ESR spectral changes induced by chlorpromazine in spin-labeled erythrocyte ghost membranes

chlorpromazine interacted preferentially with membrane proteins rather than membrane lipids in the initial incorporation into human erythrocyte ghosts, as demonstrated by means of the fluorescence quenching and a maleimide spin label. In this state the membrane fluidity increased. At higher concentrations of chlorpromazine, the membrane fluidity decreased and a motionally restricted signal from fatty acid spin labels appeared predominantly. However, no such signal appeared in protein-free vesicles. The temperature and pH dependences of the outer hyperfine splitting of this restricted signal were very similar to those of bovine serum albumin. On the basis of sodium dodecyl sulfate-polyacrylamide gel electrophoresis of chlorpromazine-treated and -untreated ghosts, it was found that there was no significant difference in membrane proteins between both samples except for the changes of a few bands which were not directly concerned with the occurrence of this restricted signal. These results suggest that the fatty acid spin labels bind preferably to membrane proteins as the lipid domain becomes packed with chlorpromazine.     

The effect of chlorpromazine on some properties DNA in solution.

The effect of chlorpromazine [2-chloro-10-(3-dimethylaminopropyl)-phenothiazine] on calf thymus DNA has been investigated by spectrophotometric, equilibrium dialysis, thermal denaturation, sedimentation and viscosity methods. The absorption spectra of DNA undergo two important changes upon binding to chlorpromazine, namely, the displacement of peaks to longer wavelength (ranging from 5-8 nm) and a decrease in the optical density. The extent of binding of chlorpromazine to native calf thymus DNA, AS MEASURED BY SPECTROPHOTOMETRIC METHOD, IS DECREASED WITH INCREASING SODIUM CHLORIDE Concentration. A curvature in the Scatchard plot suggests two types of binding processes. Chlorpromazine decreases the optical density at higher temperatures without affecting the Tm of DNA. In its presence, the absorption spectra of purine deoxynucleosides (dA, dG) and of deoxynucleotides (dAMP, dGMP) are modified, i.e., the maxima are displaced to longer wavelength (ranging from 5-17 nm) and there is a general decrease in the optical density. No such effect is observed with pyrimidine deoxynucleosides (dC, dT) and deoxy-nucleotides (dCMP, dTMP). A combination of electrostatic binding of the amino group of chlorpromazine sidechain with the negative phosphate groups of the DNA and a partial insertion of either of its two phenyl rings between the nucleotide base pairs of the DNA plus the binding caused by mutual interaction between different chlorpromazine molecules at higher concentration is proposed as a probable mode of binding of chlorpromazine to DNA.     

ESR spectral changes induced by chlorpromazine in spin-labeled erythrocyte ghost membranes

Chlorpromazine interacted preferentially with membrane proteins rather than membrane lipids in the initial incorporation into human erythrocyte ghosts, as demonstrated by means of the fluorescence quenching and a maleimide spin label. In this state the membrane fluidity increased. At higher concentrations of chlorpromazine, the membrane fluidity decreased and a motionally restricted signal from fatty acid spin labels appeared predominantly. However, no such signal appeared in protein-free vesicles. The temperature and pH dependences of the outer hyperfine splitting of this restricted signal were very similar to those of bovine serum albumin. On the basis of sodium dodecyl sulfate-polyacrylamide gel electrophoresis of chlorpromazine-treated and -untreated ghosts, it was found that there was no significant difference in membrane proteins between both samples except for the changes of a few bands which were not directly concerned with the occurrence of this restricted signal. These results suggest that the fatty acid spin labels bind preferably to membrane proteins as the lipid domain becomes packed with chlorpromazine.     

Effect of nucleotides and their analogues on essential light chains in myosin head

The domain movement in myosin head plays a decisive role in the energy transduction process of the muscle contraction. During hydrolysis of ATP, the specific formation of strong binding of myosin head for actin causes conformational changes. As a consequence, the light chain-binding motif generates the powerstroke. In our work maleimide spin labels were covalently attached to Cys-177 residue of ELC in subfragment-1 (S1). Our goal was to study the orientation dependence and the motion of S1, which were incorporated into glycerinated skeletal muscle fibres. The electron paramagnetic resonance spectroscopy (EPR) spectra of the probes depended strongly on the orientation of the fibre axis relative to the magnetic field, indicating that the essential light chain (ELC) and the neck were ordered. The probes were undergoing rapid motion within a cone. The half-width of the cone was estimated to be 65+/-5 degrees (SD, n=8). Addition of ADP affected little the hyperfine splitting and the angular spread of the probe distribution. In the presence of ADP and orthovanadate the intensity of the spectra decreased, which showed the dissociation of S1 and this was accompanied with the disappearance of the orientation dependence.     

Mixed membranes of sphingolipids and glycerolipids as studied by spin-label ESR spectroscopy. A search for domain formation

The temperature dependences of the ESR spectra from different positional isomers of sphingomyelin and of phosphatidylcholine spin-labeled in their acyl chain have been compared in mixed membranes composed of sphingolipids and glycerolipids. The purpose of the study was to identify the possible formation of sphingolipid-rich in-plane membrane domains. The principal mixtures that were studied contained sphingomyelin and the corresponding glycerolipid phosphatidylcholine, both from egg yolk. Other sphingolipids that were investigated were brain cerebrosides and brain gangliosides, in addition to sphingomyelins from brain and milk. The outer hyperfine splittings in the ESR spectra of sphingomyelin and of phosphatidylcholine spin-labeled on C-5 of the acyl chain were consistent with mixing of the sphingolipid and glycerolipid components, in fluid-phase membranes. In the gel phase of egg sphingomyelin and its mixtures with phosphatidylcholine, the outer hyperfine splittings of sphingomyelin spin-labeled at C-14 of the acyl chain of sphingomyelin are smaller than those of the corresponding sn-2 chain spin-labeled phosphatidylcholine. This is in contrast to the situation with sphingomyelin and phosphatidylcholine spin-labeled at C-5, for which the outer hyperfine splitting is always greater for the spin-labeled sphingomyelin. The behavior of the C-14 spin-labels is attributed to a different geometry of the acyl chain attachments of the sphingolipids and glycerolipids that is consistent with their respective crystal structures. The two-component ESR spectra of sphingomyelin and phosphatidylcholine spin-labeled at C-14 of the acyl chain directly demonstrate a broad two-phase region with coexisting gel and fluid domains in sphingolipid mixtures with phosphatidylcholine. Domain formation in membranes composed of sphingolipids and glycerolipids alone is related primarily to the higher chain-melting transition temperature of the sphingolipid component.     

Identification of the substrate radical intermediate derived from ethanolamine during catalysis by ethanolamine ammonia-lyase

Rapid-mix freeze-quench (RMFQ) methods and electron paramagnetic resonance (EPR) spectroscopy have been used to characterize the steady-state radical in the deamination of ethanolamine catalyzed by adenosylcobalamin (AdoCbl)-dependent ethanolamine ammonia-lyase (EAL). EPR spectra of the radical intermediates formed with the substrates, [1-13C]ethanolamine, [2-13C]ethanolamine, and unlabeled ethanolamine were acquired using RMFQ trapping methods from 10 ms to completion of the reaction. Resolved 13C hyperfine splitting in EPR spectra of samples prepared with [1-13C]ethanolamine and the absence of such splitting in spectra of samples prepared with [2-13C]ethanolamine show that the unpaired electron is localized on C1 (the carbinol carbon) of the substrate. The 13C splitting from C1 persists from 10 ms throughout the time course of substrate turnover, and there was no evidence of a detectable amount of a product like radical having unpaired spin on C2. These results correct an earlier assignment for this radical intermediate [Warncke, K., et al. (1999) J. Am. Chem. Soc. 121, 10522-10528]. The EPR signals of the substrate radical intermediate are altered by electron spin coupling to the other paramagnetic species, cob(II)alamin, in the active site. The dipole-dipole and exchange interactions as well as the 1-13C hyperfine splitting tensor were analyzed via spectral simulations. The sign of the isotropic exchange interaction indicates a weak ferromagnetic coupling of the two unpaired electrons. A Co2+-radical distance of 8.7 A was obtained from the magnitude of the dipole-dipole interaction. The orientation of the principal axes of the 13C hyperfine splitting tensor shows that the long axis of the spin-bearing p orbital on C1 of the substrate radical makes an angle of approximately 98 degrees with the unique axis of the d(z2) orbital of Co2+.     

ESR spectral analysis of the molecular motion of spin labels in lipid bilayers and membranes based on a model in terms of two angular motional parameters and rotational correlation times.

Electron spin resonance (ESR) spectral line shapes are calculated for a nitroxide spin-labeled molecule undergoing rapid restricted rotations (twisting) about its long molecular axis while simultaneously tumbling within a cone. Explicit expressions are derived for the hyperfine splittings and g-values, as well as for the secular contributions to the motionally modulated linewidths. The present model is useful for analyzing the restricted twisting and tumbling motions, and rotational correlation times, of spin-labeled molecules in bilayers. Simulated spectra compare well with experimental spectra of lecithin bilayers marked with cholestane spin label, over a wide temperature range.     

Organization of nucleosomes and spacer DNA in chromatin fibres

In this paper we analyse in detail the orientation of X-ray diffraction diagrams obtained from the following materials: nucleosome cores, whole nuclei and the sodium and thallium salts of H1-depleted nucleohistone and of briefly digested chromatin. Our analysis indicates that spacer DNA is organized in bundles of parallel segments which contribute to the equatorial maxima in the diagrams. Several models are compatible with this organization, in particular a modified solenoid model in which the central part is filled with such a bundle of spacer DNA segments parallel to the axis of the fibre. It is also shown that spacer DNA is covered by histones, probably the N-terminal regions. This observation indicates that the differential activity of nucleases on chromatin is strongly influenced by conformational features of DNA. An analysis of the orientation of the low angle rings found in the X-ray diffraction patterns of H1-depleted nucleohistone shows that the 11 nm peak has maxima which are ～ 0.007 nm^?1 off the meridian. The 5.5 and 8 nm peaks have a meridional maximum plus two side maxima which occur at spacings between 0.02 and 0.055 nm^?1 from the meridian, depending on the conditions. A comparison of these results with those reported by Finch et al.¹ for crystals indicates that in fibres the nucleosome cores are arranged with their short axis perpendicular to the axis of the fibre. Some evidence on the path of DNA in the nucleosome cores is also obtained.     

A detailed study of Li-DNA fibres at various salt concentrations reveals a non-helical B-DNA and a possible similarity of solution and solid state structures

A thorough investigation of salt concentration dependence of lithium DNA fibres is made using X-ray diffraction. While for low salt the C-form pattern is obtained, crystalline B-type diffraction patterns result on increasing the salt concentration. The salt content in the gel (from which fibres are drawn) is estimated by equilibrium dialysis using the Donnan equilibrium principle. The salt range giving the best crystalline B pattern is determined. It is found that in this range meridional reflections occur on the fourth and sixth layer lines. In addition, the tenth layer meridian is absent at a particular salt concentration. These results strongly suggest the presence of non-helical features in the DNA molecule. Preliminary analysis of the diffraction patterns indicates a structural variability within the B-form itself. Further, the possibility of the structural parameters of DNA being similar in solid state and in solution is discussed.     

Gelation properties of extruded lemon cell walls and their water-soluble pectins

The amount of water-soluble pectins was largely increased after extrusion-cooking of lemon fibres. These pectins showed the ability to form a gel in the presence of sucrose and at acidic pH. The gels obtained with the water-extracted pectins after extrusion-cooking and with pectins acid-extracted on a laboratory scale were softer than those prepared with commercial citrus pectins. The water-extracted pectins after extrusion-cooking and the pectins acid-extracted on a laboratory scale contained long neutral side-chains and required a higher sucrose concentration to gel than the commercial citrus pectins. The extruded lemon fibres showed the ability to form gels in the presence of sucrose and at acidic pH. The gels obtained with the extruded fibres containing some water-solube pectins of high molecular weight were stronger than those obtained with the extruded fibres containing higher amounts of more depolymerised water-soluble pectins. The extruded fibres containing 12.5–14.9% of water-soluble pectins of high molecular weight (intrinsic viscosity: 413–504 mL/g) were those showing the better gelation properties.     

Electron spin resonance studies of radicals obtained by the reaction of alpha-tocopherol and its model compound with superoxide ion.

alpha-Tocopherol (vitamin E) and its model compound, 6-hydroxy-2,2,5,7,8-pentamethylchroman, were found to be oxidized by O2- to yield free radicals which were detected at room temperature by ESR spectroscopy. The ESR spectra of these radicals showed seven main lines with additional hyperfine structure and have the same g-values at 2.0046. Assignments of the ESR spectra were done on the basis of the spectra of the free radicals of deuterated hydroxypentamethylchroman obtained from the same reaction with O2-. The radicals observed are chromanoxyls generated by the abstraction of hydrogen from the 6-hydroxy group of tocopherols.     

Electron nuclear double resonance studies of radicals produced by the PbO2 oxidation of α-tocopherol and its model compound in solution

The electron nuclear double resonance (ENDOR) spectra of chromanoxyl radicals obtained by the PbO₂ oxidation of α-tocopherol and its model compound were observed in t-butylbenzene, and the proton hyperfine coupling constants were correctly determined. Each of the two β- and γ-methylene protons in the chromanoxyl ring shows an equivalent hyperfine splitting, suggesting that the heterocyclic ring attached to the aromatic ring are coplanar with the plane of the aromatic system. A comparison of the hyperfine couplings in α-tocopheroxyl radical and its model shows that the introduction of a long-isoprenoid-chain in the α-tocopherol in place of a methyl group in the model compound has very little effect on the unpaired spin distribution or molecular structure of the chromanoxyl skeleton. The results of McLachlan molecular orbital (MO) calculations were found to be in satisfactory agreement with the ‘experimental’ spin densities evaluated from the hyperfine coupling constants.     

Study of binding of spin probes of the carboline and benzocarboline series to bovine serum albumin

The dependence of the external and internal wide hyperfine extreme shifts of the ESR spectra on temperature and viscosity for spin-probes in solution of BSA was studied. Seven homologous spin-probes of carboline and benzocarboline derivatives were used. The obtained dependences are a consequence of the involvement of the spin-probe in two types of rotation: an anisotropic fast reorientation with tau > 10(-9) s with respect to a macromolecule and the isotropic one with tau > 10(-8) s due to rotation of the macromolecule itself. It was shown, that extrapolation values of a separation between hyperfine extreme do not reflect the degree of the immediate spin-probe environment polarity, but are determined by the hyperfine tenzor partial averaging as a result of the rapid anisotropic reorientation of the spin-probe. All spin-probes used were shown to be bound by the BSA molecule in the near vicinity of the tryptophan residue. The rotation correlation time of the BSA molecule was determined to be equal to 40 ns.     

An examination of the cyanide derivative of bovine superoxide dismutase with electron-nuclear double resonance

The Cu(II) sites of native, azido- and cyano-derivatives of bovine superoxide dismutase (superoxide:superoxide oxidoreductase, EC 1.15.1.1) have been examined by electron-nuclear double resonance (ENDOR). The ENDOR spectrum of the native protein taken at the g parallel extreme shows resolved structure due to the directly coordinated N-atoms of the histidine ligands. These spectra are too complex for interpretation but suggest inequivalent coupling between the electronic spin and the four ligand N-atoms. By contrast, the azido protein reveals one type of nitrogen with well-resolved hyperfine and quadrupole splittings (Azz = 37.9 +/- 1 MHz, Pzz = 1.54 +/- 0.02 MHz), and the cyano from reveals one well-resolved set of nitrogen lines (Azz = 47.8 +/- 0.4 MHz, Pzz = 1.62 +/- 0.01 MHz) and one type of partially resolved nitrogen (Azz = 37.0 +/- 1 MHz). The cyano form also reveals a complex spectrum in the low-frequency domain (1-10 MHz). Through isotopic substitution and computer stimulation, the spectrum is shown to be a composite of the ENDOR from the remote imidazole nitrogens and the cyanide nitrogen. The component of the hyperfine constant perpendicular to the C14N bonds axis is A perpendicular N = 3.9 +/- 0.3 MHz and along the bond axis is A perpendicular N approximately equal to 5.7 MHz. The quadrupole interaction appears to be greatest along the CN axis with Qz'z' = 1.0 +/- 0.1 MHz and Qx'x'y'y' approximately 0. Based on an analysis of the hyperfine and quadrupole interactions seen at two extremes of the electron paramagnetic spectrum, we propose a square-planar arrangement of three imidazole nitrogen and one CN- carbon around the copper. Within this plane two imidazole nitrogens are strongly coupled and magnetically equivalent, the third is inequivalent (slightly weaker hyperfine interactions) and forms a trans relationship with the cyanide. This model is consistent with other observations on the cyano-derivative.     

Circular dichroism of flow-oriented nucleic acids. II. Comparison between observed and calculated spectra.

The ultraviolet circular dichroism (CD) of oriented DNA and RNA molecules is calculated by an extension of Johnson and Tinoco's theory [(1969) Biopolymers 7 , 727–749] for unoriented molecules. The calculations are carried out for molecular models of A-DNA, B-DNA, planar B-DNA, C-DNA, and RNA-11-α. The calculated curves are compared to measured spectra [(1975) J. Mol. Biol. 92 , 449–466] Chung and Holzwarth, for oriented solutions of DNA in buffer, DNA in 6 M LiCl or in ethylene glycol, and double-stranded viral RNA. The calculation, which considers only base–base interactions, predicts that the CD of B-DNA, measured with light propagating parallel to the helix axis, should be large and semiconservative, whereas the CD for light propagating perpendicular to the helix axis should be nonconservative. These predictions agree qualitatively with the experimental observations for DNA in buffer; agreement improves if one assumes the bases to be exactly perpendicular to the helix axis. For the other geometries, agreement is less satisfactory, but qualitative agreement with experiment is obtained and the signs of the specific CD spectra are in accord with observations.     

Simulation of the S2 state multiline electron paramagnetic resonance signal of photosystem II: a multifrequency approach.

The S2 state electron paramagnetic resonance (EPR) multiline signal of Photosystem II has been simulated at Q-band (35 Ghz), X-band (9 GHz) and S-band (4 GHz) frequencies. The model used for the simulation assumes that the signal arises from an essentially magnetically isolated MnIII-MnIV dimer, with a ground state electronic spin ST = 1/2. The spectra are generated from exact numerical solution of a general spin Hamiltonian containing anisotropic hyperfine and quadrupolar interactions at both Mn nuclei. The features that distinguish the multiline from the EPR spectra of model manganese dimer complexes (additional width of the spectrum (195 mT), additional peaks (22), internal "superhyperfine" structure) are plausibly explained assuming an unusual ligand geometry at both Mn nuclei, giving rise to normally forbidden transitions from quadrupole interactions as well as hyperfine anisotropy. The fitted parameters indicate that the hyperfine and quadrupole interactions arise from Mn ions in low symmetry environments, corresponding approximately to the removal of one ligand from an octahedral geometry in both cases. For a quadrupole interaction of the magnitude indicated here to be present, the MnIII ion must be 5-coordinate and the MnIV 5-coordinate or possibly have a sixth, weakly bound ligand. The hyperfine parameters indicate a quasi-axial anisotropy at MnIII, which while consistent with Jahn-Teller distortion as expected for a d4 ion, corresponds here to the unpaired spin being in the ligand deficient, z direction of the molecular reference axis. The fitted parameters for MnIV are very unusual, showing a high degree of anisotropy not expected in a d3 ion. This degree of anisotropy could be qualitatively accounted for by a histidine ligand providing pi backbonding into the metal dxy orbital, together with a weakly bound or absent ligand in the x direction.     

A spin label that binds to myosin heads in muscle fibers with its principal axis parallel to the fiber axis.

We have used an indane-dione spin label (2-[-oxyl-2,2,5,5-tetramethyl-3-pyrrolin-3-yl)methenyl]in dane-1,3-dione), designated InVSL, to study the orientation of myosin heads in bundles of chemically skinned rabbit psoas muscle fibers, with electron paramagnetic resonance (EPR) spectroscopy. After reversible preblocking with 5,5'-dithiobis(2-nitro-benzoic acid) (DTNB), we were able to attach most of the spin label covalently and rigidly to either Cys 707 (SH1) or Cys 697 (SH2) on myosin heads. EPR spectra of labeled fibers contained substantial contributions from both oriented and disordered populations of spin labels. Similar spectra were obtained from fibers decorated with InVSL-labeled myosin heads (subfragment 1), indicating that virtually all the spin labels in labeled fibers are on the myosin head. We specifically labeled SH2 with InVSL after reversible preblocking of the SH1 sites with 1-fluoro-2,4-dinitrobenzene (FDNB), resulting in a spectrum that indicated only disordered spin labels. Therefore, the oriented and disordered populations correspond to labels on SH1 and SH2, respectively. The spectrum of SH2-bound labels was subtracted to produce a spectrum corresponding to SH1-bound labels, which was used for further analysis. For this corrected spectrum, the angle between the fiber axis and the principal axis of the spin label was fitted well by a Gaussian distribution centered at theta o = 11 +/- 1 degree, with a full width at half-maximum of delta theta = 15 +/- 2 degrees. The unique orientation of InVSL, with its principal axis almost parallel to the fiber axis, makes it complementary to spin labels previously studied in this system. This label can provide unambiguous information about axial rotations of myosin heads, since any axial rotation of the head must be reflected in the same axial rotation of the principal axis of the probe, thus changing the hyperfine splitting. Therefore, InVSL-labeled fibers have ideal properties needed for further exploration myosin head orientation and rotational motion in muscle.     

Chlorpromazine: a potential anticancer agent?

The antipsychotic drug chlorpromazine causes scission of the DNA in PY815 mouse mastocytoma cells or isolated PY815 cell nuclei and the broken DNA reseals when chlorpromazine is removed from nuclei. These properties suggest that chlorpromazine interferes with topoisomerase action as do several other DNA-intercalating anti-cancer drugs. However, protein is not associated with the broken DNA after chlorpromazine treatment suggesting a different mode of action on the topoisomerase. Reasons why chlorpromazine may have potential as anti-cancer agent are considered.     

ESR spectroscopy of flow-oriented cation radicals of phenothiazine derivatives and phenoxathiin intercalated in DNA.

Several derivatives of the phenothiazine cation radicals intercalated into DNA have been investigated using a new flow orientation technique. The anisotropic hyperfine coupling constants of both the parallel and the perpendicular orientation relative to the magnetic field were measured and compared to previous results, which used different techniques. The phenoxathiin cation radical could also be stabilized by intercalation into DNA at pH 4, but the orientation technique revealed no further information due to the poor resolution of the experimental spectra.