Conformational investigation of alpha,beta-dehydropeptides. XV: N-acetyl-alpha,beta-dehydroamino acid N 'N '-dimethylamides: conformational properties from infrared and theoretical studies.

The FTIR spectra were analysed in the region of the nu(s)(N-H), AI(C=O) and nu(s)(Calpha=Cbeta) bands for a series of Ac-DeltaXaa-NMe2, where DeltaXaa = DeltaAla, (Z)-DeltaAbu, (Z)-DeltaLeu, (Z)-DeltaPhe and DeltaVal, to determine a predominant solution conformation of these alpha,beta-dehydropeptide-related molecules. Measurements were taken in CCl4, DCM and MeCN solutions. In the same way, spectra of saturated analogues Ac-Xaa-NMe2, where Xaa = Ala, Abu, Leu, Phe and Val, were investigated. To help interpret the spectroscopic results, conformational maps were calculated by the B3LYP/6-31+G** method. Also, the relative energies of all conformers of the dehydro compounds in vacuo as well as in the studied solvents in addition to the theoretical IR frequencies of these conformers were calculated. For comparison, molecules of two saturated analogues, Ac-L-Ala-NMe2 and Ac-L-Phe-NMe2, were calculated in a similar way. Both unsaturated and saturated compounds, which have an aliphatic side chain, occur in CCl4 and DCM mainly as a mixture of extended conformers with the C5 H-bond and open conformers. As solvent polarity increases, participation of the open conformers also increases, and in MeCN, the model amides are almost exclusively in the open form, except Ac-DeltaAla-NMe2, which shows a small amount of the H-bonded conformer. Ac-DeltaAla-NMe2 and Ac-DeltaAbu-NMe2 have stronger C5 hydrogen bonds than those of their saturated counterparts. As the calculations indicate, the open conformation of the unsaturated amides is conformer H/F with phi, psi -44 +/- 5 degrees, 127 +/- 4 degrees. This is the second lowest in energy conformer in vacuo and in CCl4 and the lowest one in more polar solvents. The open conformation of Ac-L-Ala-NMe2 constitutes conformer C with phi, psi -101.5 degrees, 112.7 degrees. For Ac-DeltaAla-NMe2 and Ac-DeltaAbu-NMe2, FTIR also reveals the presence of a third conformer. Calculations indicate that is the semiextended conformer D with the N1-H1...N2 hydrogen bond/contact. In all solvents, Ac-L-Phe-NMe2 and Ac-(Z)-DeltaPhe-NMe2 show only the extended E and the open H/F, respectively. In both there is an amide/pi(Ph) interaction.     

Conformational investigation of alpha, beta-dehydropeptides. XI. Molecular and crystal structure of Ac-(Z)-deltaPhe-NMe2 as compared to those of related molecules.

A series of three homologous dimethyldiamides Ac-(Z)-deltaPhe-NMe2, Ac-L-Phe-NMe2 and Ac-DL-Phe-NMe2 have been synthesized and their structures determined from single-crystal X-ray diffraction data. To learn more about the conformational preferences of the compounds studied, the fully relaxed phi, psi conformational energy maps on the free molecules of Ac-deltaAla-NMe2 and Ac-(Z)-deltaPhe-NMe2 were obtained with the HF/3-21G method and the calculated minima re-optimized with the DFT/B3LYP/6-31G** method. The crystal state results have been compared with the literature data. The studied dimethyldiamide Ac-deltaXaa-NMe2 combines the double bond in positions alpha, beta and the C-terminal tertiary amide within one molecule. As the representative probe with deltaXaa = deltaAla, (Z)-deltaLeu and (Z)-deltaPhe shows, in the solid state they adopt the conservative conformation with phi, psi approximately -45 degrees, approximately 130 degrees and with a non-planar tertiary amide bond, whatever the packing forces are. This conformation is located on the Ramachandran map in region H/F, which is of high-energy for common amino acids, but not so readily accessible to them. The free molecule calculations on Ac-deltaAla-NMe2 and Ac-(Z)-deltaPhe-NMe2 reveal that, in spite of dissimilar overall conformational profiles of these molecules, this structure is one of their low-energy conformers and for Ac-(Z)-deltaPhe-NMe2 it constitutes the global minimum. So, the theoretical results corroborate those experimental results proving that this structure is robust enough to avoid conformational distortion due to packing forces. In contrast to Ac-deltaXaa-NMe2, the saturated Ac-L/DL-Xaa-NMe2 shows the constancy of the associative patterns but do not prefer any molecular structure in the solid state.     

Entrapping unusual folding characteristics of the beta-Ala residues in a model peptide: Boc-beta-Ala-Aib-beta-Ala-NHCH3.

Crystal structure analysis of a model peptide: Boc-beta-Ala-Aib-beta-Ala-NHCH3 (beta-Ala: 3-amino propionic acid; Aib: alpha-aminoisobutyric acid) revealed distinct conformational preferences for folded [phi approximately 136 degrees, mu approximately -62 degrees, psi approximately 100 degrees] and semifolded [phi approximately 83 degrees, mu approximately -177 degrees, psi approximately -117 degrees] structures of the N-and C-terminus beta-Ala residues, respectively. The overall folded conformation is stabilized by unusual Ni...H-Ni+1 and nonconventional C-H...O intramolecular hydrogen bonding interactions.     

Characterization of the pressure-induced intermediate and unfolded state of red-shifted green fluorescent protein--a static and kinetic FTIR,UV/VIS and fluorescence spectroscopy study

The green fluorescence proteins (GFP) are widely used as reporters in molecular and cell biology. For their use it in high-pressure microbiology and biotechnology studies, their structural properties, thermodynamic parameters and stability diagrams have to be known. We investigated the pressure stability of the red-shifted green fluorescent protein (rsGFP) using Fourier-transform infrared spectroscopy, fluorescence and UV/Vis spectroscopy. We found that rsGFP does not unfold up to approximately 9kbar at room temperature. Its unique three-dimensional structure is held responsible for the high-pressure stability. At higher temperatures, its secondary structure collapses below 9kbar (e.g. the denaturation pressure at 58 degrees C is 7.8kbar). The analysis of the IR data shows that the pressure-denatured state contains more disordered structures at the expense of a decrease of intramolecular beta-sheets. As indicated by the large volume change of DeltaV degrees (u) approximately -250(+/-50)mlmol(-1) at 58 degrees C, this highly cooperative transition can be interpreted as a collapse of the beta-can structure of rsGFP. For comparison, the temperature-induced unfolding of rsGFP has also been studied. At high temperature (T(m)=78 degrees C), the unfolding resulted in the formation of an aggregated state. Contrary to the pressure-induced unfolding, the temperature-induced unfolding and aggregation of GFP is irreversible. From the FT-IR data, a tentative p,T-stability diagram for the secondary structure collapse of GFP has been obtained. Furthermore, changes in fluorescence and absorptivity were found which are not correlated to the secondary structural changes. The fluorescence and UV/Vis data indicate smaller conformational changes in the chromophore region at much lower pressures ( approximately 4kbar) which are probably accompanied by the penetration of water into the beta-can structure. In order to investigate also the kinetics of this initial step, pressure-jump relaxation experiments were carried out. The partial activation volumes observed indicate that the conformational changes in the chromophore region when passing the transition state are indeed rather small, thus leading to a comparably small volume change of -20 ml mol(-1) only. The use of the chromophore absorption and fluorescence band of rsGFP in using GFP as reporter for gene expression and other microbiological studies under high pressure conditions is thus limited to pressures of about 4kbar, which still exceeds the pressure range relevant for studies in vivo in micro-organisms, including piezophilic bacteria from deep-sea environments.     

Geometrical and conformational preferences of the 9-fluorenylmethoxycarbonyl-amino moiety.

Structural parameters, originating from x-ray crystallographic data, have been compiled for 13 derivatives of amino acids, peptides and related compounds, which contain a total of 14 Fmoc-NH- moieties. For these moieties, molecular geometries and conformations--described by the omegao, theta1, theta2 and theta3' torsion angles--were analysed and compared with the corresponding parameters for the Z-NH- and Boc-NH-moieties (290 and 553, respectively). To gain a deeper insight into the conformational features of the Fmoc-NH- moiety, ab initio free molecule calculations were performed for fully relaxed minima. Also the potential energy surface as a function of the torsion angles (theta3', theta2) was generated. The conformational features of the Fmoc-NH- moiety: (i) two possible values for the angle omegao (approximately 180 degrees or, rarely, approximately theta degrees) and (ii) the angle theta1 = 180 degrees +/- 15 degrees, are common to the Z-NH- and Boc-NH- systems. By contrast, the theta2 and theta3 angles in the Fmoc, Z and Boc groups differ essentially. In the Fmoc groups theta2 mostly has values of 180 degrees +/- 30 degrees and values up [115 degrees] seem to be forbidden, whereas fewer than half of the Z groups adopt theta2 approximately 180 degrees and the remainder have theta2 in the range of [90 degrees +/- 20 degrees]. On the other hand, the Boc methyl groups are staggered. The theta3 values observed for Fmoc are limited to the regions of 180 degrees +/- 20 degrees and 160 degrees +/- 20 degrees], while for the Z group a variety of theta3 occurs. The orientation of the fluorenyl vs the urethane function is mostly trans. Our results suggest a lower conformational flexibility for the Fmoc group compared with that of the Z group. Our calculations confirm that the observed conformational features for the Fmoc-NH- moiety are inherent properties. The Fmoc-NH-moiety in crystals involves the participation of its O=C-NH functionality in hydrogen bonds.     

Design of peptides with branched beta-carbon dehydro-residues: syntheses, crystal structures and molecular conformations of two peptides, (I) N-Carbobenzoxy-DeltaVal-Ala-Leu-OCH3 and (II) N-Carbobenzoxy-DeltaIle-Ala-Leu-OCH3.

Highly specific structures can be designed by inserting dehydro-residues into peptide sequences. The conformational preferences of branched beta-carbon residues are known to be different from other residues. As an implication it was expected that the branched beta-carbon dehydro-residues would also induce different conformations when substituted in peptides. So far, the design of peptides with branched beta-carbon dehydro-residues at (i + 1) position has not been reported. It may be recalled that the nonbranched beta-carbon residues induced beta-turn II conformation when placed at (i + 2) position while branched beta-carbon residues induced beta-turn III conformation. However, the conformation of a peptide with a nonbranched beta-carbon residue when placed at (i + 1) position was not found to be unique as it depended on the stereochemical nature of its neighbouring residues. Therefore, in order to induce predictably unique structures with dehydro-residues at (i + 1) position, we have introduced branched beta-carbon dehydro-residues instead of nonbranched beta-carbon residues and synthesized two peptides: (I) N-Carbobenzoxy-DeltaVal-Ala-Leu-OCH3 and (II) N-Carbobenzoxy-DeltaIle-Ala-Leu-OCH3 with DeltaVal and DeltaIle, respectively. The crystal structures of peptides (I) and (II) have been determined and refined to R-factors of 0.065 and 0.063, respectively. The structures of both peptides were essentially similar. Both peptides adopted type II beta-turn conformations with torsion angles; (I): phi1 = -38.7 (4) degrees, psi1 = 126.0 (3) degrees; phi2 = 91.6 (3) degrees, psi2 = -9.5 (4) degrees and (II): phi1 = -37.0 (6) degrees, psi1 = 123.6 (4) degrees, phi2 = 93.4 (4), psi2 = -11.0(4) degrees respectively. Both peptide structures were stabilized by intramolecular 4-->1 hydrogen bonds. The molecular packing in both crystal structures were stabilized in each by two identical hydrogen bonds N1...O1' (-x, y + 1/2, -z) and N2...O2' (-x + 1, y + 1/2, -z) and van der Waals interactions.     

Temperature and pressure effects on structural and conformational properties of POPC/SM/cholesterol model raft mixtures--a FT-IR, SAXS, DSC, PPC and Laurdan fluorescence spectroscopy study

We report on the effects of temperature and pressure on the structure, conformation and phase behavior of aqueous dispersions of the model lipid "raft" mixture palmitoyloleoylphosphatidylcholine (POPC)/bovine brain sphingomyelin (SM)/cholesterol (Chol) (1:1:1). We investigated interchain interactions, hydrogen bonding, conformational and structural properties as well as phase transformations of this system using Fourier transform-infrared (FT-IR) spectroscopy, small-angle X-ray scattering (SAXS), differential scanning calorimetry (DSC) coupled with pressure perturbation calorimetry (PPC), and Laurdan fluorescence spectroscopy. The IR spectral parameters in combination with the scattering patterns from the SAXS measurements were used to detect structural and conformational transformations upon changes of pressure up to 7-9 kbar and temperature in the range from 1 to about 80 degrees C. The generalized polarization function (GP) values, obtained from the Laurdan fluorescence spectroscopy studies also reveal temperature and pressure dependent phase changes. DSC and PPC were used to detect thermodynamic properties accompanying the temperature-dependent phase changes. In combination with literature fluorescence spectroscopy and microscopy data, a tentative p,T stability diagram of the mixture has been established. The data reveal a broad liquid-order/solid-ordered (lo+so) two-phase coexistence region below 8+/-2 degrees C at ambient pressure. With increasing temperature, a lo+ld+so three-phase region is formed, which extends up to approximately 27 degrees C, where a liquid-ordered/liquid-disordered (lo+ld) immiscibility region is formed. Finally, above 48+/-2 degrees C, the POPC/SM/Chol (1:1:1) mixture becomes completely fluid-like (liquid-disordered, ld). With increasing pressure, all phase transition lines shift to higher temperatures. Notably, the lo+ld (+so) phase coexistence region, mimicking raft-like lateral phase separation in natural membranes, extends over a rather wide temperature range of about 40 degrees C, and a pressure range, which extends up to about 2 kbar for T=37 degrees C. Interestingly, in this pressure range, ceasing of membrane protein function in natural membrane environments has been observed for a variety of systems.     

Conformations of beta-amino acid residues in peptides: X-ray diffraction studies of peptides containing the achiral residue 1-aminocyclohexaneacetic acid, beta3,3Ac6c

The conformational preferences of the 3,3-disubstituted beta-amino acid residue, 1-aminocyclohexaneacetic acid (beta3,3Ac6c) have been investigated by determining the crystal structures of the parent amino acid, the hydrochloride derivative, 10 protected derivatives and di and tripeptides. The symmetrical cyclohexyl substituent at the beta-position restricts the values of the torsion angles phi (N--C(beta)) and theta (C(beta)--C(alpha)) to approximately gauche values (+/-60 degrees ). Relatively few intramolecularly hydrogen bonded conformations are observed. In the dipeptide Boc-beta(3,3)Ac6c-beta(3,3)Ac6c-NHMe a C6 hydrogen bond is observed. In Piv-Pro-beta(3,3)Ac6c-NHMe a C11 hydrogen bonded hybrid alphabeta turn is characterized. In a majority of cases the amino group occupies the axial position in the cyclohexane ring. The conformations observed are compared with crystallographically observed structures for other beta-residues, including beta(2,2)Ac6c.     

The twists and turns of beta-peptides.

Recently, it has been discovered that peptides composed of beta-amino acids are capable of adopting novel secondary structures demonstrating that peptides composed of alpha-amino acids are not unique in their ability to fold into well-defined structures. Cyclic as well as acyclic peptides composed of beta-amino acid residues adopt turn, helical, and sheet-like conformations. Here, we discuss the synthesis and conformational preferences of individual, substituted beta-amino acids as well as the structures that peptides composed of these residues, beta-peptides, may adopt.     

Side-chain conformations in an unfolded protein: chi1 distributions in denatured hen lysozyme determined by heteronuclear 13C, 15N NMR spectroscopy.

Using a 13C and 15N-labelled sample, multi-dimensional heteronuclear NMR techniques have been carried out to characterise hen lysozyme denatured in 8 M urea at pH 2.0. The measurement of 3J(C',Cgamma) and 3J(N,Cgamma) coupling constants has enabled side-chain chi1 torsion angle populations to be probed in the denatured polypeptide chain. Analysis of the coupling constant data has allowed the relative populations of the three staggered rotamers about chi1 to be defined for 51 residues. The amino acids can broadly be divided into five classes that show differing side-chain conformational preferences in the denatured state. These range from a strong preference for the -60 degrees chi1 rotamer for methionine and leucine (74-79 % population) to a favouring of the +60 degrees chi1 rotamer for threonine (67 % population). The differences in behaviour reflect the steric and electrostatic characteristics of the side-chains concerned. A close agreement is seen between the chi1 populations calculated from the experimental coupling constant data and predictions from the statistical model for a random coil that uses the chi1 torsion angle distributions in a data base of native protein structures. Short-range interactions therefore dominate in determining the local conformational properties of side-chains in a denatured protein. Deviations are, however, observed for many of the aromatic residues involved in hydrophobic clusters within the denatured protein. For these residues the effects of additional non-local interactions in the clusters presumably play a major role in determining the chi1 preferences.     

Reduced temperature dependence of collective conformational opening in a hyperthermophile rubredoxin.

Spatially localized differences in the conformational dynamics of the rubredoxins from the hyperthermophile Pyrococcus furiosus (Pf) and the mesophile Clostridium pasteurianum (Cp) are monitored via amide exchange measurements. As shown previously for the hyperthermophile protein, nearly all backbone amides of the Cp rubredoxin exhibit EX(2) hydrogen exchange kinetics with conformational opening rates of >1 s(-)(1). Significantly slower amide exchange is observed for Pf rubredoxin in the region surrounding the metal site and the proximal end of the three-stranded beta-sheet, while for the rest of the structure, the exchange rates at 23 degrees C are similar for both proteins. For the multiple-turn region comprising residues 14-32 in both rubredoxins, the uniformity of both the exchange rate constants and the values of the activation energy at the slowly exchanging sites is consistent with a model of solvent exposure via a subglobal cooperative conformational opening. In contrast to the common expectation of increased rigidity in the hyperthermophile proteins, below room temperature Pf rubredoxin exhibits a larger apparent flexibility in this multiple-turn region. The smaller enthalpy for the conformational opening process of this region in Pf rubredoxin reflects the much weaker temperature dependence of the underlying conformational equilibrium in the hyperthermophile protein.     

Conformational and dynamic differences between N. meningitidis serogroup B and C polysaccharides, using n.m.r. spectroscopy and molecular mechanics calculations

1H-N.m.r. spectroscopy has been used to determine the conformation in aqueous solution of the sialic acid residues of the N. meningitidis serogroup B and non-O-acetylated (O-Ac-)-C polysaccharides, and of N-acetylneuraminic acid (NeuNAc). In all cases, the sugar adopts the 2C5 conformation. The side-chain of NeuNAc adopts a conformation such that H-7 and H-8 are approximately anti-periplanar. This conformation is also found in the (O-Ac-)-C polysaccharide, whereas H-7 and H-8 are gauche in the B polysaccharide. Molecular mechanics calculations have been used to probe the conformational preferences of the variously linked sialic acid residues, and the results are in general agreement with those based on the 1H-n.m.r. data. The 13C-n.m.r. spin-lattice relaxation-times have been interpreted in terms of the molecular dynamics of the B and (O-Ac-)-C polysaccharides. Molecular correlation times have been calculated and details of internal rotational or segmental motion elucidated. The C polysaccharide is characterised by internal or segmental motion in the C-7 to C-9 side-chain of the sialic acid repeating-unit, whereas the B polysaccharide has little or no such movement and tumbles in solution as a rigid species with internal rotation of only the pendant C-9 group. The conformational differences suggest a substantially different three-dimensional structure in solution for these polysaccharides.     

New type of helix and 2(7) ribbon structure formation in poly DeltaLeu peptides: construction of a single-handed template

alpha,beta-Dehydroamino acid residues due to the presence of Calpha = Cbeta double bond influences the main chain and the side chain conformations. These residues have interesting chemical features including the increased resistance to enzymatic degradation. The chain length dependent conformational behavior of poly alpha,beta-dehydroleucine (DeltaLeu) peptides in both the pure forms Z and E and their various combinations like alternate ZE/EZ etc. have been investigated by using quantum mechanical method PCILO (perturbative configuration interaction of localized orbitals). The conformational states in alternate Z and E forms, with Phi, Psi values of -10 degrees , 105 degrees /1 degrees , -88 degrees for Z form and 35 degrees , 22 degrees /-34 degrees , -27 degrees for the E form are found to be the most stable and degenerate than the states in pure Z and E forms and the EZ form etc. The repeated Phi, Psi values give rise to altogether new types of left and right handed helices, and their stability increases with increasing chain length. These structures are stabilized by intramolecular hydrogen bonding, carbonyl-carbonyl interactions and hydrophobic interactions between the side chains of DeltaZLeu and DeltaELeu residues. The 2(7) ribbon structure (seven-membered hydrogen-bonded ring involving two consecutive amino acid residues) is found to be most stable and degenerate in the pentapeptide Ac-DeltaELeu5-NHMe, due to the formation of maximum hydrogen bonds. A right-handed template from achiral DeltaLeu peptides has been achieved by incorporating L-Leu at the C-terminal or D-Leu at the N-terminal.     

Conformational comparison of mu-selective endomorphin-2 with its C-terminal free acid in DMSO solution, by 1H NMR spectroscopy and molecular modeling calculation.

In order to make clear the structural role of the C-terminal amide group of endomorphin-2 (EM2, H-Tyr-Pro-Phe-Phe-NH2), an endogenous mu-receptor ligand, in the biological function, the solution conformations of endomorphin-2 and its C-terminal free acid (EM2OH, H-Tyr-Pro-Phe-Phe-OH), studied using two-dimensional 1H NMR measurements and molecular modeling calculations, were compared. Both peptides were in equilibrium between the cis and trans isomers around the Tyr-Pro omega bond in a population ratio of approximately/= 1:2. The lack of significant temperature and concentration dependence of NH protons suggested that the NMR spectra reflected the conformational features of the respective molecules themselves. Fifty possible 3D structures for the each isomer were generated by the dynamical simulated annealing method under the proton-proton distance constraints derived from the ROE cross-peaks. These energy-minimized conformers, which were all in the phi torsion angles estimated from J(NHCalphaH) coupling constants within +/- 30 degrees, were then classified in groups one or two according to the folding backbone structures. All trans and cis EM2 conformers adopt an open conformation in which their extended backbone structures are twisted at the Pro2-Phe3 moiety. In contrast, the trans and cis conformers of EM2OH show conformational variation between the 'bow'-shaped extended and folded backbone structures, although the cis conformers of its zwitterionic form are refined into the folded structure of the close disposition of C- and N-terminal groups. These results indicate clearly that the substitution of carboxyl group for C-terminal amide group makes the peptide flexible. The conformational requirement for mu-receptor activation has been discussed based on the active form proposed for endomorphin-1 and by comparing conformational features of EM2 and EM2OH.     

Probing the conformational heterogeneity of the acetylaminofluorene-modified 2'-deoxyguanosine and DNA by 19F NMR spectroscopy.

19F NMR spectroscopy was used to probe the conformation of a DNA adduct derived from the carcinogen 7-fluoro-N-acetyl-2-aminofluorene (FAAF) in three structural contexts: as a monomer and incorporated into single- and double-stranded DNA. The 19F NMR spectrum of dG-C8-FAAF [N-(deoxyguanosin-8-yl)-N-acetyl-7-fluoro-2-aminofluorene] in methanol at -30 degrees C exhibited four interconvertible signals in a 11:52:26:11 ratio. Dynamic NMR analysis indicated that the four torsional isomers arise from restricted rotation about the amide (gamma) (14.4 kcal/mol) and the guanyl-nitrogen (alpha) bonds. The conformational heterogeneity persisted in a single strand FAAF-12-mer, d(CTTCTTG[FAAF]ACCTC), whose 19F NMR spectrum at 22 degrees C and pH 7.0 gave only two signals in a 40:60 ratio, instead of four. The two 19F signals followed a two-site exchange with the rotation barrier of 14.7 kcal/mol about the amide (gamma') bond. A similar conformational theme was observed in the FAAF-12-mer duplex, d(CTTCTTG[FAAF]ACCTC).d(GAGGTCAAGAAG), which revealed two 19F resonances in a 41:59 ratio at 22 degrees C and pH 7.0. According to solvent-induced isotope and magnetic anisotropy effects, the two duplex conformers adopt exclusively a base displacement structure, being different only in their relative acetyl group orientations, cis (gamma' approximately 180 degrees) or trans (gamma' approximately 0 degrees ). Dynamic NMR data indicated that the two conformers do not exchange over a wide range of temperatures. This contrasts with the nonacetylated counterpart, which exhibits an equilibrium between the "B-type" and "stacked" conformers [Zhou, L., et al. (1997) J. Am. Chem. Soc. 119, 5384-5389]. The exclusive stacked nature of the AAF adducts may provide insight into why AAF adducts are more mutagenic and prone to repair than the nonacetylated AF adducts.     

Structural flexibility of canonical 2'-deoxyribonucleotides in DNA-like conformations

Quantitative characteristics of structural flexibility of the DNA elementary monomer units -5'-deoxycytidylic, 5'-thymidylic, 5'-deoxyadenylic and 5'-deoxyguanylic acid molecules--have been calculated with original methods. Root-mean-square deviations from equilibrium for all conformational parameters, caused by nuclei thermal or quantum zero-point vibrations, have been found to lie within 4 degrees divided by 25 degrees at 0 K and 7 degrees divided by 50 degrees at 298 K and corresponding relaxed force constants--within 1 divided by 35 kcal/mol x rad(-2). Their values have been found to be sensitive to the molecule's conformation. It has been proven, that the torsion angle gamma is the most rigid one whereas relaxed force constants for all other conformational variables are lower and comparable to each other. The data obtained could serve for development of structural-dynamical models of the DNA.     

On the structural significance of the linkage region constituents of N-glycoproteins: an X-ray crystallographic investigation using models and analogs

The linkage region constituents, namely, 2-acetamido-2-deoxy-beta-D-glucopyranose and asparagine are conserved in the N-glycoproteins of all the eukaryotes. The present work is aimed at understanding the reasons for the occurrence of GlcNAc and Asn as the linkage region constituents. A total of six sugar amides have been designed as models and analogs of the linkage region and their crystal structures have been solved. This is the first report on the X-ray crystallographic investigation of the effect of systematic changes in the linkage sugar as well as its aglycon moiety on the N-glycosidic torsion, psi(N) (O5-C1-N1-C1(')). This also forms the first report on the crystal structure of a model of L-RhabetaAsn, a variant linkage found in the surface layer glycoprotein of Bacillus stearothermophillus. Among the models and analogs examined, the acetamido derivatives of Man and Xyl, the linkage sugars of O-glycoproteins, show a psi(N) value of -114.5 degrees and -121.2 degrees, respectively, deviating maximum from the value of -89.8 degrees reported for the model compound GlcNAcbetaNHAc. The L-Rha and Gal derivatives also show noticeable deviations. The psi(N) values, -89.5 degrees and -91.0 degrees, of the propionamide derivatives of Glc and GlcNAc (analogs of GlcbetaGln and GlcNAcbetaGln, respectively) agree well with those (-93.8 degrees and -89.8 degrees ) reported for their corresponding acetamide derivatives suggesting Gln could serve as well as Asn as the linkage region amino acid. However, the rotational freedom about the additional C-C bond would lead to altered rigidity of the linkage region. An analysis of packing reveals that the molecular assembly of these compounds is driven by different infinite and finite chains of hydrogen bonds. The double pillaring of hydrogen bonds involving the amide groups at C1 and C2 is seen as a unique packing feature characteristic of beta-1-N-acyl derivatives of GlcNAc. Based on the findings of the present study, it is speculated that the linkage region constituents of the eukaryotic N-glycoproteins appear to fulfill three essential structural requirements: rigidity, planarity, and linearity and these are met by the trisaccharide core and Asn at the linkage region.     

Conformational properties of N-acetyl-N-methyl-alpha,beta-dehydroalanine N'-methylamide

The conformational properties of Ac-Delta(Me)Ala-NHMe (N-acetyl-N-methyl-alpha,beta-dehydroalanine N'-methylamide), as the simplest model of N-methyl-alpha,beta-dehydroamino acids, was examined with theoretical methods and in comparison with Ac-DeltaAla-NHMe and Ac-DeltaAla-NMe(2). The N-terminal amide of the Delta(Me)Ala residue easily adopts the configuration cis and the torsion angles phi, psi are highly flexible. The Delta(Me)Ala residue is a conformational flexibilizer as compared to the parent DeltaAla, which is a conformational stiffener. This seems to be the reason why Delta(Me)Ala is found in small natural cyclic peptides, where it ensures the conformational flexibility necessary for biological action.     

Conformational stability and activity of ribonuclease T1 with zero, one, and two intact disulfide bonds

Ribonuclease T1 has two disulfide bonds linking cysteine residues 2-10 and 6-103. We have prepared a derivative of ribonuclease T1 in which one disulfide bond is broken and the cysteine residues carboxymethylated, (2-10)-RCM-T1, and three derivatives in which both disulfides are broken and the cysteine residues reduced, R-T1, carboxamidomethylated, RCAM-T1, or carboxymethylated, RCM-T1. The RNA hydrolyzing activity of these proteins has been measured, and urea and thermal denaturation studies have been used to determine conformational stability. The activity, melting temperature, and conformational stability of the proteins are: ribonuclease T1 (100%, 59.3 degrees C, 10.2 kcal/mol), (2-10)-RCM-T1 (86%, 53.3 degrees C, 6.8 kcal/mol), R-T1 (53%, 27.2 degrees C, 3.0 kcal/mol), RCAM-T1 (43%, 21.2 degrees C, 1.5 kcal/mol), and RCM-T1 (35%, 16.6 degrees C, 0.9 kcal/mol). Thus, the conformational stability is decreased by 3.4 kcal/mol when one disulfide bond is broken and by 7.2-9.3 kcal/mol when both disulfide bonds are broken. It is quite remarkable that RNase T1 can fold and function with both disulfide bonds broken and the cysteine residues carboxymethylated. The large decrease in the stability is due mainly to an increase in the conformational entropy of the unfolded protein which results when the constraints of the disulfide bonds on the flexibility are removed. We propose a new equation for predicting the effect of a cross-link on the conformational entropy of a protein: delta Sconf = -2.1 - (3/2)R 1n n, where n is the number of residues between the side chains which are cross-linked. This equation gives much better agreement with experimental results than other forms of this equation which have been used previously.     

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.