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.     

Estimates of ϕ and ψ torsion angles in proteins from one-, two- and three-bond nuclear spin-spin couplings: Application to staphylococcal nuclease

Summary Calculated coupling constants (³J_H ^N _H , ¹J_{C H} , ²J_CH , ¹J_{C N} and ²J_{C N}) from our accompanying paper [Edison, A.S. et al. (1994) J. Biomol. NMR, 4, 519–542] have been used to generate error surfaces that can provide estimates of the and angles in proteins. We have used experimental coupling data [³J_H ^N _H : Kay, L.E. et al. (1989) J. Am. Chem. Soc., 111, 5488–5490; ¹J_{C H} : Vuister, G.W. et al. (1993) J. Biomol. NMR, 3, 67–80; ²J_CH : Vuister, G.W. and Bax, A. (1992) J. Biomol. NMR, 2, 401–405; ¹J_{C N} and ²J_{C N}: Delaglio, F. et al. (1991) J. Biomol. NMR, 1, 439–446] to create error surfaces for selected residues of the protein staphylococcal nuclease. The residues were chosen to include all those with five experimental couplings, as well as some with four experimental couplings, to demonstrate the relative importance of ³J_H ^N _H and ¹J_{C H} . For most of the cases, we obtained good agreement between the X-ray structure [Loll, P.J. and Lattman, E.E. (1989) Protein Struct. Funct. Genet., 5, 183–201] and the NMR data.Abbreviations CUPID Contin Uous ProbabIlity Distribution analysis of rotamers - ⁿJ_AB single-bond (n=1), geminal (n=2), or vicinal (n=3) coupling constant between nuclei A and B - NOE nuclear Overhauser enhancement - r² correlation coefficient     

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.     

Evaluation of the influence of anisotropic indirect nuclear spin-spin coupling tensors on effective residual dipolar couplings for model peptides

Residual dipolar couplings (RDCs) observed between nuclear spins in molecules in partially oriented media have become a valuable source of information for NMR spectroscopists seeking to structurally characterize biological macromolecules. Examination of the form of the direct (D) and indirect (J) nuclear spin-spin coupling Hamiltonians indicates that all observed RDCs contain an unknown contribution from the anisotropic part of J (J) in addition to the direct dipolar contribution, D _PQ. Here, we evaluate the influence of J on RDCs through a series of DFT calculations on model peptides. Very small corrections to one-bond RDCs measured between heavy atoms in peptides and proteins are recommended: +0.51% for N-C spin pairs, and +0.45% for C-C spin pairs. The corrections to RDCs involving at least one proton are negligible. This latter point is likely to be equally applicable to nucleic acids and oligosaccharides in addition to peptides and proteins. Finally, the orientations of the J(N, C) and J(C, C) tensors in the molecular framework are reported for glycylglycine.     

Surface charge density estimation by 9-aminoacridine fluorescence titration: improvements and limitations

A large number of surface charge density () and surface potential (_o) estimations have been based on 1) titrations of the fluorescence of 9-aminoacridine released from the diffuse double layer adjacent to negatively charged membrane surfaces by non-adsorbing monovalent and divalent cations, and 2) calculations using experimental data from the titration curves and the Gouy-Chapman theory of the diffuse double layer. In this paper we discuss the different simplifying approximations employed in the earlier calculations and recommend modified formulas for the calculations. The latter have been derived without any simplifying approximation concerning the ionic (electrolyte) composition of the titration assays. We also show that depends, to some extent, on the concentrations of buffer and vesicles in the assays and present experimental evidence that decamethonium (decane-1,10-bis-trimethylammonium), a bulky organic divalent cation, can be satisfactorily used for the estimation of under well-defined conditions, despite its putative interaction with membranes.Abbreviations 9-AA 9-aminoacridine - (DeM)²⁺ decamethonium - (DiM)²⁺ dimethonium - EDTA ethylenediaminetetraacetic acid - EGTA ethylene glyol-bis(-aminoethyl ether) N,N,N,N-tetraacetic acid - (HeM)²⁺ hexamethonium - MES 2-(N-morpholino) ethanesulfonic acid - MOPS 4-morpholinopropanesulfonic acid - PM plasma membrane - Tris tris(hydroxymethyl)aminomethane - surface charge density - _o surface potential Correspondence to: A. Bérczi     

Measurement of15N-13C J couplings in staphylococcal nuclease

Summary ¹⁵N-C and¹⁵N-C J couplings were measured for the backbone of staphylococcal nuclease, uniformly enriched with¹⁵N and¹³C. It is found that the^IJ_C'N coupling is similar for -sheet, J=14.8 ± 0.5 and for -helix, J = 14.8 ± 0.4 but tends to be larger for the unstructured N- and C-terminal ends of the protein (J=15.6 ± 0.5). On average,¹J_NC are smaller for -helical residues (J=9.6 ± 0.3 Hz) compared to -sheet (J=10.9 ± 0.8 Hz) and a substantial difference is observed for²J_NC in -helices (J=6.4 ± 0.4 Hz) and -sheets (J=8.3 ± 0.8 Hz).Dedicated to the memory of Professor V.F. Bystrov     

Pulse schemes for the measurement of3 JC′Cγ and3 JNCγ scalar couplings in 15N,13C uniformly labeled proteins

Pulse sequences are presented for the measurement of³J_CC and³J_NC scalar couplings for allC containing residues in¹⁵N,¹³C uniformly labeled proteins. The methodsdescribed are based on quantitative J correlation spectroscopy pioneered byBax and co-workers [Bax et al. (1994) Methods Enzymol., 239, 79–105].The combination of ³J_CC and³J_NC scalar coupling constants allows theassignment of discrete rotameric states about the ₁ torsion angle in cases where such states exist or, alternatively,facilitates the establishment of noncanonical ₁conformations or the presence of rotameric averaging. The methods areapplied to a 1.5 mM sample of staphylococcal nuclease.     

Genetic analysis of bacterial blight resistance in seventy-four cultivars of rice,Oryza sativa L.

Summary The genetics of resistance to bacterial blight, Xanthomonas oryzae (Uyeda and Ishiyama) Dowson, for 74 cultivars of rice, Oryza sativa L., was studied. The PX061 isolate of bacterial blight from the Philippines was used for inoculation of parental and hybrid populations. Single dominant genes at the Xa 4 locus convey resistance in 38 cultivars. Of these, 18 are resistant at all stages of plant growth and thus have the Xa 4 ^aallele for resistance. However, 20 are susceptible up to maximum tillering stage but are resistant at booting and flowering stages. These cultivars have the Xa 4 ^ballele for resistance. Thirty-two cultivars have single recessive genes for resistance which are allelic to xa 5.The resistance in DV85, DV86 and DZ78 is conditioned by two genes. At maximum tillering stage xa 5 conveys resistance. However, at later growth stages an additional dominant gene, designated Xa 7 in DZ78, also gives resistance. The dominant genes of DV85 and DV86 are probably allelic to Xa 7. Xa 7 segregates independently of Xa 4, xa 5 and Xa 6, however like Xa 6, it conveys resistance at booting and post-booting stages only.The resistance in PI 231129 is conditioned by a single recessive gene, designated xa 8. It also segregates independently of Xa 4, xa 5 and Xa 6.     

Genetic control of polyunsaturated fatty acid biosynthesis in flax (Linum usitatissimum) seed oil

Summary The inheritance of two mutants of flax (Linum usitatissimum), having altered proportions of the C18 polyunsaturated fatty acids, linoleic and linolenic, was examined. Both lines, M1589 and M1722, are homozygous for a single gene mutation which reduces linolenic acid content from 34% to 22% and raises linoleic acid from 15% to 27%. Genetic analysis of crosses involving M1589, M1722 and their parental cultivar Glenelg revealed that these mutations are in different unlinked genes and exhibit additive (codominant) gene action. The symbolsLn1 andLn2 are proposed for the mutated genes in M1589 and M1722, respectively. Recombinant genotypes homozygous for the mutant alleles at both loci are very low in linolenic acid (2%) and high in linoleic acid (48%), with unaltered proportions of other fatty acids. The complete inverse correlation between linoleic and linolenic acids (r=-0.98) indicates that the mutations block the synthesis of linolenic acid at the linoleic desaturation step.     

Local helix content in an alanine-rich peptide as determined by the complete set of 3JHNα coupling constants

Summary Alanine-rich peptides serve as models for exploring the factors that control helix structure in peptides and proteins. Scalar CH-NH couplings (³J_HN) are an extremely useful measure of local helix content; however, the large alanine content in these peptides leads to significant signal overlap in the CH region of ¹H 2D NMR spectra. Quantitative determination of all possible ³J_HN values is, therefore, very challenging. Szyperski and co-workers [(1992) J. Magn. Reson., 99, 552–560] have recently developed a method for determining ³J_HN from NOESY spectra. Because ³J_HN may be determined from 2D peaks outside of the CH region, there is a much greater likelihood of identifying resolved resonances and measuring the associated coupling constants. It is demonstrated here that ³J_HN can be obtained for every residue in the helical peptide Ac-(AAAAK)₃A-NH₂. The resulting ³J_HN profile clearly identifies a helical structure in the middle of the peptide and further suggests that the respective helix termini unfold via distinct pathways.Abbreviations ³J_HN three-bond CH-NH scalar coupling constant - NOE nuclear Overhauser enhancement - NOESY two-dimensional nuclear Overhauser spectroscopy - COSY two-dimensional correlated spectroscopy - DQF-COSY two-dimensional double-quantum-filtered correlated spectroscopy - TOCSY two-dimensional total correlation spectroscopy To whom correspondence should be addressed.Deceased March 5, 1996.     

The use of 1JCαHα coupling constants as a probe for protein backbone conformation

Summary Simple pseudo-3D modifications to the constant-time HSQC and HCACO experiments are described that allow accurate (±0.5 Hz) measurement of one bond J_CH coupling constants in proteins that are uniformly enriched with ¹³C. An empirical ,-surface is calculated which describes the deviation of ¹J_CH from its random coil value, using 203 ¹J_CH values measured for residues in the proteins calmodulin, staphylococcal nuclease, and basic pancreatic trypsin inhibitor, for which and are know with good precision from previous X-ray crystallographic studies. Residues in -helical conformation exhibit positive deviations of 4–5 Hz, whereas deviations in -sheet are small and, on average, slightly negative. Data indicate that ¹J_CH depends primarily on , and that ¹J_CH may be useful as a qualitative probe for secondary structure. Comparison of ¹J_CH coupling constants measured in free calmodulin and in its complex with a 26-aminoacid peptide fragment of myosin light-chain kinase confirm that the calmodulin secondary structure is retained upon complexation but that disruption of the middle part of the central helix is even more extensive than in free calmodulin. Supplementary material available from the authors: One table listing 352 ¹J_CH and ¹J-values, together with ,-values for 203 residues of known conformation. Two figures showing (a) a Ramachandran plot of the ,-values of 203 residues used in deriving ¹J(,), and (b) the r.m.s.d. ¹J(,) distribution.     

Measurement of one-bond 15N-13C′ dipolar couplings in medium sized proteins

A simple and accurate method is described for measurement of ¹ J _CN splittings in isotopically enriched proteins. The method is of the quantitative J correlation type, and the ¹ J _CN splitting is derived from the relative intensity in two 3D TROSY-HNCO spectra with ¹ J _CN dephasing intervals of 1/(2¹ J _CN) (reference intensity) and 1/¹ J _CN (residual intensity). If the two spectra are recorded under identical conditions and with the same number of scans, the random error in the ¹ J _CN value extracted in this manner is inversely related to the signal-to-noise (S/N) in the reference spectrum. A S/N of 30:1 in the reference spectrum yields random errors of less than 0.2 Hz in the extracted ¹ J _CN value. Dipolar couplings obtained from the difference in ¹ J _CN splitting in the isotropic and liquid crystalline phase for the C-terminal domain of calmodulin are in excellent agreement with its 1.68-Å crystal structure, but agree considerably less with the 2.2-Å structure.     

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.     

One-bond carbon-proton coupling constants: Angular dependence in β-linked oligosaccharides

Summary The angular dependence of¹J_C,H in model compounds related to -linked oligosaccharides has been established by FPT INDO quantum chemical calculations. Values calculated for models of (1 1)-, (1 2)-, (1 3)- and (1 4)-linked disaccharides were compared, and the effect of the orientation of HO-2 elucidated. The angular dependence of¹J_C,H on the torsional angles ^H and ^H and the solvent dielectric constant (s) was characterized in the form:¹J_C,H = A cos2+B cos + C sin2 + D since + E + Fe. The¹J_C,H values, measured by DEPT methods for C-1-H-1 and C-X-H-X in cellobiose, cyclic trisaccharide and hexopyranoses were used to adjust the calculated angular dependences. Based on the occurrence of the conformers for agarobiose, neoagarobiose, mannobiose and methyl -xylobioside, the thermodynamically averaged <¹J_C,H > values were calculated. The results obtained (<¹J_C-1,H-1 > 162.4, <¹J_{C-4, H-4} > 147.6 Hz for methyl -xylobioside; <¹J_C-1,H-1 > 162.4 and <¹J_C-4,H-4] > 147.6 Hz for mannobiose; <¹J_C-1,H-1 > 162.8 Hz for neo agarobiose and <¹J_C-1,H-1 > 163.2 Hz for agarobiose) agree well with the experimental values of 162.7, 147.5, 160.4, 147.2, 160.9 and 165.7 Hz, respectively.     

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).     

Human λ light chain locus: Organization and DNA sequences of three genomicJ regions

Evidence for the genomic organization of human lambda light chain joining (J) region gene segments is presented. A mouse J probe was used in Southern hybridizations to localize joining region sequences in a cosmid clone containing the genomic cluster of six human lambda constant (C) region gene segments. The results of these hybridizations suggest the presence of at least one J gene segment upstream from each constant region gene segment. The DNA sequences indicate that the human JI, J2, and J3 gene segments have consensus nonamer and heptamer sequences, proposed to be involved in V-J joining, are capable of encoding the known amino acid sequences for the respective J peptides, and have a sequence which could give functional RNA splice site at the end of their coding regions. Our data show that a single functional J is located 1.3 or 1.6 kb upstream of each of the C gene segments known to encode the Mcg, Kern^– Oz^–, and Kern^–Oz⁺ isotypes. Therefore, the gene organization of this region of the human lambda locus is J1 CI -J2C2-J3C3. The DNA sequences ofJ 1,J 2, andJ 3 presented in this paper establish that a singleJ gene segment precedes each expressed C gene segment, and support a model for the evolution of the human JC clusters where JICI andJ2C2-J3C3. arose from different ancestral JC units.     

Quantification of soil carbon inputs under elevated CO2: C3 plants in a C4 soil

The objective of this investigation was to quantify the differences in soil carbon stores after exposure of birch seedlings (Betula pendula Roth.) over one growing season to ambient and elevated carbon dioxide concentrations. One-year-old seedling of birch were transplanted to pots containing C₄ soil derived from beneath a maize crop, and placed in ambient (350 L L^–1) and elevated (600 L L^–1) plots in a free-air carbon dioxide enrichment (FACE) experiment. After 186 days the plants and soils were destructively sampled, and analysed for differences in root and stem biomass, total plant tissue and soil C contents and ¹³C values. The trees showed a significant increase (+50%) in root biomass, but stem and leaf biomasses were not significantly affected by treatment. C isotope analyses of leaves and fine roots showed that the isotopic signal from the ambient and elevated CO₂ supply was sufficiently distinct from that of the C₄ soil to enable quantification of net root C input to the soil under both ambient and elevated CO₂. After 186 days, the pots under ambient conditions contained 3.5 g of C as intact root material, and had gained an additional 0.6 g C added to the soil through root exudation/turnover; comparable figures for the pots under elevated CO₂ were 5.9 g C and 1.5 g C, respectively. These data confirm the importance of soils as an enhanced sink for C under elevated atmospheric CO₂ concentrations. We propose the use of C₄ soils in elevated CO₂ experiments as an important technique for the quantification of root net C inputs under both ambient and elevated CO₂ treatments.     

Sugar conformation of a stereospecific 2′-R or 2′-S deuterium-labeled DNA decamer studied with proton-proton J coupling constants

The sugar conformation of a DNA decamer was studied with proton-proton ³J coupling constants. Two samples, one comprising stereospecifically labeled 2-R-²H for all residues and the other 2-S-²H, were prepared by the method of Kawashima et al. [J. Org. Chem. (1995) 60, 6980–6986; Nucleosides Nucleotides (1995) 14, 333–336], the deuterium labeling being highly stereospecific 99% for all 2-²H, 98% for 2-²H of A, C, and T, and 93% for 2-²H of G). The ³J values of all H1-H2 and H1-H2 pairs, and several H2-H3 and H2-H3 pairs were determined by line fitting of 1D spectra with 0.1–0.2 Hz precision. The observed J coupling constants were explained by the rigid sugar conformation model, and the sugar conformations were found to be between C3-exo and C2-endo with _m values of 26° to 44°, except for the second and 3 terminal residues C2 and C10. For the C2 and C10 residues, the lower fraction of S-type conformation was estimated from J_H1H2 and J_H1H2 values. For C10, the N–S two-site jump model or Gaussian distribution of the torsion angle model could explain the observed J values, and 68% S-type conformation or C1-exo conformation with 27° distribution was obtained, respectively. The differences between these two motional models are discussed based on a simple simulation of J-coupling constants.     

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).     

Simplified typing of mouse hemoglobin (Hbb) phenotypes using cystamine

Cellulose acetate electrophoresis of mouse hemoglobins modified with the disulfide reagent cystamine permits rapid, unequivocal discrimination of all combinations of the codominant mouse hemoglobin single (Hbb ^s ) and diffuse (Hbb ^d and Hbb ^p ) alleles. The single, diffuse major, diffuse d-minor, and diffuse p-minor adult hemoglobins are all resolved by this method, which depends on the presence of a cysteine in the chains of diffuse mice which is not found in the chain of single mice.This work was supported by research grants ACS-VC58 and NIH CA-01074. The Jackson Laboratory is fully accredited by the American Association for Accreditation of Laboratory Animal Care.