Structural stability of short subsequences of the tropomyosin chain

The native tropomyosin molecule is a parallel, registered, α-helical coiled coil made from two 284-residiic chains. Long excised subsequences (≥ 95 residues) form the same structure with comparable thermal stability. Here, we investigate local stability using shorter subsequences (20-50 residues) that are chemically synthesized or excised from various regions along the protein chain. Thermal unfolding studies of such shorter peptides by CD in the same solvent medium used in extant studies of the parent protein indicate very low helix content, almost no coiled-coil formation, and high thermal lability of such secondary structure as does form. This behavior is in stark contrast to extant data on leucine-zipper peptides and short “designed” synthetic peptides, many of which have high α-helix content and form highly stable coiled coils. The existence of short coiled coils calls into question the older idea that short subsequences of a protein have little structure. The present study supports the older view, at least in its application to tropomyosin. The intrinsic local α-helical propensity and helix–helix interaction in this prototypical α-helical protein is sufficiently weak as to require not only dimerization, but macro-molecular amplification in order to attain its native conformation in common benign media near neutral pH. © 1995 John Wiley & Sons, Inc.     

Specific sequences determine the stability and cooperativity of folding of the C-terminal half of tropomyosin

Tropomyosin is a flexible 410 A coiled-coil protein in which the relative stabilities of specific regions may be important for its proper function in the control of muscle contraction. In addition, tropomyosin can be used as a simple model of natural occurrence to understand the inter- and intramolecular interactions that govern the stability of coiled-coils. We have produced eight recombinant tropomyosin fragments (Tm(143-284(5OHW),) Tm(189-284(5OHW)), Tm(189-284), Tm(220-284(5OHW)), Tm(220-284), Tm(143-235), Tm(167-260), and Tm(143-260)) and one synthetic peptide (Ac-Tm(215-235)) to investigate the relative conformational stability of different regions derived from the C-terminal region of the protein, which is known to interact with the troponin complex. Analytical ultracentrifugation experiments show that the fragments that include the last 24 residues of the molecule (Tm(143-284(5OHW)), Tm(189-284(5OHW)), Tm(220-284(5OHW)), Tm(220-284)) are completely dimerized at 10 microm dimer (50 mm phosphate, 100 mm NaCl, 1.0 mm dithiothreitol, and 0.5 mm EDTA, 10 degrees C), whereas fragments that lack the native C terminus (Tm(143-235),Tm(167-260), and Tm(143-260)) are in a monomer-dimer equilibrium under these conditions. The presence of trifluoroethanol resulted in a reduction in the [theta](222)/[theta](208) circular dichroism ratio in all of the fragments and induced stable trimer formation only in those containing residues 261-284. Urea denaturation monitored by circular dichroism and fluorescence revealed that residues 261-284 of tropomyosin are very important for the stability of the C-terminal half of the molecule as a whole. Furthermore, the absence of this region greatly increases the cooperativity of urea-induced unfolding. Temperature and urea denaturation experiments show that Tm(143-235) is less stable than other fragments of the same size. We have identified a number of factors that may contribute to this particular instability, including an interhelix repulsion between g and e' positions of the heptad repeat, a charged residue at the hydrophobic coiled-coil interface, and a greater fraction of beta-branched residues located at d positions.     

Design, synthesis and structural characterization of model heterodimeric coiled-coil proteins.

We report the design and synthesis of model heterodimeric coiled-coil proteins and the packing contribution of interchain hetero-hydrophobic side-chains to coiled-coil stability. The heterodimeric coiled-coils are obtained by oxidizing two 35-residue polypeptide chains, each containing a cysteine residue at position 2 and differing in amino acid sequences in the hydrophobic positions ("a" and "d") responsible for the formation and stabilization of the coiled-coil. In each peptide, a single Ala residue was substituted for Leu at position "a" or "d". The formation and stability of heterodimeric coiled-coils were investigated by circular dichroism studies in the presence and absence of guanidine hydrochloride and compared to the corresponding homodimeric coiled-coils. The coiled-coil proteins with an Ala substitution at position "a" were less stable than those with an Ala substitution at position "d" in both the homodimeric (Ala-Ala interchain interactions) and heterodimeric (Leu-Ala interchain interactions ) coiled-coils. The 70-residue disulfide bridged peptides (homo- and heterodimeric coiled-coils) can be readily separated by reversed-phase chromatography (RPC) even though they have identical amino acid compositions as well as in the hydrophobic "a" and "d" positions. The elution of the 70-residue peptides prior to their corresponding 35-residue monomers suggests that these proteins are retaining a large portion of their coiled-coil structure during RPC at pH2 and their retention behavior correlates with protein stability.     

Thermal unfolding equilibria in homodimeric chicken gizzard tropomyosin coiled coils

CD studies are presented on thermal unfolding of coiled-coil homodimers of two genetic variant chains of chicken gizzard tropomyosin (CG-Tm). The experiments include the effects of cross-linking both isoforms and the dependence on protein concentration of unfolding in both reduced isoforms, variables not examined in extant work. The general shapes of the unfolding curves for singly cross-linked species depend on whether the crosslink is at C190 (its site on one isoform) or at C36 (its site on the other). These curves are compared with extant ones for various cross-linked species of rabbit tropomyosin. The comparison supports the view that the unfolding behavior of cross-linked species results from a complex interaction of strain at the cross-link, local variations in structural stability, and loop entropy. The observed concentration dependence of the transition temperature for the uncross-linked (reduced) species of CG-Tm is very small (2.9°C) for one variant homodimer and unobservably small (< 2°C) for the other in the 100-fold concentration range (～ 0.01–1.0 mg/mL) accessible here. These experimental values of ΔT_m are much smaller than are predicted from extant values of the van't Hoff transition enthalpies, calling the latter into question. © 1994 John Wiley & Sons, Inc.     

Clustering of large hydrophobes in the hydrophobic core of two-stranded alpha-helical coiled-coils controls protein folding and stability

The de novo design and biophysical characterization of two 60-residue peptides that dimerize to fold as parallel coiled-coils with different hydrophobic core clustering is described. Our goal was to investigate whether designing coiled-coils with identical hydrophobicity but with different hydrophobic clustering of non-polar core residues (each contained 6 Leu, 3 Ile, and 7 Ala residues in the hydrophobic core) would affect helical content and protein stability. The disulfide-bridged P3 and P2 differed dramatically in alpha-helical structure in benign conditions. P3 with three hydrophobic clusters was 98% alpha-helical, whereas P2 was only 65% alpha-helical. The stability profiles of these two analogs were compared, and the enthalpy and heat capacity changes upon denaturation were determined by measuring the temperature dependence by circular dichroism spectroscopy and confirmed by differential scanning calorimetry. The results showed that P3 assembled into a stable alpha-helical two-stranded coiled-coil and exhibited a native protein-like cooperative two-state transition in thermal melting, chemical denaturation, and calorimetry experiments. Although both peptides have identical inherent hydrophobicity (the hydrophobic burial of identical non-polar residues in equivalent heptad coiled-coil positions), we found that the context dependence of an additional hydrophobic cluster dramatically increased stability of P3 (Delta Tm approximately equal to 18 degrees C and Delta[urea](1/2) approximately equal to 1.5 M) as compared with P2. These results suggested that hydrophobic clustering significantly stabilized the coiled-coil structure and may explain how long fibrous proteins like tropomyosin maintain chain integrity while accommodating polar or charged residues in regions of the protein hydrophobic core.     

Coiled-Coil Response to Mechanical Force: Global Stability and Local Cracking

Coiled coils are important structural motifs formed by two or more amphipathic α-helices that twist into a supercoil. These motifs are found in a wide range of proteins, including motor proteins and structural proteins, that are known to transmit mechanical loads. We analyze atomically detailed simulations of coiled-coil cracking under load with Milestoning. Milestoning is an approach that captures the main features of the process in a network, quantifying kinetics and thermodynamics. A 112-residue segment of the β-myosin S2 domain was subjected to constant-magnitude (0–200 pN) and constant-direction tensile forces in molecular dynamics simulations. Twenty 20 ns straightforward simulations at several load levels revealed that initial single-residue cracking events (Ψ > 90°) at loads <100 pN were accompanied by rapid refolding without either intra- or interhelix unfolding propagation. Only initial unfolding events at the highest load (200 pN) regularly propagated along and between helices. Analysis of hydrophobic interactions and of interhelix hydrogen bonds did not show significant variation as a function of load. Unfolding events were overwhelmingly located in the vicinity of E929, a charged residue in a hydrophobic position of the heptad repeat. Milestoning network analysis of E929 cracking determined that the mean first-passage time ranges from 20 ns (200 pN) to 80 ns (50 pN), which is ∼20 times the mean first-passage time of an isolated helix with the same sequence.     

Phosphorylation of alpha alpha- and beta beta-tropomyosin and synthetic peptide analogues

A tropomyosin kinase partially purified from chicken embryos was used to study the phosphorylation mechanism of alpha alpha- and beta beta-tropomyosin and synthetic peptides containing the site of phosphorylation at Ser-283 and corresponding to residues 264-284 of the tropomyosin isoforms. The apparent Km is 47 microM for alpha alpha- and 265 microM for beta beta-tropomyosin, whereas the Vmax values are similar. The alpha [264-284] and beta [264-284] peptides have apparent Km values of 500 microM and 650 microM, respectively, and Vmax values similar to that of the intact tropomyosin. This indicates that the conformation of the phosphorylation site at the COOH-terminal end of tropomyosin contributes significantly to the phosphorylation of the substrate. Furthermore, the marginal difference in the Km values of the alpha- and beta-peptide cannot account for the 5-fold difference in the Km of the native alpha alpha and beta beta isoforms, suggesting that the conformations of alpha alpha- and beta beta-tropomyosin at the phosphorylation sites are significantly different. Phosphorylation of beta-peptide analogues, each with a single substitution corresponding to the alpha sequence, indicates that His-276 and Ile-284 have negative influences on the phosphorylation of the beta-peptide, whereas Met-281 improves it. Direct analyses of the time courses of phosphorylation of alpha alpha-tropomyosin at 37 degrees C, where head-to-tail polymerization is minimized, show that a single exponential can fit the data satisfactorily. This indicates a random phosphorylation of two identical chains.(ABSTRACT TRUNCATED AT 250 WORDS)     

Amino acid sequence of chicken gizzard beta-tropomyosin. Comparison of the chicken gizzard, rabbit skeletal, and equine platelet tropomyosins

Chicken gizzard beta-tropomyosin has the same chain length (284 residues) as other muscle tropomyosins, and is most closely related to the beta component of rabbit skeletal muscle. The majority of the amino acid substitutions are restricted to two regions of the structure, residues 185-216 and 258-284. The altered sequences at the COOH-terminal ends (residue 258-284) of the two gizzard components are very similar to each other and to those in platelet tropomyosin and can be correlated with the reduced affinity of interaction of all three tropomyosins with skeletal troponin T and its T1 fragment. The virtually identical NH2-terminal sequences of all four muscle tropomyosin chains indicates that the gizzard proteins' greater ability to polymerize head-to-tail is due to the sequence changes at its COOH terminus. On the other hand, the weaker head-to-tail aggregation of the platelet protein must be due to its NH2-terminal sequence alterations. Examination of the distribution of amino acids and the frequency of their substitution in the a to g positions of the repeating pseudoheptapeptide for all five tropomyosin sequences (four muscle and one platelet) emphasizes the importance of Glu residues at position e. Examination of those features of the muscle sequences implicated in the stabilization of their coiled-coil structures and in their interactions with F-actin suggest only marginal differences among them, with the possible exception of the chicken gizzard gamma component.     

Stabilizing and destabilizing clusters in the hydrophobic core of long two-stranded alpha-helical coiled-coils

Detailed sequence analyses of the hydrophobic core residues of two long two-stranded alpha-helical coiled-coils that differ dramatically in sequence, function, and length were performed (tropomyosin of 284 residues and the coiled-coil domain of the myosin rod of 1086 residues). Three types of regions were present in the hydrophobic core of both proteins: stabilizing clusters and destabilizing clusters, defined as three or more consecutive core residues of either stabilizing (Leu, Ile, Val, Met, Phe, and Tyr) or destabilizing (Gly, Ala, Cys, Ser, Thr, Asn, Gln, Asp, Glu, His, Arg, Lys, and Trp) residues, and intervening regions that consist of both stabilizing and destabilizing residues in the hydrophobic core but no clusters. Subsequently, we designed a series of two-stranded coiled-coils to determine what defines a destabilizing cluster and varied the length of the destabilizing cluster from 3 to 7 residues to determine the length effect of the destabilizing cluster on protein stability. The results showed a dramatic destabilization, caused by a single Leu to Ala substitution, on formation of a 3-residue destabilizing cluster (DeltaT(m) of 17-21 degrees C) regardless of the stability of the coiled-coil. Any further substitution of Leu to Ala that increased the size of the destabilizing cluster to 5 or 7 hydrophobic core residues in length had little effect on stability (DeltaT(m) of 1.4-2.8 degrees C). These results suggested that the contribution of Leu to protein stability is context-dependent on whether the hydrophobe is in a stabilizing cluster or its proximity to neighboring destabilizing and stabilizing clusters.     

Structure and flexibility of the tropomyosin overlap junction

To be effective as a gatekeeper regulating the access of binding proteins to the actin filament, adjacent tropomyosin molecules associate head-to-tail to form a continuous super-helical cable running along the filament surface. Chimeric head-to-tail structures have been solved by NMR and X-ray crystallography for N- and C-terminal segments of smooth and striated muscle tropomyosin spliced onto non-native coiled-coil forming peptides. The resulting 4-helix complexes have a tight coiled-coil N-terminus inserted into a separated pair of C-terminal helices, with some helical unfolding of the terminal chains in the striated muscle peptides. These overlap complexes are distinctly curved, much more so than elsewhere along the superhelical tropomyosin cable. To verify whether the non-native protein adducts (needed to stabilize the coiled-coil chimeras) perturb the overlap, we carried out Molecular Dynamics simulations of head-to-tail structures having only native tropomyosin sequences. We observe that the splayed chains all refold and become helical. Significantly, the curvature of both the smooth and the striated muscle overlap domain is reduced and becomes comparable to that of the rest of the tropomyosin cable. Moreover, the measured flexibility across the junction is small. This and the reduced curvature ensure that the super-helical cable matches the contours of F-actin without manifesting localized kinking and excessive flexibility, thus enabling the high degree of cooperativity in the regulation of myosin accessibility to actin filaments.     

The thermal denaturation of nonpolymerizable alpha alpha-tropomyosin and its segments as a function of ionic strength

Nonpolymerizable tropomyosin (NPTm) is found to unfold thermally at high ionic strength almost exactly as the parent protein, but it does not aggregate at low ionic strength. Thus, NPTm can be used as a tropomyosin surrogate whose coiled-coil structural stability can be probed by varying the ionic strength. Studies of NPTm by CD show that increasing ionic strength stabilizes the coiled-coil structure. CD spectra over a wide range of helix content, obtained by varying either temperature or ionic strength, show an isodichroic point at 203 nm, suggesting a local, residue-level, two-state model. At given temperature, such a local helix in equilibrium random equilibrium suggests ln [phi h/(1-phi h)] = A1 + A2In, wherein phi h is the fraction helix, and A1, A2, and n are constants. In the low ionic strength region, theoretical limiting laws for ionic strength mediated charge-charge, dipole-dipole, and apolar-apolar (salting out) interactions give, respectively, n = 0.5, 1.0, and 1.0. Our experimental values for 40 degrees C, where the data span a wide range of helix content, show n = 1.0, suggesting that ionic strength stabilizes either by reducing dipole-dipole repulsions or by enhancing hydrophobic interactions, both probably interhelix in nature. Two segments of tropomyosin, 11Tm127 and 142Tm281, neither of which aggregate at low ionic strength, give results similar to those for NPTm, i.e., n = 0.96 and 0.84, respectively.     

Molecular Dynamics Simulations of Homo-oligomeric Bundles Embedded Within a Lipid Bilayer

Using molecular dynamics simulations, we studied the structure, interhelix interactions, and dynamics of transmembrane proteins. Specifically, we investigated homooligomeric helical bundle systems consisting of synthetic α-helices with either the sequence Ac-(LSLLLSL)₃-NH₂ (LS2) or Ac-(LSSLLSL)₃-NH₂ (LS3). The LS2 and LS3 helical peptides are designed to have amphipathic characteristics that form ion channels in membrane. We simulated bundles containing one to six peptides that were embedded in palmitoyl-oleoyl-phosphatidylcholine (POPC) lipid bilayer and placed between two lamellae of water. We aim to provide a fundamental understanding of how amphipathic helical peptides interact with each other and their dynamical behaviors in different homooligomeric states. To understand structural properties, we examined the helix lengths, tilt angles of individual helices and the entire bundle, interhelix distances, interhelix cross-angles, helix hydrophobic-to-hydrophilic vector projections, and the average number of interhelix hydrophilic (serine–serine) contacts lining the pore of the transmembrane channel. To analyze dynamical properties, we calculated the rotational autocorrelation function of each helix and the cross-correlation of the rotational velocity between adjacent helices. The observed structural and dynamical characteristics show that higher order bundles containing four to six peptides are composed of multiple lower order bundles of one to three peptides. For example, the LS2 channel was found to be stable in a tetrameric bundle composed of a “dimer of dimers.” In addition, we observed that there is a minimum of two strong hydrophilic contacts between a pair of adjacent helices in the dimer to tetramer systems and only one strong hydrophilic interhelix contact in helix pairs of the pentamer and hexamer systems. We believe these results are general and can be applied to more complex ion channels, providing insight into ion channel stability and assembly.     

The structure of the carboxyl terminus of striated alpha-tropomyosin in solution reveals an unusual parallel arrangement of interacting alpha-helices

Coiled coils are well-known as oligomerization domains, but they are also important sites of protein-protein interactions. We determined the NMR solution structure and backbone (15)N relaxation rates of a disulfide cross-linked, two-chain, 37-residue polypeptide containing the 34 C-terminal residues of striated muscle alpha-tropomyosin, TM9a(251-284). The peptide binds to the N-terminal region of TM and to the tropomyosin-binding domain of the regulatory protein, troponin T. Comparison of the NMR solution structure of TM9a(251-284) with the X-ray structure of a related peptide [Li, Y., Mui, S., Brown, J. H., Strand, J., Reshetnikova, L., Tobacman, L. S., and Cohen, C. (2002) Proc. Natl. Acad. Sci. U.S.A. 99, 7378-7383] reveals significant differences. In solution, residues 253-269 (like most of the tropomyosin molecule) form a canonical coiled coil. Residues 270-279, however, are parallel, linear helices, novel for tropomyosin. The packing between the parallel helices results from unusual interface residues that are atypical for coiled coils. Y267 has poor packing at the coiled-coil interface and a lower R(2) relaxation rate than neighboring residues, suggesting there is conformational flexibility around this residue. The last five residues are nonhelical and flexible. The exposed surface presented by the parallel helices, and the flexibility around Y267 and the ends, may facilitate binding to troponin T and formation of complexes with the N-terminus of tropomyosin and actin. We propose that unusual packing and flexibility are general features of coiled-coil domains in proteins that are involved in intermolecular interactions.     

The CD of two-chain coiled coils: experiments on tropomyosin and tropomyosin segments in the tyrosine/disulfide spectral region

CD experiments are reported for several coiled-coil species in the tyrosine/disulfide (approximately 250-350-nm) region. Intact noncross-linked tropomyosin (approximately 3 degrees C) shows a negative nonsymmetric band maximal at 280 nm. This spectrum is the sum over six tyrosines/chain, and has conformational significance, since it disappears on denaturation. Experiments on an excised coiled-coil segment, each of whose chains comprise residues 11-127 of the tropomyosin sequence and only one tyrosine (Y60), reveal that not all tyrosines are alike. The spectrum at 3 degrees C shows a small negative maximum at approximately 285 nm and a substantial, hitherto unknown, positive band at approximately 270 nm, the latter masked in the parent protein by the negative contribution from the other tyrosines. A noncross-linked coiled-coil segment comprising residues 142-281, in which Y60 is absent, shows no such positive band. This peculiarity of Y60 is confirmed by absorbance spectra, with the extinction coefficient of Y60 larger in benign media than the average of the other tyrosines. Intact (3 degrees C) C190 cross-linked tropomyosin is known to yield, besides tyrosine contributions, a positive maximum at approximately 300 nm. Subtracting the corresponding data for noncross-linked tropomyosin shows that the disulfide spectrum itself actually has two equal, partly resolved bands at, respectively, 250 and 280 nm. The existence of a chiral disulfide argues for a relatively rigid, perhaps strained, local coiled coil. A C190 cross-linked segment comprising residues 142-281 shows a chiral disulfide spectrum like tropomyosin's, but another segment, comprising residues 168-284, shows none; thus removal of residues 142-167 causes loss of chirality at C190, over 20 residues away. These spectra thus contain important information on the subtle local differences in coiled-coil structures.     

The use of spectral decomposition via the convex constraint algorithm in interpreting the CD-observed unfolding transitions of C coils

Decomposition of CD spectra for the unfolding of both coiled-coil and single-helical molecules is carried out via the convex constraint algorithm (CCA) [A. Perczel, M. Hollósi, G. Tusnády, and G. D. Fasman (1991) Protein Engineering, Vol. 4, pp. 669–679]. Examined are (1) our thermal unfolding data for rabbit αα-tropomyosin and chicken gizzard γγ- tropomyosin coiled coils, and for a35-residue, tropomyosin-model peptide that forms single helices, not coiled coils; (2) extent pH-induced unfolding data for 50- and 400-residue poly-L -glutamic acid. Each set of spectra shows a sharp isodichroic point near 203 nm. We find here that the CCA is of sharply limited use for analyzing such data. The component spectra obtained for a given substance not only depend on the particular experimental spectra included and on the chosen number of component spectra, but all pass through the experimental isodichroic point. The latter is physically unlikely for more than three component spectra, and physically impossible for conformers, such as β structures, having known isodichroic points elsewhere. Our conclusions are in contrast to those of an extant decomposition via CCA of thermal spectra for rabbit αα-tropomyosin [N. J. Greenfield and S. E. Hitchcock-DeGregori(1993) Protein Science, Vol. 2, pp. 1263-1273] that postulates the existence of five conformers, including β structures, in the unfolding. Moreover, an extant diagnostic based on the θ₂₂₂/θ₂₀₈ ratio and allegedly distinguishing between spectra for coiled coil and for single α-helix is shown here to be unreliable. © 1995 John Wiley & Sons, Inc.     

Molecular Dynamics Simulations of Homo-oligomeric Bundles Embedded Within a Lipid Bilayer

Using molecular dynamics simulations, we studied the structure, interhelix interactions, and dynamics of transmembrane proteins. Specifically, we investigated homooligomeric helical bundle systems consisting of synthetic α-helices with either the sequence Ac-(LSLLLSL)₃-NH₂ (LS2) or Ac-(LSSLLSL)₃-NH₂ (LS3). The LS2 and LS3 helical peptides are designed to have amphipathic characteristics that form ion channels in membrane. We simulated bundles containing one to six peptides that were embedded in palmitoyl-oleoyl-phosphatidylcholine (POPC) lipid bilayer and placed between two lamellae of water. We aim to provide a fundamental understanding of how amphipathic helical peptides interact with each other and their dynamical behaviors in different homooligomeric states. To understand structural properties, we examined the helix lengths, tilt angles of individual helices and the entire bundle, interhelix distances, interhelix cross-angles, helix hydrophobic-to-hydrophilic vector projections, and the average number of interhelix hydrophilic (serine–serine) contacts lining the pore of the transmembrane channel. To analyze dynamical properties, we calculated the rotational autocorrelation function of each helix and the cross-correlation of the rotational velocity between adjacent helices. The observed structural and dynamical characteristics show that higher order bundles containing four to six peptides are composed of multiple lower order bundles of one to three peptides. For example, the LS2 channel was found to be stable in a tetrameric bundle composed of a “dimer of dimers.” In addition, we observed that there is a minimum of two strong hydrophilic contacts between a pair of adjacent helices in the dimer to tetramer systems and only one strong hydrophilic interhelix contact in helix pairs of the pentamer and hexamer systems. We believe these results are general and can be applied to more complex ion channels, providing insight into ion channel stability and assembly.     

Porcine platelet tropomyosin: Purification,characterization and paracrystal formation

Porcine platelet tropomyosin has been isolated by hydroxyapatite chromatography following isoelectric precipitation and ethanol fractionation. A single component (M_r = 30,000 on polyacrylamide gel electrophoresis in sodium dodecyl sulphate) was obtained in a variety of gel electrophoretic systems, including urea/sodium dodecyl sulphate and isoelectric focussing, suggesting the presence of a single polypeptide species. This contrasts with the observations by others using horse platelet tropomyosin or tropomyosins isolated from brain, where two polypeptides were found. The amino acid composition of porcine platelet tropomyosin was virtually identical to that of the horse platelet protein except for the presence of a single cysteine residue in the pig protein, whereas horse tropomyosin contains two. Oxidation of this sulphydryl group produced a molecule of over 60,000 M_r on polyacrylamide gels in sodium dodecyl sulphate, suggesting by analogy with skeletal muscle tropomyosin that the two chains had been linked and therefore existed in register in the coiled-coil structure. Cleavage at the cysteine produced a fragment of M_r = 19,000, indicating that this residue was located about one-third of the distance from a molecular end.Magnesium paracrystals of platelet tropomyosin were examined by electron microscopy following negative staining and found to have a repeat of 345 Å, close to that expected for an extended alpha-helical coiled-coil with an apparent M_r of 30,000. The repeating unit was centrosymmetric and the appearance of broken paracrystals suggested that the molecular ends lie on a dyad axis. Location of the sulphydryl residues in the paracrystals by labelling with N-pyrrolo-isomaleimide showed two bands separated by approximately 80 Å, which was consistent with the location of the molecular ends on a dyad.The amount of tropomyosin present was estimated as 2·2% of the total platelet protein. This implied a molar ratio of G-actin to tropomyosin of about 14:1, based on previous estimates of the actin content in porcine platelets. Assuming that one molecule of tropomyosin will bind six molecules of actin (based on the reduced molecular length of the platelet protein), there was not sufficient tropomyosin to bind to more than half the total actin in the cell.     

Compatibility of the conformationally rigid CF3-Bpg side chain with the hydrophobic coiled-coil interface

3-(Trifluoromethyl)bicyclopent-[1.1.1]-1-yl glycine (CF₃-Bpg) has previously been established as a useful ¹⁹F NMR label to analyse the structures of oligomeric membrane-active peptides or transmembrane segments. To systematically examine the effect of side chain volume, conformational rigidity, and hydrophobicity of CF₃-Bpg in polypeptide environments the amino acid was incorporated into an established coiled-coil based screening system. A single substitution of either valine (position a16) or leucine (position d19) within the hydrophobic core of the heteromeric coiled coil has practically no effect on its structure. Despite its comparatively high hydrophobicity, however, the stiff and bulky side chain of CF₃-Bpg is not so well accommodated by the hydrophobic core as it leads to a more pronounced destabilization than observed for other, more polar fluorinated amino acids which carry more flexible side chains. CF₃-Bpg is therefore a useful ¹⁹F NMR label, though not for monitoring the stability of such helix–helix interactions.     

Modeling of Peptides in Implicit Membrane-Mimetic Media

Abstract

Lipid bilayer plays a crucial role in folding of membrane peptides and their stabilization in the membrane-bound state. Correct treatment of the media effects is thus essential for realistic simulations of peptides in bilayers. Previously (Volynsky et al., 1999), we proposed an efficient solvation model which mimics heterogeneous membrane-water system. The model is based on combined employment of atomic solvation parameters for water and hydrocarbon, which approximate hydrated headgroups and acyl chains of lipids, respectively. In this study, the model is employed in non-restrained Monte Carlo simulations of several peptides: totally apolar 20-residue poly-L-Leu, hydrophobic peptide with polar edges, and strongly amphiphilic pep-tide. The principal goals are: to explore energy landscape of these peptides in membrane; to characterize the structures of low-energy states and their orientations with respect to the bilayer. Simulations were performed starting from different structures (unordered or helical) and orientations. It was found that the membrane environment significantly promotes an α-helical conformation for all the peptides, while their energetically favourable orientations are quite different. Thus, poly-Leu was immobilized inside the membrane, the hydrophobic peptide with polar termini adapted transbilayer orientation, whereas the amphiphilic peptide stayed on the lipid-water interface in peripherial orientation. Energy barriers between different states were characterized. The computational results were compared with the experimental structural data.     

Cloning of milk-derived bioactive peptides in <Emphasis Type="Italic">Streptococcus thermophilus</Emphasis>

The enzymatic breakdown of milk proteins releases bioactive peptides. Two such peptides are the 11-residue antimicrobial peptide from bovine lactoferrin (BL-11) and the 12-residue hypotensive peptide from α_s1-casein (C-12). These two peptides have now been cloned in Streptococcus thermophilus to develop strains that enhance the functionality and nutritional value of dairy food products. Nucleic acid sequences encoding the peptides were generated by overlapping PCR and were subsequently cloned into a new expression vector under control of the ST₂₂₀₁ promoter. S. thermophilus transformants were successfully identified using GFP as a selectable marker. The presence of the synthetic gene constructs in S. thermophilus was confirmed by PCR. Electronic supplementary material The online version of this article (doi:) contains supplementary material, which is available to authorized users.