1.0 and 23.0 ns).

Classes of hydration sites at protein-water interfaces: the source of contrast in magnetic resonance imaging

Immobilized protein solute, approximately 20 wt %, alters the longitudinal and transverse nuclear magnetic relaxation rates 1/T1 and 1/T2 of solvent water protons in a manner that makes their values indistinguishable from those of a typical human tissue. There is now a quantitative theory at the molecular level (S.H. Koenig and R. D. Brown III (1993) Magn. Reson. Med. 30:685-695) that accounts for this, as a function of magnetic field strength, in terms of several distinguishable classes of water-binding sites at the protein-water interface at which significant relaxation and solute-solvent transfer of proton Zeeman energy occur. We review the arguments that these several classes of sites, characterized by widely disparate values of the resident lifetimes tau M of the bound waters, are associated with different numbers of hydrogen bonds that stabilize the particular protein-water complex. The sites that dominate relaxation-and produce contrast in magnetic resonance imaging (MRI), which derives from 1/T1 and 1/T2 of tissue water protons-have tau M approximately 10(-6)s. These, which involve four hydrogen bonds, occupy < or = 1% of the protein-water interface. Sites that involve three bonds, although more numerous, have < or = 20% smaller intrinsic effect on relaxation. The greater part of the "traditional" hydration monolayer, with even shorter-lived hydrogen-bonded waters, has little influence on solvent relaxation and is relatively unimportant in MRI. Finally, we argue, from the data, that most of the protein of tissue (a typical tissue is mostly protein) must be rotationally immobile (with Brownian rotational relaxation times slower than that of a 5 x 10(7) Da (very heavy) globular protein). We propose a functional basis for this immobilization ("cytoplasmic order"), and then indicate a way in which this order can break down ("cytoplasmic chaos") as a result of neoplastic transformation (cancer) and alter water-proton rates of pathological tissue and, hence, image contrast in MRI.

Reduced chaperone-like activity of alpha A(ins)-crystallin, an alternative splicing product containing a large insert peptide

alpha-Crystallin is a multimeric protein complex which is constitutively expressed at high levels in the vertebrate eye lens, where it serves a structural role, and at low levels in several non-lenticular tissues. Like other members of the small heat shock protein family, alpha-crystallin has a chaperone-like activity in suppressing nonspecific aggregation of denaturing proteins in vitro. Apart from the major alpha A- and alpha B-subunits, alpha-crystallin of rodents contains an additional minor subunit resulting from alternative splicing, alpha A(ins)-crystallin. This polypeptide is identical to normal alpha A-crystallin except for an insert peptide of 23 residues. To explore the structural and functional consequences of this insertion, we have expressed rat alpha A- and alpha A(ins)-crystallin in Escherichia coli. The multimeric particles formed by alpha A(ins) are larger and more disperse than those of alpha A, but they are native-like and display a similar thermostability and morphology, as revealed by gel permeation chromatography, tryptophan fluorescence measurements, and electron microscopy. However, as compared with alpha A, the alpha A(ins)-particles display a diminished chaperone-like activity in the protection of heat-induced aggregation of beta low-crystallin. Our experiments indicate that alpha A(ins)-multimers have a 3-4-fold reduced substrate binding capacity, which might be correlated to their increased particle size and to a shielding of binding sites by the insert peptides. The structure-function relationship of the natural mutant alpha A(ins)-crystallin may shed light on the mechanism of chaperone-like activity displayed by all small heat shock proteins.

Light scattering by bovine alpha-crystallin proteins in solution: hydrodynamic structure and interparticle interaction

We have studied diluted bovine eye lens alpha-crystallin solutions by using light scattering. The protein particles were modeled as hard spheres, showing electrostatic repulsion, due to surplus electric charges, and weak attractive interaction. The repulsive potential VR is defined by the radius of the particles, the Debye length kappa-1, and the number of charges at the Gouy layer; the attractive potential has been described by the London-van der Waals potential and is defined by the Hamaker constant A. We have used the diluted gas approximation and the one component macrofluid model to relate the experimental static factor Ki to the theoretical expression of the interaction potential V(x). This resulted in a Hamaker constant A of 0.06 +/- 0.01 KBT and an effective charge q ranging from 18 +/- 1 at low ionic strength (omega = 0.0022 M) to 50 +/- 5 at high ionic strength (omega = 0.1472 M).

A molecular theory of relaxation and magnetization transfer: application to cross-linked BSA, a model for tissue

Homogeneous soft tissue, as regards its magnetic relaxation properties, is well-modeled by solutions of cross-linked protein (see Koenig and Brown, Prog. NMR Spectr. 22, 487 (1991)). Interactions at the solute-solvent interface alter the hydrodynamics of solvent water, and also couple the solute and solvent proton Zeeman energy reservoirs, giving hydrodynamic and cross-relaxation contributions to water proton relaxation that respond differently to deuteration of solvent. We report measurements of the magnetic field dependence of 1/T1 of water protons in cross-linked bovine serum albumin (BSA), for partially deuterated solvent and, in order to separate these two contributions, of 1/T1 of deuterons. The major experimental finding is that, in addition to recently identified water-binding sites on protein (covering approximately 0.2% of the surface) with water lifetimes of about 1 microsecond, there is another group of sites with lifetimes of about 23 ns, covering approximately 2% of the surface, which are evident in both proton and deuteron data. In addition, we have formulated a theory of interfacial proton-proton magnetic interactions which--with these four parameters, plus two that quantify the protein-water coupling at each site--can account for all the proton and deuteron data, in both native and cross-linked BSA.