Liposomal heme as oxygen carrier under semi-physiological conditions. Orientation study of heme embedded in a phospholipid bilayer by an electrooptical method

The meso-tetra(alpha,alpha,alpha,alpha(o-pivalamidophenyl]porphinato iron-mono(1-lauryl-2-methylimidazole) complex embedded in the bilayer of dimyristoylphosphatidylcholine (liposomal heme) binds molecular oxygen reversibly at pH 7 and 37 degrees C. Orientation of the iron porphyrin complex in the phospholipid bilayer was studied by electric birefringence and dichroism. It was observed that both the phospholipid bibilayer of liposome and the porphyrin plane are oriented nearly in parallel to the electric field. Therefore the angle between the porphyrin plane and the bilayer is considered to be practically small.     

State of heme in heme c systems: Cytochrome c and heme c models

Polarized resonance Raman spectra of horse heart ferricytochrome c as a function of pH in the range 1.0–12, in the presence of the extrinsic ligands imidazole, cyanide, and azide, and in 4 M urea, are reported, as are resonance Raman spectra of heme undecapeptide in the presence of imidazole, pH 6.8 and pH 2.0, and with cyanide at pH 6.8. The range of investigation is 140–1700 cm^?1, using the 5145-, 4880-, and 4579-Å excitations. The spectra have been analyzed in terms of complexity, sensitivity, and the conformation-heme energetics of the systems. The state of heme in various forms is analyzed with regard to heme energetics, core size, nature of planarity, and coordination configuration. All low-spin forms of heme c systems, cytochrome c, and heme models are concluded to be hexacoordinated, in-plane heme iron systems. The effect of the location of the heme in the protein environment is found to be a slight expansion of the porphyrin core, ～0.01 Å, while the covalent linkage of heme to protein and a mixed nature of axial coordination configuration seem to have little effect on the energetics of the heme group. Complex formation with extrinsic ligand, imidazole, cyanide, or azide, results in a slight contraction of the heme core. The formation of cytochrome c form IV, the alkaline form, is shown to follow a process with apK _a of about 8.4, and similarly, acidic form II is created following the prior formation of an intermediate form with apK _a of about 3.6. The precursor to form IV is interpreted as containing perturbation of the pyrrol rings, whereas the precursor to the acidic form seems to reflect alteration of the energetics of the C_αC_{m α} structures of the heme group. The acidic form of heme undecapeptide is a hexacoordinated high-spin heme with an estimated displacement of 0.25 Å from the heme plane. The pH 2 form of cytochrome c is also a hexacoordinated high-spin form with two weak axial ligands, but iron is in the plane of the porphyrin ring.     

Liposomal heme as oxygen carrier under semiphysiological condition

To prepare a potent synthetic oxygen carrier in aqueous media, the iron(II) picket fence porphyrin complex with one hydrophobic imidazole was incorporated into a lipid bilayer of phosphatidylcholine. The incorporation was confirmed by gel permeation chromatography and ultracentrifugation, which indicates the complex being trapped in the multilayer liposome. The liposomal iron(II) porphyrin complex could bind molecular oxygen reversibly in neutral aqueous media and in the serum of a rat blood at 25°C.     

Structure of the liposome composed of lipid-heme and phospholipids

The amphiphilic heme derivative, 5,10,15,20-tetra(α,α,α,α-o-(2′,2′-dimethyl-20′-(2′-trimethylammonioethyl) phosphonatoxyicosanamido)pheny)phorphinatoiron(II) (lipid-heme), formed a stable liposome (Φ ≈ 400 Å) with phospholipids. Differential scanning calorimetry showed that incorporation of the lipid-heme in the liposome bilayer (lipid/lipid-heme > 25) causes no disordering of the bilayer structure. Ligation of a bulky ligand to the lipid-heme liposome indicated that the lipid-heme situates facing predominantly outwards in the liposome. The closed vesicle structure and the stability of the lipid-heme liposome were also confirmed by the encapsulating capability of the fluorescence compound.     

Syntheses and characterization of cobalt(II) complexes of dimeric ‘picket fence’ porphyrins

A series of dimeric picket fence porphyrinatocobalt(II) complexeses in which the length of the bridging chain controls the dioxygen affinity was newly derived from the coupling of two meso-mono- (β-o-aminophenyl)-tris-(α,α,α-o-pivaloylamidophenyl)- porphyrins with (CH₂)_n(COCl)₂ (n = 1, 3, 5 or 7). Some of the dimeric complexes form a unique ‘sandwich structure’ upon binding with certain bidentate ligands, and their dioxygen affinities are greatly increased compared with those for corresponding monomeric complexes. The relationship observed between the length of the bridging chain and the dioxygen affinity of the dimer complex having a sandwich structure is interpreted in terms of the displacement mechanism of the metal atom from a porphyrin plane.     

Thermotropic and barotropic phase transitions of N-methylated dipalmitoylphosphatidylethanolamine bilayers

In order to understand the effect of polar head group modification on the thermotropic and barotropic phase behavior of phospholipid bilayer membranes, the phase transitions of dipalmitoylphosphatidylethanolamine (DPPE), dipalmitoylphosphatidyl-N-methylethanolamine (DPMePE), dipalmitoylphosphatidyl-N,N-dimethylethanolamine (DPMe₂PE) and dipalmitoylphosphatidylcholine (DPPC) bilayer membranes were observed by differential scanning calorimetry and high-pressure optical methods. The temperatures of the so-called main transition from the gel (L_β) or ripple gel (P_β′) phase to the liquid crystalline (L_α) phase were almost linearly elevated by applying pressure. The slope of the temperature-pressure boundary, dT/dp, was in the range of 0.220-0.264 K MPa⁻¹ depending on the number of methyl groups in the head group of lipids. The main-transition temperatures of N-methylated DPPEs decreased with increasing size of head group by stepwise N-methylation. On the other hand, there was no significant difference in thermodynamic quantities of the main transition between the phospholipids. With respect to the transition from the subgel (L_c) phase to the lamellar gel (L_β or L_β′) phase, the transition temperatures were also elevated by applying pressure. In the case of DPPE bilayer the L_c/L_β transition appeared at a pressure higher than 21.8 MPa. At a pressure below 21.8 MPa the L_c/L_α transition was observed at a temperature higher than the main-transition temperature. The main (L_β/L_α) transition can be recognized as the transformation between metastable phases in the range from ambient pressure to 21.8 MPa. Polymorphism in the gel phase is characteristic of DPPC bilayer membrane unlike other lipid bilayers used in this study: the L_β′, P_β′ and pressure-induced interdigitated gel (L_βI) phases were observed only in the DPPC bilayer. Regarding the bilayers of DPPE, DPMePE and DPMe₂PE, the interdigitation of acyl chain did not appear even at pressures as high as 200 MPa.     

Synthesis, spectroscopic and structural characterization of the high-spin Fe(II) cyanato-N and thiocyanato-N “picket fence” porphyrin complexes

Two new iron(II) five-coordinated porphyrin complexes [Na(2,2,2-crypt)] [Fe^II(TpivPP)(NCO)] (1) (TpivPP = α,α,α,α-tetrakis(o-pivalamidophenyl) porphyrin known as picket fence porphyrin and 2,2,2-crypt is the cryptand-222) and [K(2,2,2-crypt)][Fe^II(TpivPP)(NCS)] (2) have been prepared and characterized. The UV-Vis and IR spectroscopic data are consistent with a cyanato-N and thiocyanato-N ferrous porphyrinates. The Mössbauer data and the X-ray structural analysis indicate that the Fe(II) cation in 1 and 2 is high-spin (S = 2) and has the (d_xy)²(d_xz)¹(d_yz)¹(d_z²)¹(d_x²-y²)¹ ground state electronic configuration.For complex 1, the average equatorial iron-pyrrole N bond length (Fe-N_p = 2.120(2) Å), the distance between the iron and the 24-atom mean plane of the porphyrin ring (Fe-P_C = 0.6805(7) Å) and the distance between the iron and the plane made by the four pyrrole nitrogens (Fe-P_N = 0.5923(12) Å) are longer than those of complex 2 and similar five-coordinated Fe(II) high-spin porphyrinates. This is probably due to the significant electronic repulsion of the d_x²-y² and d_xy orbitals by the negative charge of the pyrrole N atoms in case of 1.     

Horse heart ferricytochromec: Conformation and heme configuration of high ionic strength acidic forms

The absorption, circular dichroism, and resonance Raman spectra of horse heart ferricytochromec in the presence of 0.2 M KCl, 0.1 M NaClO₄, and 0.2 M KNO₃, in thepH region 7 to 0.5, have been investigated to determine the nature and the course of the processes involved. As in the absence of salts (Myer, Y., and Saturno, A. F. (1990)J. Protein Chem.,9, 379–387), the change from neutral to low acidicpH's in the presence of salts is a three-step process: state III _s ?state III _s,a ?state II _s ?state I _s , withpK _a 's of 3.5±0.2, 2.2±0.2, and 1.1±0.2, and with two, one, and one number of protons, respectively. The addition of salts at neutralpH's has little or no effect on the protein conformation and the heme-iron configuration (i.e., they remain the same, low-spin hexacoordinated heme iron with a Met-80-Fe-His-18 axial coordination), but such addition does cause a slight tightening of the heme crevice and the enlargement of the porphyrin core. State III _s,a is a folded state with about the same degree of folding and with a similar spin state and coordination configuration of iron, but the heme crevice is loosened and the porphyrin core is smaller. Both states II _s and I _s are also essentially folded forms, but with a smaller degree of protein secondary structure. State II _s has a high-spin hexacoordinated heme iron with a water molecule and a protonated and/or hydrogen-bonded imidazole of his-18 as the two axial ligates; and state I _s has a high-spin pentacoordinated heme iron, which is about 0.49 Å out of the porphyrin plane, with a protonated and/or hydrogen-bonded imidazole nitrogen as the only axial ligate. The addition of anions causes the stabilization of the protein secondary structures and the state III _a →state II transition. The mode of effectiveness of anions appears to be nonspecific (i.e., because of electrostatic shielding and/or disruption of salt bridges).     

The effects of selected monopyrroles on various aspects of heme biosynthesis and degradation in the rat

The effects of four monopyrroles on porphyrin biosynthesis and excretion in the rat were studied. All four compounds investigated significantly increased total urinary porphyrin excretion and hepatic porphyrin levels while the effects on fecal excretion were equivocal. Peak porphyrin production elicited by treatment with ethyl 3-acetyl-2,4-dimethylpyrrole-5-carboxylate was found to be dose dependent, as was the time of maximum excretion. The effects of 3-ethyl-5-hydroxy-4,5-dimethyl-Δ³-pyrrolin-2-one, a compound excreted in abnormally high levels in the urine of patients with hepatic porphyria, were studied in greater depth. It was found that this compound caused an increase in the activity of δ-aminolevulinic acid synthase, in vivo, which was associated with a depression of microsomal levels of heme and cytochrome P-450. This depression of heme levels could not be related to increased catabolism or nonenzymic breakdown. It is suggested that the primary effect of this and the other compounds on porphyrin metabolism is a reduction in heme formation by a mechanism at present unclear.     

Orientation of membrane fragments by electric field

Purple membrane fragments from Halobacterium halobium were oriented by a static electric field in a water suspension. It was found that an electric field of approx. 20 V/cm is sufficient to achieve practically complete orientation; the purple membranes have a permanent electric dipole moment of (6 ±1)· 10^?23 C · m, the orientation of the retinal transition moment relative to the direction of the electric dipole moment, θ, is (59 ± 1)⁰, and the purple membrane rotational diffusion constant D_rot = 0.65 s^?1. It was found that because of the electrophoretic movement of the particles a hydrodynamic velocity gradient builds up which also orients the purple membranes.     

Behavior of silkworm yolk protein on phospholipid membranes

During early development, the plasma membrane of silkworm (Bombyx mori) eggs undergoes a superficial cleavage that separates the blastodermal protoplasm and the yolk. To test whether the blastoderm absorbs yolk through the plasma membrane in B. mori, we studied the interaction of phospholipid membranes and yolk using a phospholipid planar bilayer membrane (PBM) and liposomes. In addition, egg-specific protein (ESP; 225 kDa), a yolk protein that is specific to B. mori eggs, was collected by fractionating the eggs. Liposomes were mixed with either B. mori yolk or ESP, and observed under an electron microscope. This showed that the phospholipid membrane was spanned by fine particles 10-20 nm in diameter. Both yolk and ESP caused the PBM to become extraordinarily leaky, with a membrane potential of −70 mV for yolk and −198 mV for ESP. These results suggest that although it is a water-soluble protein, ESP permeates the phospholipid membrane without the help of enzymes.     

Coarse-grained simulations of the membrane-active antimicrobial Peptide maculatin 1.1

Maculatin 1.1 (M1.1) is a membrane-active antimicrobial peptide (AMP) from an Australian tree frog that forms a kinked amphipathic α-helix in the presence of a lipid bilayer or bilayer-mimetic environment. To help elucidate its mechanism of membrane-lytic activity, we performed a total of ∼8 μs of coarse-grained molecular dynamics (CG-MD) simulations of M1.1 in the presence of zwitterionic phospholipid membranes. Several systems were simulated in which the peptide/lipid ratio was varied. At a low peptide/lipid ratio, M1.1 adopted a kinked, membrane-interfacial location, consistent with experiment. At higher peptide/lipid ratios, we observed spontaneous, cooperative membrane insertion of M1.1 peptide aggregates. The minimum size for formation of a transmembrane (TM) aggregate was just four peptides. The absence of a simple and well-defined central channel, along with the exclusion of lipid headgroups from the aggregates, suggests that a pore-like model is an unlikely explanation for the mechanism of membrane lysis by M1.1. We also performed an extended 1.25 μs simulation of the permeabilization of a complete liposome by multiple peptides. Consistent with the simpler bilayer simulations, formation of monomeric interfacial peptides and TM peptide clusters was observed. In contrast, major structural changes were observed in the vesicle membrane, implicating induced membrane curvature in the mechanism of active antimicrobial peptide lysis. This contrasted with the behavior of the nonpore-forming model peptide WALP23, which inserted into the vesicle to form extended clusters of TM α-helices with relatively little perturbation of bilayer properties.     

Interactions of bovine lactoferricin with acidic phospholipid bilayers and its antimicrobial activity as studied by solid-state NMR

Bovine lactoferricin (LfcinB) is an antimicrobial peptide released by pepsin cleavage of lactoferrin. In this work, the interaction between LfcinB and acidic phospholipid bilayers with the weight percentage of 65% dimyristoylphosphatidylglycerol (DMPG), 10% cardiolipin (CL) and 25% dimyristoylphosphatidylcholine (DMPC) was investigated as a mimic of cell membrane of Staphylococcus aureus by means of quartz crystal microbalance (QCM) and solid-state ³¹P and ¹H NMR spectroscopy. Moreover, we elucidated a molecular mechanism of the antimicrobial activity of LfcinB by means of potassium ion selective electrode (ISE). It turned out that affinity of LfcinB for acidic phospholipid bilayers was higher than that for neutral phospholipid bilayers. It was also revealed that the association constant of LfcinB was larger than that of lactoferrin as a result of QCM measurements. ³¹P DD-static NMR spectra indicated that LfcinB interacted with acidic phospholipid bilayers and bilayer defects were observed in the bilayer systems because isotropic peaks were clearly appeared. Gel-to-liquid crystalline phase transition temperatures (Tc) in the mixed bilayer systems were determined by measuring the temperature variation of relative intensities of acyl chains in ¹H MAS NMR spectra. Tc values of the acidic phospholipid and LfcinB-acidic phospholipid bilayer systems were 21.5 °C and 24.0 °C, respectively. To characterize the bilayer defects, potassium ion permeation across the membrane was observed by ISE measurements. The experimental results suggest that LfcinB caused pores in the acidic phospholipid bilayers. Because these pores lead the permeability across the membrane, the molecular mechanism of the antimicrobial activity could be attributed to the pore formation in the bacterial membrane induced by LfcinB.     

Reduced Lateral Mobility of Lipids and Proteins in Crowded Membranes

Coarse-grained molecular dynamics simulations of the E. coli outer membrane proteins FhuA, LamB, NanC, OmpA and OmpF in a POPE/POPG (3∶1) bilayer were performed to characterise the diffusive nature of each component of the membrane. At small observation times (<10 ns) particle vibrations dominate phospholipid diffusion elevating the calculated values from the longer time-scale bulk value (>50 ns) of 8.5×10⁻⁷ cm² s⁻¹. The phospholipid diffusion around each protein was found to vary based on distance from protein. An asymmetry in the diffusion of annular lipids in the inner and outer leaflets was observed and correlated with an asymmetry in charged residues in the vicinity of the inner and outer leaflet head-groups. Protein rotational and translational diffusion were also found to vary with observation time and were inversely correlated with the radius of gyration of the protein in the plane of the bilayer. As the concentration of protein within the bilayer was increased, the overall mobility of the membrane decreased reflected in reduced lipid diffusion coefficients for both lipid and protein components. The increase in protein concentration also resulted in a decrease in the anomalous diffusion exponent α of the lipid. Formation of extended clusters and networks of proteins led to compartmentalisation of lipids in extreme cases.     

Molecular Dynamics Simulations of the Rotary Motor F0 under External Electric Fields across the Membrane

The membrane-bound component F₀, which is a major component of the F₀F₁-ATP synthase, works as a rotary motor and plays a central role in driving the F₁ component to transform chemiosmotic energy into ATP synthesis. We conducted molecular dynamics simulations of b₂-free F₀ in a 1-palmitoyl-2-oleoyl-phosphatidylcholine lipid bilayer for tens of nanoseconds with two different protonation states of the cAsp-61 residue at the interface of the a-c complex in the absence of electric fields and under electric fields of ±0.03 V/nm across the membrane. To our surprise, we observed that the upper half of the N-terminal helix of the c₁ subunit rotated about its axis clockwise by 30°. An energetic analysis revealed that the electrostatic repulsion between this N-terminal helix and subunit c₁₂ was a major contributor to the observed rotation. A correlation map analysis indicated that the correlated motions of residues in the interface of the a-c complex were significantly reduced by external electric fields. The deuterium order parameter (S_CD) profile calculated by averaging all the lipids in the F₀-bound bilayer was not very different from that of the pure bilayer system, in agreement with recent ²H solid-state NMR experiments. However, by delineating the lipid properties according to their vicinity to F₀, we found that the S_CD profiles of different lipid shells were prominently different. Lipids close to F₀ formed a more ordered structure. Similarly, the lateral diffusion of lipids on the membrane surface also followed a shell-dependent behavior. The lipids in the proximity of F₀ exhibited very significantly reduced diffusional motion. The numerical value of S_CD was anticorrelated with that of the diffusion coefficient, i.e., the more ordered lipid structures led to slower lipid diffusion. Our findings will help elucidate the dynamics of F₀ depending on the protonation state and electric field, and may also shed some light on the interactions between the motor F₀ and its surrounding lipids under physiological conditions, which could help to rationalize its extraordinary energy conversion efficiency.     

Coupling of Membrane Nanodomain Formation and Enhanced Electroporation near Phase Transition

Biological cells are enveloped by a heterogeneous lipid bilayer that prevents the uncontrolled exchange of substances between the cell interior and its environment. In particular, membranes act as a continuous barrier for salt and macromolecules to ensure proper physiological functions within the cell. However, it has been shown that membrane permeability strongly depends on temperature and, for phospholipid bilayers, displays a maximum at the transition between the gel and fluid phase. Here, extensive molecular dynamics simulations of dipalmitoylphosphatidylcholine bilayers were employed to characterize the membrane structure and dynamics close to phase transition, as well as its stability with respect to an external electric field. Atomistic simulations revealed the dynamic appearance and disappearance of spatially related nanometer-sized thick ordered and thin interdigitating domains in a fluid-like bilayer close to the phase transition temperature (T_m). These structures likely represent metastable precursors of the ripple phase that vanished at increased temperatures. Similarly, a two-phase bilayer with coexisting gel and fluid domains featured a thickness minimum at the interface because of splaying and interdigitating lipids. For all systems, application of an external electric field revealed a reduced bilayer stability with respect to pore formation for temperatures close to T_m. Pore formation occurred exclusively in thin interdigitating membrane nanodomains. These findings provide a link between the increased membrane permeability and the structural heterogeneity close to phase transition.     

Fluidity of phospholipid bilayers and membranes after exposure to osmium tetroxide and gluteraldehyde

The response of fluid bilayer regions to osmium tetroxide and glutaraldehyde fixation was examined in phospholipid multilayers and in nerve bundles from the walking legs of the lobster Homarus americanus. The samples were spinlabeled either with 5-doxylstearic acid (the 4′4′-dimethyloxazolidine-N-ozyl derivative of 5-ketostearic acid) or the maleimide spin label, 4-maleimido-2,2,6,6-tetramethylpiperidine-1-oxyl. Osmium tetroxide fixation abolishes the characteristic orientation of the spin-labeled lipid bilayer regions and virtually eliminates motion on the electron spin resonance time scale. Glutaraldehyde treatment reduces the motion of maleimide spin labels covalently attached to proteins. However, in contrast to osmium tetroxide fixation, glutaraldehyde has essentially no effect on the orientation and mobility in the fluid bilayer regions, and hence probably does not restrict directly the potential for translational motion in membrane phospholipid bilayer regions.     

Depth of α-synuclein in a bilayer determined by fluorescence, neutron reflectometry, and computation

α-Synuclein (α-syn) membrane interactions are implicated in the pathogenesis of Parkinson's disease. Fluorescence and neutron reflectometry (NR) measurements reveal that α-syn penetrates ～9–14 Å into the outer leaflet of the bilayer, with a substantial portion of the membrane-bound polypeptide extending into the aqueous solvent. For the first time, to our knowledge, we used NR to obtain direct quantitative evidence of α-syn-induced membrane thinning. To examine the effect of specific residues on membrane penetration depths, we used a series of W4-containing N-terminal peptides. We identified that the first 15 residues (P15) nearly recapitulate the features of the full-length protein (i.e., partition constants, molecular mobility, and insertion of the W4 side chain into the bilayer), and found that as few as the first four N-terminal residues are sufficient for vesicle binding. Although at least one imperfect amphipathic repeat sequence (KAKEGV) is required for α-helical formation, secondary structural formation has little effect on membrane affinity. To develop an N-terminal α-syn model for bilayer interactions, we performed molecular-dynamics simulations of the P15 peptide submerged in a bilayer. The simulation results are highly consistent with experimental data indicating a broad low-energy region (8.5–14.5 Å) for W4 insertion.     

Clustering of α-Synuclein on Supported Lipid Bilayers: Role of Anionic Lipid, Protein, and Divalent Ion Concentration

α-Synuclein is the major component of Lewy body inclusions found in the brains of patients with Parkinson's disease. Several studies indicate that α-synuclein binds to negatively charged phospholipid bilayers. We examined the binding of α-synuclein to membranes containing different amounts of negatively charged lipids using supported lipid bilayers, epifluorescence microscopy, fluorescence recovery after photobleaching, and bulk fluorescence techniques. The membranes contained phosphatidylcholine and phosphatidylglycerol. In the absence of protein, these lipids mix uniformly. Our results show that the propensity of α-synuclein to cluster on the membrane increases as the concentration of anionic lipid and/or protein increases. Regions on the lipid bilayer where α-synuclein is clustered are enriched in phosphatidylglycerol. We also observe divalent metal ions stimulate protein cluster formation, primarily by promoting lipid demixing. The importance of protein structure, lipid demixing, and divalent ions, as well as the physiological implications, will be discussed. Because membrane-bound α-synuclein assemblies may play a role in neurotoxicity, it is of interest to determine how membranes can be used to tune the propensity of α-synuclein to aggregate.