NMR spin grouping and correlation exchange analysis. Application to low hydration NaDNA paracrystals.

The NMR spin-grouping technique is applied to low hydration oriented fibers of NaDNA to study the role of exchange in determining the apparent (observed) spin relaxation of the system. The analysis proceeds in three steps: first, the apparent proton relaxation is measured at high fields, with both selective and nonselective inversion pulse sequences, and in the rotating frame. The spin-grouping technique is used in all spin-lattice relaxation measurements to provide the optimum apparent relaxation characterization of the sample. Next, all apparent results are analyzed for exchange. In this analysis the results from the high field and rotating frame experiments (which probe the exchange at two different time scales) are correlated to determine the inherent (or true) spin relaxation parameters of each of the proton groups in the system. The results of selective inversion T1 measurements are also incorporated into the exchange analysis. Finally, the dynamics of each spin group are inferred from the inherent relaxation characterization. The low hydration NaDNA structure is such that the exchange between the protons on the water and those on the NaDNA is limited, a priori, to dipolar mixing. The results of the exchange analysis indicate that the dipolar mixing between water and NaDNA protons is faster than the spin diffusion within the NaDNA proton group itself. The spin-diffusion on the macromolecule is the bottleneck for the exchange between the water protons and the NaDNA protons. The water protons serve as the relaxation sink both at high fields and in the rotating frame for the total NaDNA-water spin bath. The inherent relaxation of the water is characteristic of water undergoing anisotropic motion with a fast reorientational correlation time about one axis (5 X 10(-10) less than or equal to tau r less than or equal to 8 X 10(-9)S) which is about three orders of magnitude slower than that of water in the bulk; and a slow tumbling correlation time for this axis (1.5 x 10(-7) less than or equal to tau t less than or equal to 8 x 10(-7)S) which is two orders of magnitude slower yet.     

14N1H and 2H1H cross-relaxation in hydrated proteins.

The frequency dependence of the proton spin-lattice relaxation time T1 of solid hydrated bovine serum albumin and alpha-chymotrypsin has been measured over 4.5 decades in the range 10(4) to 3 X 10(8) Hz mainly by the aid of the field-cycling technique. The comparison between H2O- and D2O-hydrated samples permitted the distinction of exchangeable and unexchangeable protons. In all cases the 14N1H cross-relaxation dips due mainly to the amide groups have been observed. In addition, in the case of the deuterium exchanged proteins a 2H1H quadrupole dip appears. The amide groups act as relaxation sinks due to the coupling of the amide proton to 14N and adjacent protons. Outside of the dip regions the proton-proton coupling dominates. The fluctuations of the 14N1H and 1H1H interactions are of a different type. The unexchangeable protons show a T1 dispersion outside of the quadrupole dip regions given by the exceptional power law T1 approximately v0.75 +/- 0.05. It is shown that apart from structural information of the 14N spectra, 14N1H cross-relaxation spectroscopy permits the determination of correlation times in the range 10(-7) s less than tau less than 10(-4)S.     

Water in barnacle muscle. III. NMR studies of fresh fibers and membrane-damaged fibers equilibrated with selected solutes.

Water in barnacle muscle has been studied using NMR techniques. Fresh fibers are compared with membrane-damaged fibers treated with solutes that greatly alter fixed charge and total water content. Both water (97%) and solute (3%) protons are visible in continuous wave spectra of oriented fresh fibers. No local field inhomogeneities were detected, nor are cell solutes significantly bound. In pulse experiments, all cell water is visible and exhibits a single exponential decay. In fresh fibers, T2 approximately or equal to 40 ms; faster decaying signals are assigned to immobile and mobile protons on macromolecules. T1 and T1p are frequency dependent. Using equations derived for a two-compartment model with fast exchange, we calculate the following: tau b, the correlation time for anisotropic rotational motion of bound water; Sb, its order parameter; tau ex, the correlation time for exchange between bound and free fractions; f, the fraction of water bound; and Hr, the grams of water bound per gram of macromolecule. Whereas f varies inversely with total water content, the other parameters are virtually constant, with values: tau b approximately or equal to 1.3 X 10(-8) S; tau ex approximately or equal to 8 X 10(-6) s; Sb approximately or equal to 0.06; and Hr approximately or equal to 0.1g H2O/g macromolecule. Thus, the NMR relaxation detectable properties of water bound to macromolecules are unaffected by solutes that greatly alter the macromolecular surface charge.     

The relationship between the transverse and longitudinal nuclear magnetic resonance relaxation rates of muscle water.

Whole frog sartorius and gastrocnemius muscles were incubated in Ringer's solutions, either unenriched or enriched with H2 17Oor 2D2O. Subsequently, the rates of transverse (1/T2) and of longitudinal (1/T1) nuclear magnetic relaxation were measured for 17O, 2D, and 1H at room temperature and at 8.1 MHz. The ratio (T1/T2) for 17O was measured to be approximately 1.5-2.0, close to the value roughly estimated from the Larmor frequency dependence of 1/T1 alone over the range 4.3-8.1 MHz. On the other hand (T1/T2) for 2D and 1H were both measured to lie in the range 9-11. Insofar as the entire 17O signal was detected, the data indicate the presence of an exchange mechanism between the major fraction of intracellular water and a minor fraction characterized by enhanced rates of relaxation. Possible molecular mechanisms are presented.     

Hydration of Escherichia coli lipids. Deuterium T1 relaxation time studies of phosphatidylglycerol, phosphatidylethanolamine and phosphatidylcholine

The hydration properties of Escherichia coli lipids (phosphatidylglycerol, phosphatidylethanolamine) and synthetic 1,2-dioleoyl-sn-glycero-3-phosphocholine in H2O/2H2O mixtures (9:1, v/v) were investigated with 2H-NMR. Comparison of the 2H2O spin lattice relaxation time (T1) as a function of the water content revealed a remarkable quantitative similarity of all three lipid-H2O systems. Two distinct hydration regions could be discerned in the T1 relaxation time profile. (1) A minimum of 11-16 water molecules was needed to form a primary hydration shell, characterized by an average relaxation time of T1 approximately equal to 90 ms. (2) Additional water was found to be in exchange with the primary hydration shell. The exchange process could be described in terms of a two-site exchange model, assuming rapid exchange between bulk water with T1 = 500 ms and hydration water with T1 = 80-120 ms. Analysis of the linewidth and the residual quadrupole splitting (at low water content) confirmed the size of the primary hydration layer. However, each lipid-water system exhibited a somewhat different linewidth behavior, and a detailed molecular interpretation appeared to be preposterous.     

Pulsed nuclear magnetic resonance study of 17-O, 2-D, and 1-H of water in frog striated muscle.

Whole gastrocnemius muscles were incubated in Ringer's solution enriched with H2-17O; the paired contralateral gastrocnemius muscles were incubated in a similar solution enriched with deuterons, as well. Subsequently, the longitudinal relaxation times (T1) were measured 17-O, 2-D, and 1-H, both at 8.1 MHz and at 4.3 MHz. The results indicate that: (a) the absolute values of T1 characterizing the three nuclides are different in muscle and pure water. (b) the longitudinal relaxation rates of all three have an identical frequency dependence over the range studied, (c) the ratio (T1)2D/(T1)17ois the same in muscle water and pure water, while the ratio (T1)1H/(T1)17o is 2.1 times greater in pure water than it is in muscle water, and (d) 30-49 percent substitution of 2-D for 1-H has very little effect on the spin-lattice relaxation of tissue water protons. These data suggest that muscle water is in rapid exchange between a small fraction of immobilized molecules and a large fraction of free water. The results render unlikely the possibility that hypothetical ordering of muscle water significantly contributes to its longitudinal relaxation.     

Water T2 relaxation in sugar solutions

1H spin-spin relaxation times of water were measured with the CPMG sequence in dilute aqueous solutions of glucitol, mannitol, glycerol, glycol, the methyl D-pyranosides of alpha-glucose, beta-glucose, alpha-galactose, beta-galactose, alpha-xylose, beta-xylose, beta-arabinose and sucrose, alpha,alpha-trehalose, beta-maltose, maltotriose and maltoheptaose. The relaxation-time dispersion was measured by varying the CPMG pulse spacing, tau. These data were interpreted by means of the Carver-Richards model in which exchange between water protons and labile solute hydroxyl protons provides a significant contribution to the relaxation. From the dependences on temperature and tau, parameters characteristic of the pool of hydroxyls belonging to a given solute were extracted by nonlinear regression, including: the fraction of exchangeable protons, P, the chemical-shift difference between water protons and hydroxyl protons, deltaomega, the intrinsic spin-spin relaxation time, T2, and the chemical exchange rate, k. These solute-specific parameters are related, respectively, to the concentration, identity, mobility and exchange life-time of the hydroxyl site. At 298 K, values of deltaomega, T2 and k were found to be of the order of 1 ppm, 100 ms and 1000 s(-1), respectively. Effects of molecular size, conformation and solute concentration were investigated. The exchange mechanism was characterised by Eyring activation enthalpies and entropies with values in the ranges 50-70 kJ mol(-1) and -10 to 60 J K(-1)mol(-1), respectively.     

The effect of cytochrome P-450cam on the NMR relaxation rate of water protons.

Cytochrome P-450cam in the native, substrate-free state (Fe3+, S = 1/2) substantially reduces the NMR relaxation times, T1 and T2, of water protons. Temperature and frequency dependences of T1 and T2 were measured; they are consistent with a model of one or two protons exchanging between a binding site on a heme ligand and bulk water. The relevant parameters of this model have been deduced from the data. The spin relaxation time of the heme iron, tau S similar to 0.5 ns at 25 degrees C, is unusually long for a low spin ferric heme protein but is compatible with the line widths measured for paramagnetically shifted heme resonances. The proton residence time on the ligand, tau M similar to 1 microsecond at 25 degrees C, follows an Arrhenius law with activation energy EM similar to 15 kcal/mol. A scalar hyperfine interaction A/h = 2.2 MHz (3.1 MHz for one-proton exchange) of the found proton(s) with the heme iron is deduced from the difference between T1 and T2 observed in the fast exchange limit. The iron-proton distance is found to be 2.9 A (2.6 A for one-proton exchange). Variation of pH between pH 6.4 and 8.6 does not affect T1. The bearing of these results on the question of the axial heme ligand is discussed.     

Relaxation phenomena in human erythrocyte suspensions.

Previous work has shown that the application of the Joule heating temperature jump technique of Eigen and de Maeyer to an istonic suspension of human erythrocytes induced an interiorization of [3H-A1glucose and a hemolysis of the red cells (Tsong, T.Y., and E. Kingsley, J. Biol. Chem. 250:786 [1975]). The result was interpreted as due to the thermal osmosis effect. Further considerations of the various effects of the Joule heating technique indicate that the hemolysis of the red cells may also be caused by the rapid dielectric perturbation of the cell membranes. By means of turbidity measurements of the suspensions we have detected at least four relaxation times. Two of the faster ones (tau1 approximately 20 mus and tau2 approximately 5 ms) are tentatively attributed to water relaxations in the membrane structures. The other two are attributed to membrane ruptures (tlag approximately 0.1s) and the hemolysis reaction (tau3 approximately 0.5 s). Studies with the erythrocytes from different hematological disorders indicate that whereas the two slower relaxations are sensitive to the overall physical property of the red cell membranes the two faster relaxations are not. These observations are consistent with the above assignment of the relaxation processes. The apparent activation energies are, above assignment of the relaxation processes. The apparent activation energies are, respectively, 8.4, 12.0, and 11.8 kcal/mol for the tau1, tau2, and tau3 reactions. Experiments with erythrocyte ghosts indicate a single relaxation for the water permeation, and biphasic kinetics for the membrane rupture and resealing reactions. The phenomena reported here may contribute to our understanding of water transport and molecular release in cellular systems.     

The interaction between water and the polar head in inverted phosphatidylcholine micelles. A 2H and 31P relaxation study.

2H and 31P spin-lattice relaxation times (T1) were studied for inverted egg phosphatidylcholine micelles in CCl4 as functions of 2H2O concentration. When the 2h2O/phosphatidylcholine mole ratio changed from 1.0 to 18.0, T1 of 31P increased by about 2.6 fold, whereas T1 of 2H increased by about 50 fold. A quantitative analysis of the deuterium T1 data showed that there is only one water molecule tightly bound to the polar head, and it is in rapid exchange with the rest of the water molecules. The activation energy for the deuterium T1 was 7.1 +/- 0.8 kcal/mol(30 +/- 3 kJ/mol), and was independent of the 2H2O concentration.     

31P and 2H NMR studies of structure and motion in bilayers of phosphatidylcholine and phosphatidylethanolamine

The structural and motional properties of mixed bilayers of phosphatidylcholine (PC) and phosphatidylethanolamine (PE) have been examined by using wide-line 31P, 14N, and 2H NMR. 2H and 14N NMR data showed that in mixed bilayers containing both PC and PE the conformations of the head-group moieties are essentially identical with those observed for bilayers containing a single phospholipid species. Equimolar amounts of cholesterol induce also only a small change in head-group conformation. 31P T1 relaxation measurements (at 300 MHz) at various temperatures of bilayers containing phospholipids with a mixture of phosphocholine and phosphoethanolamine head-groups and unsaturated fatty acid residues revealed in all cases a clearly defined minimum corresponding to the condition omega O tau C-1 approximately 1. For all phospholipid mixtures studied, the 31P T1 relaxation was homogeneous over the whole powder spectrum and could be fitted to a single-exponential decay. The 31P vs temperature profiles were analyzed by a simple correlation model following the analysis of Seelig et al. (1981) [Seelig, J., Tamm, L., Hymel, L., & Fleischer, S. (1981) Biochemistry 20, 3922-3932]. Rotational diffusion of the phosphate moiety in bilayers of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) was slower than that of 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC), and the activation energy was increased by a factor of 1.7 to 31.4 kJ mol-1.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

1H and 31P relaxation rate studies of the interaction of phosphoenolpyruvate and its analogues with avian phosphoenolpyruvate carboxykinase

The interactions of the substrate phosphoenolpyruvate and the substrate analogues (Z)-phosphoenol-alpha-ketobutyrate and (E)-phosphoenol-alpha-ketobutyrate with the enzyme-Mn complex of chicken liver phosphoenolpyruvate carboxykinase have been investigated by 1H and by 31P nuclear relaxation rate studies. Studies of the 1H and the 31P relaxation rates of the ligands in the binary Mn-ligand complexes show that these ligands interact with the metal ion via the phosphate group but not through the carboxylate. An inner sphere coordination complex is formed but the metal-ligand complex is not in the most extended conformation. In the relaxation rate studies of the ligands in the presence of the enzyme, conditions were adjusted so that all of the Mn2+ that was added resided in the ternary enzyme-Mn-ligand complex. The 1H relaxation rates for each of the three ligands were measured at 100 and at 300 MHz. In each case the normalized paramagnetic effects showed that 1/(pT2p) was greater than 1/(pT1p). A frequency dependence of the 1/(pT1p) and 1/(pT2p) values was also measured. The correlation time, tau c, for the Mn-1H interaction was calculated from the frequency dependence of 1/(pT1p) assuming a maximal frequency dependence of tau c and assuming no frequency dependence of tau c and from the T1M/T2M ratios at each frequency. The tau c values for all of the complexes, calculated at 100 MHz, varied from approximately 0.3 to 2.0 ns. These values were used to calculate the Mn-1H distances in each of the ternary complexes. The relaxation rates of 31P were also measured.(ABSTRACT TRUNCATED AT 250 WORDS)     

Application of NMRD to hydration of rubredoxin and a variant containing a (Cys-S)3FeIII(OH) site

Hydration of oxidized rubredoxin (Fe(III)(S-Cys)(4) center) was investigated by (1)H and (17)O relaxation measurements of bulk water as a function of the applied magnetic field (nuclear magnetic relaxation dispersion). Oxidized rubredoxin showed an increased water (1)H relaxation profile with respect to the diamagnetic gallium derivative or reduced species. Analysis of the data shows evidence of exchangeable proton(s) approximately 4.0-4.5 A from the metal ion, the exchange time being longer than 10(-10) s and shorter than 10(-5) s. The correlation time for the proton-electrons interaction is 7 x 10(-11) s and is attributed to the effective electron relaxation time. Its magnitude is consistent with the large signal linewidths of the protein donor nuclei, observed in high resolution NMR spectra. For reduced rubredoxin, such correlation time is proposed to be smaller than 10(-11) s. (17)O relaxation measurements suggest the presence of at least one long-lived protein-bound water molecule. Analogous relaxation measurements were performed on the C6S rubredoxin variant, whose iron(III) center has been previously shown to be coordinated to three cysteine residues and a hydroxide ion above pH 6. (1)H nuclear magnetic relaxation dispersion profiles indicate increased hydration with respect to the wild-type.     

Nuclear magnetic relaxation by the manganese in aqueous suspensions of chloroplasts

Proton and oxygen-17 NMR relaxation rate (T1-1 and T2-1) data are presented for aqueous suspensions of dark-adapted chloroplasts. It is concluded from the dependence of the proton relaxation rates (PRR) upon Mn concentration that T1-1 and T2-1 are determined largely by the loosely bound Mn present in the chloroplast membranes. The frequency and temperature dependences of PRR are characteristic of Mn(II). The effects of oxidants (e.g., ferricyanide) and reductants (e.g., tetraphenylboron) on the PRR indicate that only about one-third to one-fourth of the loosely bound Mn is present in the dark-adapted chloroplasts as Mn(II), the remainder being in a higher oxidation state(s), probably Mn(III). The frequency dependence of the PRR for the chloroplast suspensions was fitted by a simplified form of the Solomon-Bloembergen-Morgan equations, and the following parameters were obtained: tauS = (1.1 +/- 0.1) X 10(-8) S; tauM = (2.2 +/- 0.2) X 10(-8) S; and B = (0.9 +/- 0.09) X 10(19). The oxygen-17 T1 and T2 data for suspensions before and after treatment with a detergent are consistent with the location of the manganese in the interior of the thylakoids. An analysis of the relaxation rates shows that the average lifetime of a water molecule inside a thylakoid is greater than 1 ms.     

Cytochrome c folds through a smooth funnel

A dominant feature of folding of cytochrome c is the presence of nonnative His-heme kinetic traps, which either pre-exist in the unfolded protein or are formed soon after initiation of folding. The kinetically trapped species can constitute the majority of folding species, and their breakdown limits the rate of folding to the native state. A temperature jump (T-jump) relaxation technique has been used to compare the unfolding/folding kinetics of yeast iso-2 cytochrome c and a genetically engineered double mutant that lacks His-heme kinetic traps, H33N,H39K iso-2. The results show that the thermodynamic properties of the transition states are very similar. A single relaxation time tau(obs) is observed for both proteins by absorbance changes at 287 nm, a measure of solvent exclusion from aromatic residues. At temperatures near Tm, the midpoint of the thermal unfolding transitions, tau(obs) is four to eight times faster for H33N,H39K iso-2 (tau(obs) approximately 4-10 ms) than for iso-2 (tau(obs) approximately 20-30 ms). T-jumps show that there are no kinetically unresolved (tau < 1-3 micros T-jump dead time) "burst" phases for either protein. Using a two-state model, the folding (k(f)) and unfolding (k(u)) rate constants and the thermodynamic activation parameters standard deltaGf, standard deltaGu, standard deltaHf, standard deltaHu, standard deltaSf, standard deltaSu are evaluated by fitting the data to a function describing the temperature dependence of the apparent rate constant k(obs) (= tau(obs)(-1)) = k(f) + k(u). The results show that there is a small activation enthalpy for folding, suggesting that the barrier to folding is largely entropic. In the "new view," a purely entropic kinetic barrier to folding is consistent with a smooth funnel folding landscape.     

Oxygen-17 relaxation times in the blood sera of rats with various cancers. Can a systemic effect be detected?

17O NMR relaxation times of water in the serum of rats with various cancers were measured. No systemic effect could be detected at 4.7 and 8.4 T. The serum T1(17O) value was 7.6 +/- 0.5 ms at 37 degrees C independent of the magnetic field. T2(17O) was approximately half T1(17O). The 17O relaxation times could be determined at a faster rate than the 1H relaxation times.     

Lipari-Szabo approach as a tool for the analysis of macromolecular gadolinium(III)-based MRI contrast agents illustrated by the [Gd(EGTA-BA-(CH2)12)] n n + polymer

The parameters governing the water proton relaxivity of the [Gd(EGTA-BA-(CH2)12)]nn+ polymeric complex were determined through global analysis of 17O NMR, EPR and nuclear magnetic relaxation dispersion (NMRD) data [EGTA-BA2- = 3,12-bis(carbamoylmethyl)- 6,9-dioxa-3,12-diazatetradecanedioate(2-)]. The Lipari-Szabo approach that distinguishes the global motion of the polymer (tau g) from the local motion of the Gd(III)-water vector (tau l) was necessary to describe the 1H and 17O longitudinal relaxation rates; therefore for the first time it was included in the global simultaneous analysis of the EPR, 17O NMR and NMRD data. The polymer consists on average of only five monomeric units, which limits the intramolecular hydrophobic interactions operating between the (CH2)12 groups. Hence the global rotational correlation time is not very high (tau g298 = 3880 +/- 750 ps) compared to the corresponding DTPA-BA-based polymer (about 15 monomeric units), where tau g298 = 6500 ps. As a consequence, the relaxivity is limited by the rotation, which precludes the advantage obtained from the fast exchanging chelating unit (kex298 = 2.2 +/- 0.1 x 10(6) s-1).     

Nuclear magnetic resonance studies of amino acids and proteins. Rotational correlation times of proteins by deuterium nuclear magnetic resonance spectroscopy

We show that measurement of the spin-lattice (T1) and spin-spin (T2) relaxation times (or line widths) of irrotationally bound 2H nuclei in macromolecules undergoing isotropic rotational motion outside of the extreme narrowing limit (i.e., for the case omega 02 tau R2 much greater than 1) permits determination of both the rotational correlation time (tau R) of the macromolecule and the electric quadrupole coupling constant (e2qQ/h) of the 2H label. The technique has the advantage over 13C nuclear magnetic resonance (NMR) that no assumptions about bond lengths (which appear to the sixth power in 13C relaxation studies) or relaxation mechanisms need to be made, since relaxation will always be quadrupolar, even for aromatic residues at high field. Asymmetry parameter (eta) uncertainties are shown to cause negligible effects on tau R determinations, and in any case it is shown that both e2qQ/h and eta may readily be determined in separate solid-state experiments. By way of example, we report 2H NMR results on aqueous lysozyme (EC 3.2.1.17) at 5.2 and 8.5 T (corresponding to 2H-resonance frequencies of 34 and 55 MHz). Interpretation of the results in terms of the isotropic rigid-rotor model yields e2qQ/h values of approximately equal to 170 or approximately equal to 190 kHz, respectively, for the imidazolium and free-base forms of [epsilon 1-2H] His-15 lysozyme in solution, in excellent agreement with e2qQ/h values of approximately 167 and approximately 190 kHz obtained for the free amino acids in the solid state. In principle, the method may in suitable cases permit comparison between the dynamic structures of proteins in solution and in the crystalline solid state.     

2H magnetic relaxation of 2H2O absorbed by wool.

D2O absorbed by intact wool fibers was studied by solid-state 2H nuclear magnetic resonance (NMR) spectroscopy. In wool fibers swollen in D2O, the deuteron transverse magnetization and the spin-locked magnetization revealed a non-exponential decay. At least two NMR phases with different sets of the NMR relaxation parameters, T(1rho) (2H) and T2 2H, have been detected that may be a manifestation of two different morphological phases of the cortex of the fiber.