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Derek Marsh

Publications and source records attributed to Derek Marsh.

At least 19 recordsLinked to original sources

TOAC spin labels in the backbone of alamethicin: EPR studies in lipid membranes.

Alamethicin is a 19-amino-acid residue hydrophobic peptide that produces voltage-dependent ion channels in membranes. Analogues of the Glu(OMe)(7,18,19) variant of alamethicin F50/5 that are rigidly spin-labeled in the peptide backbone have been synthesized by replacing residue 1, 8, or 16 with 2,2,6,6-tetramethyl-piperidine-1-oxyl-4-amino-4-carboxyl (TOAC), a helicogenic nitroxyl amino acid. Conventional electron paramagnetic resonance spectra are used to determine the insertion and orientation of the TOAC(n) alamethicins in fluid lipid bilayer membranes of dimyristoyl phosphatidylcholine. Isotropic (14)N-hyperfine couplings indicate that TOAC(8) and TOAC(16) are situated in the hydrophobic core of the membrane, whereas the TOAC(1) label resides closer to the membrane surface. Anisotropic hyperfine splittings show that alamethicin is highly ordered in the fluid membranes. Experiments with aligned membranes demonstrate that the principal diffusion axis lies close to the membrane normal, corresponding to a transmembrane orientation. Combination of data from the three spin-labeled positions yields both the dynamic order parameter of the peptide backbone and the intramolecular orientations of the TOAC groups. The latter are compared with x-ray diffraction results from alamethicin crystals. Saturation transfer electron paramagnetic resonance, which is sensitive to microsecond rotational motion, reveals that overall rotation of alamethicin is fast in fluid membranes, with effective correlation times <30 ns. Thus, alamethicin does not form large stable aggregates in fluid membranes, and ionic conductance must arise from transient or voltage-induced associations.

Alamethicin↗

Elastic curvature constants of lipid monolayers and bilayers.

Bending elasticity is an important property of lipid vesicles, non-lamellar lipid phases and biological membranes. Experimental values of the mean curvature moduli, k(c), of lipid bilayers and of the monolayer leaflets of inverted hexagonal (H(II)) phases of lipids are tabulated here for easy reference. Experimental estimates of the Gaussian curvature modulus, k (c), are also included. Consideration is given to the relation between the bending moduli of bilayers and the constituent monolayer leaflets. Useful mathematical relations involving the bending moduli and spontaneous curvature are summarized.

Elasticity↗

Curvature elasticity and refolding of OmpA in large unilamellar vesicles.

The stability of OmpA in large unilamellar vesicles of dilauroyl phosphatidylcholine was studied using different concentrations of urea. The effective energy of unfolding, as determined from refolding experiments, is greater than that for small sonicated unilamellar vesicles by an amount that is compatible with estimates of the elastic energy of highly curved vesicles. The on-rate for refolding and insertion is slower for large unilamellar vesicles than for small unilamellar vesicles, which indicates a contribution of vesicle strain also to the free energy of the transition state.

Bacterial Outer Membrane Proteins↗

Membrane elastic fluctuations and the insertion and tilt of beta-barrel proteins.

Folding of porin-like beta-barrel outer membrane proteins can be achieved in the presence of phospholipid vesicles, and takes place concurrently with incorporation into the membrane. The pronounced dependence found for the insertion of the protein OmpA on membrane thickness (Kleinschmidt, J. H., and L. K. Tamm. 2002. J. Mol. Biol. 324:319-330) is analyzed in terms of the effects of out-of-plane elastic fluctuations on the area dilation modulus (Evans, E., and W. Rawicz. 1990. Phys. Rev. Lett. 64:2094-2097). For unstrained large unilamellar vesicles, the elastic free energy for membrane insertion is predicted to depend on the fourth power of the membrane thickness. The influence of thermally induced bending fluctuations on the effective tilt of the OmpA beta-barrel in disaturated phosphatidylcholine membranes of different thicknesses (Ramakrishnan, M., J. Qu, C. L. Pocanschi, J. H. Kleinschmidt, and D. Marsh. 2005. Biochemistry. 44:3515-3523) is also considered. A contribution to the orientational order parameter that scales as the inverse second power of the membrane thickness is predicted.

Bacterial Outer Membrane Proteins↗

Lipid-protein interactions with the Na,K-ATPase.

Studies of lipid interactions with membranous Na,K-ATPase by using electron spin resonance spectroscopy in conjunction with spin-labelled lipids are reviewed. The lipid stoichiometry, selectivity and exchange dynamics at the lipid-protein interface can be determined, in addition to information on the configuration and rotational dynamics of the protein-associated lipid chains. These parameters, particularly the stoichiometry and selectivity, are related directly to the intramembranous structure of the Na,K-ATPase, and can be used to check the integrity of extensively trypsinised preparations.

Cardiolipins↗

Lipid conformation in crystalline bilayers and in crystals of transmembrane proteins.

Dihedral torsion angles evaluated for the phospholipid molecules resolved in the X-ray structures of transmembrane proteins in crystals are compared with those of phospholipids in bilayer crystals, and with the phospholipid conformations in fluid membranes. Conformations of the lipid glycerol backbone in protein crystals are not restricted to the gauche C1-C2 rotamers found invariably in phospholipid bilayer crystals. Lipid headgroup conformations in protein crystals also do not conform solely to the bent-down conformation, with gauche-gauche configuration of the phospho-diester, that is characteristic of phospholipid bilayer membranes. This suggests that the lipids that are resolved in crystals of membrane proteins are not representative of the entire lipid-protein interface. Much of the chain configurational disorder of the membrane-bound lipids in crystals arises from energetically disallowed skew conformations. This indicates a configurational heterogeneity in the lipids at a single binding site: eclipsed conformations occur also in some glycerol backbone torsion angles and C-C torsion angles in the lipid headgroups. Stereochemical violations in the protein-bound lipids are evidenced by one-third of the ester carboxyl groups in non-planar configurations, and certain of the carboxyls in the cis configuration. Some of the lipid structures in protein crystals have the incorrect enantiomeric configuration of the glycerol backbone, and many of the branched methyl groups in structures of the phytanyl chains associated with bacteriorhodopsin crystals are in the incorrect S-configuration.

Binding Sites↗

Association of alpha-synuclein and mutants with lipid membranes: spin-label ESR and polarized IR.

Alpha-synuclein is a presynaptic protein, the A53T and A30P mutants of which are linked independently to early-onset familial Parkinson's disease. The association of wild-type alpha-synuclein with lipid membranes was characterized previously by electron spin resonance (ESR) spectroscopy with spin-labeled lipids [Ramakrishnan, M., Jensen, P. H., and Marsh, D. (2003) Biochemistry 42, 12919-12926]. Here, we study the interaction of the A53T and A30P alpha-synuclein mutants and a truncated form that lacks the acidic C-terminal domain with phosphatidylglycerol bilayer membranes, using anionic phospholipid spin labels. The strength of the interaction with phosphatidylglycerol membranes lies in the order: wild type approximately truncated > A53T > A30P > fibrils approximately 0, and only the truncated form interacts with phosphatidylcholine membranes. The selectivity of the interaction of the mutant alpha-synucleins with different spin-labeled lipid species is reduced considerably, relative to the wild-type protein, whereas that of the truncated protein is increased. Polarized infrared (IR) spectroscopy is used to study the interactions of the wild-type and truncated proteins with aligned lipid membranes and additionally to characterize the fibrillar form. Wild-type alpha-synuclein is natively unfolded in solution and acquires secondary structure upon binding to membranes containing phosphatidylglycerol. Up to 30-40% of the amide I band intensity of the membrane-bound wild-type and truncated proteins is attributable to beta-sheet structure, at the surface densities used for IR spectroscopy. The remainder is alpha-helix and residual unordered structure. Fibrillar alpha-synuclein contains 62% antiparallel beta-sheet and is oriented on the substrate surface but does not interact with deposited lipid membranes. The beta-sheet secondary-structural elements of the wild-type and truncated proteins are partially oriented on the surface of membranes with which they interact.

Circular Dichroism↗

Time-resolved electron spin resonance studies of spin-labelled lipids in membranes.

Recently, developments in time-resolved spin-label electron spin resonance (ESR) spectroscopy have contributed considerably to the study of biomembranes. Two different applications of electron spin echo spectroscopy of spin-labelled phospholipids are reviewed here: (1) the use of partially relaxed echo-detected ESR spectra to study the librational lipid-chain motions in the low-temperature phases of phospholipid bilayers; (2) the use of electron spin echo envelope modulation spectroscopy to determine the penetration of water into phospholipid membranes. Results are described for phosphatidylcholine bilayer membranes, with and without equimolar cholesterol, that are obtained with phosphatidylcholine spin probes site-specifically labelled throughout the sn-2 chain.

Cholesterol↗

A divalent-ion binding site on the 16-kDa proton channel from Nephrops norvegicus--revealed by EPR spectroscopy.

As purified from the hepatopancreas of Nephrops norvegicus, the 16-kDa proton channel proteolipid is found to contain an endogenous divalent ion binding site that is occupied by Cu2+. The EPR spectrum has g-values and hyperfine splittings that are characteristic of type 2 Cu2+. The copper may be removed by extensive washing with EDTA. Titration with Ni2+ then induces spin-spin interactions with nitroxyl spin labels that are attached either to the unique Cys54, or to fatty acids intercalated in the membrane. Paramagnetic relaxation enhancement by the fast-relaxing Ni2+ is used to characterise the binding and to estimate distances from the dipolar interactions. The Ni2+-binding site on the protein is situated around 14-18 A from the spin label on Cys54, and is at a similar distance from a lipid chain spin-labelled on the 5 C-atom, but is more remote from the C-9 and C-14 positions of the lipid chains.

Animals↗

Orientation of TOAC amino-acid spin labels in alpha-helices and beta-strands.

The orientation of alpha-helices or beta-strands, e.g., in membranes, can be determined from EPR order parameters of (2,2,6,6-tetramethyl-piperidine-1-oxy-4-amino-4-carboxylic acid) TOAC amino-acid spin labels incorporated in the polypeptide backbone. This requires knowledge of the inclination of the nitroxide axes, relative to the alpha-helix or beta-strand axis. Crystal structures of TOAC-containing peptides are used to derive the spin-label orientation relative to refined alpha-poly-l-alanine and beta-poly-l-alanine structures. The spin-label z-axes of the two mirror-image TOAC twist-boat conformers are inclined at 13+/-2 degrees and 65+/-3 degrees , respectively, to the alpha-helix axis, or at 25+/-3 degrees and 32+/-3 degrees to the beta-strand axis.

Alanine↗

Oxygen profiles in membranes.

Transmembrane profiles of molecular oxygen in lipid bilayers are not only significant for membrane physiology and pathology, but also are essential to the determination of membrane protein structure by site-directed spin labeling. Oxygen profiles obtained with spin-labeled lipid chains have a Boltzmann sigmoidal dependence on the depth into each lipid leaflet, which represents a two-compartment distribution between outer and inner regions of the membrane, with a transfer free energy that depends linearly on distance from the dividing planes. Transmembrane profiles for intramembrane polarity, and for water penetration into the membrane, have an identical form, but are of the reverse sign. Comparison with recently published oxygen profiles from a site-specifically spin-labeled alpha-helical transmembrane peptide validates the use of spin-labeled lipids for all these profiles and provides the necessary bridge to generate the full bilayer from a single lipid leaflet.

Biophysics↗

Structural characterization of Na,K-ATPase from shark rectal glands by extensive trypsinization.

Extensive trypsinization of Na,K-ATPase from the salt gland of Squalus acanthias removes about half of the extramembranous protein mass of the alpha-subunit, while leaving the beta-subunit intact. Sequence analysis and epitope recognition of the remaining alpha-peptides show that transmembrane segments M1/M2 and M3/M4 are present when trypsinization is performed in either NaCl or RbCl. The M5/M6 segment and the intact 19-kDa peptide (M7-M10) are detected in Rb-trypsinized membranes but not in Na-trypsinized membranes. The L7/L8 loop is associated with Na-trypsinized membranes, indicating the presence of an M7/M8 or M8/M9 fragment. Freeze-fracture electron microscopy of both Rb- and Na-trypsinized membranes reveals intramembranous particles that indicate a retained cluster of peptides, even in the absence of an intact 19-kDa fragment. The rotational diffusion of covalently spin-labeled trypsinized complexes is studied in the presence of poly(ethylene glycol) or glycerol by using saturation transfer electron spin resonance. Rotational correlation times in aqueous poly(ethylene glycol) are longer than in glycerol solutions of the same viscosity and increase nonlinearly with the viscosity of the suspending medium, indicating that poly(ethylene glycol) induces aggregation of the tryptic peptides (and beta-subunit) within the membrane. The aggregates of enzyme trypsinized in the presence of NaCl are larger than those for enzyme trypsinized in RbCl, at both low and high aqueous viscosities. Similarities in mobility for native and Rb-trypsinized enzymes suggest either a change in average orientation of the spin-label upon trypsinization or that trypsinization leads to a reorganized protein structure that is more prone to aggregation.

Amino Acid Sequence↗

Stoichiometry of lipid interactions with transmembrane proteins--Deduced from the 3D structures.

The stoichiometry of the first shell of lipids interacting with a transmembrane protein is defined operationally by the population of spin-labeled lipid chains whose motion is restricted directly by the protein. Interaction stoichiometries have been determined experimentally for a wide range of alpha-helical integral membrane proteins by using spin-label ESR spectroscopy. Here, we determine the spatially defined number of first-shell lipids at the hydrophobic perimeter of integral membrane proteins whose 3D structure has been determined by X-ray crystallography and lipid-protein interactions characterized by spin-labeling. Molecular modeling is used to build a single shell of lipids surrounding transmembrane structures derived from the PDB. Constrained energy optimization of the protein-lipid assemblies is performed by molecular mechanics. For relatively small proteins (up to 7-12 transmembrane helices), the geometrical first shell corresponds to that defined experimentally by perturbation of the lipid-chain dynamics. For larger, multi-subunit alpha-helical proteins, the lipids perturbed directly by the protein may either exceed or be less in number than those that can be accommodated at the intramembranous perimeter. In these latter cases, the motionally restricted spin-labeled lipids can be augmented by intercalation, or can correspond to a specific subpopulation at the protein interface, respectively. For monomeric beta-barrel proteins, the geometrical lipid stoichiometry corresponds to that determined from lipid mobility for a 22-stranded barrel, but fewer lipids are motionally restricted than can be accommodated around an eight-stranded barrel. Deviations from the geometrical first shell, in the beta-barrel case, are for the smaller protein with a highly curved barrel.

Bacterial Outer Membrane Proteins↗

Water concentration profiles in membranes measured by ESEEM of spin-labeled lipids.

Electron spin-echo envelope modulation (ESEEM) spectroscopy of phospholipids spin-labeled systematically down the sn-2 chain was used to detect the penetration of water (D2O) into bilayer membranes of dipalmitoyl phosphatidylcholine with and without 50 mol % cholesterol. Three-pulse stimulated echoes allow the resolution of two superimposed 2H-ESEEM spectral components of different widths, for spin labels located in the upper part of the lipid chains. Quantum chemical calculations (DFT) and ESEEM simulations assign the broad spectral component to one or two D2O molecules that are directly hydrogen bonded to the N-O group of the spin label. Classical ESEEM simulations establish that the narrow spectral component arises from nonbonded water (D2O) molecules that are free in the hydrocarbon chain region of the bilayer membrane. The amplitudes of the broad 2H-ESEEM spectral component correlate directly with those of the narrow component for spin labels at different positions down the lipid chain, reflecting the local H-bonding equilibria. The D2O-ESEEM amplitudes decrease with position down the chain toward the bilayer center, displaying a sigmoidal dependence on position that is characteristic of transmembrane polarity profiles established by other less direct spin-labeling methods. The midpoint of the sigmoidal profile is shifted toward the membrane center for membranes without cholesterol, relative to those with cholesterol, and the D2O-ESEEM amplitude in the outer regions of the chain is greater in the presence of cholesterol than in its absence. For both membrane types, the D2O amplitude is almost vanishingly small at the bilayer center. The water-penetration profiles reverse correlate with the lipid-chain packing density, as reflected by 1H-ESEEM intensities from protons of the membrane matrix. An analysis of the H-bonding equilibria provides essential information on the binding of water molecules to H-bond acceptors within the hydrophobic interior of membranes. For membranes containing cholesterol, approximately 40% of the nitroxides in the region adjacent to the lipid headgroups are H bonded to water, of which ca. 15% are doubly H bonded. Corresponding H-bonded populations in membranes without cholesterol are ca. 20%, of which ca. 6% are doubly bonded.

Computer Simulation↗

Domain formation in sphingomyelin/cholesterol mixed membranes studied by spin-label electron spin resonance spectroscopy.

Interactions of palmitoylsphingomyelin with cholesterol in multilamellar vesicles have been studied over a wide range of compositions and temperatures in excess water by using electron spin resonance (ESR) spectroscopy. Spin labels bearing the nitroxide free radical group on the 5 or 14 C-atom in either the sn-2 stearoyl chain of phosphatidylcholine (predominantly 1-palmitoyl) or the N-stearoyl chain of sphingomyelin were used to determine the mobility and ordering of the lipids in the different phases. Two-component ESR spectra of the 14-position spin labels demonstrate the coexistence first of gel (L(beta)) and liquid-ordered (L(o)) phases and then of liquid-ordered and liquid-disordered (L(alpha)) phases, with progressively increasing temperature. These phase coexistences are detected over a limited range of cholesterol contents. ESR spectra of the 5-position spin labels register an abrupt increase in ordering at the L(alpha)-L(o) transition and a biphasic response at the L(beta)-L(o) transition. Differences in outer splitting between the C14-labeled sphingomyelin and phosphatidylcholine probes are attributed to partial interdigitation of the sphingomyelin N-acyl chains across the bilayer plane in the L(o) state. In the region where the two fluid phases, L(alpha) and L(o), coexist, the rate at which lipids exchange between phases (<<7 x 10(7) s(-)(1)) is much slower than translational rates in the L(alpha) phase, which facilitates resolution of two-component spectra.

Cholesterol↗

Structural characterization of copper(II) binding to alpha-synuclein: Insights into the bioinorganic chemistry of Parkinson's disease.

The aggregation of alpha-synuclein (AS) is characteristic of Parkinson's disease and other neurodegenerative synucleinopathies. We demonstrate here that Cu(II) ions are effective in accelerating AS aggregation at physiologically relevant concentrations without altering the resultant fibrillar structures. By using numerous spectroscopic techniques (absorption, CD, EPR, and NMR), we have located the primary binding for Cu(II) to a specific site in the N terminus, involving His-50 as the anchoring residue and other nitrogen/oxygen donor atoms in a square planar or distorted tetragonal geometry. The carboxylate-rich C terminus, originally thought to drive copper binding, is able to coordinate a second Cu(II) equivalent, albeit with a 300-fold reduced affinity. The NMR analysis of AS-Cu(II) complexes reveals the existence of conformational restrictions in the native state of the protein. The metallobiology of Cu(II) in Parkinson's disease is discussed by a comparative analysis with other Cu(II)-binding proteins involved in neurodegenerative disorders.

Circular Dichroism↗

Orientation of beta-barrel proteins OmpA and FhuA in lipid membranes. Chain length dependence from infrared dichroism.

The outer-membrane proteins OmpA and FhuA of Escherichia coli are monomeric beta-barrels of widely differing size. Polarized attenuated total reflection infrared spectroscopy has been used to determine the orientation of the beta-barrels in phosphatidylcholine host matrices of different lipid chain lengths. The linear dichroism of the amide I band from OmpA and FhuA in hydrated membranes generally increases with increasing chain length from diC(12:0) to diC(17:0) phosphatidylcholine, in both the fluid and gel phases. Measurements of the amide I and amide II dichroism from dry samples are used to deduce the strand tilt (beta = 46 degrees for OmpA and beta = 44.5 degrees for FhuA). These values are then used to deduce the order parameters, P(2)(cos alpha), of the beta-barrels from the amide I dichroic ratios of the hydrated membranes. The orientational ordering of the beta-barrels and their assembly in the membrane are discussed in terms of hydrophobic matching with the lipid chains.

Amides↗