Effect of pH, urea, peptide length, and neighboring amino acids on alanine alpha-proton random coil chemical shifts

Accurate random coil alpha-proton chemical shift values are essential for precise protein structure analysis using chemical shift index (CSI) calculations. The current study determines the chemical shift effects of pH, urea, peptide length and neighboring amino acids on the alpha-proton of Ala using model peptides of the general sequence GnXaaAYaaGn, where Xaa and Yaa are Leu, Val, Phe, Tyr, His, Trp or Pro, and n = 1-3. Changes in pH (2-6), urea (0-1M), and peptide length (n = 1-3) had no effect on Ala alpha-proton chemical shifts. Denaturing concentrations of urea (8M) caused significant downfield shifts (0.10 +/- 0.01 ppm) relative to an external DSS reference. Neighboring aliphatic residues (Leu, Val) had no effect, whereas aromatic amino acids (Phe, Tyr, His and Trp) and Pro caused significant shifts in the alanine alpha-proton, with the extent of the shifts dependent on the nature and position of the amino acid. Smaller aromatic residues (Phe, Tyr, His) caused larger shift effects when present in the C-terminal position (approximately 0.10 vs. 0.05 ppm N-terminal), and the larger aromatic tryptophan caused greater effects in the N-terminal position (0.15 ppm vs. 0.10 C-terminal). Proline affected both significant upfield (0.06 ppm, N-terminal) and downfield (0.25 ppm, C-terminal) chemical shifts. These new Ala correction factors detail the magnitude and range of variation in environmental chemical shift effects, in addition to providing insight into the molecular level interactions that govern protein folding.     

Quantum mechanical calculations and experimental measurement of N-terminal charge effects on 1HN and 1HCα chemical shifts in peptides

Nuclear magnetic resonance spectroscopists are increasingly utilizing chemical shifts to characterize the secondary structure of proteins. The present study addresses the effects that the positively charged amino group at the N-terminus of a peptide has on ¹HN and ¹HCα chemical shifts along the chain. This information is necessary for interpreting chemical shift data for proteins and/or for peptides that are used as models for protein structure. The chemical shifts for the ¹H resonances of four peptides that differ only in the location of their N-terminii are assigned using two-dimensional nmr spectroscopy. The peptides have sequences derived from the β subunit of the glycoprotein hormone human chorionic gonadotropin (hCG-β). Comparison of the ¹HN and the ¹HCα chemical shifts for residues common to all four peptides reveals downfield shifts for ¹HN and the ¹HCα resonances within three residues of the N-terminus compared with chemical shifts in the interior of the peptide. The magnitude of the downfield shift is larger for resonances nearer the N-terminus. Quantum mechanical calculations of the ¹HN and ¹HCα chemical shifts in peptides constructed with six alanine units also predict a significant terminus effect. The calculations agree both qualitatively and quantitatively with the experimental data. The inductive nature of the end effect is confirmed in the calculations by Mulliken population analysis. End effects should be taken into account in determining protein secondary structures from chemical shifts. © 1996 John Wiley & Sons, Inc.     

Nuclear magnetic spectra of self complementary decanucleotides in solution; base sequence effect on the chemical shifts of nonexchangeable protons

The aim of this study was to attempt to determine the extent to which the chemical shifts of the nonexchangeable base protons of a DNA helix depend upon the base sequence. We measured the proton NMR spectra of twelve decadeoxynucleotides in order to carry out a "statistical" treatment. In the helices, the chemical shifts were found to be determined within +/- 0.04 ppm, largely by the nearest neighbor residues on the 5'-side, and to a smaller extent by the residue on the 3'-side. The theoretical chemical shift calculations reproduced very well the polymerization shifts measured for H2 protons of adenosines if the electrostatic field effect was taken into account. A fair agreement was also obtained for H8 protons of the adenosine and guanosine residues. However, theory underestimates the polarization effects of the base protons of cytidine. This discrepancy suggests that the conformation of this residue is different in the mononucleotides relative to double helices.     

Secondary-structure dependent chemical shifts in proteins

Chemical shift data have been collected on eight proteins that have the same conformation in solution as in their crystal structures. Ring-current shifts have been calculated and subtracted from the exerimentally measured shifts, to leave shifts that depend only on local conformation. Overall, the shifts show an approximately normal distribution with no appreciable skewness, thus confirming that ring-current shifts have the overall effect of skewing the distribution to high field. In helices, NH and C(alpha)H have a high significant tendency to resonate to high field, whereas they resonate to low field in beta-sheets. Side-chain protons resonate slightly to high field in beta-sheets. Chemical shift distributions are narrowest for side-chain protons, and widest for amide protons. When only slowly exchanging amide protons are considered, the high field shift for amide protons in helices is more pronounced, but there is only a small difference in sheets. C(alpha)H signals at the N-terminal end of helices tend to resonate to higher field than those at the C-terminal end, whereas for NH signals it is the C-terminal end that resonates to higher field. There is no significant effect of position within the helix on side-chain signals, implying that the helix dipole has little effect on shifts within the helix.     

Imino 1H- and 31P-NMR analysis of the interaction of propidium and ethidium with DNA

At low temperature and low salt concentration, both imino proton and ³¹p-nmr spectra of DNA complexes with the intercalators ethidium and propidium are in the slow-exchange region. Increasing temperature and/or increasing salt concentration results in an increase in the site exchange rate. Ring-current effects from the intercalated phenanthridinium ring of ethidium and propidium cause upfield shifts of the imino protons of A · T and G · C base pairs, which are quite similar for the two intercalators. The limiting induced chemical shifts for propidium and ethidium at saturation of DNA binding sites are approximately 0.9 ppm for A · T and 1.1 ppm for G · C base pairs. The similarity of the shifts for ethidium and propidium, in both the slow- and fast-exchange regions over the entire titration of DNA, shows that a binding model for propidium with neighbor-exclusion binding and negative ligand cooperativity is correct. The fact that a unique chemical shift is obtained for imino protons at intercalated sites over the entire titration and that no unshifted imino proton peaks remain at saturation binding of ethidium and propidium supports a neighbor-exclusion binding model with intercalators bound at alternating sites rather than in clusters on the double helix. Addition of ethidium and propidium to DNA results in downfield shifts in ³¹P-nmr spectra. At saturation ratios of intercalator to DNA base pairs in the titration, a downfield shoulder (approximately ?2.7 ppm) is apparent, which accounts for approximately 15% of the spectral area. The main peak is at ?3.9 to ?4.0 ppm relative to ?4.35 in uncomplexed DNA. The simplest neighbor-binding model predicts a downfield peak with approximately 50% of the spectral area and an upfield peak, near the chemical shift for uncomplexed DNA, with 50% of the area. This is definitely not the case with these intercalators. The observed chemical shifts and areas for the DNA complexes can be explained by models, for example, that involve spreading the intercalation-induced unwinding of the double helix over several base pairs and/or a DNA sequence- and conformation-dependent heterogeneity in intercalation-induced chemical shifts and resulting exchange rates.     

NMR studies of echinomycin bisintercalation complexes with d(A1-C2-G3-T4) and d(T1-C2-G3-A4) duplexes in aqueous solution: sequence-dependent formation of Hoogsteen A1.T4 and Watson--Crick T1.A4 base pairs flanking the bisintercalation site

We report on two-dimensional proton NMR studies of echinomycin complexes with the self-complementary d(A1-C2-G3-T4) and d(T1-C2-G3-A4) duplexes in aqueous solution. The exchangeable and nonexchangeable antibiotic and nucleic acid protons in the 1 echinomycin per tetranucleotide duplex complexes have been assigned from analyses of scalar coupling and distance connectivities in two-dimensional data sets recorded in H2O and D2O solution. An analysis of the intermolecular NOE patterns for both complexes combined with large upfield imino proton and large downfield phosphorus complexation chemical shift changes demonstrates that the two quinoxaline chromophores of echinomycin bisintercalate into the minor groove surrounding the dC-dG step of each tetranucleotide duplex. Further, the quinoxaline rings selectively stack between A1 and C2 bases in the d(ACGT) complex and between T1 and C2 bases in the d(TCGA) complex. The intermolecular NOE patterns and the base and sugar proton chemical shifts for residues C2 and G3 are virtually identical for the d(ACGT) and d(TCGA) complexes. A change in sugar pucker from the C2'-endo range to the C3'-endo range is detected at C2 on formation of the d(ACGT) and d(TCGA) complexes. In addition, the sugar ring protons of C2 exhibit upfield shifts and a large 1 ppm separation between the H2' and H2" protons for both complexes. The L-Ala amide protons undergo large downfield complexation shifts consistent with their participation in intermolecular hydrogen bonds for both tetranucleotide complexes.(ABSTRACT TRUNCATED AT 250 WORDS)     

cis-diamminedichloroplatinum(II) induced distortion of a single and double stranded deoxydecanucleosidenonaphosphate studied by nuclear magnetic resonance

The structural distortion of a single- and a double-stranded decadeoxynucleotide upon binding of cis-PtCl2(NH3)2 was studied by 1H-NMR. After selective platination of d(T-C-T-C-G-G-T-C-T-C) (I) at the central d(-GpG-) site (resulting in I-Pt), several non-exchangeable base protons as well as H1', H2', H2" and H3' protons could be assigned by means of conventional NMR double-resonance techniques. Addition of the complementary decamer strand to I and I-Pt yielded the double-stranded III and III-Pt, respectively. All non-exchangeable base, H1', and most of the H2' and H2" protons in the two double stranded compounds could be assigned using 2D-chemical shift correlation (COSY) and nuclear Overhauser enhancement (NOESY) techniques. The double stranded compound III appears to adopt a B-DNA like structure. Comparison of NOEs and proton-proton coupling constants in the d(-GpG-).cisPt part in I-Pt and III-Pt reveals that their structure displays large similarity. Significant chemical shift changes (i.e. larger than 0.1 ppm) between III and III-Pt are restricted to the central four base pairs. It follows that the outer three base pairs, located on either side of the central four base pairs in III-Pt are likely to adopt a regular B-DNA type helix. The observed large upfield and downfield chemical shifts in the d(-CpGpG-) part of III with respect to III-Pt can be rationalized by describing the distortion of the double helix as a kink. A discussion of the observed physical effects upon platination of a double-stranded oligonucleotide is presented.     

The application of 1H NMR chemical shift calculations to diastereotopic groups in proteins.

We have calculated chemical shifts for a range of diastereotopic protons in proteins (i.e. methylene protons, and the methyl groups of valine and leucine residues), using a recently optimised method for chemical shift calculation. The calculations are based on crystal structure coordinates, and have been compared with experimental stereospecific assignments. The results indicate that chemical shifts can be used to suggest stereospecific assignments with about 80% probability of being correct, in cases where both the experimental and the calculated chemical shift differences between a pair of diastereotopic protons are greater than 0.3 ppm. Inaccurate calculations are shown to be caused in most cases by differences between crystal and solution structures. Furthermore, chemical shift calculations based on NMR structures are shown to be capable of acting as a further constraint on structure, by limiting the range of side-chain conformations adopted in structures calculated from NMR data.     

Triple-resonance multidimensional NMR study of calmodulin complexed with the binding domain of skeletal muscle myosin light-chain kinase: indication of a conformational change in the central helix

Heteronuclear 3D and 4D NMR experiments have been used to obtain 1H, 13C, and 15N backbone chemical shift assignments in Ca(2+)-loaded calmodulin complexed with a 26-residue synthetic peptide (M13) corresponding to the calmodulin-binding domain (residues 577-602) of rabbit skeletal muscle myosin light-chain kinase. Comparison of the chemical shift values with those observed in peptide-free calmodulin [Ikura, M., Kay, L. E., & Bax, A. (1990) Biochemistry 29, 4659-4667] shows that binding of M13 peptide induces substantial chemical shift changes that are not localized in one particular region of the protein. The largest changes are found in the first helix of the Ca(2+)-binding site I (E11-E14), the N-terminal portion of the central helix (M72-D78), and the second helix of the Ca(2+)-binding site IV (F141-M145). Analysis of backbone NOE connectivities indicates a change from alpha-helical to an extended conformation for residues 75-77 upon complexation with M13. This conformational change is supported by upfield changes in the C alpha and carbonyl chemical shifts of these residues relative to M13-free calmodulin and by hydrogen-exchange experiments that indicate that the amide protons of residues 75-82 are in fast exchange (kexch greater than 10 s-1 at pH 7, 35 degrees C) with the solvent. No changes in secondary structure are observed for the first helix of site I or the C-terminal helix of site IV. Upon complexation with M13, a significant decrease in the amide exchange rate is observed for residues T110, L112, G113, and E114 at the end of the second helix of site III.     

Structural information from NMR secondary chemical shifts of peptide α C−H protons in proteins

The secondary chemical shift experienced by the¹H-NMR resonances of the α C?H protons in proteins can be correlated with their backbone torsional angles ψ, which dictate the orientation of the α C?H proton to the adjacent carbonyl group. It is shown that α C?H protons present in β-sheet regions experience downfield secondary shifts , whereas those in α-helix regions experience upfield secondary shifts. The predictive use of this correlation in assignment studies is illustrated for the calcium-binding protein paravalbumin, for which a crystal structure is available, and troponin C, for which no crystallographic data are available.     

Proton and phosphorus NMR studies of d-CpG(pCpG)n duplexes in solution. Helix-coil transition and complex formation with actinomycin-D.

The Watson–Crick imino and amino exchangeable protons, the nonexchangeable base and sugar protons, and the backbone phosphates for d-CpG(pCpG)_n, n = 1 and 2, have been monitored by high-resolution nmr spectroscopy in aqueous solution over the temperature range 0°–90°C. The temperature dependence of the chemical shifts of the tetramer and hexamer resonances is consistent with the formation of stable duplexes at low temperature in solution. Comparison of the spectral characteristics of the tetranucleotide with those of the hexanucleotide with temperature permits the differentiation and assignment of the cytosine proton resonances on base pairs located at the end of the helix from those in an interior position. There is fraying at the terminal base pairs in the tetranucleotide and hexanucleotide duplexes. The Watson–Crick ring imino protons exchange at a faster rate than the Watson–Crick side-chain amino protons, with exchange occurring by transient opening of the double helix. The structure of the d-CpG(pCpG)_n double helices has been probed by proton relaxation time measurements, sugar proton coupling constants, and the proton chemical shift changes associated with the helix–coil transition. The experimental data support a structural model in solution, which incorporates an anti conformation about the glycosyl bonds, C(3) exo sugar ring pucker, and base overlap geometries similar to the B-DNA helix. Rotational correlation times of 1.7 and 0.9 × 10^?9 sec have been computed for the hexanucleotide and tetranucleotide duplexes in 0.1 M salt, D₂O, pH 6.25 at 27°C. The well-resolved ³¹P resonances for the internucleotide phosphates of the tetramer and hexamer sequences at superconducting fields shift upfield by 0.2–0.5 ppm on helix formation. These shifts reflect a conformational change about the ω,ω′ phosphodiester bonds from gauche-gauche in the duplex structure to a distribution of gauche-trans states in the coil structure. Significant differences are observed in the transition width and midpoint of the chemical shift versus temperature profiles plotted in differentiated form for the various base and sugar proton and internucleotide phosphorous resonances monitoring the d-CpG(pCpG)_n helix–coil transition. The twofold symmetry of the d-CpGpCpG duplex is removed on complex formation with the antibiotic actinomycin-D. Two phosphorous resonances are shifted downfield by ～2.6 ppm and ～1.6 ppm on formation of the 1:2 Act-D:d-CpGpCpG complex in solution. Model studies on binding of the antibiotic to dinucleotides of varying sequence indicate that intercalation of the actinomycin-D occurs at the GpC site in the d-CpGpCpG duplex and that the magnitude of the downfield shifts reflects strain at the O-P-O backbone angles and hydrogen bonding between the phenoxazone and the phosphate oxygens. Actinomycin-D is known to bind to nucleic acids that exhibit a B-DNA conformation; this suggests that the d-CpG(pCpG)_n duplexes exhibit a B-DNA conformation in solution.     

Phosphorus-31 nuclear magnetic resonance of double- and triple-helical nucleic acids. Phosphorus-31 chemical shifts as a probe of phosphorus-oxygen ester bond torsional angles

The temperature dependence to the 31P NMR spectra of poly[d(GC)] . poly [d(GC)],d(GC)4, phenylalanine tRNA (yeast) and mixtures of poly(A) + oligo(U) is presented. The 31P NMR spectra of mixtures of complementary RNA and of the poly d(GC) self-complementary DNA provide torsional information on the phosphate ester conformation in the double, triple, and "Z" helix. The increasing downfield shift with temperature of the single-strand nucleic acids provides a measure of the change in the phosphate ester conformation in the single helix to coil conversion. A separate upfield peak (20-60% of the total phosphates) is observed at lower temperatures in the oligo(U) . poly(A) mixtures which is assigned to the double helix/triple helix. Proton NMR and UV spectra confirm the presence of the multistrand forms. The 31P chemical shift for the double helix/triple helix is 0.2-0.5 ppm upfield from the chemical shift for the single helix which in turn is 1.0 ppm upfield from the chemical shift for the random coil conformation.     

Relationship between nuclear magnetic resonance chemical shift and protein secondary structure

An analysis of the 1H nuclear magnetic resonance chemical shift assignments and secondary structure designations for over 70 proteins has revealed some very strong and unexpected relationships. Similar studies, performed on smaller databases, for 13C and 15N chemical shifts reveal equally strong correlations to protein secondary structure. Among the more interesting results to emerge from this work is the finding that all 20 naturally occurring amino acids experience a mean alpha-1H upfield shift of 0.39 parts per million (from the random coil value) when placed in a helical configuration. In a like manner, the alpha-1H chemical shift is found to move downfield by an average of 0.37 parts per million when the residue is placed in a beta-strand or extended configuration. Similar changes are also found for amide 1H, carbonyl 13C, alpha-13C and amide 15N chemical shifts. Other relationships between chemical shift and protein conformation are also uncovered; in particular, a correlation between helix dipole effects and amide proton chemical shifts as well as a relationship between alpha-proton chemical shifts and main-chain flexibility. Additionally, useful relationships between alpha-proton chemical shifts and backbone dihedral angles as well as correlations between amide proton chemical shifts and hydrogen bond effects are demonstrated.     

Ab-inito quantum mechanical calculations of NMR chemical shifts in nucleic acids constituents. II. Conformational dependence of the 1H and 13C chemical shifts in the ribose

The magnetic shielding constant of the different 13C and 1H nuclei of a deoxyribose are calculated for the C2' endo and C3' endo puckerings of the furanose ring as a function of the conformation about the C4'C5' bond. For the carbons the calculated variations are of several ppm, the C3' endo puckering corresponding in most cases to a larger shielding than the C2' endo one. For the protons the calculated variations of chemical shifts are all smaller than 1.3 ppm, that is of the order of magnitude of the variation of the geometrical shielding produced on these protons by the other units of a DNA double helix, with a change of the overall structure of the helix. The computations carried out on the deoxyribose-3' and 5' phosphates for several conformations of the phosphate group tend to show that the changes of conformation of the charged group of atoms produce chemical shift variations smaller than the two conformational parameters of the deoxyribose itself. The calculations carried out for a ribose do give the general features of the differences between the carbon and proton spectra of deoxynucleosides and nucleosides. The comparison of the measured and calculated phosphorylation shifts tend to show that the counterion contributes significantly, for some nuclei of the deoxyribose, to the shifts measured. The calculated magnitude of this polarization effect on carbon shifts suggests a tentative qualitative interpretation of carbon spectra of the ribose part of DNA double helices.     

NMR structural and dynamic characterization of the acid-unfolded state of apomyoglobin provides insights into the early events in protein folding

Apomyoglobin forms a denatured state under low-salt conditions at pH 2.3. The conformational propensities and polypeptide backbone dynamics of this state have been characterized by NMR. Nearly complete backbone and some side chain resonance assignments have been obtained, using a triple-resonance assignment strategy tailored to low protein concentration (0.2 mM) and poor chemical shift dispersion. An estimate of the population and location of residual secondary structure has been made by examining deviations of (13)C(alpha), (13)CO, and (1)H(alpha) chemical shifts from random coil values, scalar (3)J(HN,H)(alpha) coupling constants and (1)H-(1)H NOEs. Chemical shifts constitute a highly reliable indicator of secondary structural preferences, provided the appropriate random coil chemical shift references are used, but in the case of acid-unfolded apomyoglobin, (3)J(HN,H)(alpha) coupling constants are poor diagnostics of secondary structure formation. Substantial populations of helical structure, in dynamic equilibrium with unfolded states, are formed in regions corresponding to the A and H helices of the folded protein. In addition, the deviation of the chemical shifts from random coil values indicates the presence of helical structure encompassing the D helix and extending into the first turn of the E helix. The polypeptide backbone dynamics of acid-unfolded apomyoglobin have been investigated using reduced spectral density function analysis of (15)N relaxation data. The spectral density J(omega(N)) is particularly sensitive to variations in backbone fluctuations on the picosecond to nanosecond time scale. The central region of the polypeptide spanning the C-terminal half of the E helix, the EF turn, and the F helix behaves as a free-flight random coil chain, but there is evidence from J(omega(N)) of restricted motions on the picosecond to nanosecond time scale in the A and H helix regions where there is a propensity to populate helical secondary structure in the acid-unfolded state. Backbone fluctuations are also restricted in parts of the B and G helices due to formation of local hydrophobic clusters. Regions of restricted backbone flexibility are generally associated with large buried surface area. A significant increase in J(0) is observed for the NH resonances of some residues located in the A and G helices of the folded protein and is associated with fluctuations on a microsecond to millisecond time scale that probably arise from transient contacts between these distant regions of the polypeptide chain. Our results indicate that the equilibrium unfolded state of apomyoglobin formed at pH 2.3 is an excellent model for the events that are expected to occur in the earliest stages of protein folding, providing insights into the regions of the polypeptide that spontaneously undergo local hydrophobic collapse and sample nativelike secondary structure.     

Proton NMR study of the B----Z transition of d(CGm5CG)2 and d(CGm5CGCG)2: theory and experiment.

The magnetic shielding produced by the double helix in a B-DNA and a Z-DNA conformation is calculated for each non exchangeable proton of the oligodeoxynucleotides d(CGm5CG)2 and d(CGm5CGCG)2. The differences between the values obtained for the two helical forms are in good agreement with the variations of chemical shift measured when the salt concentration of the solution is changed from 0.1 M to 2 or 4 M. The analysis of the theoretical chemical shift variations shows that the large upfield shift observed for some of the protons of the cytidine residues is due to the sum of the ring current and local magnetic anisotropy effects of the guanines of the two nearest neighbours residues.     

Hydrogen-1 nuclear magnetic resonance investigation of high-potential iron-sulfur proteins from Ectothiorhodospira halophila and Ectothiorhodospira vacuolata: a comparative study of hyperfine-shifted resonances

Proton NMR spectra of the oxidized and reduced forms of high-potential iron-sulfur proteins (HiPIPs) were recorded at 200 MHz. The proteins studied were the HiPIPs I and II from Ectothiorhodospira halophila and Ectothiorhodospira vacuolata. Hyperfine-shifted peaks in spectra of the oxidized proteins were assigned to some of the protons of the cysteinyl ligands and aromatic residues at the active site on the basis of their chemical shifts, longitudinal relaxation times, and temperature-dependent behavior. The cysteinyl C beta-H protons were found to resonate downfield (about 100 ppm) and the C alpha-H protons upfield (about-25 ppm). This hyperfine shift pattern is consistent with the observed isotropic shift being contact in origin; it probably results from a pi-spin-transfer mechanism. The large magnitudes of the chemical shifts of peaks assigned to aromatic residues suggest that these residues interact with the iron-sulfur cluster via pi-pi overlap. Some of the hyperfine-shifted peaks observed in water were found to disappear in 2H2O solution. Such resonances probably arise from exchange-labile hydrogens of amino acid residues directly hydrogen bonded to the iron-sulfur cluster. In the case of HiPIPs I and II from E. vacuolata, whose spectra are similar except for the number of such peaks, the relative number of hydrogen bonds inferred to be present in the oxidized and reduced proteins qualitatively explains the difference between their midpoint redox potentials. On the other hand, for E. halophila HiPIPs I and II, consideration of the inferred number of hydrogen bonds alone fails to predict the sign of the difference between their midpoint redox potentials.(ABSTRACT TRUNCATED AT 250 WORDS)     

1H- and 31P-NMR studies of ditercalinium binding to a d(GCGC)2 and d(CCTATAGG)2 minihelices: a sequence specificity study

The structures of the complexes formed in aqueous solution between ditercalinium, a bis-intercalating drug, and both the self-complementary tetranucleotide d(GCGC)2 and octanucleotide d(CCTATAGG)2, have been investigated by 400-MHz 1H-nmr and 162-MHz 31P-nmr. All the nonexchangeable protons, as well as the exchangeable imino protons and the phosphorus signals, have been assigned. Both oligonucleotides have been shown to adopt a right-handed B-DNA type structure. The addition of ditercalinium to the oligonucleotides lead to the formation of complexes in slow exchange at the nmr time scale with the free helices. At all drug-to-helix ratios studied, the ditercalinium was found in the bound form, whereas free and complexed oligonucleotides were in slow exchange, allowing resonance assignments through two-dimensional chemical exchange experiments. for d(GCGC)2 the strong upfield shifts induced on all aromatic protons of both the bases and the drug by complexation with ditercalinium suggest an interaction by intercalation of the two rings. However, the loss of twofold symmetry upon binding, as well as the chemical shift variation of the drug proton signals of one of the chromophores with temperature and concentration, favor a model in which the drug-nucleotide complexes have one ring of the drug intercalated and the other stacked on top of the external base pair. The intermolecular contacts between drug protons and nucleotide protons give a defined geometry for complexation that is consistent with the proposed model. In contrast, with d(CCTATAGG)2 several drug-nucleotide complexes were formed and a large increase in line broadening was observed at high drug-to-DNA ratios, precluding a detailed analysis of these complexes. However, the large upfield shift in the imino proton resonances together with the shielding of the ditercalinium ring protons favor a model with bis-intercalation of ditercalinium. This model is supported by the downfield shift of at least 4 out of 14 phosphorus signals. The results are compared with those obtained on ditercalinium binding to the homologous sequences d(CGCG)2 and d(TTCGCGAA)2, and discussed in terms of sequence specificity.     

Periodicity of amide proton exchange rates in a coiled-coil leucine zipper peptide.

The two-stranded coiled-coil motif, which includes leucine zippers, is a simple protein structure that is well suited for studies of helix-helix interactions. The interaction between helices in a coiled coil involves packing of "knobs" into "holes", as predicted by Crick in 1953 and confirmed recently by X-ray crystallography for the GCN4 leucine zipper [O'Shea, E.K., Klemm, J.D., Kim, P.S., & Alber, T. (1991) Science 254, 539]. A striking periodicity, extending over six helical turns, is observed in the rates of hydrogen-deuterium exchange for amide protons in a peptide corresponding to the leucine zipper of GCN4. Protons at the hydrophobic interface show the most protection from exchange. The NMR chemical shifts of amide protons in the helices also show a pronounced periodicity which predicts a short H-bond followed by a long H-bond every seven residues. This variation was anticipated in 1953 by Pauling and is sufficient to give rise to a local left-handed superhelical twist characteristic of coiled coils. The amide protons that lie at the base of the "hole" in the "knobs-into-holes" packing show slow amide proton exchange rates and are predicted to have short H-bond lengths. These results suggest that tertiary interactions can lead to highly localized, but substantial, differences in stability and dynamics within a secondary structure element and emphasize the dominant nature of packing interactions in determining protein structure.     

Identification of N-terminal helix capping boxes by means of 13C chemical shifts

Summary We have examined the ¹³C and ¹³C chemical shifts of a number of proteins and found that their values at the N-terminal end of a helix provide a good predictor for the presence of a capping box. A capping box consists of a hydrogen-bonded cycle of four amino acids in which the side chain of the N-cap residue forms a hydrogen bond with the backbone amide of the N3 residue, whose side chain in turn may accept a hydrogen bond from the amide of the N-cap residue. The N-cap residue exhibits characteristic values for its backbone torsion angles, with and clustering around 94±15° and 167±5°, respectively. This is manifested by a 1–2 ppm upfield shift of the ¹³C resonance and a 1–4 ppm downfield shift of the ¹³C resonance, relative to their random coil values, and is mainly associated with the unusually large value of . The residues following the N-cap residue exhibit downfield shifts of 1–3 ppm for the ¹³C resonances and small upfield shifts for the ¹³C ones, typical of an -helix.