Vibrational CD of polypeptides. X. A study of alpha-helical oligopeptides in solution

We have measured the vibrational CD (VCD) of a series of heterooligopeptides—o-nitrophenylsulfenyl(L -Met-L -Met-L -Leu) _n-OEt, n = 6,8,10,11–in the amide A, I, and II regions. These spectra are identical in shape and magnitude, within our signal to noise limits. The VCD in each band are of exactly the shape expected for a right-handed α-helix and imply that VCD of the polypeptide α-helix is relatively unaffected by chain length down to the 18-subunit level.     

Dipole moments of random coil polypeptides

The Rotational Isomeric States model is applied to calculate dipole moments of polypeptides of the twenty natural α-amino acids in the random coil state. Dipole moments of each repeat unit (μ_i), are evaluated using a quantum mechanics procedure. Dipole moment ratios ($\text{D}{}_{\mathrm{x}}\text{=}\text{〈μ}{}^2\text{〉}\text{x}\text{μ}{}_{\mathrm{i}}{}^2\text{,}\text{x = number of repeat units}$) of homopolypeptides are calculated and extrapolated to x →?. With a few exceptions, D_? = 0.36 ± 0.1. Ten actual proteins and three enzymes are also studied; their dipole ratios (D_x′ =〈μ〉/x) range from 7.34 to 10.57 in 10^?59 C² m² (6.6–9.5 D²). Diffferences in the values of D_x′ are due mainly to the different contributions, μ_i, of the amino acid residues contained in each polymer, whereas the sequence of amino acids has a very minor effect.     

Intrinsic viscosity of ovomucoid in random coil conformation.

Ovomucoid is denatured by concentrated solutions of guanidine hydrochloride. The intrinsic viscosities of the glycoprotein in 6 M guanidine hydrochloride in the absence and presence of beta-mercaptoethanol were found to be 8.1 and 16.0 ml/g, respectively. Ovomucoid with disulphide bonds reduced exists in linear random coil conformation. However, the intrinsic viscosity of the randomly coiled protein was less than that predicted from the empirical equations describing the molecular weight dependence of intrinsic viscosities of random coil proteins in 6 M guanidine hydrochloride. On excluding the carbohydrate content of the protein, which is theoretically justified, the calculated intrinsic viscosity interestingly became closer to the measured one. The temperature dependence of the intrinsic viscosity of ovomucoid in linear random coil conformation was studied in the temperature range, 25-55 degrees. The features of the intrinsic viscosity-temperature profile are not comparable with those exhibited by other linear random coil proteins in 6 M guanidine hydrochloride.     

Discriminating 3(10)- from alpha-helices: vibrational and electronic CD and IR absorption study of related Aib-containing oligopeptides

Model peptides based on -(Aib-Ala)(n)-, and (Aib)(n)-Leu-(Aib)(2) sequences, which have varying amounts of 3(10)-helical character, were studied by use of vibrational and electronic circular dichroism (VCD and ECD) and Fourier transform infrared (FTIR) absorption spectroscopies to test the correlation of spectral response and conformation. The data indicate that these peptides, starting from a length of about four to six residues, predominantly adopt a 3(10)-helical conformation at room temperature. The longest model peptides, depending on the series, may evidence some alpha-helical contribution to the spectra, while the shorter ones, with less than six residues, have much less order. The IR absorption spectra (as supported by theory) showed only small frequency changes between 3(10)- and alpha-helices. By contrast, solvent effects are a source of much bigger perturbations. The ECD results show that the intensity ratio for the approximately 222-nm to approximately 208-nm bands, while useful for distinguishing between these two helical types in some sequences, may have a narrower range of application than VCD. However, the VCD data presented here continue to support the proposed discrimination between alpha- and 3(10)-helices based on qualitative amide I and II bandshape differences. The present study shows the intensities of the 3(10)-helical amide I (peak-to-peak) to its amide II VCD to be of the same order and useful for discriminating them from alpha-helices, whose amide I dominates the amide II in intensity. This qualitative result is experimentally independent of the amount of alphaMe-substituted residues in the sequence. These experimental VCD results are consistent in detail with theoretical spectral simulations for Ac-(Ala)(8)-NH(2), Ac-(Aib-Ala)(4)-NH(2), and Ac-(Aib)(8)-NH(2) in 3(10)- and alpha-helical conformations.     

A systematic study of the vibrational free energies of polypeptides in folded and random states

Molecular vibrations, especially low frequency motions, may be used as an indication of the rigidity or the flatness of the protein folding energy landscape. We have studied the vibrational properties of native folded as well as random coil structures of more than 60 polypeptides. The picture we obtain allows us to perceive how and why the energy landscape progressively rigidifies while still allowing potential flexibility. Compared with random coil structures, both alpha-helices and beta-hairpins are vibrationally more flexible. The vibrational properties of loop structures are similar to those of the corresponding random coil structures. Inclusion of an alpha-helix tends to rigidify peptides and so-called building blocks of the structure, whereas the addition of a beta-structure has less effect. When small building blocks coalesce to form larger domains, the protein rigidifies. However, some folded native conformations are still found to be vibrationally more flexible than random coil structures, for example, beta(2)-microglobulin and the SH3 domain. Vibrational free energy contributes significantly to the thermodynamics of protein folding and affects the distribution of the conformational substates. We found a weak correlation between the vibrational folding energy and the protein size, consistent with both previous experimental estimates and theoretical partition of the heat capacity change in protein folding.     

Solution conformation of human apolipoprotein C-1 inferred from proline mutagenesis: far- and near-UV CD study

Solution structure of lipid-free apolipoprotein C-1 (apoC-1, 6.6 kD) was analyzed by circular dichroism (CD) of 15 mutants containing single Pro or Ala substitutions in predicted alpha-helical regions. While the majority of Pro substitutions induce complete (L11P, L18P, R23P, I29P, M38P, W41P, T45P) or partial (G15P, L34P) helical unfolding, similar substitutions at other sites (A7P, Q31P, V49P, L53P) do not cause large changes in the secondary structure or stability. The results suggest that lipid-free apoC-1 is comprised of two dynamic helices that are stabilized by interhelical interactions and are connected by a short linker containing residues 30-33. We propose that the minimal folding unit in the lipid-free state of this and other exchangeable apolipoproteins comprises the helix-turn-helix motif formed of four 11-mer sequence repeats. Comparison of the helical content in lipid-free and lipid-bound apoC-1 suggests that lipid binding shifts the conformational equilibrium toward preexisting highly helical conformation. Remarkably, near-UV CD spectra of wild type and mutant apoC-1 are not significantly altered upon thermal or chemical unfolding and thus result from residual aromatic clustering that is retained in the unfolded state. Correlation of far- and near-UV CD of the mutant peptides suggests that the hydrophobic cluster containing W41 is essential for the helical stability and may form a helix nucleation site in apoC-1.     

Vibrational CD of polypeptides. XII. Reevaluation of the Fourier transform vibrational CD of poly(gamma-benzyl-L-glutamate)

Using a newly constructed Fourier transform ir (FTIR) based vibrational CD (VCD) instrument, we have found that elimination of the ellipsoidal collection mirror before the detector and its replacement by a lens leads to a significant improvement in the absorption artifact problem often seen previously in FTIR-VCD. Reduction in artifact level brings the FTIR-VCD band shape of the amide 1 band in poly(γ-benzyl-L -glutamate) into better agreement with that found with dispersive instruments. These results indicate that the difference between the spectra obtained with the two methods is not primarily a factor of resolution but is more dependent on artifact level. Thus the previously reported deconvolution of the amide I VCD results and their subsequent interpretation in terms of the helical vs. exciton mechanisms overemphasize weak features in the spectrum. Results based on deconvolution of the absorption spectrum remain valid. Further new data on the amide II and several lower energy transitions that encompass the amide III region show broad single-signed features—but of the opposite sense—in the two regions, implying that their VCD arises through mutual coupling.     

Increasing the thermostability of D-xylose isomerase by introduction of a proline into the turn of a random coil.

Thermostability can be increased by introducing prolines at suitable sites in target proteins. Two single (G138P, G247D) mutants and one double (G138P/G247D) mutant of xylose isomerase from Streptomyces diastaticus No.7, strain M1033 have been constructed by site-directed mutagenesis. With respect to the wild-type enzyme, G138P showed about a 100% increase in thermostability, and G247D showed an increased catalytic activity. Significantly, the double mutant, G138P/G247D displayed even higher activity than G247D and better heat stability than G138P. Its half life was about 2.5-fold greater than the wild-type enzyme, using xylose as a substrate. Molecular modelling suggested that the introduction of a proline residue in the turn of a random coil may cause the surrounding conformation to be tightened by reducing the backbone flexibility. The change in thermostability can, therefore, be explained based on changes in the molecular rigidity. Furthermore, the improvements in the properties of the double mutant indicated that the advantages of two single mutants can be combined effectively.     

Influence of the solvent on the conformational-dependent properties of random coil polypeptides. II. Mean square optical anisotropies and Kerr constants

Mean square optical anisotropies and molar Kerr constants were calculated for homopolypeptides of the 20 natural amino acids and of several enzymes and proteins in the random-coil state. The effect of hydration was taken into account in constructing the molecular potential that gives the conformational energies as a function of the rotational angles phi and psi of the backbone and chi(1) of the side chain. The Rotational Isomeric State model was used in calculated energies, the Valence Optical Scheme and the matrix calculus technique of Flory being employed in the evaluation of the optical properties. The results are compared with calculations for the same substances that were performed without taking into account the solvent, as well as with other similar studies. The Kerr constant is confirmed as being one of the most sensitive properties of a given polypeptide to the residue class and to the sequence of those residues.     

Alpha-helix to random coil transitions: determination of peptide concentration from the CD at the isodichroic point.

A method is presented for determining the concentrations of peptides and proteins having isodichroic points near 203 nm. The existence of an isodichroic point for a given substance indicates a local two-state (alpha-helix, random coil) population. The mean residue ellipticity at the isodichroic point, [theta lambda i], is, of course, independent of helix content. For a wide variety of synthetic and natural peptides, including both single helices and coiled coils, it is shown that [theta lambda i] is also essentially independent of substance and of whether the transition is induced by temperature, ionic strength, pH, chain length changes, amino acid substitution, or solvent perturbation. Averaging [theta lambda i] values culled from various laboratories gives -151 +/- 16 (SD, 7 sources) deg.cm2.mmol-1. In our laboratory, nonpolymerizable rabbit alpha-tropomyosin and two alpha-tropomyosin subsequences yield -135 +/- 10 (SD, 190 values) deg.cm2.mmol-1. Thus, given [theta lambda i] for a peptide of known concentration, it is possible to estimate the concentration of any other peptide provided that it has an isodichroic point at which the ellipticity is accurately measurable. It is then possible to calculate [theta lambda] at any other wavelength for which theta is known. It is advisable to determine [theta lambda i] for the best known peptide in one's own laboratory, since it depends on absolute instrument and cell calibrations and an absolute concentration determination.     

Crystal structure and conformation of polypeptides: L-leucylglycylglycylglycine

Crystals of L-leucylglycylglycylglycine, LGGG (C12H22N4O5), grown from an ethanol-water solution, are orthorhombic, space groups P2(1)2(1)2(1), with unit cell dimensions (at 22 +/- 3 degrees) a = 9.337(1), b = 10.995(1), c = 15.235(1)A, v = 1563.4 A3, Z = 4 with a density of Dobs = 1.29 g.cm-3 and Dcalc = 1.279 g.cm-3. The crystal structure was solved by the application of direct methods and refined to an R value of 0.029 for 1018 reflections with I greater than or equal to 2 sigma. The molecule exists as a zwitterion in the crystal. The trans peptide backbone takes up a folded conformation at the middle glycylglycyl link accompanied by a significant nonplanarity up to delta omega of 8 degrees at the middle peptide and is relatively more extended at the two ends. The molecules are linked together intermolecularly in an infinite sequence of head to tail 1-4' hydrogen bonds, as is typical of charged peptides. It is interesting to note that while glycylglycylglycine takes up an extended beta-sheet conformation, addition of Leu to the N-terminal results in a bent conformation.     

Electronic and vibrational optical activity of several peptides related to neurohypophyseal hormones: disulfide group conformation

Electronic and vibrational optical activity of the set of neurohypophyseal hormones and their analogs was investigated to clarify the S-S bond solution conformation. The selected compounds include oxytocin (I), lysine vasopressin (II), arginine vasopressin (III), and their analogs (IV-IX), differing widely in their pharmacological properties. We have extended the already known electronic circular dichroism data by new information provided by vibrational circular dichroism (VCD) and Raman optical activity (ROA). The use of VCD brought additional details on three-dimensional structure of the chain reversal in the ring moiety and on its left handedness. Furthermore, Raman scattering and ROA allowed us to deduce the sense of the disulfide bond torsion.     

Azobenzene-Containing polypeptides: Photoregulation of conformation in solution

Photochromic polypeptides, with 16 to 56% azobenzene groups in the side chains, have been prepared by reaction of poly(L -glutamic acid) with p-aminozaobenzene, both in the presence of dicyclohexyl carbodiimide/N-hydroxybenzotriazole and of pivaloyl chloride. Analogous modification reactions carried out on poly(L -aspartic acid) were unsuccessful owing to the formation of N-succinimide rings. In trimethylphosphate, all the azopolypeptides exhibit the α-helix CD pattern. Irradiation produces the trans-to-cis isomerization of the azo side chains, but does not induce any variations of the backbone conformation. In water, the CD spectra indicate the presence of appreciable amounts of α helix in 16 and 21% mol azo-containing poly-(L glutamates), while a β structure is present in a 36% mol azopolypeptide. Light produces conformational changes of the polypeptide conformation which are completely reversed in the dark. The extent and kind of photobehavior depend on the azo content and the pH value at which irradiation is carried out. The light-induced effects are discussed on the basis of the pH-induced order-disorder conformational transitions. In fact, the pK values and the transition curves of the dark-adapted samples were found to be different from those of the irradiated ones.     

In vitro folding and oligomerization of a membrane protein. Transition of bacterial porin from random coil to native conformation.

Porin, a channel-forming protein spanning bacterial outer membranes, was denatured in 6 M guanidinium hydrochloride or, alternatively, in sodium dodecyl sulfate at 95 degrees C. Circular dichroism spectra revealed that this protein, which in its native state consist of beta-pleated sheets as the sole detectable secondary structure, is transformed into random coil configuration in the chaotropic agent, or into alpha-helical structure in the detergent. From either state, the mature protein refolds in presence of amphiphilic molecules, attaining full structural and functional competence. As structural criteria, the native trimeric state was assayed by analytical ultracentrifugation, gel electrophoresis in sodium dodecyl sulfate, protease resistance, and circular dichroism spectroscopy. Channel formation in planar lipid bilayers reveals that the refolded protein is also functionally competent. It is concluded that the information required for the complete folding of porin is contained within the primary sequence of the mature polypeptide. The study of rapid refolding clearly reveals that this process occurs in the time range of seconds and that preexisting bilayers are not a prerequisite.