Oligomerization and conformation change in solutions of calf lens gamma II-crystallin. Results from 1/T1 nuclear magnetic relaxation dispersion profiles.

From analyses of the magnetic field dependence of 1/T1 (nuclear magnetic relaxation dispersion [NMRD] profiles) of water protons in solutions of highly purified calf lens gamma II-crystallin, we find that monomers form oligomers at relatively low concentrations, which increase in size with increasing concentration and decreasing temperature. At approximately 16% by volume and -4 degrees C, the mean oligomeric molecular weight is approximately 120-fold greater than the monomeric value of 20 kD. Below this concentration, there is no indication of any substantive change in conformation of the monomeric subunits. At higher concentrations, the tertiary structure of the monomer appears to reconfigure rather abruptly, but reversibly, as evidenced by the appearance of spectra-like 14N peaks in the NMRD profiles. The magnitudes of these peaks, known to arise from cross-relaxation of water protons through access to amide (NH) moieties of the protein backbone, indicate that the high concentration conformation is not compact, but open and extended in a manner that allows enhanced interaction with solvent. The data are analogous to those found for homogenates of calf and chicken lens (Beaulieu, C. F., J. I. Clark, R. D. Brown III, M. Spiller, and S. H. Koenig. 1988. Magn. Reson. Med. 8:47-57; Beaulieu, C. F., R. D. Brown III, J. I. Clark, M. Spiller, and S. H. Koenig. 1989. Magn. Reson. Med. 10:62-72). This unusually large dependence of oligomeric size and conformation on concentration in the physiological range is suggested as the mechanism by which osmotic equilibrium is maintained, at minimal metabolic expense, in the presence of large gradients of protein concentration in the lens in vivo (cf Vérétout and Tardieu, 1989. Eur. Biophys. J. 17:61-68). Finally, the results of the NMRD data provide a ready explanation of the low temperature phase transition, and "cold-cataract" separation of phases, observed in gamma II-crystallin solutions; we suggest that the phases that separate are the two major conformers detected by NMRD.     

Intermolecular protein interactions in solutions of calf lens alpha-crystallin. Results from 1/T1 nuclear magnetic relaxation dispersion profiles.

From analyses of the magnetic field dependence of 1/T1 (NMRD profiles) of water protons in solutions of calf lens alpha-crystallin at several concentrations, we find two regimes of solute behavior in both cortical and nuclear preparations. Below approximately 15% vol/vol protein concentration, the solute molecules appear as compact globular proteins of approximately 1,350 (cortical) and approximately 1,700 (nuclear) kD. At higher concentrations, the effective solute particle size increases, reversibly, as evidenced by the appearance of spectra-like 14N peaks in the NMRD profiles and a change in the field and temperature dependence of 1/T1. At these higher concentrations, the profiles are very similar to those of calf gamma II-crystallin, a crystallin that undergoes an analogous transition near approximately 15% protein (Koenig, S. H., C.F. Beaulieu, R. D. Brown III, and M. Spiller, 1990. Biophys. J. 57:461-469). By comparison with recent analyses of NMRD results for solutions of immobilized proteins as models for the transition from protein solutions to tissue (Koenig, S. H., and R. D. Brown III. 1991. Prog. NMR Spectr. 22:487-567), we argue that alpha-crystallin solute behaves as aggregates approximately greater than 50,000 kD as protein concentration is progressively increased above 15%. Finally, the concentration dependence of the NMRD profiles of alpha- and gamma II-crystallin can readily explain recent osmotic pressure data, in particular the intersection of the respective pressure curves at approximately 23% vol/vol (Vérétout, F., and A. Tardieu. 1989. Eur. Biophys. J. 17:61-68).     

Proton and deuteron nuclear magnetic relaxation dispersion studies of Ca2+-Mn2+-lentil lectin and Ca2+-Mn2+-pea lectin: evidence for a site of solvent exchange in common with concanavalin A

Measurements of the magnetic field dependence of the longitudinal magnetic relaxation rates (NMRD profiles) of solvent protons and deuterons led to the discovery of two classes of solvent binding sites in Ca2+-Mn2+-concanavalin A (CMPL) [Koenig, S. H., Brown, R. D., III, & Brewer, C. F. (1985) Biochemistry (second of three papers in this issue)]. In this paper, we compare proton and deuteron NMRD profiles of Ca2+-Mn2+-lentil lectin (CMLcH) and Ca2+-Mn2+-pea lectin (CMPSA) with those of CMPL. All three metalloproteins are D-mannose/D-glucose-specific lectins that have a high degree of structural similarity and require the metal ions for their biological activities. We have developed a method for the preparation of fully active metal ion derivatives of lentil lectin (LcH) and pea lectin (PSA), including the diamagnetic derivatives Ca2+-Zn2+-LcH and Ca2+-Zn2+-PSA [Bhattacharyya, L., Brewer, C. F., Brown, R. D., III, & Koenig, S. H.(1984) Biochem. Biophys. Res. Commun. 124, 857-862]. The behavior of these two lectins with regard to their NMRD profiles is essentially identical, for both the paramagnetic and diamagnetic forms. Together with CMPL, all three lectins have a common paramagnetic contribution with a negative temperature dependence of the rates, while CMPL contributes an additional component with a positive temperature dependence. The common contribution derives from the class of fast exchanging water molecules observed in the proton NMRD profile of CMPL (Koenig et al., 1985); their protons are calculated to be relatively remote from the Mn2+ ions (4.4 A for CMPL and 5.5 A for LcH and PSA).(ABSTRACT TRUNCATED AT 250 WORDS)     

Two-dimensional magnetization exchange spectroscopy of Anabaena 7120 ferredoxin. Nuclear Overhauser effect and electron self-exchange cross peaks from amino acid residues surrounding the 2Fe-2S* cluster

Hyperfine 1H NMR signals of the 2Fe-2S* vegetative ferredoxin from Anabaena 7120 have been studied by two-dimensional (2D) magnetization exchange spectroscopy. The rapid longitudinal relaxation rates of these signals required the use of very short nuclear Overhauser effect (NOE) mixing times (0.5-20 ms). The resulting pattern of NOE cross-relaxation peaks when combined with previous 1D NOE results [Dugad, L. B., La Mar, G. N., Banci, L., & Bertini, I. (1990) Biochemistry 29, 2263-2271] led to elucidation of the carbon-bound proton spin systems from each of the four cysteines ligated to the 2Fe-2S* cluster in the reduced ferredoxin. Additional NOE cross peaks were observed that provide information about other amino acid residues that interact with the iron-sulfur cluster. NOE cross peaks were assigned tentatively to Leu27, Arg42, and Ala43 on the basis of the X-ray coordinates of oxidized Anabaena 7120 ferredoxin [Rypniewski, W.R., Breiter, D.R., Benning, M.M., Wesenberg, G., Oh, B.-H., Markley, J.L., Rayment, I., & Holden, H. M. (1991) Biochemistry 30, 4126-4131]. Three chemical exchange cross peaks were detected in magnetization exchange spectra of half-reduced ferredoxin and assigned to the 1H alpha protons of Cys49 and Cys79 [both of whose sulfur atoms are ligated to Fe(III)] and Arg42 (whose amide nitrogen is hydrogen-bonded to one of the inorganic sulfurs of the 2Fe-2S* cluster). The chemical exchange cross peaks provide a means of extending assignments in the spectrum of reduced ferredoxin to assignments in the spectrum of the oxidized protein.(ABSTRACT TRUNCATED AT 250 WORDS)     

Proton longitudinal relaxation investigation of histidyl residues in human normal adult hemoglobin.

The longitudinal relaxation of the C2 protons of surface histidyl residues as well as other aromatic protons of human normal adult deoxyhemoglobin investigated at 360 MHz is discussed in terms of the theory proposed by Kalk and Berendsen for the proton longitudinal relaxation in proteins (Kalk, A., and H.J.C. Berendsen. 1976. J. Magn. Reson. 24:343-366). The role of the four paramagnetic iron atoms of deoxyhemoglobin as fast-relaxing sinks for the overall proton longitudinal relaxation is evaluated according to the model proposed by Bloembergen for the relaxation of nuclei in crystals containing paramagnetic centers (Bloembergen, N. 1949. Physica. 15:386-426). The results suggest that the effectiveness of the paramagnetic iron atoms of deoxyhemoglobin for the overall proton longitudinal relaxation is reduced as a result of slower spin diffusion and wide distribution of methyl groups within the hemoglobin molecule. Thus, deoxyhemoglobin provides a good model for investigating the influence of cross relaxation on proton longitudinal relaxation in proteins at the slow motion limit and in the presence of paramagnetic centers. For the C2 protons of surface histidyl residues, we show that the cross relaxation resulting from the interresidue dipolar interaction makes an important contribution to their longitudinal relaxation.     

Identification and localization of bound internal water in the solution structure of interleukin 1 beta by heteronuclear three-dimensional 1H rotating-frame Overhauser 15N-1H multiple quantum coherence NMR spectroscopy

The presence and location of bound internal water molecules in the solution structure of interleukin 1 beta have been investigated by means of three-dimensional 1H rotating-frame Overhauser 1H-15N multiple quantum coherence spectroscopy (ROESY-HMQC). In this experiment through-space rotating-frame Overhauser (ROE) interactions between NH protons and bound water separated by less than or equal to 3.5 A are clearly distinguished from chemical exchange effects, as the cross-peaks for these two processes are of opposite sign. The identification of ROEs between NH protons and water is rendered simple by spreading out the spectrum into a third dimension according to the 15N chemical shift of the directly bonded nitrogen atoms. By this means, the problems that prevent, in all but a very few limited cases, the interpretation, identification, and assignment of ROE peaks between NH protons and water in a 2D 1H-1H ROESY spectrum of a large protein such as interleukin 1 beta, namely, extensive NH chemical shift degeneracy and ROE peaks obscured by much stronger chemical exchange peaks, are completely circumvented. We demonstrate the existence of 15 NH protons that are close to bound water molecules. From an examination of the crystal structure of interleukin 1 beta [Finzel, B. C., Clancy, L. L., Holland, D. R., Muchmore, S. W., Watenpaugh, K. D., & Einspahr, H. M. (1989) J. Mol. Biol. 209, 779-791], the results can be attributed to 11 water molecules that are involved in interactions bridging hydrogen-bonding interactions with backbone amide and carbonyl groups which stabilize the 3-fold pseudosymmetric topology of interleukin 1 beta and thus constitute an integral part of the protein structure in solution.     

Classes of hydration sites at protein-water interfaces: the source of contrast in magnetic resonance imaging.

Immobilized protein solute, approximately 20 wt %, alters the longitudinal and transverse nuclear magnetic relaxation rates 1/T1 and 1/T2 of solvent water protons in a manner that makes their values indistinguishable from those of a typical human tissue. There is now a quantitative theory at the molecular level (S.H. Koenig and R. D. Brown III (1993) Magn. Reson. Med. 30:685-695) that accounts for this, as a function of magnetic field strength, in terms of several distinguishable classes of water-binding sites at the protein-water interface at which significant relaxation and solute-solvent transfer of proton Zeeman energy occur. We review the arguments that these several classes of sites, characterized by widely disparate values of the resident lifetimes tau M of the bound waters, are associated with different numbers of hydrogen bonds that stabilize the particular protein-water complex. The sites that dominate relaxation-and produce contrast in magnetic resonance imaging (MRI), which derives from 1/T1 and 1/T2 of tissue water protons-have tau M approximately 10(-6)s. These, which involve four hydrogen bonds, occupy < or = 1% of the protein-water interface. Sites that involve three bonds, although more numerous, have < or = 20% smaller intrinsic effect on relaxation. The greater part of the "traditional" hydration monolayer, with even shorter-lived hydrogen-bonded waters, has little influence on solvent relaxation and is relatively unimportant in MRI. Finally, we argue, from the data, that most of the protein of tissue (a typical tissue is mostly protein) must be rotationally immobile (with Brownian rotational relaxation times slower than that of a 5 x 10(7) Da (very heavy) globular protein). We propose a functional basis for this immobilization ("cytoplasmic order"), and then indicate a way in which this order can break down ("cytoplasmic chaos") as a result of neoplastic transformation (cancer) and alter water-proton rates of pathological tissue and, hence, image contrast in MRI.     

14N1H and 2H1H cross-relaxation in hydrated proteins.

The frequency dependence of the proton spin-lattice relaxation time T1 of solid hydrated bovine serum albumin and alpha-chymotrypsin has been measured over 4.5 decades in the range 10(4) to 3 X 10(8) Hz mainly by the aid of the field-cycling technique. The comparison between H2O- and D2O-hydrated samples permitted the distinction of exchangeable and unexchangeable protons. In all cases the 14N1H cross-relaxation dips due mainly to the amide groups have been observed. In addition, in the case of the deuterium exchanged proteins a 2H1H quadrupole dip appears. The amide groups act as relaxation sinks due to the coupling of the amide proton to 14N and adjacent protons. Outside of the dip regions the proton-proton coupling dominates. The fluctuations of the 14N1H and 1H1H interactions are of a different type. The unexchangeable protons show a T1 dispersion outside of the quadrupole dip regions given by the exceptional power law T1 approximately v0.75 +/- 0.05. It is shown that apart from structural information of the 14N spectra, 14N1H cross-relaxation spectroscopy permits the determination of correlation times in the range 10(-7) s less than tau less than 10(-4)S.     

Assignments of backbone 1H, 13C, and 15N resonances and secondary structure of ribonuclease H from Escherichia coli by heteronuclear three-dimensional NMR spectroscopy.

The assignments of individual magnetic resonances of backbone nuclei of a larger protein, ribonuclease H from Escherichia coli, which consists of 155 amino acid residues and has a molecular mass of 17.6 kDa are presented. To remove the problem of degenerate chemical shifts, which is inevitable in proteins of this size, three-dimensional NMR was applied. The strategy for the sequential assignment was, first, resonance peaks of amides were classified into 15 amino acid types by 1H-15N HMQC experiments with samples in which specific amino acids were labeled with 15N. Second, the amide 1H-15N peaks were connected along the amino acid sequence by tracing intraresidue and sequential NOE cross peaks. In order to obtain unambiguous NOE connectivities, four types of heteronuclear 3D NMR techniques, 1H-15N-1H 3D NOESY-HMQC, 1H-15N-1H 3D TOCSY-HMQC, 13C-1H-1H 3D HMQC-NOESY, and 13C-1H-1H 3D HMQC-TOCSY, were applied to proteins uniformly labeled either with 15N or with 13C. This method gave a systematic way to assign backbone nuclei (N, NH, C alpha H, and C alpha) of larger proteins. Results of the sequential assignments and identification of secondary structure elements that were revealed by NOE cross peaks among backbone protons are reported.     

Assignment of the backbone 1H and 15N NMR resonances of bacteriophage T4 lysozyme

The proton and nitrogen (15NH-H alpha-H beta) resonances of bacteriophage T4 lysozyme were assigned by 15N-aided 1H NMR. The assignments were directed from the backbone amide 1H-15N nuclei, with the heteronuclear single-multiple-quantum coherence (HSMQC) spectrum of uniformly 15N enriched protein serving as the master template for this work. The main-chain amide 1H-15N resonances and H alpha resonances were resolved and classified into 18 amino acid types by using HMQC and 15N-edited COSY measurements, respectively, of T4 lysozymes selectively enriched with one or more of alpha-15N-labeled Ala, Arg, Asn, Asp, Gly, Gln, Glu, Ile, Leu, Lys, Met, Phe, Ser, Thr, Trp, Tyr, or Val. The heteronuclear spectra were complemented by proton DQF-COSY and TOCSY spectra of unlabeled protein in H2O and D2O buffers, from which the H beta resonances of many residues were identified. The NOE cross peaks to almost every amide proton were resolved in 15N-edited NOESY spectra of the selectively 15N enriched protein samples. Residue specific assignments were determined by using NOE connectivities between protons in the 15NH-H alpha-H beta spin systems of known amino acid type. Additional assignments of the aromatic proton resonances were obtained from 1H NMR spectra of unlabeled and selectively deuterated protein samples. The secondary structure of T4 lysozyme indicated from a qualitative analysis of the NOESY data is consistent with the crystallographic model of the protein.     

Solution structural characteristics of cyanometmyoglobin: resonance assignment of heme cavity residues by two-dimensional NMR

Steady-state nuclear Overhauser effects (NOE), two-dimensional (2D) nuclear Overhauser effect spectroscopy (NOESY), and 2D spin correlation spectroscopy (COSY) have been applied to the fully paramagnetic low-spin, cyanide-ligated complex of sperm whale ferric myoglobin to assign the majority of the heme pocket side-chain proton signals and the remainder of the heme signals. It is shown that the 2D NOESY map reveals essentially all dipolar connectivities observed in ordinary 1D NOE experiments and expected on the basis of crystal coordinates, albeit often more weakly than in a diamagnetic analogue. For extremely broad (approximately 600-Hz) and rapidly relaxing (Tf1 approximately 3 ms) signals which show no NEOSY peaks, we demonstrate that conventional steady-state NOEs obtained under very rapid pulsing conditions still allow detection of the critical dipoar connectivities that allow unambiguous assignments. The COSY map was found to be generally less useful for the hyperfine-shifted residues, with cross peaks detected only for protons greater than 6 A from the iron. Nevertheless, numerous critical COSY cross peaks between strongly hyperfine-shifted peaks were resolved and assigned. In all, 95% (53 of 56 signals) of the total proton sets within approximately 7.5 A of the iron, the region experiencing the strongest hyperfine shifts and paramagnetic relaxation, are now unambiguously assigned. Hence it is clear that the 2D methods can be profitably applied to paramagnetic proteins. The scope and limitations of such application are discussed. The resulting hyperfine shift pattern for the heme confirmed expectations based on model compounds. In contrast, while exhibiting fortuitous 1H NMR spectral similarities, a major discrepancy was uncovered between the hyperfine shift pattern of the axially bound (F8 histidyl) imidazole in the protein and that of the imidazole in a relevant model compound [Chacko, V.P., & La Mar, G. N. (1982) J. Am. Chem. Soc. 104, 7002-7007], providing direct evidence for a protein-based deformation of axial bonding in the protein.     

Conversions of poly(2-aminodeoxyadenylate-5-halodeoxyuridylate) from B to A forms in high salt. An NMR and circular dichroism study

Proton one- and two-dimensional nuclear Overhauser enhancement (1D and 2D NOE) spectroscopy has been used to demonstrate that poly(d2NH2A-d5IU) and poly(d2NH2A-d5BrU) are converted from the B to the A conformation in high salt, as found previously for poly(d2NH2A-dT) [Borah, B., Cohen, J. S., Howard, F. B., & Miles, H. T. (1985) Biochemistry 24, 7456-7462]. The 2D NOE and 1D NOE spectra exhibit strong base proton (H8,H6)-H3' cross relaxation, suggesting short interproton distances. These results are indicative of a C3'-endo sugar pucker for both purine and pyrimidine residues in an A or closely related structure. The circular dichroism and UV spectra are consistent with the interpretation of an A conformation in high salt.     

Halide binding by the D212N mutant of Bacteriorhodopsin affects hydrogen bonding of water in the active site

Bacteriorhodopsin (BR), a membrane protein found in Halobacterium salinarum, functions as a light-driven proton pump. The Schiff base region has a quadrupolar structure with positive charges located at the protonated Schiff base and Arg82, and the counterbalancing negative charges located at Asp85 and Asp212. The quadropole inside the protein is stabilized by three water molecules, forming a roughly planar pentagonal cluster composed of these waters and two oxygens of Asp85 and Asp212 (one from each carboxylate side chain). It is known that BR lacks proton-pumping activity if Asp85 or Asp212 is neutralized by mutation, but binding of Cl- has different functional effects in mutants at these positions. Binding of Cl- to D85T converts into a chloride ion pump (Sasaki, J., Brown, L. S., Chon, Y.-S., Kandori, H., Maeda, A., Needleman, R., and Lanyi, J. K. (1995) Science 269, 73-75). On the other hand, photovoltage measurements suggested that binding of Cl- to D212N restores the proton-pumping activity at low pH (Moltke, S., Krebs, M. P., Mollaaghababa, R., Khorana, H. G., and Heyn, M. P. (1995) Biophys. J. 69, 2074-2083). In this paper, we studied halide-bound D212N mutant BR in detail. Light-induced pH changes in a suspension of proteoliposomes containing D212N(Cl-) at pH 5 clearly showed that Cl- restores the proton-pumping activity. Spectral blue-shift induced by halide binding to D212N indicates that halides affect the counterion of the protonated Schiff base, whereas much smaller halide dependence of the lambdamax than in D85T suggests that the binding site is distant from the chromophore. In fact, the K minus BR difference Fourier-transform infrared (FTIR) spectra of D212N at 77 K exhibit little halide dependence for vibrational bands of retinal and protein. The only halide-dependent bands were the C=N stretch of Arg82 and some water O-D stretches, suggesting that these groups constitute a halide-binding pocket. A strongly hydrogen-bonded water molecule is observed for halide-bound D212N, but not for halide-free D212N, which is consistent with our hypothesis that such a water molecule is a prerequisite for proton-pumping activity of rhodopsins. We concluded that halide binding near Arg82 in D212N restores the water-containing hydrogen-bonding network in the Schiff base region. In particular, the ion pair formed by the Schiff base and Asp85 through a strongly hydrogen-bonded water is essential for the proton-pumping activity of this mutant and may be controlled by the halide binding to the distant site.     

Two-dimensional 1H, 15N NMR investigation of uniformly 15N-labeled lac repressor headpiece.

15N uniformly labeled lac repressor and lac repressor headpiece were prepared. 15N NMR spectra of lac repressor were shown resolution inadequate for detailed study while the data showed that the 15N labeled N-terminal part of the protein is quite suitable for this type of study allowing future investigation of the specific interaction of the lac repressor headpiece with the lac operator. We report here the total assignment of proton 1H and nitrogen 15NH backbone resonances of this headpiece in the free state. Assignments of the 15N resonances of the protein were obtained in a sequential manner using heteronuclear multiple quantum coherence (HMQC), relayed HMQC nuclear Overhauser and relayed HMQC-HOHAHA spectroscopy. More than 80 per cent of residues were assigned by their 15NH(i)-N1H(i + 1) and 15NH(i)-N1H(i - 1) connectivities. Values of the 3JNH alpha splitting for 39 of the 51 residues of the headpiece were extracted from HMQC and HMQC-J. The observed 15NH(i)-C beta H cross peaks and the 3JNH alpha coupling constants values are in agreement with the three alpha-helices previously described [Zuiderweg, E.R.P., Scheek, R.M., Boelens, R., van Gunsteren, W.F. and Kaptein, R., Biochimie 67, 707 (1985)]. The 3JNH alpha coupling constants can be now used for a more confident determination of the lac repressor headpiece. From these values it is shown that the geometry of the ends of the second and third alpha-helices exhibit deviation from the canonical alpha-helix structure. On the basis of NOEs and 3JNH alpha values, the geometry of the turn of the helix-turn-helix motif is discussed.     

1H-NMR studies of high-potential iron-sulfur protein from the purple phototrophic bacterium, Rhodospirillum tenue

The high-potential iron-sulfur protein (HiPIP) from Rhodospirillum tenue (strain 3761) shows only a weak (20-25%) sequence similarity to HiPIPs from Chromatium vinosum, Ectothiorhodospira halophila and Ectothiorhodospira vacuolata, including the strict conservation of only two of the twelve residues assumed to be in the 4Fe-4S cluster packing region [Tedro, S. M., Meyer, T. E. and Kamen, M. D. (1979) J. Biol. Chem. 254, 1495-1500]. In spite of these differences, the general range and distribution of hyperfine-shifted 1H-NMR peaks of oxidized and reduced R. tenue HiPIP resemble those of E. halophila HiPIP I [Krishnamoorthi, R., Markley, J. L., Cusanovich, M. A., Pryzycieki, C. T. and Meyer, T. E. (1986) Biochemistry 25, 60-67]. Temperature- and pH-dependence and longitudinal relaxation behavior were determined for hyperfine-shifted peaks of the oxidized protein. Tentative assignments of peaks to ligands and aromatic residues suggest the presence of common apoprotein-active-site interactions in these proteins. Differences occur in the pattern of paramagnetically shifted peaks attributed to hydrogens bonded to the 4Fe-4S cluster. Hyperfine-shifted peaks of R. tenue HiPIP are not perturbed by pH changes in the range 5-9. In contrast, those of the C. vinosum protein exhibit a pH-dependence of chemical shifts that has been attributed to the titration of His42 [Nettesheim, D. G., Meyer, T. E., Feinberg, B. A. and Otvos, J. D. (1983) J. Biol. Chem. 258, 8235-8239]. Since R. tenue HiPIP contains no histidine, the present observation confirms the above hypothesis.     

NMR studies of the backbone protons and secondary structure of pentapeptide and heptapeptide substrates bound to bovine heart protein kinase

The conformations of enzyme-bound pentapeptide (Arg-Arg-Ala-Ser-Leu) and heptapeptide (Leu-Arg-Arg-Ala-Ser-Leu-Gly) substrates of protein kinase have been studied by NMR in quaternary complexes of the type (Formula: see text). Paramagnetic effects of Mn2+ bound at the inhibitory site of the catalytic subunit on the longitudinal relaxation rates of backbone Ca protons, as well as on side-chain protons of the bound pentapeptide and heptapeptide substrates, have been used to determine Mn2+ to proton distances which range from 8.2 to 12.4 A. A combination of the paramagnetic probe-T1 method with the Redfield 2-1-4-1-2 pulse sequence for suppression of the water signal has been used to measure distances from Mn2+ to all of the backbone amide (NH) protons of the bound pentapeptide and heptapeptide substrates, which range from 6.8 to 11.1 A. Paramagnetic effects on the transverse relaxation rates yield rate constants for peptide exchange, indicating that the complexes studied by NMR dissociate rapidly enough to participate in catalysis. Model-building studies based on the Mn2+-proton distances, as well as on previously determined distances from Cr3+-AMPPCP to side-chain protons [Granot, J., Mildvan, A.S., Bramson, H. N., & Kaiser, E. T. (1981) Biochemistry 20, 602], rule out alpha-helical, beta-sheet, beta-bulge, and all possible beta-turn conformations within the bound pentapeptide and heptapeptide substrates. The distances are fit only by extended coil conformations for the bound peptide substrates with a minor difference between the pentapeptides and heptapeptides in the phi torsional angle at Arg3C alpha and in psi at Arg2C alpha. An extended coil conformation, which minimizes the number of interactions within the substrate, would facilitate enzyme-substrate interaction and could thereby contribute to the specificity of protein kinase.     

3d haro-Noesy-ch3nh and caro-Noesy-ch3nh Experiments for Double Labeled Proteins

Precision in the determination of the 3D structures of proteins by NMR depends on obtaining an adequate number of NOE restraints. Ambiguity in the assignment of NOE cross peaks between aromatic and other protons is an impediment to high quality structure determination. Two pulse sequences, 3D H_aro-NOESY-CH₃NH and 3D C_aro-NOESY-CH₃NH, based on a modification of a technique for simultaneous detection of ¹³C-¹H (of CH₃) and ¹⁵N-¹H correlations in one measurement, are proposed in the present work. These 3D experiments, which are optimized for resolution in the ¹³C and ¹⁵N dimensions, provide NOE information between aromatic protons and methyl or amide protons. CH₂ moieties are filtered out and the CH groups in aromatic rings are selected, allowing their NOE cross peaks to be unambiguously assigned. Unambiguous NOEs connecting aromatic and methyl or amide protons will provide important restraints for protein structure calculations.     

31P NMR relaxation studies of the activation of the coenzyme phosphate of glycogen phosphorylase. The role of motion of the bound phosphate.

Spin-lattice and spin-spin relaxation rates (1/T1 and 1/T2) have been determined for the catalytically essential coenzyme phosphate at the active site of glycogen phosphorylase in both activated (R state) and inactive (T state) conformations of the enzyme. Dipolar contributions to 31P relaxation due to exchangeable protons on the phosphate group have been determined by measurement of relaxation rates at different concentrations of H2O and D2O, and field dependence studies have been performed to estimate the contribution of chemical shift anisotropy to the remaining 31P relaxation in D2O. At 109 MHz, dipolar relaxation from exchangeable protons was found to account for 50% of the spin-lattice relaxation for activated phosphorylase in 75% H2O, the remainder being due to chemical shift anisotropy. The spin-lattice relaxation rates in D2O for R-state glycogen phosphorylase are very similar to those measured for other proteins of very different size such as actin (Brauer, M., and B. D. Sykes, 1981, Biochemistry. 20:6767-6775), alkaline phosphatase (Coleman, J. E., I. D. Armitage, J. F. Chlebowski, J. D. Otvos, and A. J. M. S. Uiterkamp, 1979), and phosphoglucomutase (Rhyu, G. I., W. J. Ray, Jr., and J. L. Markley, 1984, Biochemistry. 23:252-260). In inactive (T state) phosphorylase the spin-lattice relaxation rates were almost an order of magnitude slower, while the spin-spin relaxation rates were essentially identical. These results have been analyzed by calculating the theoretically expected 31P relaxation rates in the presence of internal motions that are included in the relaxation calculation using the model-free approach of Lipari and Szabo (1982, J. Am. Chem. Soc. 104:4564-4559).(ABSTRACT TRUNCATED AT 250 WORDS)     

Pulse sequences for detection of NH2···N hydrogen bonds in sheared G⋅A mismatches via remote, non-exchangeable protons

The non-detectability of NH...N hydrogen bonds in nucleic acids due to exchange broadened imino/amino protons has recently been addressed via the use of non-exchangeable protons for detecting internucleotide 2hJ(NN) couplings. In these applications, the appropriate non-exchangeable proton is separated by two bonds from the NH...N bond. In this paper, we extend the scope of this approach to protons which are separated by four bonds from the NH...N moiety. Specifically, we consider the case of the commonly occurring sheared G x A mismatch alignment, in which we use the adenine H2 proton to report on the (A)N6H6(1.2)...N3(G) hydrogen bond, in the presence of undetectable, exchange broadened N6H6(1.2) protons. Two sequences, the 'straight-through' (H6)N6N3H2 and 'out-and-back' H2N6N3 experiments, are presented for observing these correlations in H2O and D2O solution, respectively. The sequences are demonstrated on two uniformly 15N,13C labelled DNA samples: d(G1G2G3T4T5C6A7G8G9)2, containing a G3 x (C6-A7) triad involving a sheared G3 x A7 mismatch, and d(G1G2G3C4A5G6G7T8)4, containing an A5 x (G3 x G6 x G3 x G6) x A5 hexad involving a sheared G3 x A5 mismatch.