Phosphorus-31 studies on lecithin in ethanol solutions

³¹P relaxation times of lecithin in ethanol solutions have been measured in dependence on temperature and water concentration. Trial calculations have been carried out on the assumption of a 2-site exchange model. The results suggest first, the relaxation behaviour is determined by various motional and exchange processes; second, at 29 MHz the dipole-dipole interaction between ³¹P and protons provides the dominant contribution; third, in general we are not concerned with the case of “extreme narrowing”. Moreover, there are no negligible intermolecular contributions to relaxation.     

Pulsed NMR studies of water in striated muscle non-freezing factor of water II. Spin-lattice relaxation times and the dynamics of the non-freezing fraction of water

Spin-lattice relaxation times for the water protons in frog gastrocnemius muscle are reported over the temperature range 193 to 283 °K at Larmor frequencies of 30 and 60 MHz. Results of measurements under similar conditions of the transverse relaxation times are also reported. The relaxation times of the non-freezing 20% of the muscle water are interpreted in terms of water molecules, absorbed on or interacting with the proteins, and which are undergoing anisotropic motion, probably with a distribution of correlation times. Proton spin-lattice relaxation times are also reported for muscles under tension, the tension being produced by loading of the muscles with varying weights.     

Nuclear magnetic resonance studies of the aggregation of dihexanoyllecithin and of diheptanolyllecithin in aqueous solutions.

Aggregation of 1,2-dihexanoyl-sn-glycero-3-phosphocholine (dihexanoyllecithin) and 1,2-diheptanoyl-sn-glycero-3-phosphocholine (diheptanoyllecithin) in aqueous solutions has been investigated by 1H nuclear magnetic resonance spectroscopy. The chemical shifts and line widths of the NMR signals of the lecithins are dependent on the total concentration of lecithin above the critical micelle concentration. Signals for both lecithins in the aggregated state exhibit line widths which are appreciably smaller than the dipolar line width calculated using the overall rotational correlation time of the micelle. Signals of the alpha-methylene protons of the carboxylic acid side chains of dihexanoyllecithin and diheptanoyllecithin undergo the greatest change in chemical shift on aggregation. A single averaged spectrum of the alpha-methylene protons is observed in lecithin solutions of concentrations ranging from one to four times the critical micelle concentration demonstrating that individual lecithin molecules are in rapid exchange, with respect to a frequency of 18 Hz, between the monomeric and the aggregated states. Plots of the chemical shift of the alpha-methylene protons versus concentration of lecithin approximate a micelle formation curve. At about five times the critical micelle concentration for both dihexanoyllecithin and diheptanoyllecithin the alpha-methylene pattern indicates that there are at least two magnetic environments for lecithin molecules in the aggregated state. Furthermore, individual lecithin molecules are in slow exchange between the two environments which are distinguished by a chemical shift difference of about 2 Hz.     

Dynamics of erabutoxin b as studied by nuclear magnetic resonance. Relaxation studies of methyl proton resonances

Longitudinal and transverse relaxation times were measured for well-resolved and assigned methyl proton resonances of erabutoxin b at 270 MHz, 300 MHz and 500 MHz. Both longitudinal and transverse magnetization decay curves are non-exponential due to cross-relaxation and cross-correlation effects. The longitudinal and transverse relaxation rates were obtained from the initial slope of both magnetization decay curves. The correlation times for the isotropic tumbling motion of the protein were determined to be 2.82 ns at 300 K and 1.62 ns at 330 K from the analysis of the relaxation data of some alpha protons. Using these values, the relaxation data of methyl protons were fitted to various theoretical models. Most of the methyl resonances could be fitted well to a model which allowed methyl rotation (in the range 0.01-0.05 ns) and an external contribution from protons assumed to be in positions derived from X-ray coordinates. The data for a few methyl groups, however, could not be fitted in this way. For these a smaller number of external protons than predicted by the X-ray coordinates was assumed. Additionally, a larger amplitude motion had to be introduced into the model for particular residues. This additional motion requires concerted protein motion close to these residues, since the X-ray structure suggests that steric hindrance would prevent local motion. These results are consistent with the idea of a flexible and dynamic structure for proteins.     

Electron spin relaxation time of Fe(III) in high spin heme proteins.

The electron spin relaxation time of high spin Fe(III), taus, was determined from the frequency dependence (5-100 MHz) of the longitudinal proton relaxation rates of water in solutions of catalase, metmyoglobin and acid ferricytochrome c. In all three high-spin heme proteins the relaxation rates incrased below 25 MHz, while no frequency dependence was observed above that frequency. The results are interpreted by assuming that taus, which modulates the dipolar interaction between the unpaired electrons of the iron and the water protons, is frequently independent. Its value was determined to be (6 +/- 1) - 10(-11) s.     

Solvent proton relaxation of aqueous solutions of the serum proteins alpha 2-macroglobulin, fibrinogen, and albumin.

The longitudinal, transverse, and spin-locked rotating frame relaxation rates have been measured for water protons in aqueous solutions of the human serum proteins albumin, fibrinogen, and alpha 2-macroglobulin in the physiological concentration range below 50 g/liter, corresponding to an upper limit for molarity of 725, 147, and 69 microM, respectively. The linear concentration dependence of all the relaxation rates measured at 100 MHz was used to provide the molar sensitivities of each relaxation process for each of the protein solutes. Both the solute dependence and the relaxation-process dependence of the molar sensitivities have been analyzed in terms of a model that has emerged from previous R1 dispersion measurements. This analysis demonstrates consistency between our data and that model for the active motions and their motional rates.     

Nuclear magnetic relaxation dispersion in monoclinic lysozyme crystals

Nuclear magnetic relaxation measurements are reported as a function of field strength corresponding to the frequency range from 0.01 to 20 MHz for water protons in monoclinic lysozyme crystals at 278 and 298 K. Though the instrumentation used selects only a portion of the total magnetization to sample, the data clearly indicate a field dependence of the relaxation rate that signals the presence of slow motions characterized by time constants in the range of tenths of microseconds and slower. The data support, but do not uniquely prove, the hypothesis that this time scale is that appropriate to the isotropic averaging of locally anisotropic water molecule motion at the protein surface.     

Molecular motions and phase transitions. NMR relaxation times studies of several lecithins.

The spin-lattice relaxation time, T1, and the dipolar energy relaxation time, TD, were measured as a function of temperature. The materials studied were samples of anhydrous L-dipalmitoyl lecithin, DL-dipalmitoyl lecithin, L-dimyristoyl lecithin, DL-dimyristoyl lecithin and their monohydrates, and of anhydrous egg yolk lecithin. It is shown that TD is a much more sensitive parameter than T1 for the determination of the Chapman phase transition. Comparison between T1 and TD provides information about new types of slow molecular motions below and above the phase transition temperature. It is suggested that the relaxation mechanisms for T1 and TD in the gel phase are governed by segmental motion in the phospholipid molecule. A new metastable phase was detected in dimyristoyl lecithin monohydrates. This phase could only be detected from the dipolar energy relaxation times.     

A pulsed N.M.R study of D2O bound to 1,2 dipalmitoyl phosphatidylcholine

Spin lattice relaxation times in both the lab and rotating frame, have been measured for deuterons (²H) in a number of unsonicated dispersions of 1,2 dipalmitoyl phosphatidylcholine in D₂O over a range of resonant frequencies from 13 MHz to 1 MHz for temperatures from ?20°C to 65°C.The proton (¹H) spin lattice relaxation time for the lecithin was measured for resonant frequencies of 8.5 MHz, and 40 MHz over a similar range of temperatures.The results agree with broadline measurements by Salsbury et al. [1], and for the liquid crystal phase are consistent with an anisotropic tumbling model of the water molecules bound to the lecithin headgroup. This tumbling occurs with correlation times of ≤10^?10 sec and ≈ 10^?6 sec about axes parallel to and perpendicular to the bisector of the D-O-D angle within a D₂O molecule, hydrogen bonded to the negatively charged phosphate headgroup.     

NMR observation of the interaction of small oligopeptides with phospholipid vesicles

Using proton spin-lattice relaxation times, the interaction of small oligopeptides with sonicated vesicles of synthetic β-γ-dimyristoyl L-α-lecithin has been monitored at 29°C in D₂O. The measured relaxation times for the lecithin choline methyl, alkyl chain, and terminal methyl protons were observed to shorten markedly with increasing concentration of peptide, the relaxation remaining exponential. Noticeable resonance broadening was observed at the highest peptide concentration studied. The data reported are for the effect of the pharmacologically active pentapeptide methionine-enkephalin. Similar results have been observed for the effect of tetraglycine. The relaxation of the observable resonances of the added peptide appear to be unaffected. The results are discussed in terms of peptide-vesicle interactions.     

Towards MRI contrast agents of improved efficacy. NMR relaxometric investigations of the binding interaction to HSA of a novel heptadentate macrocyclic triphosphonate Gd(III)-complex

 A novel heptacoordinating ligand consisting of a thirteen-membered tetraazamacrocycle containing the pyridine ring and bearing three methylenephosphonate groups (PCTP-[13]) has been synthesized. Its Gd(III) complex displays a remarkably high longitudinal water proton relaxivity (7.7 mM^–1 s^–1 at 25  °C, 20 MHz and pH 7.5) which has been accounted for in terms of contributions arising from (1) one water molecule bound to the metal ion, (2) hydrogen-bonded water molecules in the second coordination sphere, or (3) water molecules diffusing near the paramagnetic chelate. Variable-temperature ¹⁷O-NMR transverse relaxation data indicate that the residence lifetime of the metal-bound water molecule is very short (8.0 ns at 25  °C) with respect to the Gd(III) complexes currently considered as contrast agents for magnetic resonance imaging. Furthermore, GdPCTP-[13] interacts with human serum albumin (HSA), likely through electrostatic forces. By comparing water proton relaxivity data for the GdPCTP-[13]-HSA adduct, measured as a function of temperature and magnetic field strength, with those for the analogous adduct with GdDOTP (a twelve-membered tetraaza macrocyclic tetramethylenephosphonate complex lacking a metal-bound water molecule), it has been possible to propose a general picture accounting for the main determinants of the relaxation enhancement observed when a paramagnetic Gd(III) complex is bound to HSA. Basically, the relaxation enhancement in these systems arises from (1) water molecules in the hydration shell of the macromolecule and protein exchangeable protons which lie close to the interaction site of the paramagnetic complex and (2) the metal bound water molecule(s). As far as the latter contribution is concerned, the interaction with the protein causes an elongation of the residence lifetime of the metal-bound water molecule, which limits, to some extent, the potential relaxivity enhancement expected upon the binding of the paramagnetic complex to HSA. Received: 27 January 1997 / Accepted: 12 May 1997     

Proton and deuteron relaxation of muscle water over wide ranges of resonance frequencies.

The spin-lattice relaxation time (T1) of water protons in mouse muscle was studied from 10(4) to 10(8) Hz at several temperatures, and the deuteron T1 of muscle water was studied from 2.0 X 10(3) to 1.54 X 10(7) Hz at several temperatures. Proton T1's of muscle and brain water with different D2O contents were measured at 25 degrees C and 35 MHz. From the results of variable frequency and temperature measurements and the data of isotope substitution, it is concluded that the major relaxation mechanism for the protons in muscle water is the intermolecular dipolar interaction between the protons of the macromolecules and the protons of the water molecules in the hydration layer. It is also suggested that the relaxation of deuterons can be accounted for a very small fraction of water molecules directly hydrogen-bonded to the macromolecules.     

NMR Investigations of the interaction of water with lecithin in benzene solutions

NMR investigations of ¹H (chemical shifts, line widths) and of ³¹P (relaxation times, T₁) performed on the three-component system of lecithin-benzene-water show that there is an interaction of water with the phosphate group in two regions of different mobility and structure. A fast exchange of the water molecules takes place between both regions. The region of strong interaction involves about 2 and that of the weaker interaction about 5 water molecules per lecithin molecule. When the water concentration is increased a third region is formed which is assigned to the water molecules that are located beyond the two regions of interaction with the phosphate group, but within the micelle. This water has a different structure from that of the second region of interaction with the phosphate group and may also have a different mobility.Addition of water increases the motion of the head groups of the lecithin molecules. This is due to a loosening of the packing of lecithin molecules.     

Effect of valinomycin on the structure of water-lecithin liposomes]

It has been established that water--lecithin liposomes in the heptane phase are formed in the course of equilibration of lecithin solution in heptane with water phase containing Na, K-picrate. The salts penetrate both the water nucleus of liposomes and their lecithin shell. The addition of valinomycin to this system does not change the water content in liposomes, but considerably increases the salt absorbed by the lipid shell of liposomes. A characteristic S-shape curve showing the relation between picrate extraction and the valinomycin concentration might be explained as an indication of a cooperative change of the structure of lecithin shell. This phase transition is induced by one valinomycin molecule per 10(3)--10(4) lecithin molecules.     

Dielectric relaxation in lecithin/cholesterol/water-mixtures

The dielectric spectrum of aqueous solutions of dimyristoyl-l-3-phosphatidylcholine and dipalmitoyl-l-3-phosphatidylcholine with admixed cholesterol has been determined by means of a pulse reflection method which was used to measure the complex permittivity of the solutions as a function of frequency between 100 kHz and 50 MHz. Measurements have been performed at various concentrations of cholesterol in dependence of temperature around the crystal-line/liquid-crystalline phase transition temperature of the solutions.The measured dielectric spectra are treated in terms of a Debye-function. The dielectric relaxation strength and the relaxation time decrease distinctly with increasing cholesterol concentration. In addition, the data are treated on the basis of a theoretical solution model in order to allow for conclusions concerning the lecithin head group motion in the lipid bilayer surface. One important result is that increasing cholesterol concentration affects the interaction of the lecithin head groups and increases their mobility. These effects already occur at small concentrations of cholesterol.     

Pulsed NMR studies on water in striated muscle III. The effects of water content

Pulsed NMR is used to study the kinetics of dehydration of frog gastrocnemius muscle. In addition, measurements are reported of the variation of the spin-lattice (T₁) and transverse (T₂) nuclear magnetic relaxation times of the water protons as a function of water content. The proton transverse relaxation and freezing properties of the water in muscles which had been dehydrated and then rehydrated are also investigated. Correlation of the double-exponential dehydration kinetics with the transverse relaxation at various water contents provides strong evidence for the evidence of a fraction of muscle water (10–20%) which is sufficiently strongly held to the solid substance of the muscle to make it relatively slowly removed under conditions of zero relative humidity but which is still dynamically very mobile on average. This is supported by the dependence of T₁ on water content. The relaxation times are interpreted qualitatively in terms of a number of possible effects which are at present not distinguishable. The properties of the dehydrated-rehydrated muscles indicated changes in the muscle proteins which affect the transverse relaxation of the water protons and the freezing properties of the muscle water.     

Biochemical and proton NMR characterization of the isolated functional beta-subunit of coupling factor one from spinach chloroplasts

Beta subunits have been dissociated from CF1 of spinach chloroplasts, purified by HPLC and characterized by two-dimensional electrophoresis and fluorescence emission. The solutions of isolated beta subunits are able to hydrolyze MgATP; this ATPase activity is an intrinsic property of the beta molecule. From proton NMR at 300 and 500 MHz, it is shown that the preparations are fully reproducible and that beta subunits remain monomeric with 75% aliphatic protons associated with rigid parts of the molecule. The other 25% give rise to separate resonances and belong to mobile side-chains and/or to flexible regions. The measurement of the transverse relaxation times T2 has permitted a detailed characterization of the molecular dynamics of the isolated beta subunits.     

Dielectric behaviour of frozen DNA in solution

In this article, measurements are reported on ice and frozen DNA solutions between 100 Hz–10 MHz. Pure ice is shown to exhibit single relaxation behaviour, which confirms previous work taken over a more restricted frequency range. The frozen DNA solution displays double‐dispersion behaviour. One dispersion centred around 3 kHz is due to a defect mechanism while the other, centred around 2 MHz, may be attributed to counterion flow through the water immediately adjacent to the DNA molecule. Bioelectromagnetics 20:40–45, 1999. © 1999 Wiley‐Liss, Inc.     

Principles of quantitative analysis of two-dimensional spectra of nuclear Overhauser effect in evaluation of protein and peptide conformation

To elucidate potentialities of two-dimensional homonuclear Overhauser effect (NOESY) spectra of peptides and proteins for their spatial structure determination, impact of experimental parameters and intrinsic properties of the investigated molecule on proton cross-peak volumes in NOESY spectra was analysed. Recommendations which could increase accuracy of cross-peak volume measurements were suggested. Influence of intrinsic properties of a molecule (spin-lattice relaxation times T1, correlation time tau C and surrounding protons) on the volume of cross-peak for particular protons was analyzed using a complete relaxation matrix of the (formula; see text) helix of gramicidin A. Nonselective relaxation time T1 of the protons was found to affect only slightly the results of cross-peak volumes computer simulation, whereas correlation time tau C and surrounding protons seriously influenced cross-peak volumes. Nevertheless, cross-peak volumes between NH, C alpha H and C beta H protons of a dipeptide fragment of the entire molecule could be accurately simulated using the relaxation matrix of the individual dipeptide. Thus local conformations (torsion angles phi, psi and chi 1) of amino acid residues could be deduced independently of one another and prior to the complete analysis of a molecular structure. The result can be obtained even in the presence of spin-diffusion at mixing times providing maximal volumes of cross-peaks in NOESY spectra.     

Structure of alamethicin in solution: nuclear magnetic resonance relaxation studies

An NMR relaxation study at 500 MHz of the icosapeptide antibiotic alamethicin is reported. This study lends further support to the partly helical, partly extended, amphiphilic, and dimeric structure recently proposed for this peptide in methanolic solutions [Banerjee, U., Tsui, F. P., Balasubramanian, T. N., Marshall, G. R., & Chan, S. I. (1983) J. Mol. Biol. 165, 757]. The N-acetyl methyl groups toward the N terminus of alamethicin in this solvent system were found to exhibit unusual NMR relaxation behavior. The decay of the transverse magnetization due to these protons was nonexponential, but the spin-lattice relaxation recovery of the longitudinal magnetization was exponential. In a solution saturated with urea, however, both decays were exponential. These observations are shown to be consistent with the proposed structure. Studies in water yielded qualitatively similar but more complex results. The transverse relaxation times suggest further aggregation in water and indicate that the larger aggregates in water may be made up of the smaller units observed in methanol.