Multicomponent spectra from 31P-NMR studies of the phase equilibria in the system dioleogylphosphatidylcholine-dioleoylphosphatidylthanolamine-water

The phase equilibria in mixtures of dioleoylphosphatidylcholine (DOPC), dioleoylphosphatidylethanolamine (DOPE) and water were studied by ³¹P-NMR and ²H-NMR. The chemical shift anisotropy is greater for DOPC than for DOPE (6–9 ppm in the lamellar phase). This difference can most probably be ascribed to different order parameters for the two lipid head groups. ³¹P-NMR spectra recorded from a lamellar phase formed by DOPC-DOPE-water below maximum hydration exhibit two resolved, superimposed powder spectra. The chemical shift anisotropy for both phospholipids has greater values at excess water contents than below maximum hydration, and the spectral resolution between DOPC and DOPE in the lamellar phase is strikingly diminished at excess water contents. From ³¹P-NMR spectra it is possible to observe relative differences in composition between different lipid phase existing in equilibrium. The proportion of DOPE is decreased in the lamellar phase, and is increased in the reversed hexagonal phase, when these phases exist in equilibrium.     

400 MHz two-dimensional nuclear Overhauser spectroscopy on anesthetic interaction with lipid bilayer

Interaction between a volatile anesthetic, methoxyflurane, and dipalmitoylphosphatidylcholine (DPPC) vesicle membrane was analyzed by nuclear Overhauser effect (NOE) difference spectroscopy and two-dimensional nuclear Overhauser spectroscopy (NOESY). The NOE difference spectra were obtained by selectively irradiating methoxy protons (hydrophobic end) of the anesthetic: a negative nuclear Overhauser effect of -2.94% was observed with the choline methyl protons of DPPC. The NOESY spectra revealed a cross-peak between the anesthetic methoxy protons and the choline methyl protons. A dipole-dipole interaction exists between the hydrophobic end of the anesthetic and the hydrophilic head group of DPPC. No other cross-peaks were observed. The anesthetic orients itself at the membrane/water interface by interacting with the hydrophilic surface of the DPPC membrane, leaving the hydrophilic end of the anesthetic molecule in the aqueous phase. The preferred residence site of dipolar volatile anesthetics is the membrane/water interface.     

Proton homonuclear correlated spectroscopy as an assignment tool for hyperfine-shifted resonances in medium-sized paramagnetic proteins: cyanide-ligated yeast cytochrome c peroxidase as an example.

Two types of homonuclear proton COSY experiments are shown to be useful in making resonance assignments in cyanide-ligated cytochrome c peroxidase, a 34 kDa paramagnetic heme protein. Both magnitude COSY and phase-sensitive COSY experiments provide spectra useful for making proton assignments to resonances of strongly relaxed hyperfine-shifted protons. This initial investigation demonstrates that COSY experiments combined with NOESY experiments are feasible for hyperfine-shifted protons of paramagnetic proteins larger than metmyoglobins and ferricytochromes c, for which the nuclear spin-lattice relaxation times are in the range 70-300 ms. Taken together, COSY and NOESY experiments, although not yet widely applied to paramagnetic metalloproteins, provide a reliable protocol for accurately assigning hyperfine-shifted resonances that are part of a metalloenzyme's active site. Specific examples of expected proton homonuclear COSY connectivities that were not observed in these experiments are presented, and utilization of COSY with respect to the proton resonance line widths and apparent nuclear relaxation times is discussed. The COSY experiments presented here provide valuable verification of previously proposed hyperfine resonance assignments for cyanide-ligated cytochrome c peroxidase, which were made by using NOESY experiments alone, and in several instances expand these assignments to additional protons in particular amino acid spin systems.     

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.     

Interactions of antibody aromatic residues with a peptide of cholera toxin observed by two-dimensional transferred nuclear Overhauser effect difference spectroscopy

The interactions between a peptide of cholera toxin and the aromatic amino acids of the TE33 antipeptide antibody, cross-reactive with the toxin, have been studied by NOESY difference spectroscopy. The 2D difference between the NOESY spectrum of the Fab with a 4-fold excess of the peptide and that of the peptide-saturated Fab reveals cross-peaks growing with excess of the peptide. These cross-peaks are due to magnetization transfer between the Fab and neighboring bound peptide protons, and a further transfer to the free peptide protons by exchange between bound and free peptide (transferred NOE). Additional cross-peaks appearing in the difference spectrum are due to a combination of intramolecular interactions between bound peptide protons and exchange between bound and free peptide. Assignment of cross-peaks is attained by specific deuteration of antibody aromatic amino acids using also the resonance assignment of the free peptide, deduced from the COSY spectrum of the peptide solution. The antibody combining site is found to be highly aromatic. We have identified one or two histidine, two tyrosine, and two tryptophan residues and one phenylalanine residue of the antibody interacting with valine-3, proline-4, glycine-5, glutamine-7, histidine-8, and aspartate-10 of the peptide. The 2D TRNOE difference spectroscopy can be used to study protein-ligand interactions, given that the ligand off rate is fast relative to the spin-lattice relaxation time of the protein and ligand protons (about 1 s). The resolution obtained in the difference spectra implies that the technique is equally applicable for studying proteins having a molecular weight larger than 50,000.(ABSTRACT TRUNCATED AT 250 WORDS)     

Hydrophobic molecules in lecithin-water systems. I. Formation of reversed hexagonal phases at high and low water contents.

The system dioleoylphosphatidylcholine (DOPC)-n-dodecane-2H2O was investigated with different nuclear magnetic resonance (NMR) techniques: (a) a tentative phase diagram was determined by 2H- and 31P-NMR, (b) translational diffusion coefficients were determined for the three components with the pulsed magnetic field gradient NMR technique, and (c) order parameters for perdeuterated n-dodecane were obtained by 2H-NMR. n-Dodecane induces the formation of reversed hexagonal (HII) phases at low and high water concentrations, and cubic phases at low water contents. The translational diffusion coefficients of n-dodecane in a cubic phase with 6 mol water per mol DOPC, and in an HII phase with 48 mol water per mol DOPC, were just approximately 2.5 times lower than in pure dodecane. Perdeuterated dodecane gave large quadrupole splittings in a lamellar phase, much smaller in an HII phase at low water contents, and a narrow single peak in an HII phase at high water contents. This latter observation indicates that a large fraction of the dodecane molecules is located in separate regions between the water cylinders. Our results support the model given by Gruner concerning the aggregation of membrane lipids in the presence of hydrophobic molecules.     

Complete assignment of the imino protons of Escherichia coli valine transfer RNA: two-dimensional NMR studies in water

The imino proton spectrum of Escherichia coli valine tRNA has been studied by two-dimensional nuclear Overhauser effect spectroscopy (NOESY) in H2O solution. The small nuclear Overhauser effects from the imino proton of an internal base pair to the imino protons of each nearest neighbor can be observed as off-diagonal cross-peaks. In this way most of the sequential NOE connectivity trains for all the helices in this molecule can be determined in a single experiment. AU resonances can be distinguished from GC resonances by the AU imino NOE to the aromatic adenine C2-H, thus leading to specific base-pair assignments. In general, the NOESY spectrum alone is not capable of assigning every imino proton resonance even in well-resolved tRNA spectra. Multiple proton peaks exhibit more than two cross-peaks, resulting in ambiguous connectivities, and coupling between protons with similar chemical shifts produces cross-peaks that are incompletely resolved from the diagonal. The sequence of the particular tRNA determines the occurrence of the latter problem, which can often be solved by careful one-dimensional experiments. The complete imino proton assignments of E. coli valine tRNA are presented.     

Magic-angle spinning NMR studies of molecular organization in multibilayers formed by 1-octadecanoyl-2-decanoyl-sn-glycero-3-phosphocholine.

Magic-angle spinning 1H and 13C nuclear magnetic resonance (NMR) have been employed to study 50%-by-weight aqueous dispersions of 1-octadecanoyl-2-decanoyl-sn-glycero-3-phosphocholine (C[18]:C[10]PC) and 1-octadecanoyl-2-d19-decanoyl-PC (C[18]:C[10]PC-d19), mixed-chain phospholipids which can form interdigitated multibilayers. The 1H NMR linewidth for methyl protons of the choline headgroup has been used to monitor the liquid crystalline-to-gel (LC-to-G) phase transition and confirm variations between freezing and melting temperatures. Both 1H and 13C spin-lattice relaxation times indicate unusual restrictions on segmental reorientation at megahertz frequencies for C(18):C(10)PC as compared with symmetric-chain species in the LC state; nevertheless each chemical moiety of the mixed-chain phospholipid exhibits motional behavior that may be classified as liquidlike. Two-dimensional nuclear Overhauser spectroscopy (NOESY) on C(18):C(10)PC and C(18):C(10)PC-d19 reveals cross-peaks between the omega-methyl protons of the C18 chain and the N-methyl protons of the phosphocholine headgroup, and several experimental and theoretical considerations argue against an interpretation based on spin diffusion. Using NMR relaxation times and NOESY connectivities along with a computational formalism for four-spin systems (Keepers, J. W., and T. L. James. 1984. J. Magn. Reson. 57:404-426), an estimate of 3.5 A is obtained for the average distance between the omega-methyl protons of the C18 chain and the N-methyl protons of the phosphocholine headgroup. This finding is consistent with a degree of interdigitation similar to that proposed for organized assemblies of gel-state phosphatidylcholine molecules with widely disparate acyl-chain lengths (Hui, S. W., and C.-H. Huang. 1986. Biochemistry. 25:1330-1335); however, acyl-chain bendback or other intermolecular interactions may also contribute to the NOESY results. For multibilayers of C(18):C(10)PC in the gel phase, 13C chemical-shift measurements indicate that trans conformers predominate along both acyl chains. 13C Spin-lattice relaxation times confirm the unusual motional restrictions noted in the LC state; nevertheless, 13C and 1H rotating-frame relaxation times indicate that the interdigitated arrangement enhances chain or bilayer motions which occur at mid-kilohertz frequencies.     

Phase equilibria of model milk membrane lipid systems

The phase behaviour of mixtures of recombined milk membrane lipids dioleoylphosphatidylcholine (DOPC), sphingomyelin (SM), dioleoylphosphatidylethanolamine (DOPE), phosphatidylinositol (PI) and dioleoylphosphatidylserine (DOPS) in 60% water was examined as a function of temperature between 5 and 90 degrees C. The aim was to examine under which lipid composition the average properties turn from balanced over to hydrophobic. The phase boundaries were determined by small angle X-ray diffraction (SAXD) and differential scanning calorimetry (DSC). The lamellar phase was dominating in the DOPC/SM/DOPE system. The phase boundary for the reversed hexagonal phase was only observed at high DOPE content within the examined temperature interval. The anionic phospholipids PI and DOPS induced a swollen lamellar phase, but no significant change of the transition between the lamellar phase and the reversed hexagonal phase was observed.     

Influence of membrane-spanning alpha-helical peptides on the phase behavior of the dioleoylphosphatidylcholine/water system

The effect of solubilized hydrophobic peptides on the phase behavior of dioleoylphosphatidylcholine (DOPC)/water system was studied by 2H- and 31P-NMR spectroscopy and by x-ray diffraction, and partial phase diagrams were constructed. The utilized peptides were HCO-AWW(LA)5WWA-NHCH2CH2OH (WALP16), which is an artificial peptide designed to resemble a transmembrane part of a membrane protein; and VEYAGIALFFVAAVLTLWSMLQYLSAAR (Pgs peptide E), a peptide that is identical to one of the putative transmembrane segments of the membrane-associated protein phosphatidylglycerophosphate synthase (Pgs) in Escherichia coli. Circular dichroism spectroscopy suggests that both peptides are mostly alpha-helical in DOPC vesicles. The most striking features in the phase diagram of the WALP16/DOPC/water system are 1) a single lamellar liquid crystalline (L alpha) phase forms only at very low peptide concentrations. 2) At low water content and above a peptide/lipid molar ratio of approximately 1:75 a reversed hexagonal liquid crystalline (H[II]) phase coexists with an L alpha phase, while in excess water this phase forms at a peptide/lipid molar ratio of approximately 1:25. 3) At peptide/lipid ratios > or =1:6 a single H(II) phase is stable. Also, the Pgs peptide E strongly affects the phase behavior, and a single L alpha phase is only found at low peptide concentrations (peptide/lipid molar ratios <1:50), and water concentrations <45% (w/w). Higher peptide content results in coexistence of L alpha and isotropic phases. Generally, the fraction of the isotropic phase increases with increasing temperature and water concentration, and at 80% (w/w) water content only a single isotropic phase is stable at 55 degrees C. Thus, both peptides were found to be able to induce nonlamellar phases, although different in structure, in the DOPC/water system. The phase transitions, the extensions of the one-phase regions, and the phase structures observed for the two systems are discussed in terms of the molecular structure of the two peptides and the matching between the hydrophobic lengths of the peptides and the bilayer thickness of DOPC.     

Interaction of the peptide antibiotic alamethicin with bilayer- and non-bilayer-forming lipids: influence of increasing alamethicin concentration on the lipids supramolecular structures

Incorporation of the helical antimicrobial peptide alamethicin from aqueous phase into hydrated phases of dioleoylphosphatidylethanolamine (DOPE) and dioleoylphosphatidylcholine (DOPC) was investigated within a range of peptide concentrations and temperatures by time-resolved synchrotron X-ray diffraction. It was found that alamethicin influences the organizations of the non-bilayer-forming (DOPE) and the bilayer-forming (DOPC) lipids in different ways. In DOPC, only the bilayer thickness was affected, while in DOPE new phases were induced. At low peptide concentrations (<1.10(-4) M), an inverted hexagonal (H(II)) phase was observed as with DOPE dispersions in pure buffer solution. A coexistence of two cubic structures was found at the critical peptide concentration for induction of new lipid/peptide phases. The first one Q224 (space group Pn3m) was identified within the entire temperature region studied (from 1 to 45 degrees C) and was found in coexistence with H(II)-phase domains. The second lipid/peptide cubic structure was present only at temperatures below 16 degrees C and its X-ray reflections were better fitted by a Q212 (P4(3)32) space group, rather than by the expected Q229 (Im3m) space group. At alamethicin concentrations of 1 mM and higher, a nonlamellar phase transition from a Q224 cubic phase into an H(II) phase was observed. Within the investigated range of peptide concentrations, lamellar structures of two different bilayer periods were established with the bilayer-forming lipid DOPC. They correspond to lipid domains of associated and nonassociated helical peptide. The obtained X-ray results suggest that the amphiphilic alamethicin molecules adsorb from the aqueous phase at the lipid head group/water interface of the DOPE and DOPC membranes. At sufficiently high (>1.10(-4) M) solution concentrations, the peptide is probably accommodated in the head group region of the lipids thus inducing structural features of mixed lipid/peptide phases.     

Fourier-transform infrared spectroscopy study of dioleoylphosphatidylcholine and monooleoylglycerol in lamellar and cubic liquid crystals

The liquid-crystalline phases of the systems monooleoylglycerol (MO)/water, dioleoylphosphatidylcholine (DOPC)/water, and MO/DOPC/water have been studied by Fourier-transform infrared (FTIR) spectroscopy. In the latter ternary system, the sn-3 OH group of MO competes with water to interact with the polar head group of DOPC, and an intramolecular hydrogen bonding of MO is broken up. The hydration of the ester carbonyl groups in the lamellar phases of both the MO/water and DOPC/water systems increases with increasing water content. Similarly, the addition of small amounts either of MO to a DOPC/water system or of DOPC to an MO/water system also results in an increase in the hydration of the ester carbonyl groups. This leads to an unfavorable hydrocarbon-water contact which is counteracted by the formation of a cubic phase, except for the DOPC/water system, where the lamellar phase is stable also at the highest water concentrations. The phase behavior of the different systems can be described in terms of lipid monolayer curvature and molecular packing in the lipid aggregates. Finally, it is shown by the water association band in the FTIR spectrum that the water hydrogen bonding is considerably different in the liquid-crystalline phases than in bulk water.     

Phase equilibria of mixtures of plant galactolipids. The formation of a bicontinuous cubic phase

The chloroplast galactolipids monogalactosyldiacylglycerol (MGDG) and digalactosyldiacylglycerol (DGDG) were isolated from wheat leaves. The phase equilibria of galactolipid-water systems with MGDG / DGDG molar ratios equal to 0:1, 1:2, 1.2:1, 2:1 and 1:0 were investigated, using nuclear magnetic resonance (NMR) methods. MGDG and DGDG form reversed hexagonal and lamellar phases, respectively, at temperatures between 10 and 40°C at all water contents studied (up to about 14 mol ²H₂O per mol lipid). The galactolipid mixtures show a complex phase forming reversed hexagonal, lamellar and reversed cubic phases, depending on water content and temperature. It was found that the water hydration is similar for the lamellar and hexagonal phases formed by DGDG and MGDG, respectively. The non-lamellar phase areas increase with increasing content of MGDG. Small-angle X-ray measurements show that the cubic phase belongs to the Ia3d space group. From translational diffusion studies by NMR it is concluded that the structure of this cubic phase is bicontinuous.     

Minor groove hydration of DNA in aqueous solution: sequence-dependent next neighbor effect of the hydration lifetimes in d(TTAA)2 segments measured by NMR spectroscopy.

The hydration in the minor groove of double stranded DNA fragments containing the sequences 5'-dTTAAT, 5'-dTTAAC, 5'-dTTAAA and 5'-dTTAAG was investigated by studying the decanucleotide duplex d(GCATTAATGC)2 and the singly cross-linked decameric duplexes 5'-d(GCATTAACGC)-3'-linker-5'-d(GCGTTAATGC)-3' and 5'-d(GCCTTAAAGC)-3'-linker-5'-d(GCTTTAAGGC)-3' by NMR spectroscopy. The linker employed consisted of six ethyleneglycol units. The hydration water was detected by NOEs between water and DNA protons in NOESY and ROESY spectra. NOE-NOESY and ROE-NOESY experiments were used to filter out intense exchange cross-peaks and to observe water-DNA NOEs with sugar 1' protons. Positive NOESY cross-peaks corresponding to residence times longer than approximately 0.5 ns were observed for 2H resonances of the central adenine residues in the duplex containing the sequences 5'-dTTAAT and 5'-dTTAAC, but not in the duplex containing the sequences 5'-dTTAAA and 5'-dTTAAG. In all nucleotide sequences studied here, the hydration water in the minor groove is significantly more mobile at both ends of the AT-rich inner segments, as indicated by very weak or negative water-A 2H NOESY cross-peaks. No positive NOESY cross-peaks were detected with the G 1'H and C 1'H resonances, indicating that the minor groove hydration water near GC base pairs is kinetically less restrained than for AT-rich DNA segments. Kinetically stabilized minor groove hydration water was manifested by positive NOESY cross-peaks with both A 2H and 1'H signals of the 5'-dTTAA segment in d(GCATTAATGC)2. More rigid hydration water was detected near T4 in d(GCATTAATGC)2 as compared with 5'-d(GCATTAACGC)-3'-linker-5'-d(GCGTTAATGC)-3', although the sequences differ only in a single base pair. This illustrates the high sensitivity of water-DNA NOEs towards small conformational differences.     

New phases of phospholipids and implications to the membrane fusion problem

Membrane fusion is a ubiquitous process in eukaryotic cells. When two membranes fuse, lipid must undergo molecular rearrangements at the point of merging. To understand how lipid structure transitions occur, scientists studied the phase transition of lipid between the lamellar (L(alpha)) phase and the inverted hexagonal (H(II)) phase, based on the idea that lipid must undergo a similar rearrangement as in fusion. However, previous investigations on the system of dioleoylphosphatidylcholine (DOPC) and dioleoylphosphatidylethanolamine (DOPE) did not reveal intermediate phases between the L(alpha) and H(II) phases. Recently, we found a rhombohedral phase of diphytanoylphosphatidylcholine between its L(alpha) and H(II) phases using substrate-supported samples. Here we report the observation of two new phases in the DOPC-DOPE system: a rhombohedral phase and a distorted hexagonal phase. The rhombohedral phase confirms the stalk hypothesis for the L(alpha)-H(II) transition, but the phase of stable stalks exists only for a certain range of spontaneous curvature. The distorted hexagonal phase exists only in a lipid mixture. It implies that lipids may demix to adjust its local spontaneous curvature in order to achieve energy minimum under stress.     

Proton NMR T1, T2, and T1 rho relaxation studies of native and reconstituted sarcoplasmic reticulum and phospholipid vesicles.

The phospholipids protons of native and reconstituted sarcoplasmic reticulum (SR) membrane vesicles yield well-resolved nuclear magnetic resonance (NMR) spectra. Resonance area measurements, guided by the line shape theory of Bloom and co-workers, imply that we are observing a large fraction of the lipid intensity and that the protein does not appear to reduce the percent of the signal that is well resolved. We have measured the spin-lattice (T1) and spin-spin (T2) relaxation rates of the choline, methylene, and terminal methyl protons at 360 MHz and the spin-lattice relaxation rate in the rotating frame (T1 rho) at 100 MHz. Both the T1 and T2 relaxation rates are single exponential processes for all of the resonances if the residual water proton signal is thoroughly eliminated by selective saturation. The T1 and T2 relaxation rates increase as the protein concentration increases, and T2 rate decrease with increasing temperature. This implies that the protein is reducing both high frequency (e.g., trans-gauche methylene isomerizations) and low frequency (e.g., large amplitude, chain wagging) lipid motions, from the center of the bilayer to the surface. It is possible that spin diffusion contributes to the effect of protein on lipid T1's although some of the protein-induced T1 change is due to motional effects. The T2 relaxation times are observed to be near 1 ms for the membranes with highest protein concentration and approximately 10 ms for the lipids devoid of protein. This result, combined with the observation that the T2 rates are monophasic, suggests that at least two lipid environments exist in the presence of protein, and that the lipids are exchanging between these environments at a rate greater than 1/T2 or 10(3) s-1. The choline resonance yields single exponential T1 rho relaxation in the presence and absence of protein, whereas the other resonances measured exhibit biexponential relaxation. Protein significantly increases the single T1 rho relaxation rate of the choline peak while primarily increasing the T1 rho relaxation rate of the more slowly relaxing component of the methylene and methyl resonances.     

Phase diagram of 1,2-dioleoylphosphatidylethanolamine (DOPE):water system at subzero temperatures and at low water contents.

The phase behavior of partially hydrated 1, 2-dioleoylphosphatidylethanolamine (DOPE) has been studied using differential scanning calorimetry and X-ray diffraction methods together with water sorption isotherms. DOPE liposomes were dehydrated in the H(II) phase at 29 degrees C and in the L(alpha) phase at 0 degrees C by vapor phase equilibration over saturated salt solutions. Other samples were prepared by hydration of dried DOPE by vapor phase equilibration at 29 degrees C and 0 degrees C. Five lipid phases (lamellar liquid crystalline, L(alpha); lamellar gel, L(beta); inverted hexagonal, H(II); inverted ribbon, P(delta); and lamellar crystalline, L(c)) and the ice phase were observed depending on the water content and temperature. The ice phase did not form in DOPE suspensions containing <9 wt% water. The L(c) phase was observed in samples with a water content of 2-6 wt% that were annealed at 0 degrees C for 2 or more days. The L(c) phase melted at 5-20 degrees C producing the H(II) phase. The P(delta) phase was observed at water contents of <0.5 wt%. The phase diagram, which includes five lipid phases and two water phases (ice and liquid water), has been constructed. The freeze-induced dehydration of DOPE has been described with the aid of the phase diagram.     

Measurements of water proton NMR spin-lattice relaxation time in the rotating frame (T1p) for studying motions in solutions of giant macro-molecules and supramolecular particles (T2 virus)

Spin-spin relaxation time (T2), spin-lattice relaxation time (T1), and spin-lattice relaxation time in the rotating frame (T1p) of water protons in solutions of bacteriophage T2 were studied by pulsed nuclear magnetic resonance. The frequency dependence of the measurements exhibits a dispersion implying existence of a fraction of water molecules in solution with a correlation time distribution centered at approximately 10(-5) sec which is strongly influenced by the reorientational motions of virus particles. Experiments were carried out with two forms of bacteriophage T2 existing at pH 5.4 and 7.8 respectively. The different structures of the virus at these two pH values are reflected in the NMR relaxation behavior of water protons.     

Sequence-specific 1H NMR assignments and secondary structure of porcine motilin

The solution structure of the 22-residue peptide hormone motilin has been studied by circular dichroism and two-dimensional 1H nuclear magnetic resonance spectroscopy. Circular dichroism spectra indicate the presence of alpha-helical secondary structure in aqueous solution, and the secondary structure can be stabilized with hexafluoro-2-propanol. Sequence-specific assignments of the proton NMR spectrum of porcine motilin in 30% hexafluoro-2-propanol have been made by using two-dimensional NMR techniques. All backbone proton resonances (NH and alpha CH) and most of the side-chain resonances have been assigned by using double-quantum-filtered COSY, RELAYED-COSY, and NOESY experiments. Simulations of NOESY cross-peak intensities as a function of mixing time indicate that spin diffusion has a relatively small effect in peptides the size of motilin, thereby allowing the use of long mixing times to confidently make assignments and delineate secondary structure. Sequential alpha CH-NH and NH-NH NOESY connectivities were observed over a significant portion of the length of the peptide. A number of medium-range NOESY cross-peaks indicate that the peptide is folded into alpha-helix from Glu9 to Lys20, which agrees favorably with the 50% helical content determined from CD measurements. The intensities of selected NOESY cross-peaks relative to corresponding diagonal peaks were used to estimate a rotational correlation time of approximately 2.5 ns for the peptide, indicating that the peptide exists as a monomer in solution under the conditions used here.     

Direct estimation of base-pair exchange kinetics in oligo-DNA by a combination of NOESY and ROESY experiments.

A new method for the determination of the kinetics of exchange of the imino protons of DNA duplex is reported using a combination NOESY and ROESY experiments at short mixing times (< or = 20 ms). These results have been compared with the commonly used longitudinal relaxation approach through the T1 measurement. To calculate kex and pi ex by ROESY-NOESY experiment, the volume of the cross-peaks between imino protons and water in the NOESY and ROESY spectra have been measured separately from the magnetization term. This work shows that the present approach for the measurement of the kinetics of slow exchanging imino protons of DNA duplex is comparable to the saturation recovery experiment in which the exchange rate can be accelerated by the addition of a base catalyst. The present ROESY-NOESY approach has been found to be particularly useful and reasonably accurate for the measurement of exchange kinetics of both the fast- and slow-exchanging imino protons in DNA duplex both under non-physiological and physiological condition where the saturation recovery method can not be used.