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Cell aggregation in the marine sponge Microciona prolifera is mediated by a multimillion molecular-mass aggregation factor, termed MAF. Earlier investigations revealed that the cell aggregation activity of MAF depends on two functional domains: (i) a Ca(2+)-independent cell-binding domain and (ii) a Ca(2+)-dependent proteoglycan self-interaction domain. Structural analysis of involved carbohydrate fragments of the proteoglycan in the self-association established a sulfated disaccharide beta-D: -GlcpNAc3S-(1-->3)-alpha-L: -Fucp and a pyruvated trisaccharide beta-D: -Galp4,6(R)Pyr-(1-->4)-beta-D: -GlcpNAc-(1-->3)-alpha-L: -Fucp. Recent UV, SPR, and TEM studies, using BSA conjugates and gold nanoparticles of the synthetic sulfated disaccharide, clearly demonstrated self-recognition on the disaccharide level in the presence of Ca(2+)-ions. To determine binding forces of the carbohydrate-carbohydrate interactions for both synthetic MAF oligosaccharides, atomic force microscopy (AFM) studies were carried out. It turned out that, in the presence of Ca(2+)-ions, the force required to separate the tip and sample coated with a self-assembling monolayer of thiol-spacer-containing beta-D: -GlcpNAc-(1-->3)-alpha-L: -Fucp-(1-->O)(CH(2))(3)S(CH(2))(6)S- was found to be quantized in integer multiples of 30 +/- 6 pN. No binding was observed between the two monolayers in the absence of Ca(2+)-ions. Cd(2+)-ions could partially induce the self-interaction. In contrast, similar AFM experiments with thiol-spacer-containing beta-D: -Galp4,6(R)Pyr-(1-->4)-beta-D: -GlcpNAc-(1-->3)-alpha-L: -Fucp-(1-->O)(CH(2))(3)S(CH(2))(6)S- did not show a binding in the presence of Ca(2+)-ions. Also TEM experiments of gold nanoparticles coated with the pyruvated trisaccharide could not make visible aggregation in the presence of Ca(2+)-ions. It is suggested that the self-interaction between the sulfated disaccharide fragments is stronger than that between the pyruvated trisaccharide.

Transmembrane (TM) alpha-helical peptides with neutral flanking residues such as tryptophan form highly ordered striated domains when incorporated in gel-state 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) bilayers and inspected by atomic force microscopy (AFM) (1). In this study, we analyze the molecular organization of these striated domains using AFM, photo-cross-linking, fluorescence spectroscopy, nuclear magnetic resonance (NMR), and X-ray diffraction techniques on different functionalized TM peptides. The results demonstrate that the striated domains consist of linear arrays of single TM peptides with a dominantly antiparallel organization in which the peptides interact with each other and with lipids. The peptide arrays are regularly spaced by +/-8.5 nm and are separated by somewhat perturbed gel-state lipids with hexagonally organized acyl chains, which have lost their tilt. This system provides an example of how domains of peptides and lipids can be formed in membranes as a result of a combination of specific peptide-peptide and peptide-lipid interactions.

In this study we address the stability of integration of proteins in membranes. Using dynamic atomic force spectroscopy, we measured the strength of incorporation of peptides in lipid bilayers. The peptides model the transmembrane parts of alpha-helical proteins and were studied in both ordered peptide-rich and unordered peptide-poor bilayers. Using gold-coated AFM tips and thiolated peptides, we were able to observe force events which are related to the removal of single peptide molecules out of the bilayer. The data demonstrate that the peptides are very stably integrated into the bilayer and that single barriers within the investigated region of loading rates resist their removal. The distance between the ground state and the barrier for peptide removal was found to be 0.75 +/- 0.15 nm in different systems. This distance falls within the thickness of the interfacial layer of the bilayer. We conclude that the bilayer interface region plays an important role in stably anchoring transmembrane proteins into membranes.

The nucleation and growth of a calcium phosphate (Ca-P) coating deposited on titanium implants from simulated body fluid was investigated by using atomic force microscopy (AFM) and environmental scanning electron microscopy (ESEM). Forty titanium alloy plates were assigned into two groups. One group with a smooth surface having a maximum roughness R(max) < 0.10 microm (s-Ti6Al4V) and a group with a rough surface with an R(max) < 0.25 microm (r-Ti6Al4V) were used. Titanium samples were immersed in SBF concentrated by five (SBF x 5) from 10 min to 5 h and examined by AFM and ESEM. Scattered Ca-P deposits of approximately 15 nm in diameter appeared after only 10 min of immersion in SBF x 5. These Ca-P deposits grew up to 60-100 nm after 4 h on both s- and r-Ti6Al4V substrates. With increasing immersion time, the packing of Ca-P deposits with size of tens of nanometers in diameter formed larger globules and then a continuous Ca-P film on titanium substrates. A direct contact between the Ca-P coating and the Ti6Al4V surface was observed. The Ca-P coating was composed of nanosized deposits and of an interfacial glassy matrix. This interfacial glassy matrix might ensure the adhesion between the Ca-P coating and the Ti6Al4V substrate. In the case of s-Ti6Al4V substrate, failures within this interfacial glassy matrix were observed overtime. Part of the glassy matrix remained on s-Ti6Al4V while part detached with the Ca-P film. The Ca-P coating detached from the smooth substrate, whereas the Ca-P film extended onto the whole rough titanium surface over time. In the case of r-Ti6Al4V, the Ca-P coating covered evenly the substrate after immersion in SBF x 5 for 5 h. The present study suggested that the heterogeneous nucleation of Ca-P on titanium was immediate and did not depend on the Ti6Al4V surface topography. The further growth and mechanical attachment of the final Ca-P coating strongly depended on the surface, for which a rough topography was beneficial.

In this study the interaction of the antimicrobial peptide clavanin A with phosphatidylcholine bilayers is investigated by DSC, NMR, and AFM techniques. It is shown that the peptide interacts strongly and specifically with the lipids, resulting in increased order-disorder phase transition temperatures, phase separation, altered acyl chain and headgroup packing, and a drastically changed surface morphology of the bilayer. These results are interpreted in terms of clavanin-specific interactions with lipids and are discussed in the light of the different mechanisms by which clavanin A can destroy the barrier function of biological membranes.

Pulmonary surfactant forms a monolayer of lipids and proteins at the alveolar air/liquid interface. Although cholesterol is a natural component of surfactant, its function in surface dynamics is unclear. To further elucidate the role of cholesterol in surfactant, we used a captive bubble surfactometer (CBS) to measure surface activity of spread films containing dipalmitoylphosphatidylcholine/1-palmitoyl-2-oleoylphosphatidylcholine/1-palmitoyl-2-oleoylphosphatidylglycerol (DPPC/POPC/POPG, 50/30/20 molar percentages), surfactant protein B (SP-B, 0.75 mol %), and/or surfactant protein C (SP-C, 3 mol %) with up to 20 mol % cholesterol. A cholesterol concentration of 10 mol % was optimal for reaching and maintaining low surface tensions in SP-B-containing films but led to an increase in maximum surface tension in films containing SP-C. No effect of cholesterol on surface activity was found in films containing both SP-B and SP-C. Atomic force microscopy (AFM) was used, for the first time, to visualize the effect of cholesterol on topography of SP-B- and/or SP-C-containing films compressed to a surface tension of 22 mN/m. The protrusions found in the presence of cholesterol were homogeneously dispersed over the film, whereas in the absence of cholesterol the protrusions tended to be more clustered into network structures. A more homogeneous dispersion of surfactant lipid components may facilitate lipid insertion into the surfactant monolayer. Our data provide additional evidence that natural surfactant, containing SP-B and SP-C, is superior to surfactants lacking one of the components, and furthermore, this raises the possibility that the cholesterol found in surfactant of warm-blooded mammals does not have a function in surface activity.

The determinants for the formation of multilayers upon compression of surfactant monolayers were investigated by compressing films, beyond the squeeze-out plateau, to a surface tension of 22 millinewtons/m. Atomic force microscopy was used to visualize the topography of lipid films containing varying amounts of native surfactant protein B (SP-B). These films were compared with films containing synthetic peptides based on the N terminus of human SP-B: monomeric mSP-B-(1-25) or dimeric dSP-B-(1-25). The formation of typical hexagonal network structures as well as the height of protrusions were shown to depend on the concentration of SP-B. Protrusions of bilayer height were formed from physiologically relevant concentrations of 0.2-0.4 mol % (4.5-8.5 wt %) SP-B upwards. Much higher concentrations of SP-B-(1-25) peptides were needed to obtain network structures, and protrusion heights were not equal to those found for films with native SP-B. A striking observation was that while protrusions formed in films of 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC)/1,2-dipalmitoyl-sn-glycero-3-(phospho-rac-(1-glycerol)) (DPPG) (80/20) had single bilayer thickness, those formed in DPPC/1-palmitoyl-2-oleoyl-sn-glycero-3-(phospho-rac-(1-glycerol)) (80/20) had various heights of multilayers, whereas those seen in DPPC/1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine/DPPG (60/20/20) were mainly of bilayer height. For the first time direct observations by atomic force microscopy show (i) that a certain minimal concentration of SP-B is required for the formation of layered protrusions upon film compression, (ii) that protrusion height depends on whether the phospholipids contain an unsaturated fatty acyl chain, and (iii) that protrusion height also depends on whether the unsaturated acyl chain is present in phosphatidylcholine or in phosphatidylglycerol.

Lateral segregation in biological membranes leads to the formation of domains. We have studied the lateral segregation in gel-state model membranes consisting of supported dipalmitoylphosphatidylcholine (DPPC) bilayers with various model peptides, using atomic force microscopy (AFM). The model peptides are derivatives of the Ac-GWWL(AL)(n)WWA-Etn peptides (the so-called WALP peptides) and have instead of tryptophans, other flanking residues. In a previous study, we found that WALP peptides induce the formation of extremely ordered, striated domains in supported DPPC bilayers. In this study, we show that WALP analogues with other uncharged residues (tyrosine, phenylalanine, or histidine at pH 9) can also induce the formation of striated domains, albeit in some cases with a slightly different pattern. The WALP analogues with positively charged residues (lysine or histidine at low pH) cannot induce striated domains and give rise to a completely different morphology: they induce irregularly shaped depressions in DPPC bilayers. The latter morphology is explained by the fact that the positively charged peptides repel each other and hence are not able to form striated domains in which they would have to be in close vicinity. They would reside in disordered, fluidlike lipid areas, appearing below the level of the ordered gel-state lipid domains, which would account for the irregularly shaped depressions.

Evidence is accumulating that in cell membranes microdomains exist, also referred to as rafts or detergent resistant membranes. In this study, atomic force microscopy is used to study supported lipid bilayers, consisting of a fluid phosphatidylcholine, sphingomyelin and cholesterol. Domains were visualized of which the morphology and size depended on the cholesterol concentration. The presence of cholesterol was found to induce bilayer coupling. At 30 mol% cholesterol, a change in percolation phase was observed, and at 50 mol%, when both fluid lipids and solid lipids are saturated with cholesterol, phase separation was still observed. In addition, we were able to directly visualize the resistance of domains against non-ionic detergent.

Atomic force microscopy (AFM) is nowadays frequently applied to determine interaction forces between biological molecules. Starting with the detection of the first discrete unbinding forces between ligands and receptors by AFM only several years ago, measurements have become more and more quantitative. At the same time, theories have been developed to describe and understand the dynamics of the unbinding process and experimental techniques have been refined to verify this theory. In addition, the detection of molecular recognition forces has been exploited to map and image the location of binding sites. In this review we discuss the important contributions that have led to the development of this field. In addition, we emphasize the potential of chemically well-defined surface modification techniques to further improve reproducible measurements by AFM. This increased reproducibility will pave the way for a better understanding of molecular interactions in cell biology.

We used atomic force microscopy (AFM) to study the lateral organization of transmembrane TmAW(2)(LA)(n)W(2)Etn peptides (WALP peptides) incorporated in phospholipid bilayers. These well-studied model peptides consist of a hydrophobic alanine-leucine stretch of variable length, flanked on each side by two tryptophans. They were incorporated in saturated phosphatidylcholine (PC) vesicles, which were deposited on a solid substrate via the vesicle fusion method, yielding hydrated gel-state supported bilayers. At low concentrations (1 mol %) WALP peptides induced primarily line-type depressions in the bilayer. In addition, striated lateral domains were observed, which increased in amount and size (from 25 nm up to 10 microm) upon increasing peptide concentration. At high peptide concentration (10 mol %), the bilayer consisted mainly of striated domains. The striated domains consist of line-type depressions and elevations with a repeat distance of 8 nm, which form an extremely ordered, predominantly hexagonal pattern. Overall, this pattern was independent of the length of the peptides (19-27 amino acids) and the length of the lipid acyl chains (16-18 carbon atoms). The striated domains could be pushed down reversibly by the AFM tip and are thermodynamically stable. This is the first direct visualization of alpha-helical transmembrane peptide-lipid domains in a bilayer. We propose that these striated domains consist of arrays of WALP peptides and fluidlike PC molecules, which appear as low lines. The presence of the peptides perturbs the bilayer organization, resulting in a decrease in the tilt of the lipids between the peptide arrays. These lipids therefore appear as high lines.

The force sensor of an atomic force microscope (AFM) is sensitive enough to measure single molecular binding strengths by means of a force-distance curve. In order to combine high-force sensitivity with the spatial resolution of an AFM in topography mode, adhesion mode has been developed. Since this mode generates a force-distance curve for every pixel of an image, the measurement speed in liquid is limited by the viscous drag of the cantilever. We have equipped our adhesion mode AFM with a cantilever that has a low viscous drag in order to reach pixel frequencies of 65 Hz. Optimized filtering techniques combined with an auto-zero circuitry that reduces the drift in the deflection signal, limited high- and low-frequency fluctuations in the height signal to 0.3 nm. This reduction of the height noise, in combination with a thermally stabilized AFM, allowed the visualization of individual molecules on mica with an image quality comparable to tapping mode. The lateral resolution in both the topography and the simultaneously recorded adhesion image are only limited by the size of the tip. Hardware and software position feedback systems allows individual molecules to be followed in time during more than 30 min with scan sizes down to 60 x 60 nm2.

Atomic force microscopy is one of the few techniques that allow analysis of biological recognition processes at the single-molecule level. A major limitation of this approach is the nonspecific interaction between the force sensor and substrate. We have modeled the nonspecific interaction by looking at the interaction potential between a conical Si3N4 tip with a spherical end face and a mica surface in solution, using DLVO (Derjaguin, Landau, Verwey, Overbeek) theory and numerical calculations. Insertion of the tip-sample potential in a simulation of an approach-retract cycle of the cantilever gives the well-known force-distance curve. Simulating a force-distance curve at low salt concentration predicts a discrete hopping of the tip, caused by thermal fluctuations. This hopping behavior was observed experimentally and gave rise to a novel approach to making measurements in adhesion mode that essentially works in the repulsive regime. The distance between tip and sample will still be small enough to allow spacer-involved specific interactions, and the percentage of nonspecific interactions of the bare tip with the mica is minimized. We have validated this physical model by imaging intercellular adhesion molecule 1 (ICAM-1) antigen with a tip functionalized with anti-ICAM-1 antibody. The measurement demonstrated that a significant decrease in the number of nonspecific interactions was realized, and the topographical image quality and the specific bonding capability of the tip were not affected.

Specific molecular recognition events, detected by atomic force microscopy (AFM), so far lack the detailed topographical information that is usually observed in AFM. We have modified our AFM such that, in combination with a recently developed method to measure antibody-antigen recognition on the single molecular level (Hinterdorfer, P., W. Baumgartner, H. J. Gruber, K. Schilcher, and H. Schindler, Proc. Natl. Acad. Sci. USA 93:3477-3481 (1996)), it allows imaging of a submonolayer of intercellular adhesion molecule-1 (ICAM-1) in adhesion mode. We demonstrate that for the first time the resolution of the topographical image in adhesion mode is only limited by tip convolution and thus comparable to tapping mode images. This is demonstrated by imaging of individual ICAM-1 antigens in both the tapping mode and the adhesion mode. The contrast in the adhesion image that was measured simultaneously with the topography is caused by recognition between individual antibody-antigen pairs. By comparing the high-resolution height image with the adhesion image, it is possible to show that specific molecular recognition is highly correlated with topography. The stability of the improved microscope enabled imaging with forces as low as 100 pN and ultrafast scan speed of 22 force curves per second. The analysis of force curves showed that reproducible unbinding events on subsequent scan lines could be measured.

The interactions between a bacterial precursor protein and phospholipids in bilayer-based model membrane systems is addressed in this study. The precursor-lipid interactions were assessed from the side of the lipid phase by fluorescence and electron spin resonance spectroscopy, using the precursor of the Escherichia coli outer membrane protein PhoE. The role of the signal sequence, as part of the precursor, in this interaction was investigated by using cysteine-based site-directed spectroscopy. For this purpose, purified cysteine-containing mutants of prePhoE, which were made by site-directed mutagenesis of the signal sequence part and of the mature part, and defined lipids were used. The location of the fluorescently labeled cysteine residues was established by resonance energy transfer and quenching experiments and those of the corresponding spin-labeled cysteine residues by paramagnetic relaxation enhancement. It was demonstrated that precursor-phospholipid interactions exist in model membrane systems and also that these interactions were dependent on the presence of anionic phospholipids and resulted in a deep insertion of (parts of) the precursor into the lipid bilayer. Furthermore, the results with the cysteine mutations in the signal sequence of the precursor indicate that both termini of the signal sequence are located near or at the membrane surface, with only the fluorescence of the labeled cysteines in the signal sequence part being protected against aqueous quenchers. The results demonstrate that, when part of the intact precursor, the signal sequence experiences similar lipid-protein interactions as do isolated signal peptides. They also indicate that the signal sequence inserts entirely as a looped structure into the membrane. In addition, the data also indicate that the mature part of the precursor has an affinity for the membrane.

The interaction of the 25-residue presequence of yeast cytochrome oxidase subunit IV with lipid bilayers composed of phosphatidylglycerol, cardiolipin, or their (1:4) mixtures with phosphatidylcholine has been studied by spin-label ESR spectroscopy. Binding of the presequence progressively broadens the gel-to-fluid phase transition of dimyristoylphosphatidylglycerol bilayers, leading to abolition of the transition at a peptide/lipid ratio of > or = 1:5 mol/mol. The mobility of phosphatidylglycerol spin-labeled at the 5-position of the sn-2 chain is decreased in both gel and fluid phases on binding the presequence, with a progressively increasing ESR spectral anisotropy in the fluid phase. The ESR spectra of phosphatidylglycerol spin-labeled at the 14-position of the sn-2 chain contain a second motionally restricted component, in addition to the fluid bilayer spectral component, that arises from direct interaction of the bound presequence with the lipid chains. The proportion of this motionally restricted component is greater for dioleoylphosphatidylglycerol bilayers (corresponding to 2-3 lipids per peptide) than for cardiolipin bilayers (1-2 lipids/peptide), and this component is present also in the mixed bilayers containing 80% phosphatidylcholine. The ESR spectra of the presequence spin-labeled with a maleimide derivative at cysteine-19 evidence high mobility in solution and a very strong reduction in mobility on binding to bilayers containing negatively charged lipids. At low peptide to lipid ratios, the ESR spectra of the spin-labeled presequence sense the phase transition of dimyristoylphosphatidylglycerol.(ABSTRACT TRUNCATED AT 250 WORDS)

The effects of SecA-lipid interactions on lipid mobility were studied by electron spin resonance (ESR) spectroscopy in bilayer systems containing phospholipids spin-labeled at different positions along the acyl chain. The SecA protein, which functions in protein translocation at the cytosolic side of the E. coli inner membrane, was found to decrease the mobility of the lipids upon its interaction with the membrane. The restriction of lipid motion, at all chain positions measured, reflects the ability of SecA to penetrate the membrane. At a 49:1 lipid/protein molar ratio, a second, motionally more restricted component is observed in ESR spectra of phospholipids spin-labeled close to the methyl ends of the chains (12th and 14th positions). Furthermore, SecA was found to eliminate the order-to-disorder phase transition of 1,2-dimyristoyl-sn-glycero-3-phosphoglycerol bilayers. A remarkably strong reduction in the ability of SecA to penetrate the membrane was found when the nucleotides ATP and ADP+P(i) were present. The presence of the non-hydrolyzable analogue AMP-PNP had no effect. These results clearly demonstrate that SecA perturbs, in a nucleotide dependent manner, lipid mobility upon insertion into the bilayer. The implications of these findings for translocation of precursor proteins across the E. coli inner membrane are discussed.

The mitochondrial precursor protein horse heart apocytochrome c was spin-labeled on the cysteine residue at position 14 or 17 in the N-terminal region, and the mature protein yeast cytochrome c was similarly labeled on the single free cysteine residue at position 102 at the C-terminal. The proteins were bound to negatively charged phospholipid bilayers, and the accessibility of the spin-labeled cysteine residues to lipid-soluble molecular oxygen and to the lipid-impermeant chromium oxalate anion was determined from the saturation properties of the ESR spectra. Binding of the protein was found to have a considerable effect on the local oxygen concentrations within the lipid bilayer. The accessibilities of the spin-labeled proteins relative to those obtained for phospholipids spin-labeled either in the headgroup or at positions in the sn-2 acyl chain, in the presence of unlabeled protein, identify the position of the spin-labeled cysteine residues in the phospholipid bilayer. The spin label on apocytochrome c bound to phosphatidylglycerol bilayers lies between the 5- and 14-C positions of the lipid acyl chain. Admixture of > or = 75 mol % phosphatidylcholine induces an additional surface-associated apocytochrome c population. The spin label on native and heat-denatured cytochrome c is located at the membrane surface. These different extents of membrane penetration correlate also with the reduction in local oxygen concentration experienced by spin-labeled phospholipids on binding of apo- and holocytochrome c. The possible biological implications of the data are discussed.

Apocytochrome c derived from horse heart cytochrome c was spin-labeled on the cysteine residue at position 14 or 17 in the N-terminal region of the primary sequence, and cytochrome c from yeast was spin-labeled on the single cysteine residue at sequence position 102 in the C-terminal region. The spin-labeled apocytochrome c and cytochrome c were bound to fluid bilayers composed of different negatively charged phospholipids that also contained phospholipid probes that were spin-labeled either in the headgroup or at different positions in the sn-2 acyl chain. The location of the spin-labeled cysteine residues on the lipid-bound proteins was determined relative to the spin-label positions in the different spin-labeled phospholipids by the influence of spin-spin interactions on the microwave saturation properties of the spin-label electron spin resonance spectra. The enhanced spin relaxation observed in the doubly labeled systems arises from Heisenberg spin exchange, which is determined by the accessibility of the spin-label group on the protein to that on the lipid. It is found that the labeled cysteine groups in horse heart apocytochrome c are located closest to the 14-C atom of the lipid acyl chain when the protein is bound to dimyristoyl- or dioleoyl-phosphatidylglycerol, and to that of the 5-C atom when the protein is bound to a dimyristoylphosphatidylglycerol/dimyristoylphosphatidylcholine (15:85 mol/mol mixture. On binding to dioleoylphosphatidylglycerol, the labeled cysteine residue in yeast cytochrome c is located closest to the phospholipid headgroups but possibly between the polar group region and the 5-C atom of the acyl chains. These data determine the extent to which the different regions of the proteins are able to penetrate negatively charged phospholipid bilayers.

Apocytochrome c has been spin-labeled with a nitroxide derivative of maleimide on a cysteine residue at either position 14 or position 17 in the N-terminus. Yeast cytochrome c was spin-labeled with the same maleimide derivative on its single free cysteine residue at position 102 in the C-terminus. The ESR spectra of spin-labeled apocytochrome c have been characterized in different environments with respect both to the conformation of the protein and to its association with lipid. In buffer, the spectrum of spin-labeled apocytochrome c indicates high mobility, characteristic of the unfolded structure of the apoprotein, and that of spin-labeled cytochrome c is only slightly less mobile, suggesting that the site labeled is situated at the surface of the folded holoprotein. Upon binding the spin-labeled protein to negatively charged lipid membranes composed of dioleoylphosphatidylglycerol (DOPG), the ESR spectra of apocytochrome c evidence a large reduction in the mobility of the spin-label group, as also do those of yeast cytochrome c. In the case of apocytochrome c, this immobilization most likely arises from both an increase in secondary structure and a partial penetration of the protein into the lipid bilayer, in addition to the electrostatic interaction with the lipid headgroups, whereas for cytochrome c the immobilization observed arises primarily from an intimate association with the membrane surface. When the spin-labeled holocytochrome c is denatured by heating and is bound to DOPG bilayer membranes, a rather mobile ESR spectrum is observed, which demonstrates that the spin-label is located at the surface of the membrane in this case. The ESR spectra of spin-labeled apocytochrome c bound to mixed bilayers of dimyristoylphosphatidylglycerol and dimyristoylphosphatidylcholine (DMPC) consist of both an immobile and a mobile component. The proportion of the mobile component is increased by increasing the mole fraction of the zwitterionic DMPC in the mixed bilayers. The mobile component represents a localization of apocytochrome c at the membrane surface, whereas the immobile component most probably represents the penetration of the precursor protein into the membrane interior. The immobile component assigned to membrane penetration of the precursor protein is still present at negatively charged lipid contents comparable to those in the native mitochondrial system. The results are discussed in relation to the conformation of apocytochrome c, its interaction with lipid, and the import of the apoprotein into mitochondria.

The location of phospholipids, spin-labeled in the headgroup or at various positions of the sn-2 chain, incorporated in bilayer membranes of dimyristoylphosphatidylcholine, dimyristoylphosphatidylglycerol or dioleoylphosphatidylglycerol, has been calibrated in terms of their accessibility to paramagnetic relaxation agents. A power saturation approach has been used to determine the spin-label relaxation times, which in turn is influenced by spin-spin interactions with the different paramagnetic species. The effect of different paramagnetic relaxation agents on the power saturation behaviour of the spin-labeled lipids has been used to determine the relaxation enhancement which is quantified in terms of an accessibility parameter. Molecular oxygen, which dissolves preferentially in the lipid phase and the water-soluble, membrane-impermeant chromium oxalate anion are shown to report reliably on the accessibility of spin-labels located in one of the two phases. On the other hand, an uncharged, polar nickel-iminodiacetic acid complex is shown to enhance relaxation of spin-labels in both phases. These calibrations are essential for the study of the interaction of basic proteins with anionic lipid membranes.

The topology of apocytochrome c, the heme-free precursor of the mitochondrial protein cytochrome c, was investigated in a lipid-associated form. For this purpose photochemically induced dynamic nuclear polarization 1H nuclear magnetic resonance (CIDNP 1H NMR) spectroscopy and quenching of tryptophan and tyrosine fluorescence by acrylamide were applied to an apocytochrome c-sodium dodecyl sulfate (SDS) micellar system. A pH titration of the chemical shifts of the histidine C2 proton resonances of apocytochrome c, using conventional 1H NMR, yielded pK(a)'s of 5.9 +/- 0.1 and 6.2 +/- 0.1, which were assigned to histidine-18 and -33 and histidine-26, respectively. In the presence of SDS micelles an average pK(a) of 8.1 +/- 0.1 was obtained for all histidine C2 protons. Photo-CIDNP enhancements of the histidine, tryptophan, and tyrosine residues, contained in the intact apocytochrome c and in chemically and enzymatically prepared fragments of the precursor, were reduced in the presence of SDS micelles. Similarly, the quenching of the tryptophan fluorescence of the polypeptides by acrylamide was diminished in the presence of SDS. These results indicate the aromatic residues studied are localized in the interface of the SDS micelle.