The conformation of the cytoplasmic helix 8 of the CB1 cannabinoid receptor using NMR and circular dichroism

The cytoplasmic helix domain (fourth cytoplasmic loop, helix 8) of numerous GPCRs such as rhodopsin and the beta-adrenergic receptor exhibits unique structural and functional characteristics. Computational models also predict the existence of such a structural motif within the CB1 cannabinoid receptor, another member of the G-protein coupled receptor superfamily. To gain insights into the conformational properties of this GPCR component, a peptide corresponding to helix 8 of the CB1 receptor with a small contiguous segment from transmembrane helix 7 (TM7) was chemically synthesized and its secondary structure determined by circular dichroism (CD) and solution NMR spectroscopy. Our studies in DPC and SDS micelles revealed significant alpha-helical structure while in an aqueous medium, the peptide exhibited a random coil configuration. The relative orientation of helix 8 within the CB1 receptor was obtained from intermolecular 31P-1H and 1H-1H NOE measurements. Our results suggest that in the presence of an amphipathic membrane environment, helix 8 assumes an alpha helical structure with an orientation parallel to the phospholipid membrane surface and perpendicular to TM7. In this model, positively charged side chains interact with the lipid headgroups while the other polar side chains face the aqueous region. The above observations may be relevant to the activation/deactivation of the CB1 receptor.     

Position and motions of the S4 helix during opening of the Shaker potassium channel

The four voltage sensors in voltage-gated potassium (Kv) channels activate upon membrane depolarization and open the pore. The location and motion of the voltage-sensing S4 helix during the early activation steps and the final opening transition are unresolved. We studied Zn(2+) bridges between two introduced His residues in Shaker Kv channels: one in the R1 position at the outer end of the S4 helix (R362H), and another in the S5 helix of the pore domain (A419H or F416H). Zn(2+) bridges readily form between R362H and A419H in open channels after the S4 helix has undergone its final motion. In contrast, a distinct bridge forms between R362H and F416H after early S4 activation, but before the final S4 motion. Both bridges form rapidly, providing constraints on the average position of S4 relative to the pore. These results demonstrate that the outer ends of S4 and S5 remain in close proximity during the final opening transition, with the S4 helix translating a significant distance normal to the membrane plane.     

Structural characterization of the pore forming protein TatAd of the twin-arginine translocase in membranes by solid-state 15N-NMR

The transmembrane protein TatA is the pore forming unit of the twin-arginine translocase (Tat), which has the unique ability of transporting folded proteins across the cell membrane. This ATP-independent protein export pathway is a recently discovered alternative to the general secretory (Sec) system of bacteria. To obtain insight in the translocation mechanism, the structure and alignment in the membrane of the well-folded segments 2-45 of TatAd from Bacillus subtilis was studied here. Using solid-state NMR in bicelles containing anionic lipids, the topology and orientation of TatAd was determined in an environment mimicking the bacterial membrane. A wheel-like pattern, characteristic for a tilted transmembrane helix, was observed in 15N chemical shift /15N-1H dipolar coupling correlation NMR spectra. Analysis of this PISA wheel revealed a 14-16 residue long N-terminal membrane-spanning helix which is tilted by 17 degrees with respect to the membrane normal. In addition, comparison of uniformly and selectively 15N-labeled TatA2-45 samples allowed determination of the helix polarity angle.     

Cholesterol stimulates and ceramide inhibits Sticholysin II-induced pore formation in complex bilayer membranes

The pore forming capacity of Sticholysin II (StnII; isolated from Stichodactyla helianthus) in bilayer membranes containing 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC), palmitoylsphingomyelin (PSM) and either cholesterol or palmitoyl ceramide (PCer) has been examined. The aim of the study was to elucidate how the presence of differently ordered PSM domains affected StnII oligomerization and pore formation. Cholesterol is known to enhance pore formation by StnII, and our results confirmed this and provide kinetic information for the process. The effect of cholesterol on bilayer permeabilization kinetics was concentration-dependent. In the concentration regime used (2.5–10 nmol cholesterol in POPC:PSM 80:20 by nmol), cholesterol also increased the acyl chain order in the fluid PSM domain and thus decreased bilayer fluidity, suggesting that fluidity per se was not responsible for cholesterol's effect. Addition of PCer (2.5–10 nmol) to the POPC:PSM (80:20 by nmol) bilayers attenuated StnII-induced pore formation, again in a concentration-dependent fashion. This addition also led to the formation of a PCer-rich gel phase. Addition of cholesterol to PCer-containing membranes could partially reduce the inhibitory effect of PCer on StnII pore formation. We conclude that the physical state of PSM (as influenced by either cholesterol or PCer) affected StnII binding and pore formation under the conditions examined.     

One protein, two enzymes revisited: a structural entropy switch interconverts the two isoforms of acireductone dioxygenase

Acireductone dioxygenase (ARD) catalyzes different reactions between O2 and 1,2-dihydroxy-3-oxo-5-(methylthio)pent-1-ene (acireductone) depending upon the metal bound in the active site. Ni2+ -ARD cleaves acireductone to formate, CO and methylthiopropionate. If Fe2+ is bound (ARD'), the same substrates yield methylthioketobutyrate and formate. The two forms differ in structure, and are chromatographically separable. Paramagnetism of Fe2+ renders the active site of ARD' inaccessible to standard NMR methods. The structure of ARD' has been determined using Fe2+ binding parameters determined by X-ray absorption spectroscopy and NMR restraints from H98S ARD, a metal-free diamagnetic protein that is isostructural with ARD'. ARD' retains the beta-sandwich fold of ARD, but a structural entropy switch increases order at one end of a two-helix system that bisects the beta-sandwich and decreases order at the other upon interconversion of ARD and ARD', causing loss of the C-terminal helix in ARD' and rearrangements of residues involved in substrate orientation in the active site.     

The conformation of the cytoplasmic helix 8 of the CB1 cannabinoid receptor using NMR and circular dichroism

The cytoplasmic helix domain (fourth cytoplasmic loop, helix 8) of numerous GPCRs such as rhodopsin and the β-adrenergic receptor exhibits unique structural and functional characteristics. Computational models also predict the existence of such a structural motif within the CB1 cannabinoid receptor, another member of the G-protein coupled receptor superfamily. To gain insights into the conformational properties of this GPCR component, a peptide corresponding to helix 8 of the CB1 receptor with a small contiguous segment from transmembrane helix 7 (TM7) was chemically synthesized and its secondary structure determined by circular dichroism (CD) and solution NMR spectroscopy. Our studies in DPC and SDS micelles revealed significant α-helical structure while in an aqueous medium, the peptide exhibited a random coil configuration. The relative orientation of helix 8 within the CB1 receptor was obtained from intermolecular ³¹P-¹H and ¹H-¹H NOE measurements. Our results suggest that in the presence of an amphipathic membrane environment, helix 8 assumes an alpha helical structure with an orientation parallel to the phospholipid membrane surface and perpendicular to TM7. In this model, positively charged side chains interact with the lipid headgroups while the other polar side chains face the aqueous region. The above observations may be relevant to the activation/deactivation of the CB1 receptor.     

Interaction of the eukaryotic pore-forming cytolysin equinatoxin II with model membranes: 19F NMR studies

Sea anemones produce a family of 18-20 kDa proteins, the actinoporins, which lyse cells by forming pores in cell membranes. Sphingomyelin plays an important role in their lytic activity, with membranes lacking this lipid being largely refractory to these toxins. As a means of characterising membrane binding by the actinoporin equinatoxin II (EqTII), we have used 19F NMR to probe the environment of Trp residues in the presence of micelles and bicelles. Trp was chosen as previous data from mutational studies and truncated analogues had identified the N-terminal helix of EqTII and the surface aromatic cluster including tryptophan residues 112 and 116 as being important for membrane interactions. The five tryptophan residues were replaced with 5-fluorotryptophan and assigned by site-directed mutagenesis. The 19F resonance of W112 was most affected in the presence of phospholipid micelles or bicelles, followed by W116, with further change induced by the addition of sphingomyelin. Although binding to phosphatidylcholine is not sufficient to enable pore formation in bilayer membranes, this interaction had a greater effect on the tryptophan residues in our studies than the subsequent interaction with sphingomyelin. Furthermore, sphingomyelin had a direct effect on EqTII in both model membranes, so its role in EqTII pore formation involves more than simply an indirect effect mediated via bulk lipid properties. The lack of change in chemical shift for W149 even in the presence of sphingomyelin indicates that, at least in the model membranes studied here, interaction with sphingomyelin was not sufficient to trigger dissociation of the N-terminal helix from the beta-sandwich, which forms the bulk of the protein.     

Incorporation of transmembrane peptides from the vacuolar H(+)-ATPase in phospholipid membranes: spin-label electron paramagnetic resonance and polarized infrared spectroscopy

Peptides were designed that are based on candidate transmembrane sequences of the V o-sector from the vacuolar H (+)-ATPase of Saccharomyces cerevisiae. Spin-label EPR studies of lipid-protein interactions were used to characterize the state of oligomerization, and polarized IR spectroscopy was used to determine the secondary structure and orientation, of these peptides in lipid bilayer membranes. Peptides corresponding to the second and fourth transmembrane domains (TM2 and TM4) of proteolipid subunit c (Vma3p) and of the putative seventh transmembrane domain (TM7) of subunit a (Vph1p) are wholly, or predominantly, alpha-helical in membranes of dioleoyl phosphatidylcholine. All three peptides self-assemble into oligomers of different sizes, in which the helices are differently inclined with respect to the membrane normal. The coassembly of rotor (Vma3p TM4) and stator (Vph1p TM7) peptides, which respectively contain the glutamate and arginine residues essential to proton transport by the rotary ATPase mechanism, is demonstrated from changes in the lipid interaction stoichiometry and helix orientation. Concanamycin, a potent V-ATPase inhibitor, and a 5-(2-indolyl)-2,4-pentadienoyl inhibitor that exhibits selectivity for the osteoclast subtype, interact with the membrane-incorporated Vma3p TM4 peptide, as evidenced by changes in helix orientation; concanamycin additionally interacts with Vph1p TM7, suggesting that both stator and rotor elements contribute to the inhibitor site within the membrane. Comparison of the peptide behavior in lipid bilayers is made with membranous subunit c assemblies of the 16-kDa proteolipid from Nephrops norvegicus, which can substitute functionally for Vma3p in S. cerevisiae.     

Initial structural and dynamic characterization of the M2 protein transmembrane and amphipathic helices in lipid bilayers

Amphipathic helices in membrane proteins that interact with the hydrophobic/hydrophilic interface of the lipid bilayer have been difficult to structurally characterize. Here, the backbone structure and orientation of an amphipathic helix in the full-length M2 protein from influenza A virus has been characterized. The protein has been studied in hydrated DMPC/DMPG lipid bilayers above the gel to liquid-crystalline phase transition temperature by solid-state NMR spectroscopy. Characteristic PISA (Polar Index Slant Angle) wheels reflecting helical wheels have been observed in uniformly aligned bilayer preparations of both uniformly 15N labeled and amino acid specific labeled M2 samples. Hydrogen/deuterium exchange studies have shown the very slow exchange of some residues in the amphipathic helix and more rapid exchange for the transmembrane helix. These latter results clearly suggest the presence of an aqueous pore. A variation in exchange rate about the transmembrane helical axis provides additional support for this claim and suggests that motions occur about the helical axes in this tetramer to expose the entire backbone to the pore.     

Pore formation by equinatoxin, a eukaryotic pore-forming toxin, requires a flexible N-terminal region and a stable beta-sandwich

Actinoporins are eukaryotic pore-forming proteins that create 2-nm pores in natural and model lipid membranes by the self-association of four monomers. The regions that undergo conformational change and form part of the transmembrane pore are currently being defined. It was shown recently that the N-terminal region (residues 10-28) of equinatoxin, an actinoporin from Actinia equina, participates in building of the final pore wall. Assuming that the pore is formed solely by a polypeptide chain, other parts of the toxin should constitute the conductive channel and here we searched for these regions by disulfide scanning mutagenesis. Only double cysteine mutants where the N-terminal segment 1-30 was attached to the beta-sandwich exhibited reduced hemolytic activity upon disulfide formation, showing that other parts of equinatoxin, particularly the beta-sandwich and importantly the C-terminal alpha-helix, do not undergo large conformational rearrangements during the pore formation. The role of the beta-sandwich stability was independently assessed via destabilization of a part of its hydrophobic core by mutations of the buried Trp117. These mutants were considerably less stable than the wild-type but exhibited similar or slightly lower permeabilizing activity. Collectively these results show that a flexible N-terminal region and stable beta-sandwich are pre-requisite for proper pore formation by the actinoporin family.     

Structure and Dynamics of the Membrane-Bound Form of Pf1 Coat Protein: Implications of Structural Rearrangement for Virus Assembly

The three-dimensional structure of the membrane-bound form of the major coat protein of Pf1 bacteriophage was determined in phospholipid bilayers using orientation restraints derived from both solid-state and solution NMR experiments. In contrast to previous structures determined solely in detergent micelles, the structure in bilayers contains information about the spatial arrangement of the protein within the membrane, and thus provides insights to the bacteriophage assembly process from membrane-inserted to bacteriophage-associated protein. Comparisons between the membrane-bound form of the coat protein and the previously determined structural form found in filamentous bacteriophage particles demonstrate that it undergoes a significant structural rearrangement during the membrane-mediated virus assembly process. The rotation of the transmembrane helix (Q16-A46) around its long axis changes dramatically (by 160°) to obtain the proper alignment for packing in the virus particles. Furthermore, the N-terminal amphipathic helix (V2-G17) tilts away from the membrane surface and becomes parallel with the transmembrane helix to form one nearly continuous long helix. The spectra obtained in glass-aligned planar lipid bilayers, magnetically aligned lipid bilayers (bicelles), and isotropic lipid bicelles reflect the effects of backbone motions and enable the backbone dynamics of the N-terminal helix to be characterized. Only resonances from the mobile N-terminal helix and the C-terminus (A46) are observed in the solution NMR spectra of the protein in isotropic q > 1 bicelles, whereas only resonances from the immobile transmembrane helix are observed in the solid-state ¹H/¹⁵N-separated local field spectra in magnetically aligned bicelles. The N-terminal helix and the hinge that connects it to the transmembrane helix are significantly more dynamic than the rest of the protein, thus facilitating structural rearrangement during bacteriophage assembly.     

Comparison of the conformation and orientation of alamethicin and melittin in lipid membranes

The secondary structure of alamethicin in lipid membranes below and above the lipid phase transition temperature Tt is determined by Raman spectroscopy and circular dichroism (CD) measurements. In both cases structural data are obtained by fitting the experimental spectra by a superposition of the spectra of 15 reference proteins of known three-dimensional structure. According to the Raman experiments, in a lipid bilayer above Tt alamethicin is helical from residue 1 to 12, whereas below Tt the helix extends from residue 1 to 16. The remaining C-terminal part is nonhelical up to the end residue 20 both above and below Tt. A considerable lower helix content is derived from CD, namely, 38% and 46% above and below Tt, respectively, in agreement with several reported values for CD in the literature. It is shown that the commonly used set of CD spectra of water-soluble reference proteins is unsuitable to describe the CD spectra of alamethicin correctly. Therefore the secondary structure of alamethicin as derived from CD measurements is at the present state of analysis unreliable. In contrast to the case of alamethicin, the CD spectra of melittin in lipid membranes are correctly described by the reference protein spectra. The helix content of melittin is determined thereby to be 72% in lipid membranes above Tt and 75% below Tt. The data are in accord with a structure where the hydrophobic part of melittin adopts a bent helix as determined recently by Raman spectroscopy [Vogel, H., & J?hnig, F. (1986) Biophys. J. 50, 573]. The orientational order parameters of the helical parts of alamethicin and of melittin in a lipid membrane are deduced from the difference between a corresponding CD spectrum of a polypeptide in planar multibilayers and that in lipid vesicles. The presented method for determining helix order parameters is new and may be generally applicable to other membrane proteins. The orientation of the helical part of both polypeptides depends on the physical state of the lipid bilayer at maximal membrane hydration and in the ordered lipid state furthermore on the degree of membrane hydration. Under conditions where alamethicin and melittin are incorporated in an aggregated form in a fluid lipid membrane at maximal water content the helical segments are oriented preferentially parallel to the membrane normal. Cooling such lipid membranes to a temperature below Tt changes the orientation of the helical part of alamethicin as well as melittin toward the membrane plane.(ABSTRACT TRUNCATED AT 400 WORDS)     

Toward elucidating the membrane topology of helix two of the colicin E1 channel domain

The membrane-bound closed state of the colicin E1 channel domain was investigated by site-directed fluorescence labeling using a bimane fluorophore attached to each single cysteine residue within helix 2 of each mutant protein. The fluorescence properties of the bimane fluorophore were measured for the membrane-associated form of the closed channel and included fluorescence emission maximum, fluorescence anisotropy, apparent polarity, surface accessibility, and membrane bilayer penetration depth. The fluorescence data show that helix 2 is an amphipathic alpha-helix that is situated parallel to the membrane surface, but it is less deeply embedded within the bilayer interfacial region than is helix 1 in the closed channel. A least squares fit of the various data sets to a harmonic wave function indicated that the periodicity and angular frequency for helix 2 in the membrane-bound state are typical for an amphipathic alpha-helix (3.8 +/- 0.1 residues per turn and 94 +/- 4 degrees, respectively) that is located at an interfacial region of a membrane bilayer. Dual quencher analysis also revealed that helix 2 is peripherally membrane associated, with one face of the helix dipping into the interfacial region of the lipid bilayer and the other face projecting outwardly into the aqueous solvent. Finally, our data show that helices 1 and 2 remain independent helices upon membrane association with a short connector link (Tyr(363)-Gly(364)) and that short amphipathic alpha-helices participate in the formation of a lipid-dependent, toroidal pore for this colicin.     

Helical interactions and membrane disposition of the 16-kDa proteolipid subunit of the vacuolar H(+)-ATPase analyzed by cysteine replacement mutagenesis.

Theoretical mechanisms of proton translocation by the vacuolar H(+)-ATPase require that a transmembrane acidic residue of the multicopy 16-kDa proteolipid subunit be exposed at the exterior surface of the membrane sector of the enzyme, contacting the lipid phase. However, structural support for this theoretical mechanism is lacking. To address this, we have used cysteine mutagenesis to produce a molecular model of the 16-kDa proteolipid complex. Transmembrane helical contacts were determined using oxidative cysteine cross-linking, and accessibility of cysteines to the lipid phase was determined by their reactivity to the lipid-soluble probe N-(1-pyrenyl)maleimide. A single model for organization of the four helices of each monomeric proteolipid was the best fit to the experimental data, with helix 1 lining a central pore and helix 2 and helix 3 immediately external to it and forming the principal intermolecular contacts. Helix 4, containing the crucial acidic residue, is peripheral to the complex. The model is consistent not only with theoretical proton transport mechanisms, but has structural similarity to the dodecameric ring complex formed by the related 8-kDa proteolipid of the F(1)F(0)-ATPase. This suggests some commonality between the proton translocating mechanisms of the vacuolar and F(1)F(0)-ATPases.     

Control of Transmembrane Helix Dynamics by Interfacial Tryptophan Residues

Transmembrane protein domains often contain interfacial aromatic residues, which may play a role in the insertion and stability of membrane helices. Residues such as Trp or Tyr, therefore, are often found situated at the lipid-water interface. We have examined the extent to which the precise radial locations of interfacial Trp residues may influence peptide helix orientation and dynamics. To address these questions, we have modified the GW^5,19ALP23 (acetyl-GGALW⁵(LA)₆LW¹⁹LAGA-[ethanol]amide) model peptide framework to relocate the Trp residues. Peptide orientation and dynamics were analyzed by means of solid-state nuclear magnetic resonance (NMR) spectroscopy to monitor specific ²H- and ¹⁵N-labeled residues. GW^5,19ALP23 adopts a defined, tilted orientation within lipid bilayer membranes with minimal evidence of motional averaging of NMR observables, such as ²H quadrupolar or ¹⁵N-¹H dipolar splittings. Here, we examine how peptide dynamics are impacted by relocating the interfacial Trp (W) residues on both ends and opposing faces of the helix, for example by a 100° rotation on the helical wheel for positions 4 and 20. In contrast to GW^5,19ALP23, the modified GW^4,20ALP23 helix experiences more extensive motional averaging of the NMR observables in several lipid bilayers of different thickness. Individual and combined Gaussian analyses of the ²H and ¹⁵N NMR signals confirm that the extent of dynamic averaging, particularly rotational “slippage” about the helix axis, is strongly coupled to the radial distribution of the interfacial Trp residues as well as the bilayer thickness. Additional ²H labels on alanines A3 and A21 reveal partial fraying of the helix ends. Even within the context of partial unwinding, the locations of particular Trp residues around the helix axis are prominent factors for determining transmembrane helix orientation and dynamics within the lipid membrane environment.     

A complementary microscopy analysis of Sticholysin II crystals on lipid films: Atomic force and transmission electron characterizations

A new crystal form of the cytotoxin Sticholysin II (StnII) formed on lipid monolayers of 1,2-dioleoyl-sn-glycero-3-phosphatidylcholine (DOPC) has been characterized by transmission electron microscopy (TEM) and by tapping mode atomic force microscopy (AFM) under nearly physiological conditions. Both approaches show the existence of single- and double-layered 2D crystals possessing hexagonal symmetry and unit cell dimensions of a = b =10 nm and gamma = 120 degrees. However, single-layered StnII crystals could only be analysed by TEM and double-layered crystals by AFM. Considering the previously known atomic structure of native StnII and that of a tetrameric assembly, a model is proposed for this new crystal form in which StnII conserves its monomeric state upon interaction with the lipid monolayer. These results are in agreement with the existence of the so called M2 state of the actinoporins.     

Structural characterization of the pore forming protein TatAd of the twin-arginine translocase in membranes by solid-state N-NMR

The transmembrane protein TatA is the pore forming unit of the twin-arginine translocase (Tat), which has the unique ability of transporting folded proteins across the cell membrane. This ATP-independent protein export pathway is a recently discovered alternative to the general secretory (Sec) system of bacteria. To obtain insight in the translocation mechanism, the structure and alignment in the membrane of the well-folded segments 2-45 of TatA_d from Bacillus subtilis was studied here. Using solid-state NMR in bicelles containing anionic lipids, the topology and orientation of TatA_d was determined in an environment mimicking the bacterial membrane. A wheel-like pattern, characteristic for a tilted transmembrane helix, was observed in ¹⁵N chemical shift /¹⁵N-¹H dipolar coupling correlation NMR spectra. Analysis of this PISA wheel revealed a 14-16 residue long N-terminal membrane-spanning helix which is tilted by 17° with respect to the membrane normal. In addition, comparison of uniformly and selectively ¹⁵N-labeled TatA_2-45 samples allowed determination of the helix polarity angle.     

The structure of the lipid-embedded potassium channel voltage sensor determined by double-electron-electron resonance spectroscopy

A four-pulse electron paramagnetic resonance experiment was used to measure long-range inter-subunit distances in reconstituted KvAP, a voltage-dependent potassium (Kv) channel. The measurements have allowed us to reach the following five conclusions about the native structure of the voltage sensor of KvAP. First, the S1 helix of the voltage sensor engages in a helix packing interaction with the pore domain. Second, the crystallographically observed antiparallel helix-turn-helix motif of the voltage-sensing paddle is retained in the membrane-embedded voltage sensor. Third, the paddle is oriented in such a way as to expose one face to the pore domain and the opposite face to the membrane. Fourth, the paddle and the pore domain appear to be separated by a gap that is sufficiently wide for lipids to penetrate between the two domains. Fifth, the critical voltage-sensing arginine residues on the paddle appear to be lipid exposed. These results demonstrate the importance of the membrane for the native structure of Kv channels, suggest that lipids are an integral part of their native structure, and place the voltage-sensing machinery into a complex lipid environment near the pore domain.     

Solution structure of the eukaryotic pore-forming cytolysin equinatoxin II: implications for pore formation

Sea anemones produce a family of 18-20 kDa proteins, the actinoporins, that lyse cells by forming pores in cell membranes. Sphingomyelin plays an important role in their lytic activity, with membranes lacking this lipid being largely refractory to these toxins. The structure of the actinoporin equinatoxin II in aqueous solution, determined from NMR data, consists of two short helices packed against opposite faces of a beta-sandwich structure formed by two five-stranded beta-sheets. The protein core has extensive hydrophobic interfaces formed by residues projecting from the internal faces of the two beta-sheets. 15N relaxation data show uniform backbone dynamics, implying that equinatoxin II in solution is relatively rigid, except at the N terminus; its inferred rotational correlation time is consistent with values for monomeric proteins of similar mass. Backbone amide exchange rate data also support the view of a stable structure, even though equinatoxin II lacks disulfide bonds. As monitored by NMR, it unfolds at around 70 degrees C at pH 5.5. At 25 degrees C the structure is stable over the pH range 2.5-7.3 but below pH 2.5 it undergoes a slow transition to an incompletely unfolded structure resembling a molten globule. Equinatoxin II has two significant patches of positive electrostatic potential formed by surface-exposed Lys and Arg residues, which may assist its interaction with charged regions of the lipid head groups. Tyr and Trp residues on the surface may also contribute by interacting with the carbonyl groups of the acyl chains of target membranes. Data from mutational studies and truncated analogues identify two regions of the protein involved in membrane interactions, the N-terminal helix and the Trp-rich region. Once the protein is anchored, the N-terminal helix may penetrate the membrane, with up to four helices lining the pore, although other mechanisms of pore formation cannot be ruled out.     

Scanning the membrane-bound conformation of helix 1 in the colicin E1 channel domain by site-directed fluorescence labeling

Helix 1 of the membrane-associated closed state of the colicin E1 channel domain was studied by site-directed fluorescence labeling where bimane was covalently attached to a single cysteine residue in each mutant protein. A number of fluorescence properties of the tethered bimane fluorophore were measured in the membrane-bound state of the channel domain, including fluorescence emission maximum, fluorescence quantum yield, fluorescence anisotropy, membrane bilayer penetration depth, surface accessibility, and apparent polarity. The data show that helix 1 is an amphipathic alpha-helix that is situated parallel to the membrane surface. A least squares fit of the various data sets to a harmonic function indicated that the periodicity and angular frequency for helix 1 are typical for an amphipathic alpha-helix (3.7 +/- 0.1 residues per turn and 97 +/- 3.0 degrees, respectively) that is partially bathing into the membrane bilayer. Dual fluorescence quencher analysis also revealed that helix 1 is peripherally membrane-associated, with one face of the helix dipping into the lipid bilayer and the other face projecting toward the solvent. Finally, our data suggest that the helical boundaries of helix 1, at least at the C-terminal region, remain unaffected upon binding to the surface of the membrane in support of a toroidal pore model for this colicin.