Concentration-dependent hydrogen exchange kinetics of 3H-labeled S-peptide in ribonuclease S.

The hydrogen exchange kinetics of the S-peptide in ribonuclease S can be measured by first tritiating the S-peptide in the absence of S-protein and then allowing it to recombine rapidly with S-protein. Afterwards the exchange reactions of this specific segment of ribonuclease S can be studied. The exchange kinetics of bound S-peptide are complex, indicating that different protons exchange at markedly different rates. The terminal exchange reaction, involving at least five highly protected protons, has been studied as a function of pH.At low concentrations of ribonuclease S the exchange kinetics become concentration-dependent, owing to the dissociation of the S-peptide. Although the fraction of free S-peptide is always very small, its rate of exchange is several orders of magnitude faster than that of bound S-peptide, and the concentration dependence of the exchange kinetics is readily measurable. It provides a highly sensitive method for determining small dissociation constants (K_D). Values of K_D ranging from 10^?6m at pH 2.7, 0 °C, to 2 × 10^?10m at pH 7.0, 0 °C, are reported here. Our value for K_D at pH 7.0, 0 °C, confirms the data and extrapolation to 0 °C of Hearn et al. (1971).At high concentrations of ribonuclease S the terminal exchange reaction is independent of concentration. It probably results from a local unfolding reaction of the bound S-peptide. Above pH 4 the strong pH dependence of K_D closely resembles that of the apparent equilibrium constant for this local unfolding reaction. The latter may be one step in the dissociation process and we present such a model for ribonuclease S dissociation.Measurement of concentration-dependent exchange kinetics should provide a useful method of determining small dissociation constants in other systems: for example, in studies of protein-nucleic acid interactions.     

Self-association and solubility of peptides: solvent-titration study of N alpha-protected C-terminal sequences of substance P

Self-association of N^α-protected peptides related to C-terminal sequences of substance P in methylene chloride was disrupted by adding increasing amounts of various polar organic solvents. This process was monitored by the disappearance of the amide I C?O stretching band (1630 cm^?1) of strongly intermolecularly H-bonded molecules in the irabsorption spectra. The effects induced by main-chain length, incorporation at position 9 of a residue promoting folding (α-aminoisobutyric acid), the nature of solvent, and peptide concentration were established. A corollary ¹H-nmr investigation provided detailed information on the NH protons involved in the self-association process as H-bonding donors. The increasing propensity to aggregate exhibited by these peptides is paralleled by a decrease in their solubility. The impact of these results on the synthesis of substance P short sequences is briefly outlined.     

Local secondary structure in ribonuclease A denatured by guanidine · HCl near 1 °C

Recent work has shown that a short α-helix can be stable in water near 1 °C when stabilized by specific interactions between side-chains, while earlier “host-guest” results with random copolymers have shown that a short α-helix is unstable in water at all temperatures in the absence of stabilizing side-chain interactions. As regards the mechanism of protein folding, it is now reasonable on energetic grounds to consider isolated α-helices and β-sheets as the first intermediates on the pathway of protein folding. Proton nuclear magnetic resonance is used here to detect isolated secondary structures in ribonuclease A denatured by guanidine · HCl (GuHCl). Temperatures near 1 °C are used because the low-temperature stability of the C-peptide helix may be a general property of isolated secondary structures in water.Our procedure is to titrate with GuHCl the C2H resonance lines of the four histidine residues of denatured ribonuclease A. Studies of model peptides (C-peptide (lactone) and C-peptide carboxylate, residues 1 to 13 of ribonuclease A; S-peptide, residues 1 to 20) show linear titration curves for the C2H resonance of His12 above 0.5 M-GuHCl, once helix unfolding is complete. Deviations from this line are used to monitor helix formation. The GuHCl titration curves of the other three histidine residues are also linear, once unfolding is complete. The results show that the helix found in C-peptide and S-peptide is also found in denatured ribonuclease A, where it behaves as an isolated helix not stabilized significantly by interactions with other chain segments. Studies of denatured S-protein show that the remaining three His residues, His48, His105 and His119, are involved in structure only below 1 m-GuHCl at 9 °C, pH 1.9. The nature of this structure is not known. The main conclusion from this work is that the His12 helix can be observed as a stable, isolated helix in denatured ribonuclease A near 1 °C, and that none of the other three His residues is involved in a comparably stable local structure. In native ribonuclease A, His12 is within an α-helix and the other three His residues are involved in a 3-stranded β-sheet structure.The helix-coil transition of C-peptide has also been studied for other side-chain resonances by GuHCl titration. Typically, but not always, the titration curves are linear after helix unfolding takes place and resonance lines from different residues of the same amino acid type can be resolved in GuHCl solutions. This is true of the four histidine residues of ribonuclease A although their pK values in 5 m-GuHCl are nearly the same. In C-peptide, the βCH₃ resonance of Ala6 is affected strongly by GuHCl while the lines of Ala4 and Ala5 are shifted only weakly by GuHCl. Evidently the interactions between GuHCl and side-chains in an unfolded peptide depend upon neighboring groups.     

Design and characterization of a model αβ peptide

CD and nmr spectroscopy were used to compare the conformational properties of two related peptides. One of the peptides, Model AB, was designed to adopt a helix-turn-extended strand (αβ) tertiary structure in water that might be stabilized by hydrophobic interactions between two leucine residues in the amino-terminal segment and two methionine residues in the carboxyl terminal segment. The other peptide, AB Helix, has the same amino acid sequence as Model AB except that it lacks the-Pro-Met-Thr-Met-Thr-Gly segment at the carboxyl-terminus. Although the carboxyl-terminal segment of Model AB was found to be unstructured, its presence increases the number of residues in a helical conformation, shifts the pKas of three ionizable side chains by 1 pH unit or more compared to an unstructured peptide, stabilizes the peptide as a monomer in high concentrations of ammonium sulfate, increases the conformational stability of residues at the terminal ends of the helix, and results in many slowly exchanging amide protons throughout the entire backbone of the peptide. These results suggest that interactions between adjacent segments in a small peptide can have significant structure organizing effects. Similar kinds of interactions may be important in determining the structure of early intermediates in protein folding and may be useful in the de novo design of independently folding peptides. © 1995 John Wiley & Sons, Inc.     

Preferred conformations of protected homo-oligo-L-glutamate peptides in CDCl3 and CDCl3/TFA mixtures

A conformational analysis of protected glutamate homo-oligopeptides Z-[Glu(OEt)]_n-OEt (n = 2–7) was carried out in chloroform solution using high-resolution ¹H-nmr spectroscopy. At dilute peptide concentrations, the backbone NH and α-CH resonances are well resolved and can be assigned by combining extensive homonuclear decoupling experiments with data for co-oligopeptide derivatives. The structure of these peptides in solution was then assessed using information from chemical shifts, coupling constants, temperature coefficients, and titration of each oligomer with trifluoroacetic acid (TFA). The di- and tripeptides are found to be in disordered forms in deuterochloroform (CDCl₃) and CDCl₃/TFA mixtures. The tetrapeptide exhibits a folded structure with intramolecular hydrogen bonding at Glu² in CDCl₃ and undergoes a transition to increasingly disordered forms as TFA is added. The pentamer to heptamer show a folded structure with a strong intramolecular hydrogen bond at Glu² and a weaker hydrogen bond at Glu³, which are disrupted as these peptides go to random coils at high TFA/CDCl₃ ratios. In addition, the N-terminal portions of these glutamate peptides appear to be involved in side chain–main chain interactions. The results support the hypothesis that protected linear homo-oligopeptides may possess two or more segments of conformation with intramolecular folding preferred near the N-terminal portion.     

Synthesis and conformational study of peptides possessing helically arranged ΔZPhe side chains

Z-Dehydrophenylalanine (Δ^zPhe) possessing four oligopeptides, Boc-(L -Ala-Δ^zPhe-Aib)_n-OCH₃ (n = 1–4: Boc, t-butoxycarbonyl; Aib, α-aminoisobutyric acid), were synthesized, and their solution conformations were investigated by ¹H-nmr, ir, uv, and CD spectroscopy and theoretical CD calculation. ¹H-nmr (the solvent accessibility of NH groups) and ir studies indicated that all the NH groups except for those belonging to the N-terminal L -Ala-Δ^zPhe moiety participate in intramolecular hydrogen bonding in chloroform. This suggests that the peptides n = 2–4 have a 4 → 1 hydrogen-bonding pattern characteristic of 3₁₀-helical structures. The uv spectra of all these peptides recorded in chloroform and in trimethyl phosphate showed an intense maximum around 276 nm assigned to the Δ^zPhe chromophores. The corresponding CD spectra of the peptides n = 2–4 showed exciton couplets with a negative peak at longer wavelengths, whereas that of the peptide n = 1 showed only weak signals. Theoretical CD spectra were calculated for the peptides n = 2–4 of several helical conformations, on the basis of exciton chirality method. This calculation indicated that the three peptides form a helical conformation deviating from the perfect 3₁₀-helix that contains three residues per turn, and that their side chains of Δ^z Phe residues are arranged regularly along the helix. The center-to-center distance between the nearest phenyl pair(s) was estimated to be ～ 5.5 Å. The chemical shifts of the Δ^zPhe side-chain protons (H^β and aromatic H) for the peptides n = 2–4 indicated anisotropic shielding effect of neighboring phenyl group(s); the effect also supports a regular arrangement of the Δ^z Phe side chains along the helical axis. © 1993 John Wiley & Sons, Inc.     

Thermodynamic model of secondary structure for α-helical peptides and proteins

A thermodynamic model describing formation of α-helices by peptides and proteins in the absence of specific tertiary interactions has been developed. The model combines free energy terms defining α-helix stability in aqueous solution and terms describing immersion of every helix or fragment of coil into a micelle or a nonpolar droplet created by the rest of protein to calculate averaged or lowest energy partitioning of the peptide chain into helical and coil fragments. The α-helix energy in water was calculated with parameters derived from peptide substitution and protein engineering data and using estimates of nonpolar contact areas between side chains. The energy of nonspecific hydrophobic interactions was estimated considering each α-helix or fragment of coil as freely floating in the spherical micelle or droplet, and using water/cyclohexane (for micelles) or adjustable (for proteins) side-chain transfer energies. The model was verified for 96 and 36 peptides studied by ¹H-nmr spectroscopy in aqueous solution and in the presence of micelles, respectively ([set I] and [set 2]) and for 30 mostly α-helical globular proteins ([set 3]). For peptides, the experimental helix locations were identified from the published medium-range nuclear Overhauser effects detected by ¹H-nmr spectroscopy. For sets 1, 2, and 3, respectively, 93, 100, and 97% of helices were identified with average errors in calculation of helix boundaries of 1.3, 2.0, and 4.1 residues per helix and an average percentage of correctly calculated helix—coil states of 93, 89, and 81%, respectively. Analysis of adjustable parameters of the model (the entropy and enthalpy of the helix—coil transition, the transfer energy of the helix backbone, and parameters of the bound coil), determined by minimization of the average helix boundary deviation for each set of peptides or proteins, demonstrates that, unlike micelles, the interior of the effective protein droplet has solubility characteristics different from that for cyclohexane, does not bind fragments of coil, and lacks interfacial area. © 1997 John Wiley & Sons, Inc. Biopoly 42: 239–269, 1997     

Amide proton exchange used to monitor the formation of a stable alpha-helix by residues 3 to 13 during folding of ribonuclease S

We make use of the known exchange rates of individual amide proton in the S-peptide moiety of ribonuclease S (RNAase S) to determine when during folding the alpha-helix formed by residues 3 to 13 becomes stable. The method is based on pulse-labeling with [3H]H2O during the folding followed by an exchange-out step after folding that removes 3H from all amide protons of the S-peptide except from residues 7 to 14, after which S-peptide is separated rapidly from S-protein by high performance liquid chromatography. The slow-folding species of unfolded RNAase S are studied. Folding takes place in strongly native conditions (pH 6.0, 10 degrees C). The seven H-bonded amide protons of the 3-13 helix become stable to exchange at a late stage in folding at the same time as the tertiary structure of RNAase S is formed, as monitored by tyrosine absorbance. At this stage in folding, the isomerization reaction that creates the major slow-folding species has not yet been reversed. Our result for the 3-13 helix is consistent with the finding of Labhardt (1984), who has studied the kinetics of folding of RNAase S at 32 degrees C by fast circular dichroism. He finds the dichroic change expected for formation of the 3-13 helix occurring when the tertiary structure is formed. Protected amide protons are found in the S-protein moiety earlier in folding. Formation or stabilization of this folding intermediate depends upon S-peptide: the intermediate is not observed when S-protein folds alone, and folding of S-protein is twice as slow in the absence of S-peptide. Although S-peptide combines with S-protein early in folding and is needed to stabilize an S-protein folding intermediate, the S-peptide helix does not itself become stable until the tertiary structure of RNAase S is formed.     

Protection of amide protons in folding intermediates of ribonuclease A measured by pH-pulse exchange curves

pH-pulse exchange curves have been measured for samples taken during the folding of ribonuclease A. The curve gives the number of protected amide protons remaining after a 10-s pulse of exchange at pHs from 6.0 to 9.5, at 10 degrees C. Amide proton exchange is base catalyzed, and the rate of exchange increases 3000-fold between pH 6.0 and pH 9.5. The pH at which exchange occurs depends on the degree of protection against exchange provided by structure. Pulse exchange curves have been measured for samples taken at three times during folding, and these are compared to the pulse exchange curves of N, the native protein, of U, the unfolded protein in 4 M guanidinium chloride, and of IN, the native-like intermediate obtained by the prefolding method of Schmid. The results are used to determine whether folding intermediates are present that can be distinguished from N and U and to measure the average degree of protection of the protected protons in folding intermediates. The amide (peptide NH) protons of unfolded ribonuclease A were prelabeled with 3H by a previous procedure that labels only the slow-folding species. Folding was initiated at pH 4.0, 10 degrees C, where amide proton exchange is slower than the folding of the slow-folding species. Samples were taken at 0-, 10-, and 20-s folding, and their pH-pulse exchange curves were measured.(ABSTRACT TRUNCATED AT 250 WORDS)     

Exchange behavior of the H-bonded amide protons in the 3 to 13 helix of ribonuclease S

The preceding article shows that there are eight highly protected amide protons in the S-peptide moiety of RNAase S at pH 5, 0 degrees C. The residues with protected NH protons are 7 to 13, whose amide protons are H-bonded in the 3 to 13 alpha-helix, and Asp 14, whose NH proton is H-bonded to the CO group of Val47. We describe here the exchange behavior of these eight protected protons as a function of pH. Exchange rates of the individual NH protons are measured by 1H nuclear magnetic resonance in D2O. A procedure is used for specifically labeling with 1H only these eight NH protons. The resonance assignments of the eight protons are made chiefly by partial exchange, through correlating the resonance intensities in spectra taken when the peptide is bound and when it is dissociated from S-protein in 3.5 M-urea-d4, in D2O, pH 2.3, -4 degrees C. The two remaining assignments are made and some other assignments are checked by measurements of the nuclear Overhauser effect between adjacent NH protons of the alpha-helix. There is a transition in exchange behavior between pH 3, where the helix is weakly protected against exchange, and pH 5 where the helix is much more stable. At pH 3.1, 20 degrees C, exchange rates are uniform within the helix within a factor of two, after correction for different intrinsic exchange rates. The degree of protection within the helix is only 10 to 20-fold at this pH. At pH 5.1, 20 degrees C, the helix is more stable by two orders of magnitude and exchange occurs preferentially from the N-terminal end. At both pH values the NH proton of Asp 14, which is just outside the helix, is less protected by an order of magnitude than the adjacent NH protons inside the helix. Opening of the helix can be observed below pH 3.7 by changes in chemical shifts of the NH protons in the helix. At pH 2.4 the changes are 25% of those expected for complete opening. Helix opening is a fast reaction on the n.m.r. time scale (tau much less than 1 ms) unlike the generalized unfolding of RNAase S which is a slow reaction. Dissociation of S-peptide from S-protein in native RNAase S at pH 3.0 also is a slow reaction. Opening of the helix below pH 3.7 is a two-state reaction, as judged by comparing chemical shifts with exchange rates. The exchange rates at pH 3.1 are predicted correctly from the changes in chemical shift by assuming that helix opening is a two-state reaction. At pH values above 3.7, the nature of the helix opening reaction changes. These results indicate that at least one partially unfolded state of RNAase S is populated in the low pH unfolding transition.     

A pentapeptide model for an early folding step in the refolding of staphylococcal nuclease: The role of its turn propensity

Recently the folding of a staphylococcal nuclease (P117G) variant was examined with the hydrogen-deuterium (H-D) exchange technique. Many of the residues that showed significant protection are located in protection are located in β-sheet regions. About half the residues protected belong to an antiparallel β-hairpin structure (residues 21–35) in the native structure. The β-hairpin structure is formed by strands 2 and 3 of sheet 2 connected by the sequence²⁷ Y KGQP³¹ in a type I′ reverse turn conformation with a 4 → 1 hydrogen bonding between Q30 NH and Y27 C=O. We have targeted the conformational characterization of the peptide model Ac-YKGQP-NH₂ with ¹II two-dimensional nmr techniques in aqueous solution with a view to assessing its propensity to sample turn conformational forms and thus initiate the formation of β-hairpin structure. Based upon the observed dαn (i, i + 1), dαn (i, i + 3), and dnn (i, i + 1) nuclear Overhauser effect connectivities, temperature coefficients for amide protons and conformational analysis with quantum mechanical perturbative configuration interaction over localized orbitals method, we conclude that the model peptide samples turn conformational forms with reduced conformational entropy. We suggest that the turn can nucleate the formation of the β-hairpin structure in the refolding of nuclease. Observation of turn propensity for this sequence is consistent with the folding mechanism of the Greek key motif (present in Staphylococcal nuclease) proposed in the literature. © 1997 John Wiley & Sons, Inc.     

Conformations of proline residues in membrane environments

Although noted as hydrophilic residues with helix-breaking potential, proline residues are observed in putatively alpha-helical transmembrane (TM) segments of many channel-forming integral membrane proteins. In addition to the recognized property of X-Pro peptide bonds (where X = any amino acid) to occur in cis as well as trans isomeric states, the tertiary amide character of the X-Pro bond confers increased propensity for involvement of its carbonyl group in specific H-bonded structures (e.g., beta- and gamma-turns) and/or liganding interactions with positively charged species. To examine this latter situation in further detail, we identified Leu-Pro-Phe as a consensus sequence triad based on actual occurrences of intramembranous Pro residues in transport protein TM segments. Accordingly, we have undertaken the synthesis of hydrophobic peptides with potential membrane affinity, of which t-butyloxycarbonyl-L-Ala-L-Ala-L-Ala-L-Leu-L-Pro-L-Phe-OH (t-Boc-AAALPF-OH) is an initial compound. Partitioning of this peptide into model membrane environments composed of lipid micelles induces specific conformation(s) for the membrane-bound hexapeptide, as monitored by 75-MHz 13C-nmr spectral behavior of 13C-enriched Leu and Pro carbonyl carbons, and by 300-MHz 1H-nmr spectra of peptide alpha, beta, and aromatic protons. Data are interpreted in terms of an intramolecularly H-bonded inverse gamma-turn conformation in the membrane environment involving the Leu-Pro-Phe triad. The inherent structural instability of a Pro-containing segment in a TM helix due to the multiplicity of possible local conformations is discussed as a functional aspect of membrane-buried prolines in transport proteins.     

Isomerization of the Xaa-Pro peptide bond induced by ionic interactions of arginine

Inclusion of Arg or Pro residues in proteins and peptides has been proved to play an essential role in biochemical functions through ionic interactions, conformational transitions, and formation of turns as well. In this study we present the conformational properties of the Ac-Arg-Ala-Pro (1), Ac-Arg-Ala-Pro-NH₂ (2), Ac-Arg-Pro-Asp-NH₂ (3), and Ac-Arg-Pro-Asp (4) tripeptides, using ¹H-nmr spectroscopy and molecular dynamics. These peptides were modeled with the aim of studying the role of the Arg-guanidinium to carboxylate ionic interactions on the Xaa-Pro peptide bond isomerization. It was found with 1 and 4 that arginine preferentially interacts with the C-terminal carboxylate group, even though the β-carboxylate is also accessible. This tendency of the Arg moiety was found to induce the cis disposition of the Ala-Pro peptide bond in 1. It was also confirmed that the Arg…Asp side chain-side chain ionic interaction in 3 plays a key role in backbone folding and structural stabilization through a type I β-turn. The nmr pattern for 3 showed a remarkable similarity with that for various Arg-Tyr-Asp containing peptides, a sequence that is crucial for the adhesion properties of the Leishmania gp63 glycoprotein. © 1996 John Wiley & Sons, Inc.     

Nuclear magnetic resonance evidence for a structural intermediate at an early stage in the refolding of ribonuclease A

The kinetics of refolding of heat-unfolded ribonuclease A have been studied by Fourier transform proton nuclear magnetic resonance at 10 °C, pH 2. A single refolding reaction is observed: it corresponds to the slow-refolding reaction seen in stopped-flow studies of refolding at higher temperatures. There are two results of interest for the mechanism of protein folding. (1) A new resonance (X) is observed that shows the presence of a structural intermediate in refolding. (2) The α-helix close to the N-terminal end of ribonuclease A apparently forms rapidly when the unfolded protein is brought to refolding conditions.The folding intermediate has been studied by monitoring the C-2 protons of the four histidine residues. The intermediate contains one residue (X) in a partly folded environment and the other three residues in unfolded environments. The composite resonance (U) of these three protons at 10 °C agrees with the average chemical shift of the histidine residues in heat-unfolded ribonuclease A at high temperatures. During refolding at 10 °C, the resonance intensities of U and X disappear at the same rate that the spectrum of native ribonuclease A is regained.Partial deuteration experiments show that X is either histidine 12 or 119. Comparative studies of the amino-terminal fragment 1–20 of ribonuclease A indicate that X is histidine 12. The appearance of structure in this peptide can be followed by temperature-dependent changes in the chemical shift of histidine 12. At 10 °C the chemical shifts of histidine 12 and X agree closely. These results are consistent with the circular dichroism study of peptide 1–13 by Brown &; Klec (1971), who concluded that helix formation occurs at low temperatures.     

The α-Helix of Ribonuclease T1as an Independent Stability Unit: Direct Comparison of Peptide and Protein Stability

Measurements of the change in conformational stability, Δ(ΔG), upon mutation of two acidic residues at the C terminus of the helix of ribonuclease T₁have recently been reported. Here, we investigate peptides based on the sequence of the helix with the same mutations: Glu28 replaced with Gln, Asp29 replaced with Asn, and the double mutant. In addition, the mutant Lys25 to Gln was studied. Changes in helix content of the peptides with pH confirm the conclusion found in the intact protein, that the charged forms of the acidic residues destabilize the protein by destabilizing the helix. The pH-dependence of the change in confor mational free energy for the peptides and mutant proteins show fair correspondence for D29N and the double mutant. The mutants E28Q and K25Q, on the other hand, give striking agreement between the protein and peptide systems. This agreement suggests that the helix of ribonuclease T₁behaves as an independently stabilized structural unit of the intact protein and that stabilization of the helical form of the peptide is mirrored in the protein.     

Use of amide 1H-nmr titration shifts for studies of polypeptide conformation

This paper shows that backbone amide proton titration shifts in polypeptide chains are a very sensitive manifestation of intramolecular hydrogen bonding between carboxylate groups and backbone amide protons. The population of specific hydrogen-bonded structures in the ensemble of species that constitutes the conformation of a flexible nonglobular linear peptide can be determined from the extent of the titration shifts. As an illustration, an investigation of the molecular conformation of the linear peptide H-Gly-Gly-L -Glu-L -Ala-OH is described. The proposed use of amide proton titration shifts for investigating polypeptide conformation is based on 360-MHz ¹H-nmr studies of selected linear oligopeptides in H₂O solutions. It was found that only a very limited number of amide protons in a polypeptide chain show sizable intrinsic intration shifts arising from through-bond interactions with ionizable groups. These are the amide proton of the C-terminal amino acid residue, the amide protons of Asp and the residues following Asp, and possibly the amide proton of the residue next to the N-terminus. Since the intrinsic titration shifts are upfield, the downfield titration shifts arising from conformation-dependent through-space interactions, in particular hydrogen bonding between the amide protons and carboxylate groups, can readily be identified.     

Sequence and conformational effects on imino proton exchange in A.T- and A.U-containing DNA and RNA duplexes

¹H-nmr relaxation has been used to study the effect of sequence and conformation on imino proton exchange in adenine–thymine (A · T) and adenine–uracil (A · U) containing DNA and RNA duplexes. At low temperature, relaxation is caused by dipolar interactions between the imino and the adenine amino and AH2 protons, and at higher temperature, by exchange with the solvent protons. Although room temperature exchange rates vary between 3 and 12s^?1, the exchange activation energies (E_α) are insensitive to changes in the duplex sequence (alternating vs homopolymer duplexes), the conformation (B-form DNA vs A-form RNA), and the identity of the pyrimidine base (thymine vs uracil). The average value of the activation energy for the five duplexes studied, poly[d(A-T)], poly[d(A) · d(T)], poly[d(A-U)], Poly[d(A) · d(U)], and poly[r(A) · r(U)], was 16.8 ± 1.3 kcal/mol. In addition, we find that the average E_α for the A.T base pairs in a 43-base-pair restriction fragment is 16.4 ± 1.0 kcal/mol. This result is to be contrasted with the observation that the E_α of cytosine-containing duplexes depends on the sequence, conformation, and substituent groups on the purine and pyrimidine bases. Taken together, the data indicate that there is a common low-energy pathway for the escape of the thymine (uracil) imino protons from the double helix. The absolute values of the exchange rates in the simple sequence polymers are typically 3–10 times faster than in DNAs containing both A · T and G · C base pairs.     

Conformation and interactions of uteroglobin fragments 4–14 and 49–65 in aqueous solution containing surfactant micelles

The conformation of two fragments of rabbit uteroglobin is described. The peptides are PRFAHVIENLL and PQTTRENIMKLTEKIVK, corresponding to helices I and IV in the crystal structure. CD shows that both peptides interact with sodium dodecyl sulfate (SDS) micelles and change their conformation to an α-helix. The helical content estimated from the CD band at 222 nm is about 40% in each peptide. Surface tension measurements show that both peptides lower the critical micellar concentration (cmc) of SDS, with a more dramatic effect in the case of helix I. This peptide by itself acts as a surfactant, and is able to interact with SDS even below the observed cmc, forming β aggregates. Proton magnetic resonance (¹H-nmr) suggests that flexible helices are present. The longest helical stretches compatible with ¹H-nmr data extend from Phe⁶ to Leu¹⁴ for helix I and from Arg⁵³ to Ile⁶³ for helix IV. © 1993 John Wiley & Sons, Inc.     

Helicity of short E-R/K peptides

Understanding the secondary structure of peptides is important in protein folding, enzyme function, and peptide‐based drug design. Previous studies of synthetic Ala‐based peptides (>12 a.a.) have demonstrated the role for charged side chain interactions involving Glu/Lys or Glu/Arg spaced three (i, i + 3) or four (i, i + 4) residues apart. The secondary structure of short peptides (<9 a.a.), however, has not been investigated. In this study, the effect of repetitive Glu/Lys or Glu/Arg side chain interactions, giving rise to E‐R/K helices, on the helicity of short peptides was examined using circular dichroism. Short E‐R/K–based peptides show significant helix content. Peptides containing one or more E‐R interactions display greater helicity than those with similar E‐K interactions. Significant helicity is achieved in Arg‐based E‐R/K peptides eight, six, and five amino acids long. In these short peptides, each additional i + 3 and i + 4 salt bridge has substantial contribution to fractional helix content. The E‐R/K peptides exhibit a strongly linear melt curve indicative of noncooperative folding. The significant helicity of these short peptides with predictable dependence on number, position, and type of side chain interactions makes them an important consideration in peptide design.