The conformation of oxytocin in dimethylsulfoxide as revealed by carbon-13 spin-lattice relaxation times

Information was obtained on rates of overall molecular reorientation and segmental motion of amino acid sidechains of oxytocin in dimethylsulfoxide by determination of spin-lattice relaxation times (T₁) at 25 MHz for carbon-13 in natural abundance in the hormone. The T₁ values of the α-carbons of amino acid residues located in the 20-membered ring of oxytocin are all about 50 msec. The overall correlation time for the hormone backbone was estimated to be 8.8 × 10^?10 sec. The sidechains of Tyr, Ile and Gln undergo segmental motion with respect to the backbone of the ring. The T₁ value of the α-carbon of the Leu residue is greater than for any α-carbon in the ring, indicating an increased mobility of the backbone of the C-terminal acyclic peptide as compared to the ring. The β- and γ-carbons of the Pro residue undergo an exo-endo interconversion with regard to the plane formed by α-carbon, δ-carbon and N atom of the Pro pyrollidine ring. These data are discussed in light of results from other experimental and theoretical studies, including carbon-13 spin-lattice relaxation times for oxytocin in aqueous solution.     

A high-resolution 13C-nmr study of collagenlike polypeptides and collagen fibrils in solid state studied by the cross-polarization–magic angle-spinning method. Manifestation of conformation-dependent 13C chemical shifts and application to conformational characterization

We have recorded high-resolution ¹³C-nmr spectra of collagen fibrils in the solid state by the cross-polarization–magic-angle-spinning(CP–MAS)method and analyzed the spectra with reference to those of collagenlike polypeptides. We used two kinds of model polypeptides to obtain reference ¹³C chemical shifts of major amino acid residues of collagen (Gly, Pro, Ala, and Hyp): the 3₁-helical polypeptides [(Gly)_nII, (Pro)_nII, (Hyp)_n, and (Ala? Gly? Gly)_nII], and the triple-helical polypeptides [(Pro? Gly? Pro)_n and (Pro? Ala? Gly)_n]. Examination of the ¹³C chemical shifts of these polypeptides, together with our previous data, showed that the ¹³C chemical shifts of individual amino acid residues are the same, within experimental error (±0.5 ppm), among different polypeptides with different primary sequences, if the conformations are the same. We found that the ¹³C chemical shifts of Ala residues of the 3₁-helical (Ala? Gly? Gly)_n and triple-helical (Pro? Ala? Gly)_n are significantly displaced, compared with those of the α-helix, β-sheet, and silk I form, and can be utilized as excellent probes to examine conformational features of collagen-like polypeptides. Further, the ¹³C chemical shifts of Gly and Pro residues in the triple-helical polypeptides are substantially displaced from those found in (Gly)_nII and (Pro)_nII of the 3₁-helix, reflecting further conformational change from the 3₁-helix to the supercoiled triple helix. In particular, the ¹³C chemical shifts of Gly C ? O carbons of the triple-helical polypeptides are substantially displaced upfield (4.1–5.1 ppm), with respect to those of the 3₁-helical polypeptides. These displacements are interpreted by that Gly C ? O of the former is not involved in NH …? O ? C hydrogen bonds, while this carbon of the latter is linked by these kinds of hydrogen bonds. On the basis of these ¹³C chemical shifts, as reference data for the collagenlike structure, we were able to assign the ¹³C-nmr peaks of Gly, Ala, Pro, and Hyp residues of collagen fibrils, which are in good agreement with the values expected from the model polypeptides mentioned above. We also discuss a plausible conformational change of collagen fibrils during denaturation.     

Dynamic aspects of extracellular loop region as a proton release pathway of bacteriorhodopsin studied by relaxation time measurements by solid state NMR

Local dynamics of interhelical loops in bacteriorhodopsin (bR), the extracellular BC, DE and FG, and cytoplasmic AB and CD loops, and helix B were determined on the basis of a variety of relaxation parameters for the resolved ¹³C and ¹⁵N signals of [1-¹³C]Tyr-, [¹⁵N]Pro- and [1-¹³C]Val-, [¹⁵N]Pro-labeled bR. Rotational echo double resonance (REDOR) filter experiments were used to assign [1-¹³C]Val-, [¹⁵N]Pro signals to the specific residues in bR. The previous assignments of [1-¹³C]Val-labeled peaks, 172.9 or 171.1 ppm, to Val69 were revised: the assignment of peak, 172.1 ppm, to Val69 was made in view of the additional information of conformation-dependent ¹⁵N chemical shifts of Pro bonded to Val in the presence of ¹³C-¹⁵N correlation, although no assignment of peak is feasible for ¹³C nuclei not bonded to Pro. ¹³C or ¹⁵N spin-lattice relaxation times (T₁), spin-spin relaxation times under the condition of CP-MAS (T₂), and cross relaxation times (T_CH and T_NH) for ¹³C and ¹⁵N nuclei and carbon or nitrogen-resolved, ¹H spin-lattice relaxation times in the rotating flame (¹H T_1ρ) for the assigned signals were measured in [1-¹³C]Val-, [¹⁵N]Pro-bR. It turned out that V69-P70 in the BC loop in the extracellular side has a rigid β-sheet in spite of longer loop and possesses large amplitude motions as revealed from ¹³C and ¹⁵N conformation-dependent chemical shifts and T₁, T₂, ¹H T_1ρ and cross relaxation times. In addition, breakage of the β-sheet structure in the BC loop was seen in bacterio-opsin (bO) in the absence of retinal.     

Effects of molecular association on structure and dynamics of a collagenous peptide

Peptide GVKGDKGNPGWPGAPY from the triple-helix domain of type IV collagen aggregates in solution at a critical aggregation concentration of 18 mM. This molecular self association process is investigated by ¹H- and ¹³C-nmr spectroscopy. As a function of increasing peptide concentration, selective ¹H resonances are cooperatively chemically shifted by up to 0.04 ppm to apparently saturable values at high concentration. Pulsed field gradient nmr was used to derive translation diffusion constants that, as the peptide concentration is increased, also cooperatively and monotonically decrease to an apparent limiting value. An average number of 6 monomer units per aggregate have been estimated from diffusion constant and ¹³C relaxation data. Comparative ¹H nuclear Overhauser effect spectroscopy (NOESY) spectra accumulated at high and low peptide concentrations suggest that average internuclear distances are decreased as a result of peptide association. ¹³C-nmr multiplet spin-lattice relaxation and ¹³C- {¹H} NOE effects on ¹³C-enriched glycine methylene positions in the peptide demonstrate that overall molecular tumbling and backbone internal motions are attenuated in the aggregate state. Lowering the solution pD from pD 6 to pD 2 disrupts the aggregate state, suggesting a role for electrostatic interactions in the association process. Based on thermodynamic considerations, hydrophobic interactions also probably act to stabilize the aggregate state. These data are discussed in terms of an nmr/NOE constrained computer-modeled structure of the peptide. © 1993 John Wiley & Sons, Inc.     

Intrinsic proton relaxation parameters of hydrated polyglycine from two‐dimensional time domain NMR

Proton two‐dimensional time domain nmr involving T₁, T_1ρ, T_1D, and T₂ measurements was applied to hydrated polyglycine powders. The results were analyzed for magnetization exchange and found to be consistent with a general three‐site (glycine–water–glycine) exchange model. The intrinsic glycine and water proton relaxation parameters as well as the three exchange rates were obtained. Estimates of correlation times for water molecule motion at hydration sites are presented. © 1999 John Wiley & Sons, Inc. Biopoly 50: 630–640, 1999     

Influence of D and L amino-acid residues on the conformation of peptides in solution: A carbon-13 nuclear magnetic resonance study of cyclo(prolyl-leucyl)

The ¹³C chemical shifts and spin-lattice relaxation times are reported for cyclo(L -Pro-L -Leu) and cyclo(L -Pro-D -Leu). The chemical shifts of the D and L leucyl residues in the cyclic peptides differ from each other by 1.8 and 3.6 parts per million for the α and β carbons, respectively. The α-carbons of the prolyl residues differ by 1.0 ppm as a consequence of proximity to a D or an L leucyl residue. The ¹³C spin-lattic relaxation time(T₁) of the prolyl residues, but not the leucyl residues, in both compounds are indicative of difference in conformational equilibria within the pyrrolidine ring in the L -L isomer as compared to the L -D isomer. Anisotropic overall molecular reorientation is not responsible for the differences observed in the T₁ values. The differences in T₁ values and chemical shifts between cyclo(L -Pro-L -Leu) and cyclo(L -Pro-D -Leu) appear to result from a difference in conformations of the two diketopiperazine rings.     

13C-Nmr studies of ACTH: Assignment of resonances and conformational features

The biologically active ACTH(1–32) and ACTH(1–24) and other shorter peptide segments of the native hormone ACTH(1–39) were studied in aqueous solution by ¹³C-nmr. In order to identify the ¹³C resonances—except those of the carbonyls—both high-field nmr spectroscopy measurements and substitution of residues with amino acids enriched to 85% in ¹³C were carried out. The main results are (1) the direct characterization of the cis–trans isomerism of proline 24 and its effects on the directly connected and sequentially neighboring residues and (2) findings that the conformational features agree with an α-helix type organization in the N-terminal part of the ACTH molecule which is responsible for the biological activity.     

Multinuclear magnetic resonance studies of collagen molecular structure and dynamics

We have measured the percentages of cis and trans Gly-Pro and X-Hyp peptide bonds in thermally unfolded type I collagen. ¹³C-nmr solution spectra show that 16% of the Gly-Pro and 8% of the X-Hyp bonds are cis in unfolded chick calvaria collagen. These results support the hypothesis that cis–trans isomerization is that rate-limiting step in the propagation of the collagen triple helix. We have used multinuclear solid-state nmr to study the molecular dynamics of the collagen backbone in tendon, demineralized bone, and intact bone as a function of temperature, hydration, and pH. These studies show that collagen backbone motions are characterized by a broad distribution of correlation times, τ, covering the range from 10^?4 to 10^?9 s. In the case of nonmineralized collagen, the root-mean-square fluctuations in azimuthal angle, γ_rms, range from ca. 10° when τ ～ 10^?9 s to ca. 30° when τ < 10^?4 s; in the case of bone collagen, γ_rms values are about half as large as those found in nonmineralized collagen. Backbone motions are negligible at temperatures below ?25°C. This is also the case at 22°C when demineralized bone collagen is lyophilized. In contrast, flexibility of hydrated demineralized bone collagen greatly increases as pH is lowered from 7 to 2. The more limited flexibility observed at neutral pH is a consequence of the intermolecular interactions that contribute to fibril organization and strength. However, the fibrils retain significant flexibility at physiological pH, enabling them to distribute stress and dissipate mechanical energy.     

Molecular mobility of polypeptides containing proline as determined by 13C magnetic resonance

The molecular conformations and dynamics of poly(L -prolyl), poly(hydroxyl-L -prolyl), poly(L -prolyl-glycyl), poly(hydroxyl-L -prolyl), and poly(glycyl-glycyl-L -prolyl-glycyl), in aqueous solution, have been studied using ¹³C pulse Fourier transform nmr spectroscopy. From a measurement of the intensities of major and minor resonances in the spectra of the copolypeptides, it was determined that 15–20% of the glycyl-prolyl and glycyl-hydroxyprolyl peptide bonds are cis. Effective rotational correlation times (τ_eff), obtained from measurements of spin-lattice relaxation times (T₁) of individual backbone and side-chain carbons, demonstrated that backbone reorientation is approximately isotropic for the five polypeptides and is characterized by correlation times of ca. 0.3–0.6 nanoseconds as a result of rapid segmental motion. In a given polypeptide glycyl and pyrrolidine residues were found to have the same backbone correlation times, but backbone carbon τ_eff values did decrease as the glycyl content of the peptides increased. A semi-quantitative analysis of C^β, C^γ, and C^δ correlation times suggests that rapid ring motion in both prolyl and hydroxyprolyl involves primarily C^γ and C^β, with the prolyl ring being more mobile than the hydroxyprolyl ring.     

1H- and 13C-nmr investigations on cis–trans isomerization of proline peptide bonds and conformation of aromatic side chains in H-Trp-(Pro)n-Tyr-OH peptides

¹H and ¹³C high-resolution nmr spectra of cationic, zwitterionic, and anionic forms of the peptides: H-Trp-(Pro)_n-Tyr-OH, n = 0-5, and H-Trp-Pro-OCH₃ were obtained in D₂O solution. Analysis of H^α(Pro₁), H^α(Trp), C^γ(Pro), H^ε(Tyr), and H^δ(Trp) resonances provided evidence for the presence of two predominant backbone isomers: the all-trans one and another with the Trp-Pro peptide bond in cis conformation; the latter constituted about 0.8 molar fraction of the total peptide (n > 1) concentration. Relative content of these isomers varied in a characteristic way with the number of Pro residues and the ionization state of the peptides. The highest content of the cis (Trp-Pro) isomer, 0.74, was found in the anionic form of H-Trp-Pro-Tyr-OH; it decreased in the order of: anion ? zwitterion ≈ cation, and with the number of Pro residues to reach the value of 0.42 in the cationic form of H-Trp- (Pro)₅-Tyr-OH. Isomerization equilibria about Pro-Pro bond(s) were found to be shifted far (?0.9) in favor of the trans conformation. Interpretation of the measured vicinal coupling constants J_α?β′ and J_α?β″ for C^αH-C^βH₂ proton systems of Trp and Tyr side chains in terms of relative populations of g⁺, g^?, and t staggered rotamers around the χ₁ dihedral angle indicated that in all the peptides studied (a) rotation of Trp indole ring in cis (Trp-Pro) isomers is strongly restricted, and (b) rotation of Tyr phenol ring is relatively free. The most preferred χ₁ rotamer of Trp (0.8-0.9 molar fraction) was assigned as the t one on the basis of a large value of the vicinal coupling constant between the high-field H^β and carbonyl carbon atoms of Trp, estimated for the cis (Pro₁) form of H-Trp-Pro-Tyr-OH from a ¹H, ¹³C correlated spectroscopy ¹H detected multiple quantum experiment. This indicates that cis ? trans equilibrium in the Trp-Pro fragment is governed by nonbonding interactions between the pyrrolidine (Pro) and indole (Trp) rings. A molecular model of the terminal cis Trp-Pro dipeptide fragment is proposed, based on the presented nmr data and the results of our molecular mechanics modeling of low-energy conformers of the peptides, reported elsewhere. © 1993 John Wiley & Sons, Inc.     

Electrical properties of hydrated collagen. II. Semiconductor properties

The dc conductivity of hydrated bovine Achilles' tendon collagen has been determined as a function of hydration over a limited temperature range. At ambient temperature the conductivity changes from 10^?15 (Ω cm)^?1 in the dry state to about 10^?8 (Ω cm)^?1 at ～24% water content by weight. For all temperatures the conductivity increases exponentially with hydration obeying σ(h) = A exp (βh), where h is a measure of the hydration, A is independent of temperature, and the parameter β ～ T^?1. It is shown that the data may be described by an impurity-type mechanism in which the effective activation energy for the process is dependent on temperature and hydration. Conduction is assumed to be electronic with the impurity (water) acting as a donor. In the solid state the effect of water on the conductivity is reversible indicating the absence of chemical alteration of the hydrated collagen.     

Intracellular water in Artemia cysts (brine shrimp): Investigations by deuterium and oxygen-17 nuclear magnetic resonance

The dormant cysts of Artemia undergo cycles of hydration-dehydration without losing viability. Therefore, Artemia cysts serve as an excellent intact cellular system for studying the dynamics of water-protein interactions as a function of hydration. Deuterium spin-lattice (T₁) and spin-spin (T₂) relaxation times of water in cysts hydrated with D₂O have been measured for hydrations between 1.5 and 0.1 g of D₂O per gram of dry solids. When the relaxation rates (I/T₁, I/T₂) of ²H and ¹⁷O are plotted as a function of the reciprocal of hydration (1/H), an abrupt change in slope is observed near 0.6 g of D₂O (or H₂ ¹⁷O)/gram of dry solids, the hydration at which conventional metabolism is activated in this system. The results have been discussed in terms of the two-site and multisite exchange models for the water-protein interaction as well as protein dynamics models. The ²H and ¹⁷O relaxation rates as a function of hydration show striking similarities to those observed for anisotropic motion of water molecules in protein crystals.

It is suggested here that although the simple two-site exchange model or n-site exchange model could be used to explain our data at high hydration levels, such models are not adequate at low hydration levels (<0.6 g H₂O/g) where several complex interactions between water and proteins play a predominant role in the relaxation of water nuclei. We further suggest that the abrupt change in the slope of I/T₁ as a function of hydration in the vicinity of 0.6 g H₂O/g is due to a change in water-protein interactions resulting from a variation in the dynamics of protein motion.

     

Characterization of a type of β‐bend ribbon spiral generated by the repeating (Xaa–Yaa–Aib–Pro) motif: The solution structure of harzianin HC IX,a 14‐residue peptaibol forming voltage‐dependent ion channels

The three‐dimensional solution structure of harzianin HC IX, a peptaibol antibiotic isolated from the fungus Trichoderma harzianum, was determined using CD, homonuclear, and heteronuclear two‐dimensional nmr spectroscopy combined with molecular modeling. This 14‐residue peptide, Ac Aib¹ Asn² Leu³ Aib⁴ Pro⁵ Ala⁶ Ile⁷ Aib⁸ Pro⁹ Iva¹⁰ Leu¹¹ Aib¹² Pro¹³ Leuol¹⁴ (Aib, α‐aminoisobutyric acid; Iva, isovaline; Leuol, leucinol), is a main representative of a short‐sequence peptaibol class characterized by an acetylated N‐terminus, a C‐terminal amino alcohol, and the presence of three Aib‐L ‐Pro motifs at positions 4–5, 8–9, and 12–13, separated by two dipeptide units. In spite of a lower number of residues, compared to the 18/20‐residue peptaibols such as alamethicin, harzianin HC IX exhibits remarkable membrane‐perturbing properties. It interacts with phospholipid bilayers, increasing their permeability and forming voltage‐gated ion channels through a mechanism slightly differing from that proposed for alamethicin. Sequence‐specific ¹H‐ and ¹³C‐nmr assignments and conformational nmr parameters (³J_NHCαH coupling constants, quantitative nuclear Overhauser enhancement data, temperature coefficients of amide and carbonyl groups, NH–ND exchange rates) were obtained in methanol solution. Sixty structures were calculated based on 98 interproton distance restraints and 6 Φ dihedral angle restraints, using high temperature restrained molecular dynamics and energy minimization. Thirty‐seven out of the sixty generated structures were consistent with the nmr data and were convergent. The peptide backbone consists in a ribbon of overlapping β‐turns twisted into a continuous spiral from Asn² to Leuol¹⁴ and forming a 26 Å long helix‐like structure. This structure is slightly amphipathic, with the three Aib–Pro motifs aligned on the less hydrophobic face of the spiral where the Asn² side chain is also present, while the more hydrophobic bulky side chains of leucines, isoleucine, isovaline, and leucinol are located on the concave side. The repetitive (Xaa–Yaa–Aib–Pro) tetrapeptide subunit, making up the peptide sequence, is characterized by four sets of (Φ,Ψ) torsional angles, with the following mean values: Φ_i = −90°, Ψ_i = −27°; Φ_i+1 = −98°, Ψ_i+1 = −17°; Φ_i+2 = −49°, Ψ_i+2 = −50°; Φ_i+3 = −78°, Ψ_i+3 = +3°. We term this particular structure, specifically occurring in the case of (Xaa–Yaa–Aib–Pro)_n sequences, the (Xaa–Yaa–Aib–Pro)‐β‐bend ribbon spiral. It is stabilized by 4 → 1 intramolecular hydrogen bonds and differs from both the canonical 3₁₀‐helix made of a succession of type III β‐turns and from the β‐bend ribbon spiral that has been described in the case of (Aib–Pro)n peptide segments. © 1999 John Wiley & Sons, Inc. Biopoly 50: 71–85, 1999     

NMR study of silk I structure of Bombyx mori silk fibroin with 15N- and 13C-NMR chemical shift contour plots

The metastable state silk I structures of Bombyx mori silk fibroin in the solid state were studied on the basis of ¹⁵N- and ¹³C-nmr chemical shifts of Ala, Ser, and Gly residues. The ¹⁵N cross-polarization magic angle spinning (CP/MAS) nmr spectra of the precipitated fraction after chymotrypsin hydrolysis of B. mori silk fibroin with the silk I and silk II forms were measured to determine the ¹⁵N chemical shifts of Gly, Ala, and Ser residues. For comparison, ¹⁵N CP/MAS nmr chemical shifts of Ala were measured for [¹⁵N] Ala Philosamia cynthia ricini silk fibroin with antiparallel β-sheet and α-helix forms. The ¹³C CP/MAS nmr chemical shifts of Ala, Ser, and Gly residues of B. mori silk fibroin with the silk I and silk II forms, as well as ¹³C CP/MAS nmr chemical shifts of Ala residue of P. c. ricini silk fibroin with β-sheet and α-helix forms, are used for the examination of the silk I structure. Both silk I and α-helix peaks are shifted to a lower field than silk II (β-sheet) for the Cα carbons of the Ala residues, while both Cβ carbon peaks are shifted to higher field. However, the silk I peak of the ¹⁵N nucleus of the Ala residue is shifted to lower field than the silk II peak, but the α-helix peak is shifted to high field. Thus, the difference in the structure between the silk I and α-helix is reflected in a different manner between the ¹³C and ¹⁵N chemical shifts. The Cα and Cβ chemical shift contour plots for Ala and Ser residues, and the Cα plot for the Gly residue, were prepared from the Protein Data Bank data obtained for 12 proteins and used for discussing the silk I structure quantitatively from the conformation-dependent chemical shifts. The plots reported by Le and Oldfield for ¹⁵N chemical shifts were also used for the purpose. All these chemical shift data support Fossey's model (Ala: ϕ = −80°, φ = 150°, Gly: ϕ = −150°, φ = 80°) and do not support Lotz and Keith's model (Ala: ϕ = −104.6°, φ = 112.2°, Gly: ϕ = 79.8°, φ = 49.7° or Ala: ϕ = −124.5°, φ = 88.2°, Gly: ϕ = −49.8°, φ = −76.1°) as the silk I structure. © 1997 John Wiley & Sons, Inc.     

Water in normal muscle and muscle with a tumor

The total water content, the amount of non-freezable water, and the Na⁺ and K⁺ contents in the gastrocnemius muscle of albino mice with and without a solid tumor were determined. The spin-lattice relaxation time (T₁) for the water protons in the two kinds of muscle were measured at six resonance frequencies ranging from 4.5 to 60 MHz over the temperature range +37 to −65°C. Quantitatively calculated T₁ values are given. The difference in T₁ for the two types of muscle at temperatures above −5°C is attributed to the difference in the distribution ratio of water between hydration and free states, and bears no direct relation to the concentration of Na⁺.     

Evidence of α fluctuations in myoglobin's denaturation in the high temperature region: Average relaxation time from an Adam–Gibbs perspective

In this work, we derive an analytical expression for the relaxation time τ as a function of temperature T for myoglobin protein (Mb, PDB:1MBN) in the high temperature limit (T > T_g = 200 K). The method is based on a modified version of the Adam–Gibbs theory (AG theory) for the glass transition in supercooled liquids and an implementation of differential geometry techniques. This modified version of the AG theory takes into account that the entropic component in protein's denaturation has two major sources: a configurational contribution ΔS_c due to the unfolding of the highly ordered native state N and a hydration contribution ΔS^hyd arising from the exposure of non-polar residues to direct contact with solvent polar molecules. Our results show that the configurational contribution ΔS_c is temperature-independent and one order of magnitude smaller than its hydration counterpart ΔS^hyd in the temperature range considered. The profile obtained for log τ(T) from T = 200 K to T = 300 K exhibits a non-Arrhenius behavior characteristic of α relaxation mechanisms in hydrated proteins and glassy systems. This result is in agreement with recent dielectric spectroscopy data obtained for hydrated myoglobin, where at least two fast relaxation processes in the high temperature limit have been observed. The connection between the relaxation process calculated here and the experimental results is outlined.     

Conformational interconversions in peptide β-turns: Discrimination between enantiomeric conformations by chiral perturbation

The crystal structure of the model tripeptide Boc-Aib-Gly-Leu-OMe ( 1 ) reveals two independent molecules in the asymmetric unit that adopt “enantiomeric” type I and type I′ β-turn conformations with the Aib and Gly residues occupying the corner (i + 1 and i + 2) positions. ¹³C cross polarization and magic angle sample spinning spectra in the solid state also support the coexistence of two conformational species. ¹³C-nmr in CDCl₃ establishes the presence of a single species or rapid exchange between conformations. 400 MHz ¹H-nmr provides evidence for conformational exchange involving a major and minor species, with β-turn conformations supported by the low solvent exposure of Leu(3) NH and the observation of N_iH ↔ N_i+1H nuclear Overhauser effects. CD bands in the region 190–230 nm are positive, supporting a major population of type I′ β-turns. The isomeric peptide, Boc-Gly-Leu-Aib-OMe ( 2 ), adopts an “open” type II′ β-turn conformation in crystals. Solid state and solution nmr support population of a single conformational species. Chiral perturbation introduced outside the folded region of peptides may provide a means of modulating screw sense in achiral sequences. © 1998 John Wiley & Sons, Inc. Biopoly 45: 191–202, 1998     

15N-nmr spectroscopy. 20. Cis/trans isomerism and neighboring residue effects of proline-containing peptides

Five N-protected tetrapeptide esters of the structure Gly-Pro-X-X*-O-methyl were synthesized in such a way that one of the two variable amino acid residues (X) was isotopically enriched in ¹⁵N (denoted by*). The variable amino acids are glycine, alanine, leucine, valine, and phenylalanine. For the natural abundance ¹⁵N-nmr spectra of these tetrapeptide derivatives in methylene chloride only the signals of the Gly-Pro trans isomer were found. In a 2:1 mixture of acetone and dimethylsulfoxide, signals for both the cis and trans isomers were observed. Three of the five tetrapeptide derivatives show cis/trans splitting of all four nitrogen signals. The ¹⁵N-nmr spectra of Z-Pro-Pro-OH and of (D ,L -proline)_n were measured in a 2:1 mixture of acetone and dimethylsulfoxide as well as in water. The effects of solvents and neighboring residues and the influence of the cis/trans isomerism on the nmr spectra are discussed. The determination of the cis/trans equilibria and the assignment of the ¹⁵N-nmr signals of all oligopeptides were achieved by selective isotopic enrichment and by means of ¹³C-nmr spectra.     

NH2-terminal sequences of DNA-, heparin-, and gelatin-binding tryptic fragments from human plasma fibronectin

NH₂-terminal sequence analysis was performed on subregions of human plasma fibronectin including 24,000-dalton (24K) DNA-binding, 29,000-dalton (29K) gelatin-binding, and 18,000-dalton (18K) heparin-binding tryptic fragments. These fragments were obtained from fibronectin after extensive trypsin digestion followed by sequential affinity purification on gelatin-Sepharose, heparin-agarose, and DNA-cellulose columns. The gelatin-binding fragment was further purified by gel filtration on Sephadex G-100, and the DNA-binding and heparin-binding fragments were further purified by high-performance liquid chromatography. The 29K fragment had the following NH₂-terminal sequence: AlaAlaValTyrGlnProGlnProHisProGlnProPro (Pro)TyrGlyHis HisValThrAsp(His)(Thr)ValValTyrGly(Ser) ?(Ser)?-Lys. The NH₂-terminal sequence of a 50K, gelatin-binding, subtilisin fragment by L. I. Gold, A. Garcia-Pardo, B. Prangione, E. C. Franklin, and E. Pearlstein (1979, Proc. Nat. Acad. Sci. USA76, 4803–4807) is identical to positions 3–19 (with the exception of some ambiguity at position 14) of the 29K fragment. These data strongly suggest that the 29K tryptic fragment is included in the 50K subtilisin fragment, and that subtilisin cleaves fibronectin between the Ala²Val³ residues of the 29K tryptic fragment. The 18K heparin-binding fragment had the following NH₂-terminal sequence: (Glu)AlaProGlnProHisCysIleSerLysTyrIle LeuTyrTrpAspProLysAsnSerValGly?(Pro) LysGluAla?(Val)(Pro). The 29K gelatin-binding and 18K heparin-binding fragments have proline-rich NH₂-terminal sequences suggesting that they may have arisen from protease-sensitive, random coil regions of fibronectin corresponding to interdomain regions preceding macromolecular-binding domains. Both of these fragments contain the identical sequence ProGlnProHis, a sequence which may be repeated in other interdomain regions of fibronectin. The 24K DNA-binding fragment has the following NH₂-terminal sequence: SerAspThrValProSerProCysAspLeuGlnPhe ValGluValThrAspVal LysValThrIleMetTrpThrProProGluSerAla ValThrGlyTyrArgVal AspValCysProValAsnLeuProGlyGluHisGly Gln(Cys)LeuProIleSer. The sequence of positions 9–22 are homologous to positions 15–28 of the α chain of DNA-dependent RNA polymerase from Escherichia coli. The homology observed suggests that this stretch of amino acids may be a DNA-binding site.     

Salt-induced conformational change of random copolymers (Lys50Tyr50)n and (Lys50Phe50)n studied by 1H- and 13C-nuclear magnetic resonances. Aggregation behavior of helical segments

¹H- and ¹³C-nmr studies of conformational transitions of random amino acid copolymers containing aromatic residues (Lys⁵⁰Tyr⁵⁰)_n and (Lys⁵⁰Phe⁵⁰)_n in the presence of neutral salts were performed to serve as models of the aggregation behavior of polypeptides of biological significance. The ¹H and ¹³C signal intensities of Tyr and Phe residues decreased preferentially with increasing concentration of neutral salts such as NaCl and NaClO₄. This behavior contrasts with that of (Lys)_n in the presence of similar neutral salts, where the displacement of the ¹³C signal is clearly seen on transition from the random-coil to the helical conformation. On the basis of the previous conformational studies, the loss of the peak areas is ascribed to the presence of immobilized helical segments by hydrophobic interaction between aromatic side chains. The remaining resonances are due to the residual random-coil regions, since the values of nuclear Overhauser enhancements and chemical shifts are unchanged in the presence and absence of the neutral salts.