Calibration of the angular dependence of the amide proton-C alpha proton coupling constants, 3JHN alpha, in a globular protein. Use of 3JHN alpha for identification of helical secondary structure

The vicinal amide proton-C alpha proton spin-spin coupling constants, JHN alpha, in the globular protein basic pancreatic trypsin inhibitor (BPTI) have been measured using phase-sensitive correlated spectroscopy at high digital resolution. In conjunction with the crystal structure of BPTI, these data were used to calibrate the correlation between 3JHN alpha and the dihedral angle phi. The resulting "BPTI curve" is 3JHN alpha = 6.4 cos2 theta - 1.4 cos theta + 1.9 (theta = [phi - 60 degrees]). It is further shown that measurement of the spin-spin couplings 3JHN alpha presents an independent, reliable method for identification of the location of helical structure in the amino acid sequence of proteins.     

Human whole-blood O2 affinity: effect of CO2

The proton Bohr factor (phi H = alpha log PO2/alpha pH), the carbamate Bohr factor (phi C = alpha log PO2/alpha log PCO2), the total Bohr factor (phi HC = d log PO2/dpH[base excess) and the CO2 buffer factor (d log PCO2/dpH) were determined in the blood of 12 healthy donors over the whole O2 saturation (SO2) range. All three Bohr factors proved to be dependent on SO2, although to a lesser extent than reported in some of the recent literature. At SO2 = 50% and 37 degrees C, we found phi H = -0.428 +/- 0.010 (SE), phi C = 0.054 +/- 0.006, and phi HC = -0.488 +/- 0.007. The values obtained for phi H, phi C, and d log PCO2/dpH were used to calculate phi HC. Calculated and measured values of phi HC proved to be in good agreement. In an additional series of 12 specimens of human blood we determined the influence of PCO2 on phi H and the influence of pH on phi C. At SO2 = 50%, phi H varied from -0.49 +/- 0.009 at PCO2 = 15 Torr to -0.31 +/- 0.010 at PCO2 = 105 Torr and phi C from 0.157 +/- 0.015 at pH = 7.80 to 0.006 +/- 0.009 at pH = 7.00. When on the basis of these data a second-order term is taken into account, a still slightly better agreement between measured and calculated values of phi HC can be attained.     

Empirical torsional potential functions from protein structure data. Phi- and psi-potentials for non-glycyl amino acid residues.

The torsional potential functions Vt(phi) and Vt(psi) around single bonds N--C alpha and C alpha--C, which can be used in conformational studies of oligopeptides, polypeptides and proteins, have been derived, using crystal structure data of 22 globular proteins, fitting the observed distribution in the (phi, psi)-plane with the value of Vtot(phi, psi), using the Boltzmann distribution. The averaged torsional potential functions, obtained from various amino acid residues in L-configuration, are Vt(phi) = 1.0 cos (phi + 60 degrees); Vt(psi) = 0.5 cos (psi + 60 degrees) - 1.0 cos (2 psi + 30 degrees) - 0.5 cos (3 psi + 30 degrees). The dipeptide energy maps Vtot(phi, psi) obtained using these functions, instead of the normally accepted torsional functions, were found to explain various observations, such as the absence of the left-handed alpha helix and the C7 conformation, and the relatively high density of points near the line psi = 0 degrees. These functions derived from observational data on protein structures, will, it is hoped, explain various previously unexplained facts in polypeptide conformation.     

Empirical isotropic chemical shift surfaces

A list of proteins is given for which spatial structures, with a resolution better than 2.5 A, are known from entries in the Protein Data Bank (PDB) and isotropic chemical shift (ICS) values are known from the RefDB database related to the Biological Magnetic Resonance Bank (BMRB) database. The structures chosen provide, with unknown uncertainties, dihedral angles phi and psi characterizing the backbone structure of the residues. The joint use of experimental ICSs of the same residues within the proteins, again with mostly unknown uncertainties, and ab initio ICS(phi,psi) surfaces obtained for the model peptides For-(L-Ala)(n)-NH(2), with n = 1, 3, and 5, resulted in so-called empirical ICS(phi,psi) surfaces for all major nuclei of the 20 naturally occurring alpha-amino acids. Out of the many empirical surfaces determined, it is the 13C(alpha)-1H(alpha) ICS(phi,psi) surface which seems to be most promising for identifying major secondary structure types, alpha-helix, beta-strand, left-handed helix (alpha(D)), and polyproline-II. Detailed tests suggest that Ala is a good model for many naturally occurring alpha-amino acids. Two-dimensional empirical 13C(alpha)-1H(alpha) ICS(phi,psi) correlation plots, obtained so far only from computations on small peptide models, suggest the utility of the experimental information contained therein and thus they should provide useful constraints for structure determinations of proteins.     

Independence of genetic geographical variation between photoperiodic diapause, circadian eclosion rhythm, and Thr-Gly repeat region of the period gene in Drosophila littoralis

Drosophila littoralis is a latitudinally widespread European species of the Drosophila virilis group. The species has ample genetic variation in photoperiodism (adult diapause) and circadian rhythmicity (pupal eclosion rhythm), with adaptive latitudinal clines in both of them. The possible common genetic basis between the variability of photoperiodism and circadian rhythms was studied by a long-term crossing experiment. A northern strain (65 degrees N) having long critical day length (CDL = 19.9 h) for diapause, early phase of the entrained rhythm in LD 3:21 (psi(LD3:21) = 12.3 h), and short period (tau= 18.8 h) of the free-running rhythm for the eclosion rhythm was crossed with a southern strain (42 degrees N) having short CDL (12.4 h), late eclosion phase (psi(LD3:21) = 20.2 h), and long period (tau= 22.8 h). After 54 generations, including free recombination, artificial selection, and genetic drift, a novel strain resulted, having even more "southern" diapause and more "northern" eclosion rhythm characteristics than found in any of the geographical strains. The observed complete separation of eclosion rhythm characteristics from photoperiodism is a new finding in D. littoralis; in earlier studies followed for 16 generations, the changes had been mostly parallel. Evidently, the genes controlling the variability of the eclosion rhythm and photoperiodism in D. littoralis are different but closely linked. To test for the possible gene loci underlying the observed geographical variability, the period gene was studied in 10 strains covering all the known clock variability in D. littoralis. The authors sequenced the most suspected Thr-Gly region, which is known to take part in the adaptive clock variability in Drosophila melanogaster. No coding differences were found in the strains, showing that this region is not included in the adaptive clock variability in D. littoralis.     

Endogenous timing mechanism controlling the circannual pupation rhythm of the varied carpet beetle Anthrenus verbasci

This paper describes the detailed characteristics of the circannual pupation rhythm in Anthrenus verbasci determined by laboratory experiments under various photoperiods and temperatures. The frequency distribution of larval duration showed a periodic pattern over 2-3 years and the period was 37-40 weeks under a constant short-day photoperiod (light:dark 12:12) at 20 degrees C. This rhythm showed temperature compensation to some extent under a short-day photoperiod between 17.5 degrees C and 27.5 degrees C. Under alternations of a long-day (light:dark 16:8) and a short-day photoperiod, pupation occurred 21-24.5 weeks after transfer from a long-day to a short-day photoperiod. Therefore, we concluded that the timing of pupation in A. verbasci is controlled by a circannual rhythm and its zeitgeber is a change in photoperiod. Furthermore, when larvae were transferred from a long-day to a short-day photoperiod at various ages, the larval duration after the photoperiodic transfer depended on the time of the transfer. This difference can be explained by phase-dependent phase shifts in the circannual rhythm.     

Crystal structure and conformation of 5-fluorouridine: conformational preferences for 5-fluorinated pyranosides

Crystals of 5-fluorouridine (5FUrd) have unit cell dimensions a = 7.716(1), b = 5.861(2), c = 13.041(1)A, alpha = gamma = 90 degrees, beta = 96.70 degrees (1), space group P2(1), Z = 2, rho obs = 1.56 gm/c.c and rho calc = 1574 gm/c.c The crystal structure was determined with diffractometric data and refined to a final reliability index of 0.042 for the observed 2205 reflections (I > or = 3sigma). The nucleoside has the anti conformation [chi = 53.1(4) degrees] with the furanose ring in the favorite C2'-endo conformation. The conformation across the sugar exocyclic bond is g+, with values of 49.1(4) and -69.3(4) degrees for phi(theta c) and phi (infinity) respectively. The pseudorotational amplitude tau(m) is 34.5 (2) with a phase angle of 171.6(4) degrees. The crystal structure is stabilized by a network of N-H...O and O-H...O involving the N3 of the uracil base and the sugar 03' and 02' as donors and the 02 and 04 of the uracil base and 03' oxygen as acceptors respectively. Fluorine is neither involved in the hydrogen bonding nor in the stacking interactions. Our studies of several 5-fluorinated nucleosides show the following preferred conformational features: 1) the most favored anti conformation for the nucleoside [chi varies from -20 to + 60 degrees] 2) an inverse correlation between the glycosyl bond distance and the chi angle 3) a wide variation of conformations of the sugar ranging froni C2'-endo through C3'-endo to C4'-exo 4) the preferred g+ across the exocyclic C4'-C5' bond and 5) no role for the fluorine atom in the hydrogen bonding or base stacking interactions.     

Synthesis, crystal structure, and molecular conformation of N-Boc-L-Phe-dehydro-Leu-L-Val-OCH3

The peptide N-Boc-L-Phe-dehydro-Leu-L-Val-OCH3 was synthesized by the usual workup procedure and finally by coupling the N-Boc-L-Phe-dehydro-Leu-OH to valine methyl ester. It was crystallized from its solution in methanol-water mixture at 4 degrees C. The crystals belong to the triclinic space group P1 with a = 5.972(5) A, b = 9.455(6) A, c = 13.101(6) A, alpha = 103.00(4) degrees, beta = 97.14(5) degrees, gamma = 102.86(5) degrees, V = 690.8(8) A, Z = 1, dm = 1.179(5) Mg m-3 and dc = 1.177(5) Mg m-3. The structure was determined by direct methods using SHELXS86. It was refined by block-diagonal least-squares procedure to an R value of 0.060 for 1674 observed reflections. The C alpha 2-C beta 2 distance of 1.323(9) A in dehydro-Leu is an appropriate double bond length. The bond angle C alpha-C beta-C gamma in the dehydro-Leu residue is 129.4(8) degrees. The peptide backbone torsion angles are theta 1 = -168.6(6) degrees, omega 0 = 170.0(6) degrees, phi 1 = -44.5(9) degrees, psi 1 = 134.5(6) degrees, omega 1 = 177.3(6) degrees, phi 2 = 54.5(9) degrees, psi 2 = 31.1(10) degrees, omega 2 = 171.7(6) degrees, phi 3 = 51.9(8) degrees, psi T3 = 139.0(6) degrees, theta T = -175.7(6) degrees. These values show that the backbone adopts a beta-turn II conformation. As a result of beta-turn, an intramolecular hydrogen bond is formed between the oxygen of the ith residue and NH of the (i + 3)th residue at a distance of 3.134(6) A.(ABSTRACT TRUNCATED AT 250 WORDS)     

Role of azaamino acid residue in beta-turn formation and stability in designed peptide.

The structural perturbation induced by C(alpha)-->N(alpha) exchange in azaamino acid-containing peptides was predicted by ab initio calculation of the 6-31G* and 3-21G* levels. The global energy-minimum conformations for model compounds, For-azaXaa-NH2 (Xaa=Gly, Ala, Leu) appeared to be the beta-turn motif with a dihedral angle of phi= +/- 90 degrees, psi=0 degrees. This suggests that incorporation of the azaXaa residue into the i+2 position of designed peptides could stabilize the beta-turn structure. The model azaLeu-containing peptide, Boc-Phe-azaLeu-Ala-OMe, which is predicted to adopt a beta-turn conformation was designed and synthesized in order to experimentally elucidate the role of the azaamino acid residue. Its structural preference in organic solvents was investigated using 1H NMR, molecular modelling and IR spectroscopy. The temperature coefficients of amide protons, the characteristic NOE patterns, the restrained molecular dynamics simulation and IR spectroscopy defined the dihedral angles [ (phi i+1, psi i+1) (phi i+2, psi i+2)] of the Phe-azaLeu fragment in the model peptide, Boc-Phe-azaLeu-Ala-OMe, as [(-59 degrees, 127 degrees) (107 degrees, -4 degrees)]. This solution conformation supports a betaII-turn structural preference in azaLeu-containing peptides as predicted by the quantum chemical calculation. Therefore, intercalation of the azaamino acid residue into the i+2 position in synthetic peptides is expected to provide a stable beta-turn formation, and this could be utilized in the design of new peptidomimetics adopting a beta-turn scaffold.     

Conformational investigation of alpha,beta-dehydropeptides. XIII. Conformational properties of N-acetyl-alpha,beta-dehydrovaline N',N'-dimethylamide

The crystal structure of Ac-DeltaVal-NMe(2) (DeltaVal = alpha,beta-dehydrovaline) was determined by X-ray crystallography. The found angles phi = -60 degrees and psi = 125 degrees correspond exactly to the respective values of the (i + 1)th residue in idealised beta-turn II/VIa. Ab initio/DFT studies revealed that the molecule adopts the angle psi restricted only to about |130 degrees | and very readily attains the angle phi = about -50 degrees. This is in line with its solid-state conformation. Taken together, these data suggest that the DeltaVal residue combined with a C-terminal tertiary amide is a good candidate at the (i + 1)th position in a type II/VIa beta-turn.     

Biophysical studies on molecular mechanism of abortifacient action of prostaglandins. VI. Conformation energy calculation on PGE2, PGF2 alpha and 15-(s)-methyl PGF2 alpha

This paper reports the conformation energy (CE) calculations on PGE2, PGE2 alpha and 15-(s)-methyl PGE2 alpha on the basis of empirical potential energy functions for the simultaneous rotations around C7-C8 (psi), C12-C13 (theta) and C14-C15 (phi) bonds. The variation of the minimum conformation energy E for each isoenergy map in the psi theta plane with respect to phi gives two minima around 90 degrees and 240 degrees in PGE2, 60 degrees and 245 degrees in PGF2 alpha, and 60 degrees and 150 degrees in 15-(s)-methyl PGF2 alpha. The latter two forms also have a small dip at 270 degrees. The pattern of allowed low energy conformations of PGF2 alpha and 15-(s)-methyl PGF2 alpha is quite similar and is characterized by the existence of six low energy regions.     

Synthesis, crystal structure, and molecular conformation of peptide N-Boc-L-Pro-dehydro-Phe-L-Gly-OH

The peptide N-Boc-L-Pro-dehydro-Phe-L-Gly-OH was synthesized by the usual workup procedure and finally coupling the N-Boc-L-Pro-dehydro-Phe to glycine. The peptide crystallizes in monoclinic space group P2(1) with a = 8.951(4) A, b = 5.677(6) A, c = 21.192(11) A, beta = 96.97(4) degrees, V = 1069(1) A3, Z = 2, dm = 1.295(5) Mgm-3, and dc = 1.297(4) Mgm-3. The structure was determined by direct methods using SHELXS86. The structure was refined by the block-diagonal least-squares procedure to an R value of 0.074 for 1002 observed reflections. The C alpha 2-C beta 2 distance of 1.33(2) A is an appropriate double bond length. The angle C alpha 2-C beta 2-C gamma 2 is 133(1) degrees. The peptide backbone torsion angles are theta 1 = -167(1) degrees, omega 0 = 179(1) degrees, phi 1 = -48(1) degrees, psi 1 = 137(1) degrees, omega 1 = 175(1) degrees, phi 2 = 65(2) degrees, psi 2 = 15(2) degrees, omega 2 = -179(1) degrees, and phi 3 = -166(1) degrees. These values show that the Boc group has a trans-trans conformation while the peptide backbone adopts a beta-turn II conformation, which is stabilized by an intramolecular hydrogen bond of length of 3.05(1) A. The structures of dehydro-Phe containing peptides suggest that the dehydro-Phe promotes the beta-turn II conformation. The five-membered pyrrolidine ring of the Pro residue adopts an ideal C gamma-exo conformation with torsion angles chi 1(1) = -24(1) degrees, chi 2(1) = 34(1) degrees, chi 3(1) = -30(1) degrees, chi 4(1) = 15(1) degrees, and theta 0(1) = 6(1) degrees. The side-chain torsion angles in dehydro-Phe are chi 1(2) = -1(2) degrees, chi 2,1(2) = -176(1) degrees, and chi 2,2(2) = 8(2) degrees. The plane of C alpha 2-C beta 2-C gamma 2 is rotated with respect to the plane of the phenyl ring at 7(1) degrees, which indicates that the atoms of the side chain of dehydro-Phe are essentially coplanar. The molecules form a 2(1) screw axis related hydrogen-bonded rows along the b axis.     

Conformational investigation of alpha, beta-dehydropeptides. Part III. Molecular and crystal structure of acetyl-L-prolyl-alpha, beta-dehydrovaline methylamide.

The crystal structure of Ac-Pro-delta Val-NHCH3 was examined to determine the influence of the alpha,beta-dehydrovaline residue on the nature of peptide conformation. The peptide crystallizes from methanol-diethyl ether solution at 4 degrees in needle-shaped form in orthorhombic space group P2(1)2(1)2(1) with a = 11.384(2) A, b = 13.277(2) A, c = 9.942(1) A, V = 1502.7(4) A3, Z = 4, Dm = 1.17 g.cm-3 and Dc = 1.18 g.cm-3. The structure was solved by direct methods using SHELXS-86 and refined to an R value of 0.057 for 1922 observed reflections. The peptide is found to adopt a beta-bend between the type I and the type III conformation with phi 1 = -68.3(4) degrees, psi 1 = -20.1(4) degrees, phi 2 = -73.5(4) degrees and psi 2 = -14.1(4) degrees. An intramolecular hydrogen bond between the carbonyl oxygen of ith residue and the NH of (i + 3)th residue stabilizes the beta-bend. An additional intermolecular N...O hydrogen bond joins molecules into infinite chains. In the literature described crystal structures of peptides having a single alpha,beta-dehydroamino acid residue in the (i + 2) position and forming a beta-bend reveal a type II conformation.     

Correlation properties of heartbeat dynamics

In this study, we investigate correlation properties of fluctuations in heart interbeat (RR) time series in a broad range of physiological and pathological conditions. Using detrended fluctuation analysis (DFA) method we determined short-term (alpha (1)) and long-term (alpha (2)) scaling exponent. In addition, we calculated standard deviation of RR intervals (SDRR) as the simplest variability measure. We found that the difference between alpha (1) and alpha (2) is related to RR interval length. At the shortest RR intervals, which correspond to extreme physiological and pathological conditions, we found the highest reduction of variability and the biggest difference between scaling exponents. In this case, DFA reveals a white noise over short scales (alpha (1 )about 0.5) and strongly correlated noise over large scales (alpha (2) about 1.5). With an increase in RR interval, accompanied by increased variability (increase in parasympathetic control), the difference between alpha (1) and alpha (2) decreases. The difference between scaling exponents disappeared in a state of efficient autonomic control. We suggest that the complexity in heart rhythm is achieved through coupling between intrinsically controlled heart rhythm and autonomic control, and that the model of stochastic resonance mechanism could be applied to this system.     

The precision of circadian clocks: assessment and analysis in Syrian hamsters

Locomotor activity recordings of Syrian hamsters were systematically analyzed to estimate the precision of the overt circadian activity rhythm in constant darkness. Phase variation, i.e., the standard deviation of phase markers around the regression line, varied with the definition of phase. Smallest phase variation was found in the onset of wheel running activity defined by 1h running means of the raw data. Both lower and higher degrees of smoothing lead to decreased precision measured in the overt rhythm. With passive infrared recordings, the midpoint of activity defined by 3h running means was the least variable. This demonstrates that the choice of phase marker should vary between recording methods. Phase variation decreased with increasing activity and was larger in females than in males. By calculating the average cycle variation and serial covariance of consecutive cycles, we estimated the contribution of 'clock' and 'non-clock' related processes to the overt rhythm variability. Variance in precision between phase markers could be shown to be attributable mainly to nonclock processes. Variance in pacemaker cycle length appeared reduced in wheel running activity records compared with passive infrared sensing records, suggesting feedback from running activity onto pacemaker function.     

Vigilance and grouping in the southern African ground squirrel (Xerus inauris)

Animals may form groups in response to the foraging–vigilance trade‐off, through enhanced predator detection (collective detection hypothesis) or reduced predation risk to the individual (dilution hypothesis), allowing individuals to decrease vigilance levels. Both hypotheses predict decreasing individual vigilance levels with increasing group size; however, the collective detection hypothesis also predicts increasing overall group vigilance with increasing group size. However, in species in which vigilance and foraging are not mutually exclusive, where vigilance may not be as costly, neither of these hypotheses may apply. Here, we examine the relationship between group size and vigilance in the social Cape ground squirrel (Xerus inauris), a species that can combine foraging and vigilance behaviours. Ten groups were observed using scan sampling, measuring both group and individual vigilance and group size. A negative relationship existed between individual vigilance and group size and a positive relationship between group vigilance and group size. Therefore, in Cape ground squirrels, vigilance seems to be costly even though it can be combined with foraging behaviours. Furthermore, group vigilance behaviour gives support to the collective detection hypothesis, whilst individual vigilance gives support to both hypotheses.     

Rotational dynamics of the Ca-ATPase in sarcoplasmic reticulum studied by time-resolved phosphorescence anisotropy

We have investigated the microsecond rotational motions of the Ca-ATPase in rabbit skeletal sarcoplasmic reticulum (SR), by measuring the time-resolved phosphorescence anisotropy of erythrosin 5-isothiocyanate (ERITC) covalently and specifically attached to the enzyme. Over a wide range of solvent conditions and temperatures, the phosphorescence anisotropy decay was best fit by a sum of three exponentials plus a constant term. At 4 degrees C, the rotational correlation times were phi 1 = 13 +/- 3 microseconds, phi 2 = 77 +/- 11 microseconds, and phi 3 = 314 +/- 23 microseconds. Increasing the solution viscosity with glycerol caused very little effect on the correlation times, while decreasing the lipid viscosity with diethyl ether decreased the correlation times substantially, indicating that the decay corresponds to rotation of the protein within the membrane, not to vesicle tumbling. The normalized residual anisotropy (A infinity) is insensitive to viscosity and temperature changes, supporting the model of uniaxial rotation of the protein about the membrane normal. The value of A infinity (0.20 +/- .02) indicates that each of the three decay components can be analyzed as a separate rotational species, with the preexponential factor Ai equal to 1.25X the mole fraction. An empirically accurate measurement of the membrane lipid viscosity was obtained, permitting a theoretical analysis of the correlation times in terms of the sizes of the rotating species. At 4 degrees C, the dominant correlation time (phi 3) is too large for a Ca-ATPase monomer, strongly suggesting that the enzyme is primarily aggregated (oligomeric).(ABSTRACT TRUNCATED AT 250 WORDS)     

Does a biological clock reside in the eye of quail?

The site (intra- vs. extraocular) of the circadian clock driving an ocular melatonin rhythm in Japanese quail was investigated by alternately covering the left and right eyes of individual quail, otherwise held in constant light (LL), for 12-hr periods. This procedure exposed each eye to a light-dark (LD) 12:12 light cycle 180 degrees (12 hr) out of phase with the LD 12:12 light cycle experienced by the other eye. This protocol entrained the melatonin rhythm in the left eye of quail 180 degrees out of phase with the rhythm expressed in the right eye. These results are compatible with the hypothesis that an independent light-entrainable circadian pacemaker resides in each eye; they are incompatible with the hypothesis that a single (or functionally single) extraocular pacemaker drives the ocular melatonin rhythm in both eyes. However, the results are also compatible with a model in which two independent extraocular circadian pacemakers, each with an exclusive photic input from one eye, drive the ocular melatonin rhythm.     

Synthesis, crystal structure, and molecular conformation of N-Ac-dehydro-Phe-L-Val-L-Val-OCH3.

The peptide N-Ac-dehydro-Phe-L-Val-L-Val-OCH3 (C22H31N3O5) was synthesized by the usual workup procedure and finally by coupling the N-Ac-dehydro-Phe-L-Val-OH to valine methyl ester. It was crystallized from its solution in acetonitrile-water mixture at 4 degrees C. The crystals belong to the space group P1 with a = 8.900(3) A, b = 11.135(2) A, c = 12.918(2) A, alpha = 90.36(1) degrees, beta = 110.14(3) 14(3) degrees, V = 1207.7(6) A, 3Z = 2, dm = 1.156(5) Mgm-3, dc = 1.148(5) Mgm-3. The structure was determined by direct methods using SHELXS86. The structure was refined by full-matrix least-squares procedure to an R value of 0.077 for 3916 observed reflections. The molecular dimensions and conformations of the two crystallographically independent molecules are in good agreement. In the dehydro residues, the average C alpha-C beta distance is 1.31(2) A whereas the bond angle C alpha-C beta-C gamma is 132(1) degrees. The average backbone torsion angles are omega 0 = 169(1) degrees, phi 1 = -40(1) degree, psi 1 = -50(1) degree, omega 1 = -177(1) degree, phi 2 = 54(1) degree, psi 2 = 46(1) degree, omega 2 = -174(1) degree, phi 3 = 103(1) degree, psi T3 = -139(1) degree, and theta T3 = -176(1) degree. The acetyl group is in the trans conformation, while the backbone adopts a right-handed and left-handed helical conformation alternatingly.(ABSTRACT TRUNCATED AT 250 WORDS)