Angular dependence of 1J(Ni,Calphai) and 2J(Ni,Calpha(i-1)) coupling constants measured in J-modulated HSQCs

A new method to measure ¹J(N_i,C _i) and ²J(N_i,C _{(i – 1)}) coupling constants in proteins based on a J-modulated sensitivity enhanced HSQC was introduced. Coupling constants were measured in the denatured and in the native state of ubiquitin and found to depend on the conformation of the protein backbone. Using a combined data set of experimental coupling constants from ubiquitin and staphylococcal nuclease (Delaglio et al., 1991), the angular dependence of the coupling constants on the backbone angles and was investigated. It was found that the size of ²J(N_i,C _{(i – 1)}) correlates strongly with the backbone conformation, while only a weak conformational dependence on the size of ¹J(N_i,C _i) coupling constants was observed. Coupling constants in the denatured state of ubiquitin were uniform along the sequence of the protein and not dependent on a given residue type. Furthermore it was shown that the observed coupling constants were in good agreement with predicted coupling constants using a simple model for the random coil.     

Molecular switch of F0F1-ATP synthase,G-protein,and other ATP-driven enzymes

Exchange-out of amide tritium from labeled -subunit of ₃₃ complex of F₀F₁-ATP synthase was not accelerated by ATP, suggesting that hemagglutinin-type transition of coiled-coil structure did not occur in -subunit. Local topology of nucleotide binding site and switch II region of G-protein resemble those of F₁- subunit and other proteins which catalyze ATP-triggered reactions. Probably, binding of nucleotide to F₀F₁-ATP synthase induces conformational change of the switch II-like region with transforming subunit structure from open to closed form and this transformation results in loss of hydrogen bonds with the subunit, thus enabling the subunit to move.     

Paramagnetic spin catalysis of a radical recombination reaction

Recombination of the triplet state radical pair consisting of two hydrogen atoms catalysed by molecular oxygen is considered as a simulating example of a paramagnetic-exchange catalytic process. Intermolecular exchange interaction in the collision complex between the H₂ and O₂ molecules is calculatedab initio in STO-6G and 6–31 G^* basis sets with complete active space configuration interaction. Calculations are done at a fixed O–H distance (3 Å), scanning the H–H bond length from 0.6 till 12 Å at the linear geometry of collision. The mixture of the triplet (T)³ _u ⁺ and singlet (S)¹ _g ⁺ states of the hydrogen moiety is possible because both states have the same triplet symmetry in the collision complex with O₂ (³ _g ^– ). A strong mixture of the S (¹ _g ⁺ , H₂ +³ _g ^– , O₂) and T) and T (³ _u ⁺ , H₂ +³ _g ^– , O₂) states is actually obtained even at large H–H distances. The quintet and singlet states^5,1(³ _u ⁺ , H₂ +³ _g ^– , O₂) are also considered for comparison of the exchange potentials. Atr(H–H)4.4 Å the S-T splitting is approximately constant (12 cm^-1 in the STO-6G basis set; 55.5 cm^-1 in the 6–31 G^* basis set) and is determined by the exchange interaction between O₂ and the nearest hydrogen atom in the O–O...H fragment. The paramagnetic catalyst can accelerate radical recombination through the triplet-singlet nonadiabatic transition to the lowest S reactive state when the radical encounter takes place in the vicinity of the catalyst. Though we do not consider the radical dynamics in a real solvent, which modulates the exchange potentials and the T-S transitions, the nature of this mechanism of spin catalysis is obvious. The electric polarization and charge transfer are important in the analysis of the exchange interaction and radical recombination potentials for all multiplets. In accordance with the concept of spin catalysis, the electronic spin-uncoupling mechanism, induced by O₂ perturbation, has the same nature as other known catalytic processes of paramagnetic-exchange type.     

Unambiguous through-bond sugar-to-base correlations for purines in 13C, 15N-labeled nucleic acids: The HsCsNb,HsCs(N)bCb,and HbNbCb experiments

Summary A set of three 3D (¹H, ¹³C, ¹⁵N) triple-resonance correlation experiments has been designed to provide H1-H8 intraresidue sugar-to-base correlations in purines in an unambiguous and efficient manner. Together, the H_sC_sN_b, H_sC_s(N)_bC_b, and H_bN_bC_b experiments correlate the H1 sugar proton to the H8 proton of the attached base by means of the {H1, C1, N9, C8, H8} heteronuclear scalar coupling network. The assignment strategy presented here allows for unambiguous H1-H8 intraresidue correlations, provided that no two purines have both the same H1 and C1 chemical shifts and the same C8 and N9 chemical shifts. These experiments have yielded H1-H8 intraresidue sugar-to-base correlations for all five guanosines in the [¹³C, ¹⁵N] isotopically labeled RNA duplex r(GGCGCUUGCGUC)₂.     

Measurement of two-bond JCOHα coupling constants in proteins uniformly enriched with13C

Summary A simple E.COSY type technique is described for measurement of two-bond J_COH coupling constants in proteins that are uniformly enriched with¹³C. The method has been used to measure²J_COH for 132 residues in the proteins calmodulin and staphylococcal nuclease having non-overlapping H–C correlations. Measured²J_COH coupling constants fall in the 0 to –9.5 Hz range. A separate experiment, measuring the accuracy of these values, indicates a root-mean-square error of 1 Hz. Comparison of the J couplings with the dihedral back bone angles from crystallographic studies confirms a weak but statistically significant correlation between the dihedral angle and the magnitude of²J_COH, but also indicates that parameters other than have a significant effect on the value of the coupling.     

Pressure alters electronic orbital overlap in hydrogen bonds

Pressure-induced changes in ^3h J _NC scalar couplings through hydrogen bonds were investigated in the immunoglobulin binding domain of streptococcal protein G. ¹H, ¹⁵N and ¹³C triple-resonance NMR spectroscopy coupled with the on-line high pressure cell technique was used to monitor ^3h J _NC scalar couplings at 30 and 2000 bar in uniformly labeled ¹⁵N and ¹³C protein isotopes. Both increased and decreased ^3h J _NC scalar couplings were observed at high pressure. No correlation with secondary structure was apparent. The difference in coupling constants as well as pressure-induced chemical shift data suggests a compaction of the helix ends and an increase of the helix pitch at its center in response to pressure. Our data provides the first direct evidence that the electronic orbital overlap in protein backbone hydrogen bonds is altered by pressure.     

Facile measurement of polypeptide JHNHα coupling constants from HMQC-J spectra

A method, based on linewidth measurements, is described which permits the rapid and facile determination of J_HNH coupling constants from ¹⁵N labeled proteins. Using appropriately processed HMQC-J data, we have found that a simple linear relationship exists between the half-height linewidth (_1/2) of ¹⁵N–¹H cross peaks and their corresponding J_HNH coupling constants. Tests indicate that this technique permits the accurate measurement of up to 100 J_HNH coupling constants in less than 30 min. Furthermore, the J_HNH measurements can be done manually – without the need of any computer-based curve-fitting or minimization. Comparisons between J_HNH values predicted from high resolution X-ray structures and those determined using this technique indicate that the method is both accurate and precise (correlation coefficient = 0.90, rmsd = 0.75 Hz).     

A molecular dynamics simulation of crystalline α-cyclodextrin hexahydrate

The structure of crystalline -cyclodextrin (-CD) hexahydrate, form I (C₃₆H₆₀O₃₀·6H₂O, space group P2₁2₁2₁) is experimentally so well determined by X-ray and by neutron diffraction analyses that the positions of all the hydrogen atoms are available. This provides an opportunity for testing an empirical force field that is currently used in simulations of protein and nucleic acid structures by performing molecular dynamics studies employing the GROMOS program package on a system of 4 unit cells containing 16 -CD molecules and 96 water molecules.A detailed comparison of the simulated and experimentally determined crystal structures shows that the experimental positions of the -CD atoms are reproduced within 0.025 nm, well within the overall experimental accuracy of 0.036 nm; that the water molecules are on average within 0.072 nm from their experimental sites, with two thirds reproduced within experimental accuracy by the calculations; that high correlation is produced, between the occurrence of simulated and experimentally observed hydrogen bonds.The good agreement between simulated and experimental results suggests that the tested force field is reliable.     

Spatial and temporal variation in soil CO2 efflux in an old-growth neotropical rain forest, La Selva, Costa Rica

Our objectives were to quantify and compare soil CO₂ efflux of two dominant soil types in an old-growth neotropical rain forest in the Atlantic zone of Costa Rica, and to evaluate the control of environmental factors on CO₂ release. We measured soil CO₂ efflux from eight permanent soil chambers on six Oxisol sites. Three sites were developed on old river terraces (old alluvium) and the other three were developed on old lava flows (residual). At the same time we measured soil CO₂ concentrations, soil water content and soil temperature at various depths in 6 soil shafts (3 m deep). Between old alluvium sites, the two-year average CO₂ flux rates ranged from 117.3 to 128.9 mg C m^–2 h^–1. Significantly higher soil CO₂ flux occurred on the residual sites (141.1 to 184.2 mg C m^–2 h^–1). Spatial differences in CO₂ efflux were related to fine root biomass, soil carbon and phosphorus concentration but also to soil water content. Spatial variability in CO₂ storage was high and the amount of CO₂ stored in the upper and lower soil profile was different between old alluvial and residual sites. The major factor identified for explaining temporal variations in soil CO₂ efflux was soil water content. During periods of high soil water content CO₂ emission decreased, probably due to lower diffusion and CO₂ production rates. During the 2-year study period inter-annual variation in soil CO₂ efflux was not detected.     

Application of H(N)CA,CO-E.COSY experiments for calibrating the φ angular dependences of vicinal couplings J(C′i−1,Hi α), J(C′i−1,Ci β) and J(C′i−1,C′i) in proteins

A triple-resonance NMR technique suitable for the determination ofcarbonyl-related couplings in polypeptide systems is introduced. Theapplication of three novel pulse sequences to uniformly¹³C/¹⁵N-enriched proteins yields E.COSY-likemultiplet patterns exhibiting either one of the³J(C_i–1,H_i ), ³J(C_i–1,C_i ) and³J(C_i–1,C_i)coupling constants in the indirectly detected ¹³Cdimension, depending on the passive spin selected. The experiments aredemonstrated with oxidized flavodoxin from Desulfovibrio vulgaris. On thebasis of the J-values measured and the backbone -angles derived from ahigh-resolution X-ray structure of the protein, the three associated Karplusequations were reparametrized. The root-mean-square differences between theexperimental coupling constants and those predicted by the optimized Karpluscurves are 0.41, 0.33 and 0.32 Hz for³J(C_i–1,H_i ),³J(C_i–1,C_i ) and³J(C_i–1,C_i),respectively. The results are compared with the Karplus parameters previouslypublished for the same couplings.     

Two-dimensional1H NMR study of recombinant insect defensin A in water: Resonance assignments,secondary structure and global folding

Summary A 500 MHz 2D¹H NMR study of recombinant insect defensin A is reported. This defense protein of 40 residues contains 3 disulfide bridges, is positively charged and exhibits antibacterial properties. 2D NMR maps of recombinant defensin A were fully assigned and secondary structure elements were localized. The set of NOE connectivities,³J_NH-H coupling constants as well as¹H/²H exchange rates and /T temperature coefficients of NH protons strongly support the existence of an -helix (residues 14–24) and of an antiparallel -sheet (residues 27–40). Models of the backbone folding were generated by using the DISMAN program and energy refined by using the AMBER program. This was done on the basis of: (i) 133 selected NOEs, (ii) 21 dihedral restraints from³J_NH-H coupling constants, (iii) 12 hydrogen bonds mostly deduced from¹H/²H exchange rates or temperature coefficients, in addition to 9 initial disulfide bridge covalent constraints. The two secondary structure elements and the two bends connecting them involve approximately 70% of the total number of residues, which impose some stability in the C-terminal part of the molecule. The remaining N-terminal fragment forms a less well defined loop. This spatial organization, in which a -sheet is linked to an -helix by two disulfide bridges and to a large loop by a third disulfide bridge, is rather similar to that found in scorpion charybdotoxin and seems to be partly present in several invertebrate toxins.Abbreviations SCUBA Stimulated Cross peaks Under Bleached Alphas - MCD analysis Main Chain Directed analysis - CSH motif Cysteine Stabilized -Helix motif     

1H-filtered correlation experiments for assignment and determination of coupling constants in backbone labelled proteins

The implementation of [¹³C,¹³C,¹⁵N,²H] labelled amino acids into proteins allows the acquisition of high resolution triple resonance experiments. We present for the first time resonance assignments facilitated by this new labelling strategy. The absence of ¹J_C,C couplings enables us to measure ¹J_C,C scalar and ¹D_C,C residual dipolar coupling constants using modified HNCA experiments which do not suffer from sensitivity losses characteristic for ¹³C constant time experiments.     

Integration of spin-state-selective excitation into 2D NMR correlation experiments with heteronuclear ZQ/2Q π rotations for1 JXH

Spin-State-Selective Excitation (S³E), which forexample selectively excites amide proton resonances corresponding toexclusively either the or the spin state of the covalentlybound ¹⁵N atom is employed for E.COSY-type extraction ofheteronuclear J coupling constants. Instead of having one spectrum with twopeaks (corresponding to the or spin state of¹⁵N), S³E generates two spectra, each with onlyone peak for each ¹⁵N nucleus. These two spectra are generatedfrom the same data set, so that there is no reduction in sensitivitycompared to conventional ¹J_NH-resolved methods.Another interesting feature in comparison with conventional methods is that¹J_NH can be suppressed during the evolutionperiod, meaning that no heteronuclear multiplet structure is visible in the₁ frequency dimension. The S³E pulsesequence element is combined with NOESY for measurement of³J_N-H and J_N-Hcoupling constants in either a hetero- or a homonuclear correlated version.Experimental confirmation is obtained using the protein RAP 17-;97(N-terminal domain of ₂-macroglobulin ReceptorAssociated Protein).     

Conformation of the circular dumbbell d〈pCGC-TT-GCG-TT〉: Structure determination and molecular dynamics

Summary The circular DNA decamer 5-dpCGC-TT-GCG-TT-3 was studied in solution by means of NMR spectroscopy and molecular dynamics in H₂O. At a temperature of 269 K, a 50/50 mixture of two dumbbell structures (denoted L2L2 and L2L4) is present. The L2L2 form contains three Watson-Crick C-G base pairs and two two-residue loops in opposite parts of the molecule. On raising the temperature from 269 K to 314 K, the L2L4 conformer becomes increasingly dominant (95% at 314 K). This conformer has a partially disrupted G(anti)-C(syn) closing base pair in the 5-GTTC-3 loop with only one remaining (solvent-accessible) hydrogen bond between NH of the cytosine dC(1) and O6 of the guanine dG(8). The opposite 5-CTTG-3 loop remains stable. The two conformers occur in slow equilibrium (rate constant 2–20 s^–1). Structure determination of the L2L2 and L2L4 forms was performed with the aid of a full relaxation matrix approach (IRMA) in combination with restrained MD. Torsional information was obtained from coupling constants. Coupling constant analysis (³J_HH, ³J_HP, ³J_CP) gave detailed information about the local geometry around backbone torsion angles , , and , revealing a relatively high flexibility of the 5-GTTC-3 loop. The values of the coupling constants are virtually temperature-independent. Weakly constrained molecular dynamics in solvent was used to sample the conformational space of the dumbbell. The relaxation matrices from the MD simulation were averaged over r^–3 to predict dynamic NOE volumes. In order to account for the 1:1 conformational mixture of L2L2 and L2L4 present at 271 K, we also included S² factors and r^–6 averaging of the r^–3-averaged relaxation matrices. On matrix averaging, the agreement of NOE volumes with experiment improved significantly for protons located in the thermodynamically less stable 5-GTTC-3 loop. The difference in stability of the 5-CTTG-3 and 5-GTTC-3 loops is mainly caused by differences in the number of potential hydrogen bonds in the minor groove and differences in stacking overlap of the base pairs closing the minihairpin loops. The syn conformation for dC(1), favored at high temperature, is stabilized by solvation in the major groove. However, the conformational properties of the dC(1) base, as deduced from R-factor analysis and MD simulations, include a large flexibility about torsion angle .     

Measurement of two- and three-bond 13C−1H J couplings to the Cδ carbons of leucine residues in staphylococcal nuclease

Summary A new ¹H-detected 3D NMR experiment is described that permits quantitative measurement of two- and three-bond ¹³C–¹H couplings in proteins with selectively ¹³C-enriched methyl sites. The method is demonstrated for staphylococcal nuclease selectively [5,5 ¹³C]-labeled in all 11 leucine positions and ligated with thymidine 3,5-biphosphate and Ca²⁺. Two- and three-bond ¹³C methyl-proton couplings are reported and, together with the measured three-bond J_CC in uniformly ¹³C-enriched staphylococcal nuclease, the ²- and the stereospecific assignments of the C methyl group with respect to the prochiral -protons were determined. The same residues that were previously found to have high degrees of internal mobility on the basis of ¹³C relaxation times have measured coupling constants that are indicative of motional averaging.     

Measurement of residual dipolar couplings from 1Hα to 13Cα and 15N using a simple HNCA-based experiment

Novel NMR pulse schemes for simultaneous measurement of ¹ D _CHand ² D _NHresidual dipolar couplings in proteins is presented. We show that ² D _NHcoupling can be very useful for protein structure determination. The ² D _NHcoupling can be measured from ¹⁵N dimension with good accuracy on a slowly relaxing TROSY resonance, utilizing HNCA-TROSY-based experiments, which concomitantly supply large ¹ D _CHcoupling. The dynamic range of ² D _NHcoupling is comparable to ¹ D _NC coupling, but instead, it also serves non-redundant information on the course of protein backbone, thanks to rotational degree of freedom with respect to peptide bond. The HNCA-TROSY-based experiments are optimal for measuring residual dipolar couplings at high magnetic fields owing to absence of rapid transverse relaxation of carbonyl carbon. The reliability of the proposed approach was tested on ¹⁵N/¹³C human ubiquitin. A very good correlation with ubiquitin solution as well as crystal structure, for both ¹ D _CHand ² D _NHcouplings, was obtained.     

TROSY experiment for refinement of backbone psi and phi by simultaneous measurements of cross-correlated relaxation rates and 3,4J(H alpha HN) coupling constants

The TROSY principle has been introduced into a HNCA experiment, which is designed for measurements of the intraresidual and sequential H-C/H^N-N dipole/dipole and H-C/N dipole/CSA cross-correlated relaxation rates. In addition, the new experiment provides values of the ^3,4 J _{H HN} coupling constants measured in an E.COSY manner. The conformational restraints for the and angles are obtained through the use of the cross-correlated relaxation rates together with the Karplus-type dependencies of the coupling constants. Improved signal-to-noise is achieved through preservation of all coherence transfer pathways and application of the TROSY principle. The application of the [¹⁵N,¹³C]-DQ/ZQ-[¹⁵N,¹H]-TROSY-E.COSY experiment to the 16 kDa apo-form of the E. coli Heme Chaperon protein CcmE is described. Overall good agreement is achieved between and angles measured with the new experiment and the average values determined from an ensemble of 20 NMR conformers.     

Determination of heteronuclear long-range couplings to heteronuclei in natural abundance by two- and three-dimensional NMR spectroscopy

Summary A method to determine heteronuclear long-range couplings to carbon and nitrogen at natural abundance is presented and applied to two cyclic hexapeptides and the peptidomacrolide FK506. The method is applicable for proton-bearing heteronuclei. By introduction of heteronuclear half-filters in two- or three-dimensional experiments the spectra exhibit an E.COSY pattern when executed without heteronuclear decoupling. The extraction of the heteronuclear coupling constants is therefore independent of linewidth.Incyclo(-Ala-Ala-Ala-Pro-Ala-Pro-) a¹³C-_I-half-filtered TOCSY spectrum yields the³J(H^N-C) coupling constant, which can be used to remove ambiguity in the angle determination from³J(H^N-H). Incyclo(-d-Pro-Phe-Phe-Lys(Z)-Trp-Phe-) a¹⁵N-_I-half-filtered TOCSY was applied to individually assign the diastereotopic -methylene protons via the³J(H-N). In FK506 a 3D-HMQC-TOCSY without heteronuclear decoupling is used to obtain a number of heteronuclear coupling constants to carbons. These values have been applied for the assignment of diastereotopic methylene protons and determination of dihedral angles in the cyclic portion of the molecule.Dedicated to the memory of Professor V.F. Bystrov     

Measurement of 2J(H,C)- and 3J(H,C)-coupling constants by α/β selective HC(C)H-TOCSY

A new heteronuclear NMR pulse sequence for the measurement of ⁿJ(C,H) coupling constants, the /selective HC(C)H-TOCSY, is described. It is shown that the S³E element (Meissner et al., 1997a,b) can be used to obtain spin state selective coherence transfer in molecules, in which adjacent CH moieties are labeled with ¹³C. Application of the / selective HC(C)H-TOCSY to a 10nt RNA tetraloop 5-CGCUUUUGCG-3, in which the four uridine residues are ¹³C labeled in the sugar moiety, allowed measurement of two bond and three bond J(C,H) coupling constants, which provide additional restraints to characterize the sugar ring conformation of RNA in cases of conformational averaging.