Sequence Specific Molecular Recognition and Binding of a Monocationic Bis-Imidazole Lexitropsin to the Decadeoxyribonucleotide d-[(GATCCGTATG) (CATACGGATC)]: Structural and Dynamic Aspects of Intermolecular Exchange Studied by 1H-NMR

Abstract

The non-exchangeable and imino proton NMR resonances of the non self-complementary decadeoxyribonucleotide d-[(GATCCGTATG) · (GATACGGATC)] as well as those of the 1:1 complex of the monocatonic bis-imidazole lexitropsin 1 to this sequence have been assigned by using a combination of NOE difference, COSY and NOESY techniques. Confirmation of complete annealing of the two non self-complementary decamer strands to give the duplex decadeoxyribonucleotide is obtained by the detection of ten imino protons. It is established that the sugar-base orientations of all the bases in the duplex decamer are anti. From NOE studies, it is concluded that the duplex oligomer is right-handed and adopts a conformation in solution that belongs to the B family. A population analysis reveals that the sugar moieties exist predominantly in the S-form (2′-endo-3′-exo). Addition of 1 to the DNA solution leads to doubling of the resonances for CH6(4,5), GH8(6), TH6(7) and T-CH₃(7). The base, anomeric H1′ and imino proton signals for the base sequence 5′-CCGT undergo the most marked drug-induced chemical shift changes. These results provide evidence that the lexitropsin is bound to the sequence 5′-CCGT in the minor groove of the DNA NOE measurements between the amide protons (NH1 and NH4) and the imino proton (IV and V) signals confirmed the location and orientation of 1 in the 1:1 complex, with the amino terminus oriented to C(4). The specific binding of 1 to the sequence 5′-CCGT-3′ deduced in this study is in agreement with the footprinting data obtained using the Hind III/Nci I fragment from pBR322 DNA [Kissinger et al. 1987 (13)]. Intramolecular NOEs observed between H4 and H9 of the lexitropsin suggest that the molecule is not planar, but subjected to propeller twisting, in both the free and bound forms. Furthermore, NOE measurements permit assignment of the DNA duplex in the 1:1 complex to the B-form, which is similar to that of the free DNA The [(T₇A₈T₉)· (A₁₂T₁₃A₁₄)] segment of the DNA shows better stacking, by propeller twisting, compared to the rest of the molecule in the free as well as the complex forms. The intermolecular rate of exchange of 1 between the equivalent 5′-CCGT sites, at a concentration of 12 mM, is estimated to be ～88s^?1 at 308°K with ΔG≠ of 63±5 K.J mol^?1.     

1H-nmr comparative studies of polynucleotides: Conformation and dynamic structure of polyribo(uridylic) and polyribo(cytidylic) acids in neutral solution

The conformation and the dynamic structure of single-stranded poly(U) and poly(C) in neutral aqueous solution have been investigated by ¹H-nmr at two different frequencies (90 and 250 MHz) and at various temperatures. Measurements of proton chemical shifts, coupling constants J_H-H, and proton relaxation times, T₁, T₂, versus temperature show a striking difference in conformation and in dynamic structure between the two polynucleotides studied. The temperature effect on δ and J_H-H is found to be substantial for poly(C) and insignificant for poly(U). The S conformer is favored in poly(U), whereas the N conformer strongly predominates in poly(C) (?90%), similar to the case for RNAs. These results suggest that single-stranded poly(C) probably possesses a helical or partial helical structure, whereas poly(U) shows a clear preference for the random coil, in agreement with the optical results. The local motions of the ribose and base were studied at various temperatures by measurements on the relaxation times at 90 and 250 MHz. For a given temperature between 22 and 72°C, the ratio T₁(90)/T₁(250) is practically the same for all poly(U) protons, indicating that in this temperature interval the ribose base unit of poly(U) undergoes an isotropic motion characterized by a single correlation time τ_c. Above 52°C, poly(C) exhibits a dynamic structure similar to poly(U). Below this temperature, poly(C) exists in an equilibrium between randomly coiled and single-stranded helix forms. This situation is characterized by a strong cross-relaxation effect and T₁ values corresponding to a relatively short apparent correlation time. An activation energy of 4 kcal/mol was determined for the motion of the ribose–base unit in both single-stranded polynucleotides.     

Residue Specific Ribose and Nucleobase Dynamics of the cUUCGg RNA Tetraloop Motif by MNMR 13C Relaxation

The dynamics of the nucleobase and the ribose moieties in a 14-nt RNA cUUCGg hairpin-loop uniformly labeled with ¹³C and ¹⁵N were studied by ¹³C spin relaxation experiments. R₁, R_1ρ and the ¹³C-{¹H} steady-state NOE of C₆ and C_1′ in pyrimidine and C₈ and C_1′ in purine residues were obtained at 298 K. The relaxation data were analyzed by the model-free formalism to yield dynamic information on timescales of pico-, nano- and milli-seconds. An axially symmetric diffusion tensor with an overall rotational correlation time τ_c of 2.31±0.13 ns and an axial ratio of 1.35±0.02 were determined. Both findings are in agreement with hydrodynamic calculations. For the nucleobase carbons, the validity of different reported ¹³C chemical shift anisotropy values (Stueber, D. and Grant, D. M., 2002 J. Am. Chem. Soc. 124, 10539–10551; Fiala et al., 2000 J. Biomol. NMR 16, 291–302; Sitkoff, D. and Case, D. A., 1998 Prog. NMR Spectroscopy 32, 165–190) is discussed. The resulting dynamics are in agreement with the structural features of the cUUCGg motif in that all residues are mostly rigid (0.82 < S² < 0.96) in both the nucleobase and the ribose moiety except for the nucleobase of U7, which is protruding into solution (S² = 0.76). In general, ribose mobility follows nucleobase dynamics, but is less pronounced. Nucleobase dynamics resulting from the analysis of ¹³C relaxation rates were found to be in agreement with ¹⁵N relaxation data derived dynamic information (Akke et al., 1997 RNA 3, 702–709). Electronic supplementary material Electronic supplementary material is available for this article at and accessible for authorised users.     

High resolution nuclear magnetic resonance spectroscopy of glycosphingolipids. I: 360 MHz 1H and 90.5 MHz 13C NMR analysis of galactosylceramides

The high resolution ¹H and ¹³C nuclear magnetic resonance (NMR) spectra of galactosylceramides containing n-fatty acids and α-hydroxy fatty acids were recorded in dimethylsulfoxide solution with and without addition of D₂O. From the coupling constants of the sugar ring protons, a ⁴C₁ conformation can be deduced. In contrast to the conformation in aqueous solution, the C⁶ hydroxymethylene group is freely rotating around the C⁶C⁵ bond. In the ceramide residue all signals produced by protons linked to carbons bearing electronegative substituents could be attributed. The large difference in coupling constants of the methylene protons of C^1′ to the C^2′ methine proton of the sphingosine indicates a restricted rotation around the C^1′C^2′ bond. The assignments of the hydroxy and amino protons follow from the decoupling of the corresponding methine protons.     

Syn–anti equilibrium of purine bases in dinucleoside monophosphates as studied by proton longitudinal relaxation

The preferential orientations of the purine bases in dinucleoside monophosphates such as ApA, ApG, and GpA in 10^?2M neutral aqueous solutions have been investigated by proton relaxation at 250 MHz. These orientations are deduced from computer simulations of the magnetization recovery curves following a 180° nonselective pulse. The distances between the H(8) proton of a base and the ribose ring protons which are used in these calculations are obtained by minimization as a function of the glycosyl torsion angle ? of the standard deviation between the isotropic reorientation correlation times τ_R derived from the relaxation rates of these protons. The average H(1′) – H(8) distance obtained by this procedure may be readily verified from the reduction of the H(1′) relaxation rate when H(8) is substituted by a deuteron. The limits of validity of the assumption of a single correlation time τ_R governing the proton relaxation have been estimated, taking into account several possible internal motions, e.g., the rotation of the base, of the methylene exocyclic group and the N ? S interconversion of the ribose ring. For 10^?10 < τ_R < 2 × 10^?10 sec, it appears that the influence of these motions on the proton relaxation becomes perceptible when the jump rates among equilibrium positions exceed ca. 10⁹ sec^?1. The whole of the experimental results show that for the ribose ring N conformer, the orientation of the bases is found in the ranges 60° < ? < 80° (syn) and 180° < ? < 210° (anti). For ribose S conformer, it is observed that this orientation is mainly syn with 5° < ? < 90°. The average H(1′) – H(8) distance provides semiquantitative information on the overall syn or anti orientations of the base in each nucleoside moiety. At 298 K the population of the anti conformer is found to increase in the order A- pG < Ap -G ～ Gp -A < Ap -A < A-pA < G-pA . A more detailed analysis of relaxation data shows that the maximum possible fraction of the stacked form of dinucleotides, due to the occurrence of N-anti conformers in both nucleoside moieties, is in the order ApG < GpA < ApA, in agreement with previous works, with however smaller values. Lastly the deuteron linewidth in position 8 of the bases indicates a syn–anti transition rate of the order of 10⁹ sec^?1 at room temperature, without noticeable effects therefore on the proton relaxation.     

High resolution nuclear magnetic resonance studies of nigeran

Polymer motion in solution can be studied by ¹³CNMR relaxation methods, which provide information about the correlation time for C-H vectors. ¹³C-Relaxation and Nuclear Overhauser Enhancement (NOE) data may frequently be combined to determine the dipole-dipole relaxation contribution. An alternative method is proposed based on a comparison of the proton spin-lattice relaxation rates of the centre proton resonances of an unlabelled molecule with the relaxation rates of the ¹³C satellites (from ¹³C labelled molecules).Selectively labelled nigeran which is an alternating $\text{1 → 3 and 1 → 4 α-}\text{d}\text{-glucan}$ has been investigated. The discussion in terms of the occurrence of different motions for each of the two units of the polymer requires an unambiguous assignment of the two anomeric carbons. For this reason a detailed assignment of the ¹H and ¹³C Nuclear Magnetic Resonance (NMR) spectra of nigeran in dimethylsulphoxide-d₆ is described, based on T₁ and NOE measurements in addition to selective homonuclear and heteronuclear spin decoupling experiments. These values are correlated with a conformation estimated by HSEA hard-spheres calculation. The measurements of the relaxation parameters for labelled and unlabelled compounds which provide an alternative determination of the ¹³C-¹H dipole-dipole relaxation contribution in a macromolecule agree well with ¹³C-{¹H} NOE experiments.     

Conformation of the common purine (β) ribosides in solution: further evidence for a correlation between N-S state of the ribose moiety and syn-anti equilibrium

The solution conformations of adenosine, guanosine and inosine in liquid ND₃ have been determined by NMR. Comparison of the Karplus analysis of the proton HR spectra of the ribose moiety obtained in this solvent with the data from aqueous solutions of A and I proves that the conformations of the nucleosides are very similar in both liquids. From the analysis of the vicinal coupling constants of the ring protons it has been deduced that the S state C(2′)-endo is slightly preferred. The mole fraction in S approximates 0.6 for all three nucleosides. C-13 relaxation measurements have been applied in the determination of the correlation times for rotational diffusion. Only at temperatures below −40‡ C is the pseudorotation of the furanoside ring slowed down sufficiently for it not to contribute to the measured relaxation rates. From NOE studies and T¹ measurements on the individual protons it is derived that the N, C(3′)-endo, form of the ribose is correlated with an anti conformation of the base (Y≈210‡ to 220‡) and the S, C(2′)-endo, form of the ribose with a syn conformation of the base (Y≈30‡ to 50‡). The glycosyl torsion angles derived for the two conformations of A, G, and I are equal within the limits of accuracy.     

Untenability of the Heteronomous DNA Model for Poly(dA) · Poly(dT) in Solution. This DNA Adopts a Right-Handed B-DNA Duplex in Which the Two Strands are Conformationally Equivalent. A 500 MHz NMR Study Using One Dimensional NOE

Abstract

ID NOE ¹H NMR spectroscopy at 500 MHz was employed to examine the structure of poly(dA)·poly(dT) in solution. NOE experiments were conducted as a function of presaturation pulse length (50, 30, 20 and 10 msec) and.power (19 and 20 db) to distinguish the primary NOEs from spin diffusion. The 10 msec NOE experiments took 49 hrs and over 55,000 scans for each case and the difference spectra were almost free from diffusion.

The spin diffused NOE difference spectra as well as difference NOE spectra in 90% H₂O + 10% D₂O in which TNH3 was presaturated enabled to make a complete assignment of the base and sugar protons. It is shown that poly(dA) ·poly(dT) melts in a fashion in which single stranded bubbles are formed with increasing temperature.

Extremely strong primary NOEs were observed at H2′/H2″ when AH8 and TH6 were presaturated. The observed NOEs at AH2′ and that AH2″ were very similar as were the NOEs at TH2′ and TH2″. The observed NOEs at AH2′ and AH2″when AH8 was presaturated were very similar to those observed at TH2′ and TH2″ when TH6 was presaturated. In addition, presaturation of H1′ of A and T residues resulted in similar NOEs at AH2′/H2″ and TH2′/H2″ region and these NOEs at H2′ and H2″ were distinctly asymmetric as expected in a C2′-endo sugar pucker. There was not a trace of NOE at AH8 and TH6 when AH3′ and TH3′ were presaturated indicating that C3′-endo, × = 30–40° conformation is not valid for this DNA. From these NOE data, chemical shift shielding calculations and stereochemistry based computer modellings, we conclude that poly(dA)·poly(dT) in solution adopts a right- handed B-DNA duplex in which both dA and dT strands are conformationally equivalent with C2′-endo sugar pucker and a glycosyl torsion, ×, of ?73°, the remaining backbone torsion angles being φ′ = 221°, ω′ = 212°, ω = 310°, φ = 149°, ψ = 42°, ψ′ = 139°. The experimental data are in total disagreement with the heteronomous DNA model of Arnott et. al. proposed for the fibrous state. (Arnott, S., Chandrasekaran, R., Hall, I.H., and Puigjaner, L.C., Nucl. Acid Res. 11, 4141, 1983).     

Anisotropic rotational motions of poly(L-glutamic acid) in the alpha-helix conformation

The anisotropic rotational motion of the backbone and the side chains of poly(L -glutamic acid) in the α-helical structure was investigated using the ¹³C-T₁ and T₂ relaxation times of all carbon atoms with directly attached protons, obtained at a ¹³C-Larmor frequency of 67.89 MHz. The evaluation of the nmr data was carried out according to the previously derived anisotropic diffusion model, in which the macromolecule is considered a rigid rod. The rotation of the backbone is characterized by two diffusion constants, D₁ and D₃, describing the rotation perpendicular to and around the symmetry axis. The additional internal motion of the C^β-methylene group is described as a jump process with a jump rate, k₁, between two allowed rotametric states. Steric considerations indicate that the occupation of the third rotameric position is forbidden. The rotation of the C^γ-methylene group is decribed as a one-dimensional diffusion process around the C^β–C^γ bond. Investigation of the temperature dependence of the relaxation parameters led to the temperature dependence of the dynamic parameters. Activation energies were determined from these data. The dynamic parameters obtained for poly(L -glutamic acid) at 291 K are compared with the corresponding results of a previous study of poly(L -lysine). The development of an anisotropic diffusion model for the motions of the rod-shaped poly(L -lysine) α-helix and its application to the interpretation of the ¹³C-relaxation data of this molecule have already been published previously. In this model, both the overall molecular tumbling and the various internal motions have been characterized by diffusion constants or jump rates typical for each process. These dynamic parameters can be calculated from the spin–lattice relaxation times, the spin–spin relaxation times and the NOE factors of the C^α, C^β, and C^γ nuclei of the polypetide. In the present paper, we describe the application of the above-mentioned dynamic model to the interpretation of ¹³C-relaxation studies of a further homopolypeptide, poly(L -glutamic acid), in the α-helical structure. Furthermore, we studied the temperature dependence of the relaxation times of this polymer and determined the anisotropic diffusion parameters at each temperature. From their temperature dependence and from comparison of our present results with the data of our previous study of poly(L -lysine), we were able to derive new insights into the intramolecular diffusion processes and the excitation of various motions.     

Interaction of the antimalarial drug fluoroquine with DNA,tRNA, and poly(A): 19F-NMR chemical-shift and relaxation,optical absorption,and fluorescence studies

The interaction of the fluorinated antimalarial drug fluoroquine [7-fluoro-4-(diethyl-amino-1-methylbutylamino)quinoline] with DNA, tRNA, and poly(A) has been investigated by optical absorption, fluorescence, and ¹⁹F-nmr chemical-shift and relaxation methods. Optical absorption and fluorescence experiments indicate that fluoroquine binds to nucleic acids in a similar manner to that of its well-known analog chloroquine. At low drug-to-base pair ratios, binding of both drugs appears to be random. Fluoroquine and chloroquine also elevate the melting temperature (T_m) of DNA to a comparable extent. Binding of fluoroquine to DNA, tRNA, or poly(A) results in a downfield shift of about 1.5 ppm for the ¹⁹F-nmr resonance. The chemical shift of free fluoroquine depends on the isotopic composition of the solvent (D₂O vs H₂O). The solvent isotope shift is virtually eliminated by fluoroquine binding to any one of the nucleic acids. ¹⁹F-nmr relaxation experiments were carried out to measure the spin-lattice relaxation time (T₁), ¹⁹F{¹H} nuclear Overhauser effect (NOE), off-resonance intensity ratio (R), off-resonance rotating-frame spin-lattice relaxation time (T), and linewidth for fluoroquine in the nucleic acid complexes. By accounting for intramolecular proton-fluorine dipolar and chemical-shift anisotropy contributions to the fluorine relaxation, all of the relaxation parameters for the fluoroquine–DNA complex can be well described by a motional model incorporating long-range DNA bending on the order of a microsecond and an internal motion of the drug on the order of a nanosecond. Selective NOE experiments indicate that the fluorine in the drug is near the ribose protons in the RNA complexes, but not in the DNA complex. Details of the binding evidently differ for the two types of nucleic acids. This study provides the foundation for an investigation of fluoroquine in intact cells.     

Cross-correlation suppressed T1 and NOE experiments for protein side-chain 13CH2 groups

Relaxation measurements of side-chain ¹³CH₂-groups of uniformly ¹³C labeled human ubiquitin were performed at 600 MHz and 800 MHz magnetic field strength at 30°C. Dipole-dipole cross-correlated relaxation effects in T₁ experiments were suppressed by the combination of radio-frequency pulses and pulsed field gradients during the relaxation delay leading to monoexponential relaxation decays that allow a more accurate extraction of the ¹³C T₁ relaxation times. Heteronuclear ¹H-¹³C NOEs obtained by using different proton saturation schemes indicate that the influence of cross-correlation is small. The experimental T₁ and NOE data were interpreted in a model-free way in terms of a generalized order parameter and an internal correlation time.     

NMR relaxation study of water protons in Syrian hamster fetal cells at 300 MHz

TheT ₁ andT ₂ relaxation times of water protons in two cell types in culture derived from Syrian hamster fetuses (normal primary or secondary fetal cells vs BP6T tumor cells derived from the normal cells transformed by carcinogens) were measured at 7.05 Tesla magnetic field (proton frequency =300 MHz). TheT ₁/T ₂ ratios and the correlation time, τ _c , calculated from theT ₁/T ₂ ratio of cellular water protons, are significantly different in these two fibroblastic cell types of the same biological origin and with similar morphologies and growth rates in culture.     

31P nuclear magnetic resonance studies on relaxation parameters and line broadening of intracellular metabolites of HeLa cells.

The 40-MHz ³¹P nuclear magnetic resonance (nmr) spectrum of intact HeLa cells contains seven broad peaks with some detectable splittings. The linewidths were significantly broader than for those of cell-free systems such as cell extracts, indicating that the cellular environment is responsible for the unusual line broadening. Resolution of these peaks at 40 MHz is sufficient to make certain assignments and the relaxation parameters of some of the intracellular metabolites have been measured. The spin-lattice relaxation times (T₁) ranged from 0.3 s for adenosine triphosphate (ATP) to about 3 s for inorganic phosphate (P_i) and monophosphate compounds. Nuclear Overhauser enhancements (NOE) were induced by proton irradiation with the possible exception of ATP. The relaxation parameters were compared to those of cell-free compounds and in all cases T₁ and NOE were smaller for the intracellular metabolites. The relaxation parameters for ATP were affected the most. This behavior was mimicked with mixtures of cell-free metabolites containing paramagnetic ions. The larger change in both T₁ and NOE of intracellular ATP could be accounted for by selective binding of paramagnetic ions. This phenomenon also explains some of the line broadening in the cell spectrum especially that of ATP. The spin-spin relaxation times (T₂) of P₁ and monophosphate compounds as measured by a pulse technique did not account for the observed linewidths. This is due to the presence of chemical shift envelopes arising from pH heterogeneity. All resonances were broader at 146 MHz because of the line broadening by paramagnetic ions and the presence of chemical shift envelopes. Other mechanisms of line broadening may also be significant. There was little difference in resolution of spectra at 40 and 146 MHz. Water proton linewidths and T₂ values were measured for HeLa cells and for some minced tissue preparations. The water linewidth in tissue samples was broader than that in the cell suspension. The large linewidths in tissues arise mainly from chemical shift envelopes caused by magnetic field nonuniformity in the tissue samples. There appears to be a small chemical shift envelope from magnetic nonuniformity in HeLa cells as well. The ¹H results on envelopes were extrapolated to ³¹P studies on cells and tissues. Possible methods for reducing linewidths arising from the various proposed broadening mechanisms were discussed.     

Structure and Conformation of the Branch Core Triribonucleotide Containing 2′-5′ and 3′-5′ Phosphodiester Linkages (A2′p5′G 3′p5′C) in Solution,Essential for Yeast mRNA Splicing,Deduced from 1H-NMR

Abstract

The non-exchangeable ¹H-NMR signals of the branch core trinucleotide of the lariat branch site (A^2′p5′G _3′p5′C), 1) and its derivatives 2 and 3 are completely assigned using one- and two- dimensional NMR techniques including NOE, COSY, NOESY, ¹H-¹HINADEQUATE and 2D-J-resolved spectroscopy. From the vicinal coupling constants in the individual ribose rings, NOE data and T₁ measurements, the following properties of the trimers are deduced.(i)The unique stacking behavior of the trimers is S^1′N _3′N, and the sugar rings exist predominantly in the N-conformation (3′-endo-2′-exo).(ii)The sugar-base orientations appear to be anti.(iii) The branched trimers exist in solution as single-stranded right-handed conformations resembling A-RNA with stacking between the adenine and guanine residues in aqueous solution at 21°C and pH 7.2.(iv) The calculated values for the torsion angles ε^t andγ⁺ for the trimers are 201–203° and 71–86%, respectively, while the percent β¹ values are higher for the guanine (87–92%) than the cytosine residues (73–77%). The computer generated depiction of the triribonucleotide 1 is also shown. These subtle structural features may act as recognition signals for this critical lariat branch site which is essential for the second step in yeast mRNA splicing.     

Thermodynamic analysis of the physical state of water during freezing in plant tissue, based on the temperature dependence of proton spin-spin relaxation

Multi-proton spin-echo images were collected from cold-acclimated winter wheat crowns (Triticum aestivum L.) cv. Cappelle Desprez at 400 MHz between 4 and ?4 °C. Water proton relaxation by the spin-spin (T2) mechanism from individual voxels in image slices was found to be mono-exponential. The temperature dependence of these relaxation rates was found to obey Arrhenius or absolute rate theory expressions relating temperature, activation energies and relaxation rates, Images whose contrast is proportional to the Arrhenius activation energy (E_a), Gibb's free energy of activation (ΔG^?), and the entropy of activation (ΔS^?) for water relaxation on a voxel basis were constructed by post-image processing. These new images exhibit contrast based on activation energies rather than rules of proton relaxation. The temperature dependence of water proton T₂ relaxation rates permits prediction of changes in the physical state of water in this tissue over modest temperature ranges. A simple model is proposed to predict the freezing temperature kof various tissue in wheat crowns. The average E_a and ΔH^? for water proton T₂ relaxation over the above temperature range in winter wheat tissue were ?6.4 ± 14.8 and ?8.6 ± 14.8kj mol^?1, respectively. This barrier is considerably lower than the E_a for proton translation in ice at 0°C, which is reported to be between 46.0 and 56.5 kj mol^?1     

Proton NMR investigation of heme and surrounding proton in low-spin cyanide-ligated bacterial hemoglobin from Vitreoscilla

¹H NMR spectra of low-spin cyanide-ligated bacterial hemoglobin fromVitreoscilla (VtHb-CN) are reported. The assignments of the¹H NMR spectra of VtHb-CN have been made through MCOSY, NOESY, 1D TOE and SUPERWEFT experiments. Almost all resonance peaks of heme and ligated His85 are identified. The spin-lattice relaxation timeT ¹’s and the variation relationships of chemical shifts of these peaks with temperature have been acquired, from which the distances between the measured protons and Fe³⁺, and the diamagnetic chemical shifts have been acquired, respectively. The ionization constants of pK _a’s of ligated His85 are determined through pH titration of chemical shift, which is 4.95 for ligated His85 C₂H proton. The lower pK _a is attributed to the influence of the Fe³⁺ of carrying positive charge and the coordination of His85 and Fe³⁺ of heme.     

Nuclear magnetic resonance investigation of lysine–oligopeptides and a complex with d(pA)3pGpC(pT)3

We report proton magnetic resonance studies of a series of lysine oligopeptides in H₂O solution. At pH 5 the protonated ε-amino groups are seen as broad resonances; the peptide NH proton resonances are split by spin–spin coupling with the C^α-H proton, and appear at positions which depend on position in the chain and on chain length. Assignments were made by the europium shift method, and we observed the expected effect of catalysis by the terminal —NH₃⁺ of exchange of the adjacent peptide NH. Coupling constants and the temperature coefficient of chemical shift values were consistent with a non-hydrogen-bonded structure for the oligolysines. The rate and mechanism of NH hydrogen exchange were investigated by line-broadening measurements of the peptide protons as a function of pH. Exchange was found to be OH^? catalyzed, with large differences in the rate depending on position in the chain. Preliminary studies of the complex between double-helical d(pA)₃pGpC(pT)₃ and tetra(L -lysine) were performed using ¹H- and ³¹P-nmr techniques. Pmr spectra of the complex at pH values ranging from 3.98 to 8.15 showed very complicated patterns. Downfield shifts and reduction in exchange rates were observed for several tetra(L -lysine) protons. ³¹P-nmr spectra of the complex reveal an upfield shift of 1 ppm for 3′-5′ phosphate diester resonances on complexation. ³¹P T₁ relaxation times change little on complex formation at low temperature but are altered at higher temperature.     

Strong coupling effects during <Emphasis Type="Italic">X</Emphasis>-pulse CPMG experiments recorded on heteronuclear <Emphasis Type="Italic">ABX</Emphasis> spin systems: artifacts and a simple solution

Simulation and experiment have been used to establish that significant artifacts can be generated in X-pulse CPMG relaxation dispersion experiments recorded on heteronuclear ABX spin-systems, such as ¹³C _i –¹³C _j –¹H, where ¹³C _i and ¹³C _j are strongly coupled. A qualitative explanation of the origin of these artifacts is presented along with a simple method to significantly reduce them. An application to the measurement of ¹H CPMG relaxation dispersion profiles in an HIV-2 TAR RNA molecule where all ribose sugars are protonated at the 2′ position, deuterated at all other sugar positions and ¹³C labeled at all sugar carbons is presented to illustrate the problems that strong ¹³C–¹³C coupling introduces and a simple solution is proposed.     

Amide Proton Spin-Lattice Relaxation in Polypeptides: A Field-Dependence Study of the Proton and Nitrogen Dipolar Interactions in Alumichrome

The proton nuclear magnetic resonance (NMR) spin-lattice relaxation of all six amides of deferriferrichrome and of various alumichromes dissolved in hexadeutero-dimethylsulfoxide have been investigated at 100, 220, and 360 MHz. We find that, depending on the type of residue (glycyl or ornithyl), the amide proton relaxation rates are rather uniform in the metal-free cyclohexapeptide. In contrast, the ¹H spinlattice relaxation times (T₁'s) are distinct in the Al³⁺-coordination derivative. Similar patterns are observed in a number of isomorphic alumichrome homologues that differ in single-site residue substitutions, indicating that the spin-lattice relaxation rate is mainly determined by dipole-dipole interactions within a rigid molecular framework rather than by the specific primary structures. Analysis of the data in terms of ¹H—¹H distances (r) calculated from X-ray coordinates yields a satisfactory linear fit between T₁^-1 and Σr^-6 at the three magnetic fields. Considering the very sensitive r-dependence of T₁, the agreement gives confidence, at a quantitative level, both on the fitness of the crystallographic model to represent the alumichromes' solution conformation and on the validity of assuming isotropic rotational motion for the globular metallopeptides. An extra contribution to the amide proton T₁^-1 is proposed to mainly originate from the ¹H-¹⁴N dipolar interaction: this was supported by comparison with measurements on an ¹⁵N-enriched peptide. The nitrogen dipolar contribution to the peptide proton relaxation is discussed in the context of {¹H}—¹H nuclear Overhauser enhancement (NOE) studies because, especially at high fields, it can be dominant in determining the amide proton relaxation rates and hence result in a decreased effectiveness for the ¹H—¹H dipolar mechanism to cause NOE's. From the slope and intersect values of T₁^-1 vs. Σr^-6 linear plots, a number of independent estimates of τ_r, the rotational correlation time, were derived. These and the field-dependence of the T₁'s yield a best estimate <τ_r> ≈ 0.37 ns, in good agreement with 0.38 ns [unk] <τ_r> [unk] 0.41 ns, previously determined from ¹³C and ¹⁵N spin-lattice relaxation data.     

Proton and phosphorus magnetic relaxation studies on the dynamic structure of single-stranded polyriboadenylic acid

Proton and phosphorus-31 nuclear spin-lattice relaxation times (T₁) have been measured with the Fourier-transform method at 100 and 40.5 MHz, respectively, on single-stranded polyriboadenylic acid (poly(A)) in a neutral D₂O solution in the temperature range of 14–82°C. T₁ minimum is observed around 35–45°C for H(8), H(1′), and phosphorus resonances. Rotational correlation times have been deduced from the T₁ data, which indicate that the sugar–phosphate backbone as well as the base–sugar segment is undergoing rapid internal motion of 10^?8–10^?10 sec range. The molecular motion of the sugar–phosphate backbone as deduced from the phosphorus relaxation is well-characterized by a single activation enthalpy of 8.1 kal/mole for the whole temperature range of 14–82°C. Activation enthalpies of similar magnitude have been obtained for the motion of the adenine–ribose moiety from H(8) and H(1′) relaxation. The relative magnitude of T₁ for H(8) and H(1′) infers that the poly(A) nucleotide exists on the average as anti in the single-stranded form. The phosphorus T₁ value is consistent with a conformation such that both C(4′)–C(5′) and C(4′)–C(3′) bonds are nearly trans to their connected O–P bonds.