Biophysical characterization of the interaction of high-density lipoprotein (HDL) with endotoxins.

The interaction of bacterial endotoxins [lipopolysaccharide (LPS) and the 'endotoxic principle' lipid A], with high-density lipoprotein (HDL) from serum was investigated with a variety of physical techniques and biological assays. HDL exhibited an increase in the gel to liquid crystalline phase transition temperature Tc and a rigidification of the acyl chains of the endotoxins as measured by Fourier-transform infrared spectroscopy and differential scanning calorimetry. The functional groups of the endotoxins interacting with HDL are the phosphates and the diglucosamine backbone. The finding of phosphates as target groups is in accordance to measurements of the electrophoretic mobility showing that the zeta potential decreases from -50 to -60 mV to -20 mV at binding saturation. The importance of the sugar backbone as further target structure is in accordance with the remaining negative potential and competition experiments with polymyxin B (PMB) and phase transition data of the system PMB/dephosphorylated LPS. Furthermore, endotoxin binding to HDL influences the secondary structure of the latter manifesting in a change from a mixed alpha-helical/beta-sheet structure to a predominantly alpha-helical structure. The aggregate structure of the lipid A moiety of the endotoxins as determined by small-angle X-ray scattering shows a change of a unilamellar/inverted cubic into a multilamellar structure in the presence of HDL. Fluorescence resonance energy transfer data indicate an intercalation of pure HDL, and of [LPS]-[HDL] complexes into phospholipid liposomes. Furthermore, HDL may enhance the lipopolysaccharide-binding protein-induced intercalation of LPS into phospholipid liposomes. Parallel to these observations, the LPS-induced cytokine production of human mononuclear cells and the reactivity in the Limulus test are strongly reduced by the addition of HDL. These data allow to develop a model of the [endotoxin]/[HDL] interaction.     

Biophysical characterization of synthetic rhamnolipids

Synthetic rhamnolipids, derived from a natural diacylated glycolipid, RL-2,2(14), produced by Burkholderia (Pseudomonas) plantarii, were analyzed biophysically. Changes in the chemical structures comprised variations in the length, the stereochemistry and numbers of the lipid chains, numbers of rhamnoses, and the occurrence of charged or neutral groups. As relevant biophysical parameters, the gel (beta) to liquid crystalline (alpha) phase behavior of the acyl chains of the rhamnoses, their three-dimensional supramolecular aggregate structure, and the ability of the compounds to intercalate into phospholipid liposomes in the absence and presence of lipopolysaccharide-binding protein were monitored. Their biological activities were examined as the ability to induce cytokines in human mononuclear cells and to induce chemiluminescence in monocytes. Depending on the particular chemical structures, the physicochemical parameters as well as the biological test systems show large variations. This relates to the acyl chain fluidity, aggregate structure, and intercalation ability, as well as the bioactivity. Most importantly, the data extend our conformational concept of endotoxicity, based on the intercalation of naturally originating amphiphilic virulence factors into membranes from immune cells. This 'endotoxin conformation', produced by amphiphilic molecules with a hydrophilic charged backbone and apolar hydrophobic moiety, and adopting inverted cubic aggregate structures, causes high mechanical stress in target immune cells on integral proteins, eventually leading to cell activation. Furthermore, biologically inactive rhamnolipids with lamellar aggregate structures antagonize the endotoxin-induced activity in a way similar to lipid A-derived antagonists.     

Temperature dependence of dynamics and thermodynamics of the regulatory domain of human cardiac troponin C

Binding of Ca(2+) to the regulatory domain of troponin C (TnC) in cardiac muscle initiates a series of protein conformational changes and modified protein-protein interactions that initiate contraction. Cardiac TnC contains two Ca(2+) binding sites, with one site being naturally defunct. Previously, binding of Ca(2+) to the functional site in the regulatory domain of TnC was shown to lead to a decrease in conformational entropy (TDeltaS) of 2 and 0.5 kcal mol(-1) for the functional and nonfunctional sites, respectively, using (15)N nuclear magnetic resonance (NMR) relaxation studies [Spyracopoulos, L., et al. (1998) Biochemistry 37, 18032-18044]. In this study, backbone dynamics of the Ca(2+)-free regulatory domain are investigated by backbone amide (15)N relaxation measurements at eight temperatures from 5 to 45 degrees C. Analysis of the relaxation measurements yields an order parameter (S(2)) indicating the degree of spatial restriction for a backbone amide H-N vector. The temperature dependence of S(2) allows estimation of the contribution to protein heat capacity from pico- to nanosecond time scale conformational fluctuations on a per residue basis. The average heat capacity contribution (C(p,j)) from backbone conformational fluctuations for regions of secondary structure for the regulatory domain of cardiac apo-TnC is 6 cal mol(-1) K(-1). The average heat capacity for Ca(2+) binding site 1 is larger than that for site 2 by 1.3 +/- 0.8 cal mol(-1) K(-1), and likely represents a mechanism where differences in affinity between Ca(2+) binding sites for EF hand proteins can be modulated.     

Structural transitions in short-chain lipid assemblies studied by (31)P-NMR spectroscopy

The self-assembled supramolecular structures of diacylphosphatidylcholine (diC(n)PC), diacylphosphatidylethanolamine (diC(n)PE), diacylphosphatidyglycerol (diC(n)PG), and diacylphosphatidylserine (diC(n)PS) were investigated by (31)P nuclear magnetic resonance (NMR) spectroscopy as a function of the hydrophobic acyl chain length. Short-chain homologs of these lipids formed micelles, and longer-chain homologs formed bilayers. The shortest acyl chain lengths that supported bilayer structures depended on the headgroup of the lipids. They increased in the order PE (C(6)) < PC (C(9)) < or = PS (C(9) or C(10)) < PG (C(11) or C(12)). This order correlated with the effective headgroup area, which is a function of the physical size, charge, hydration, and hydrogen-bonding capacity of the four headgroups. Electrostatic screening of the headgroup charge with NaCl reduced the effective headgroup area of PS and PG and thereby decreased the micelle-to-bilayer transition of these lipid classes to shorter chain lengths. The experimentally determined supramolecular structures were compared to the assembly states predicted by packing constraints that were calculated from the hydrocarbon-chain volume and effective headgroup area of each lipid. The model accurately predicted the chain-length threshold for bilayer formation if the relative displacement of the acyl chains of the phospholipid were taken into account. The model also predicted cylindrical rather than spherical micelles for all four diacylphospholipid classes and the (31)P-NMR spectra provided evidence for a tubular network that appeared as an intermediate phase at the micelle-to-bilayer transition. The free energy of micellization per methylene group was independent of the structure of the supramolecular assembly, but was -0.95 kJ/mol (-0.23 kcal/mol) for the PGs compared to -2.5 kJ/mol (-0.60 kcal/mol) for the PCs. The integral membrane protein OmpA did not change the bilayer structure of thin (diC(10)PC) bilayers.     

Biophysical characterization of triacyl monosaccharide lipid a partial structures in relation to bioactivity

Synthetic triacyl glucosamine monosaccharide lipid A part structures corresponding to the non-reducing moiety of enterobacterial lipid A with an acyloxyacyl chain linked to position 3 of the glucosamine and an unbranched chain linked to position 2 (group 1) and vice versa (group 2) were analyzed biophysically: Fourier-transform infrared spectroscopy was performed to characterize the gel-to-liquid crystalline phase transition, the phosphate band contour, and the orientation of the glucosamine with respect to the membrane surface. Small-angle x-ray diffraction was applied for the elucidation of the supramolecular aggregate structure and, with that, of the molecular shape. With fluorescence resonance energy transfer the lipopolysaccharide-binding protein (LBP)-mediated intercalation of the lipid A partial structures into phospholipid liposomes was monitored. The physical data clearly exhibit a classification of the synthetic compounds into two groups: group 1 compounds have sharp phase transitions, indicating dense acyl chain packing and an inclination of the glucosamine backbone with respect to the membrane surface of 30 degrees with the phosphate buried in the membrane. Group 2 compounds have a very broad phase transition, indicating poorly packed acyl chains, and an inclination of -30 degrees with the phosphate group sticking outward. For the first group unilamellar phases are observed superimposed by a non-lamellar structure, and for the second one only multilamellar aggregate structures. The cytokine-inducing capacity in human mononuclear cells is relatively high for the first group and low or absent for the second group. Based on these data a model of the intra and intermolecular conformations is proposed which also extends the concept of "endotoxic conformation."     

Conformational energy and structure in canonical and noncanonical forms of tRNA determined by temperature analysis of the rate of s(4)U8-C13 photocrosslinking

Bacterial tRNAs frequently have 4-thiouridine (s(4)U) modification at position 8, which is adjacent to the C13-G22-m(7)G46 base triple in the elbow region of the tRNA tertiary structure. Irradiation with light in the UVA range induces an efficient photocrosslink between s(4)U8 and C13. The temperature dependence of the rate constants for photocrosslinking between the s(4)U8 and C13 has been used to investigate the tRNA conformational energy and structure in Escherichia coli tRNA(Val), tRNA(Phe), and tRNA(fMet) under different conditions. Corrections have been made in the measured rate constants to compensate for differences in the excited state lifetimes due to tRNA identity, buffer conditions, and temperature. The resulting rate constants are related to the rate at which the s(4)U8 and C13 come into the alignment needed for photoreaction; this depends on an activation energy, attributable to the conformational potential energy that occurs during the photoreaction, and on the extent of the structural change. Different photocrosslinking rate constants and temperature dependencies occur in the three tRNAs, and these differences are due both to modest differences in the activation energies and in the apparent s(4)U8-C13 geometries. Analysis of tRNA(Val) in buffers without Mg(2+) indicate a smaller activation energy (~13 kJ mol(-1)) and a larger apparent s(4)U8-C13 distance (~12 A) compared to values for the same parameters in buffers with Mg(2+) (~26 kJ mol(-1) and 0.36 A, respectively). These measurements are a quantitative indication of the strong constraint that Mg(2+) imposes on the tRNA flexibility and structure.     

Investigation into the acyl chain packing of endotoxins and phospholipids under near physiological conditions by WAXS and FTIR spectroscopy

The acyl chain packing of various endotoxins and phospholipids was monitored via the main wide-angle reflection between 0.410 and 0.460 nm by wide-angle X-ray scattering (WAXS) and via the absorption band of the symmetric stretching vibration of the methylene groups v(s)(CH(2)) around 2849 to 2853 cm(-1) by Fourier-transform infrared spectroscopy. The lipids investigated included various rough mutant (R) and smooth form (S) lipopolysaccharides (LPS) differing in the length of the sugar portion, lipid A, the "endotoxic principle" of LPS, and various saturated and unsaturated phospholipids with different head groups under a near physiological (>/=85%) water content. The packing density of the saturated endotoxin acyl chains is lower than those of saturated phospholipids but similar to those of monounsaturated phospholipids, each in the gel phase. The hydrophobic moiety of endotoxins thus exhibits significant conformational disorder already in the gel phase. The acyl chain packing of the endotoxins decreases with increasing length of the sugar chain lengths, which seems to be relevant to the observed differences in biological activity. For Re-LPS with different counterions (salt forms), in the presence of externally added cations or at reduced water content (50%), no change of the acyl chain packing density is deduced in the X-ray data, although the FT-IR data indicate its increase. The position of the v(s)(CH(2)) vibration is, thus, only a relative measure of lipid order, in particular when lipids with different head groups and in the presence of external agents are compared.     

Physicochemical characterization of carboxymethyl lipid A derivatives in relation to biological activity

Lipopolysaccharide (LPS) from the outer membrane of Gram-negative bacteria belongs to the most potent activators of the mammalian immune system. Its lipid moiety, lipid A, the 'endotoxic principle' of LPS, carries two negatively charged phosphate groups and six acyl chain residues in a defined asymmetric distribution (corresponding to synthetic compound 506). Tetraacyl lipid A (precursor IVa or synthetic 406), which lacks the two hydroxylated acyl chains, is agonistically completely inactive, but is a strong antagonist to bioactive LPS when administered to the cells before LPS addition. The two negative charges of lipid A, represented by the two phosphate groups, are essential for agonistic as well as for antagonistic activity and no highly active lipid A are known with negative charges other than phosphate groups. We hypothesized that the phosphate groups could be substituted by other negatively charged groups without changing the endotoxic properties of lipid A. To test this hypothesis, we synthesized carboxymethyl (CM) derivatives of hexaacyl lipid A (CM-506 and Bis-CM-506) and of tetraacyl lipid A (Bis-CM-406) and correlated their physicochemical with their endotoxic properties. We found that, similarly to compounds 506 and 406, also for their carboxymethyl derivatives a particular molecular ('endotoxic') conformation and with that, a particular aggregate structure is a prerequisite for high cytokine-inducing capacity and antagonistic activity, respectively. In other parameters such as acyl chain melting behaviour, antibody binding, activity in the Limulus lysate assay, and partially the binding of 3-deoxy-D-manno-oct-2-ulosonic acid transferase, strong deviations from the properties of the phosphorylated compounds were observed. These data allow a better understanding of endotoxic activity and its structural prerequisites.     

A Fourier transform infrared spectroscopic study of the interaction of alkaline earth cations with the negatively charged phospholipid 1, 2-dimyristoyl-sn-glycero-3-phosphoglycerol

The interaction of aqueous phospholipid dispersions of negatively charged 1,2-dimyristoyl-sn-glycero-3-phosphoglycerol, sodium salt (DMPG) with the divalent cations Mg(2+), Ca(2+) and Sr(2+) at equimolar ratios in 100 mM NaCl at pH 7 was investigated by Fourier transform infrared spectroscopy. The binding of the three cations induces a crystalline-like gel phase with highly ordered and rigid all-trans acyl chains. These features are observed after storage below room temperature for 24 h. When the gel phase is heated after prolonged incubation at low temperature phase transitions into the liquid crystalline phase are observed at 58 degrees C for the DMPG:Sr(2+), 65 degrees C for the DMPG:Mg(2+), and 80 degrees C for the DMPG:Ca(2+) complex. By subsequent cooling from temperatures above T(m) these complexes retain the features of a liquid crystalline phase with disordered acyl chains until a metastable gel phase is formed at temperatures between 38 and 32 degrees C. This phase is characterized by predominantly all-trans acyl chains, arranged in a loosely packed hexagonal or distorted hexagonal subcell lattice. Reheating the DMPG:Sr(2+) samples after a storage time of 2 h at 4 degrees C results in the transition of the metastable gel to the liquid crystalline phase at 35 degrees C. This phase transition into the liquid crystalline state at 35 degrees C is also observed for the Mg(2+) complex. However, for DMPG:Mg(2+) at higher temperatures, a partial recrystallization of the acyl chains occurs and the high temperature phase transition at 65 degrees C is also detected. In contrast, DMPG:Ca(2+) exhibits only the phase transition at 80 degrees C from the crystalline gel into the fluid state upon reheating. Below 20 degrees C, the rate of conversion from the metastable gel to a thermodynamically stable, crystalline-like gel phase decreases in the order Ca(2+)&z. Gt;Mg(2+)>Sr(2+). This conversion into the crystalline gel phase is accompanied by a complete dehydration of the phosphate groups in DMPG:Mg(2+) and by a reorientation of the polar lipid head groups in DMPG:Ca(2+) and in DMPG:Sr(2+). The primary binding sites of the cations are the PO(2)(-) groups of the phosphodiester moiety. Our infrared spectroscopic results suggest a deep penetration of the divalent cations into the polar head group region of DMPG bilayers, whereby the ester carbonyl groups, located in the interfacial region of the bilayers, are indirectly affected by strong hydrogen bonding of immobilized water molecules. In the liquid crystalline phase, the interaction of all three cations with DMPG is weak, but still observable in the infrared spectra of the DMPG:Ca(2+) complex by a slight ordering effect induced in the acyl chains, when compared to pure DMPG liposomes.     

Kinetic and thermodynamic studies of tet repressor-tetracycline interaction

Stopped-flow measurements have been employed to study the kinetics of the conformational changes in TetR (B) induced by tetracycline binding with and without Mg(2+) ions. Result of stopped-flow fluorometry measurements at pH 8.0 indicate conformational changes in the helix-turn-helix motif in the N-terminal domain and in the C-terminal inducer binding domain. Binding of tetracycline (Tc) to TetR in the absence of Mg(2+) can be described by a simple kinetics process, which is limited to the first step association without any unimolecular conformational change step upon Tc binding. The rate constants for this process are equal to 2.0 x 10(5) M(-)(1) s(-)(1) and 2.1 s(-)(1) for the forward and backward reaction, respectively, and gave the binding constant K(a) = 0.96 x 10(5) M(-)(1). The kinetics of [Tc-Mg](+) binding to TetR can be described by reactions in which the first step describes the association characterized by the rate constants k(a) = 1.4 x 10(5) M(-)(1) s(-)(1) and k(d) = 2.2 x 10(-)(2) s(-)(1) and binding constant K(a) = 6.3 x 10(6) M(-)(1). The first step of [Tc-Mg](+) association is followed by at least three conformational change steps, which occur in the inducer binding site and then propagate to the surroundings of Trp75 and Trp43 residues. The rate constants for the forward, k(c), and backward, k(-)(c), reaction for each of these conformational steps have been determined. The thermodynamics of the binding of tetracycline with and without Mg(2+) to TetR was investigated by isothermal titration calorimetry (ITC) at pH 8.0 and 25 degrees C. The measurement shows that TetR dimer possesses two equivalent binding sites for tetracycline, characterized by binding constant K(a) = 9.0 x 10(6) M(-)(1) and K(a) = 7.0 x 10(4) M(-)(1) for Tc with and without Mg(2+), respectively. The binding of the inducer to TetR, in the presence and absence of Mg(2+) ion, is an enthalpy-driven reaction characterized by DeltaH = -51 kJ mol(-)(1) and DeltaH = -33 kJ mol(-)(1), respectively. The entropy change, DeltaS, for the interaction in the presence of Mg(2+) is equal to -38.9 J K(-)(1) mol(-)(1), and for the tetracycline alone, it was estimated at -17.6 J K(-)(1) mol(-)(1).     

Phospholipid-cytochrome c interaction: evidence for the extended lipid anchorage.

Binding of cytochrome c (cyt c) to fatty acids and acidic phospholipid membranes produces pronounced and essentially identical changes in the spectral properties of cyt c, revealing conformational changes in the protein. The exact mechanism of the interaction of fatty acids and acidic phospholipids with cyt c is unknown. Binding of cyt c to liposomes with high contents (mole fraction X > 0.7) of acidic phospholipids caused spectral changes identical to those due to binding of oleic acid. Fluorescence spectroscopy of a cyt c analog containing a Zn(2+) substituted heme moiety and brominated lipid derivatives (9,10)-dibromostearate and 1-palmitoyl-2-(9,10)-dibromo-sn-glycero-3-phospho-rac-glycerol demonstrated a direct contact between the fluorescent [Zn(2+)-heme] group and the brominated acyl chain. These data constitute direct evidence for interaction between an acyl chain of a membrane phospholipid and the inside of the protein containing the heme moiety and provide direct evidence for the so-called extended-lipid anchorage of cyt c to phospholipid membranes. In this mechanism, one of the phospholipid acyl chains protrudes out of the membrane and intercalates into a hydrophobic channel in cyt c while the other chain remains in the bilayer.     

Entropic drive in the sarcoplasmic reticulum ATPase interaction with Mg2+ and Pi.

Thermodynamic quantities for the binding of Mg2+ (in the presence of Ca2+) and Pi (in the presence of Mg2+ and absence of Ca2+) to sarcoplasmic reticulum ATPase were determined from isothermal titration calorimetry measurements at 25 degrees C. Mg2+ and Pi are involved in reversal of the ATPase hydrolytic reaction, and their interactions with the ATPase are conveniently studied under equilibrium conditions. We found that the Mg2+ binding reaction is endothermic with a binding constant (Kb) = 142 +/- 4 M(-1), a binding enthalpy of 180 +/- 3 kJ mol(-1), and an entropy contribution (TdeltaSb) = 192 +/- 3 kJ mol(-1). Similarly, Pi binding is also an endothermic reaction with Kb = 167 +/- 17 M(-1), deltaHb = 65.3 +/- 5.4 kJ mol(-1), and TdeltaSb = 77.9 +/- 5.4 kJ mol(-1). Our measurements demonstrate that the ATPase can absorb heat from the environment upon ligand binding, and emphasize the important role of entropic mechanisms in energy transduction by this enzyme.     

Structural polymorphism of hydrated monoacylated maltose glycolipids

The physico-chemical properties of three fully hydrated monoacyl maltoside glycolipids were investigated with Fourier-transform infrared spectroscopy (FTIR), differential scanning calorimetry (DSC) and small-angle X-ray scattering (SAXS). The different synthesized maltoside glycoconjugates vary in the length and saturation of the fatty acid moiety, whereas the constant head group region contains a beta-linked maltose with a OC(2)-NH spacer. The compounds with saturated acyl chains showed a complex pattern of temperature-dependent behaviour, regarding the adopted three-dimensional aggregate structure of the molecules and the main phase transition from the gel to liquid crystalline phase of the acyl chains. A substitution of the saturated acyl chain with an unsaturated acyl chain led to a complete change of the structural preferences, from a high ordered stacking of the bilayers to an unilamellar arrangement of completely disordered and fluid membranes. The presence of the NH group in the spacer, compared to the compounds lacking the NH group allows the formation of a hydrogen bonding network, which influences the observed phase properties. The results of these studies of the hydrated monoacylated maltose glycolipids are discussed in relation to the thermotropic phase properties of the pure compounds in the absence of water.     

Gramicidin channels in phospholipid bilayers with unsaturated acyl chains.

In organic solvents gramicidin A (gA) occurs as a mixture of slowly interconverting double-stranded dimers. Membrane-spanning gA channels, in contrast, are almost exclusively single-stranded beta(6,3)-helical dimers. Based on spectroscopic evidence, it has previously been concluded that the conformational preference of gA in phospholipid bilayers varies as a function of the degree of unsaturation of the acyl chains. Double-stranded pi pi(5,6)-helical dimers predominate (over single-stranded beta(6,3)-helical dimers) in lipid bilayer membranes with polyunsaturated acyl chains. We therefore examined the characteristics of channels formed by gA in 1-palmitoyl-2-oleoylphosphatidylcholine/n-decane, 1,2-dioleoylphosphatidylcholine/n-decane, and 1,2-dilinoleoylphosphatidylcholine/n-decane bilayers. We did not observe long-lived channels that could be conducting double-stranded pi pi(5,6)-helical dimers in any of these different membrane environments. We conclude that the single-stranded beta(6,3)-helical dimer is the only conducting species in these bilayers. Somewhat surprisingly, the average channel duration and channel-forming potency of gA are increased in dilinoleoylphosphatidylcholine/n-decane bilayers compared to 1-palmitoyl-2-oleoylphosphatidylcholine/n-decane and dioleoylphosphatidylcholine/n-decane bilayers. To test for specific interactions between the aromatic side chains of gA and the acyl chains of the bilayer, we examined the properties of channels formed by gramicidin analogues in which the four tryptophan residues were replaced with naphthylalanine (gN), tyrosine (gT), and phenylalanine (gM). The results show that all of these analogue channels experience the same relative stabilization when going from dioleoylphosphatidylcholine to dilinoleoylphosphatidylcholine bilayers.     

Conformation of fatty acyl chains in alpha- and beta-phosphatidylcholine and phosphatidylethanolamine derivatives in sonicated vesicles

Mono- and dimethylated derivatives constitute important intermediates in the conversion of phosphatidylethanolamine (PE) to phosphatidylcholine (PC) in eucaryote membranes. 1H-NMR techniques were utilized to examine the conformation of the region of the fatty acyl chains that is close to the polar group in the series of alpha-phospholipids: PE, N-methyl-PE, N,N-dimethyl-PE, and PC. The same series of polar groups, but on phospholipid containing sn-1 and/or sn-3 fatty acyl chains (beta-phospholipids) were also examined. All of the phospholipids were in the form of small sonicated vesicles which are widely utilized as membrane models. The alpha-methylene group of the sn-1 and sn-2 fatty acyl chains of the alpha-phospholipids give rise to separate signals due to the non-equivalency of these chains with respect to the glycerol phosphate backbone on all alpha-phospholipids tested. Additionally, differences in the environment of the PC molecules as well as N-methyl-PE, and N,N-dimethyl-PE, but not PE itself on the inside and outside of the vesicles are reflected in the chemical shift of the alpha-methylene protons. On the other hand, all of the beta-phospholipids (including beta-PE) were found to reflect the inside/outside packing differences in their alpha-methylene groups. The bilayer packing does not induce any nonequivalence in the chemically equivalent acyl chains. In mixed micelles with detergents, beta-phospholipids showed one alpha-CH2 signal for all phospholipids. These results are consistent with a common conformational arrangement for the fatty acyl chains in all alpha-phospholipids that have been investigated no matter what aggregated form. The conformational arrangement in the beta-phospholipids is different, but again is similar for all of the compounds tested in various aggregated forms.     

Structural analysis of Mg2+ and Ca2+ binding to CaBP1, a neuron-specific regulator of calcium channels

CaBP1 (calcium-binding protein 1) is a 19.4-kDa protein of the EF-hand superfamily that modulates the activity of Ca(2+) channels in the brain and retina. Here we present data from NMR, microcalorimetry, and other biophysical studies that characterize Ca(2+) binding, Mg(2+) binding, and structural properties of recombinant CaBP1 purified from Escherichia coli. Mg(2+) binds constitutively to CaBP1 at EF-1 with an apparent dissociation constant (K(d)) of 300 microm. Mg(2+) binding to CaBP1 is enthalpic (DeltaH = -3.725 kcal/mol) and promotes NMR spectral changes, indicative of a concerted Mg(2+)-induced conformational change. Ca(2+) binding to CaBP1 induces NMR spectral changes assigned to residues in EF-3 and EF-4, indicating localized Ca(2+)-induced conformational changes at these sites. Ca(2+) binds cooperatively to CaBP1 at EF-3 and EF-4 with an apparent K(d) of 2.5 microM and a Hill coefficient of 1.3. Ca(2+) binds to EF-1 with low affinity (K(d) >100 microM), and no Ca(2+) binding was detected at EF-2. In the absence of Mg(2+) and Ca(2+), CaBP1 forms a flexible molten globule-like structure. Mg(2+) and Ca(2+) induce distinct conformational changes resulting in protein dimerization and markedly increased folding stability. The unfolding temperatures are 53, 74, and 76 degrees C for apo-, Mg(2+)-bound, and Ca(2+)-bound CaBP1, respectively. Together, our results suggest that CaBP1 switches between structurally distinct Mg(2+)-bound and Ca(2+)-bound states in response to Ca(2+) signaling. Both conformational states may serve to modulate the activity of Ca(2+) channel targets.     

Optical activity of doubly ordered macromolecules

In order to analyze the optical activity of poly-N-γ-carbobenzoxy-L -α,γ-diaminobutyric acid, the microscopic model we have previously worked out is here further developed. Comparison with experimental data allows us to formulate a hypothesis on the stereochemical interaction between the side chains and the backbone of the macromolecule, and on the dependence of the optical activity on the conformational state of the backbone itself. Finally, the thermodynamic parameters concerning the side chains are estimated.     

The inhibition kinetics and thermodynamic changes of tyrosinase via the zinc ion

We found that Zn(2+) conspicuously inactivated tyrosinase in a mixed-type inhibition manner: the final level of residual activity was abolished at the equilibrium state with concentration of 0.25 mM Zn(2+). Changes of both K(m) and V(max) by various concentrations of Zn(2+) in Lineweaver-Burk plot were observed. To see whether Zn(2+) also induced conformational change of tyrosinase and how thermodynamical changes by ligand binding were occurred, the intrinsic fluorescence studies as well as calorimetric measurements were conducted. The results showed that the Zn(2+) binding to tyrosinase directly induced conformational change of tyrosinase, and the changes of thermodynamic parameters such as enthalpy (DeltaH), Gibbs free-energy (DeltaG), and entropy (DeltaS) were obtained as 60+/-7.0 kJ/mol, -14.54 kJ/mol and 248.53 J/(K mol), respectively. The inactivating effect of Zn(2+) on tyrosinase was completely prevented by incubation with bovine serum albumin, which has a Zn(2+) binding motif in its structure. We suggested that Zn(2+) ligand-binding affected the substrate's accessibility due to the conformational changes and thus, the complex type of inhibition has occurred with the calorimetric changes.     

CTP:2,3-di-O-geranylgeranyl-sn-glycero-1-phosphate cytidyltransferase in the methanogenic archaeon Methanothermobacter thermoautotrophicus

CDP-2,3-di-O-geranylgeranyl-sn-glycerol synthase (CDP-archaeol synthase) activity was discovered in the membrane fraction of the methanoarchaeon Methanothermobacter thermoautotrophicus cells. It catalyzed the formation of CDP-2,3-di-O-geranylgeranyl-sn-glycerol from CTP and 2,3-di-O-geranylgeranyl-sn-glycero-1-phosphate (unsaturated archaetidic acid). The identity of the reaction product was confirmed by thin layer chromatography, fast atom bombardment-mass spectroscopy, chemical analysis, and by UV spectroscopy. One mole of the product was formed from approximately 1 mol of each of the reactants. The enzyme showed maximal activity at pH 8.5 and 55 degrees C in the presence of Mg(2+) and K(+) ions. By in vivo pulse labeling of phospholipids with (32)P(i), CDP-archaeol was found to be an intracellular intermediate. A cell-free homogenate of M. thermoautotrophicus, when incubated with l-serine, converted the product of CDP-archaeol synthase reaction to a product with the same chromatographic mobility as archaetidylserine. It was concluded from these results that both CDP-archaeol and CDP-archaeol synthase were involved in cellular phospholipid biosynthesis. Among various synthetic substrate analogs, both enantiomers of unsaturated archaetidic acid possessing geranylgeranyl chains showed similar levels of activity, while archaetidic acid with saturated or monounsaturated isoprenoid or straight chains was a poor substrate, despite having the same stereostructure as the fully active substrate. The ester analogs with geranylgeranioyl chains showed significant activities. These results suggest that the enzyme dose not recognize ether or ester bonds between glycerophosphate and hydrocarbon chains nor the stereostructure of the glycerophosphate backbone but mainly targets substrates with geranylgeranyl chains.     

Structural aspects of pressure effects on infrared spectra of mixed-chain phosphatidylcholine assemblies in D2O

The barotropic behavior of D2O dispersions of 1-stearoyl-2-caproyl-sn-glycero-3-phosphocholine, C(18):C(10)PC, a highly asymmetric phospholipid in which the length of the fully extended acyl chain at the sn-1 position of the glycerol backbone is twice as long as that at the sn-2 position, has been investigated by high-pressure Fourier transform infrared spectroscopy. This asymmetric phosphatidylcholine bilayer at room temperature displays a pressure-induced phase transition corresponding to the liquid-crystalline----gel phase transition at 1.4 kbar. A conformational ordering of the lipid acyl chains is observed to take place abruptly at the transition pressure of 1.4 kbar. However, the lamellar lipid molecules and their acyl chains remain to be orientationally disordered in the gel phase until the applied pressure reaches 5.5 kbar. In the gel phase of fully hydrated C(18):C(10)PC, the asymmetric lipid molecules assemble into mixed interdigitated bilayers with perpendicular orientation of the zigzag planes among neighboring acyl chains. The role of excess water played in the interchain structure and the behavior of excess water and bound water under high pressure are also discussed.