Solution NMR structure of the myosin phosphatase inhibitor protein CPI-17 shows phosphorylation-induced conformational changes responsible for activation.

Contractility of vascular smooth muscle depends on phosphorylation of myosin light chains, and is modulated by hormonal control of myosin phosphatase activity. Signaling pathways activate kinases such as PKC or Rho-dependent kinases that phosphorylate the myosin phosphatase inhibitor protein called CPI-17. Phosphorylation of CPI-17 at Thr38 enhances its inhibitory potency 1000-fold, creating a molecular on/off switch for regulating contraction. We report the solution NMR structure of the CPI-17 inhibitory domain (residues 35-120), which retains the signature biological properties of the full-length protein. The final ensemble of 20 sets of NMR coordinates overlaid onto their mean structure with r.m.s.d. values of 0.84(+/-0.22) A for the backbone atoms. The protein forms a novel four-helix, V-shaped bundle comprised of a central anti-parallel helix pair (B/C helices) flanked by two large spiral loops formed by the N and C termini that are held together by another anti-parallel helix pair (A/D helices) stabilized by intercalated aromatic and aliphatic side-chains. Chemical shift perturbations indicated that phosphorylation of Thr38 induces a conformational change involving displacement of helix A, without significant movement of the other three helices. This conformational change seems to flex one arm of the molecule, thereby exposing new surfaces of the helix A and the nearby phosphorylation loop to form specific interactions with the catalytic site of the phosphatase. This phosphorylation-dependent conformational change offers new structural insights toward understanding the specificity of CPI-17 for myosin phosphatase and its function as a molecular switch.

Target-induced conformational adaptation of calmodulin revealed by the crystal structure of a complex with nematode Ca(2+)/calmodulin-dependent kinase kinase peptide.

Calmodulin (CaM) is a ubiquitous calcium (Ca(2+)) sensor which binds and regulates protein serine/threonine kinases along with many other proteins in a Ca(2+)-dependent manner. For this multi-functionality, conformational plasticity is essential; however, the nature and magnitude of CaM's plasticity still remains largely undetermined. Here, we present the 1.8 A resolution crystal structure of Ca(2+)/CaM, complexed with the 27-residue synthetic peptide corresponding to the CaM-binding domain of the nematode Caenorhabditis elegans Ca(2+)/CaM-dependent kinase kinase (CaMKK). The peptide bound in this crystal structure is a homologue of the previously NMR-derived complex with rat CaMKK, but benefits from improved structural resolution. Careful comparison of the present structure to previous crystal structures of CaM complexed with unrelated peptides derived from myosin light chain kinase and CaM kinase II, allow a quantitative analysis of the differences in the relative orientation of the N and C-terminal domains of CaM, defined as a screw axis rotation angle ranging from 156 degrees to 196 degrees. The principal differences in CaM interaction with various peptides are associated with the N-terminal domain of CaM. Unlike the C-terminal domain, which remains unchanged internally, the N-terminal domain of CaM displays significant differences in the EF-hand helix orientation between this and other CaM structures. Three hydrogen bonds between CaM and the peptide (E87-R336, E87-T339 and K75-T339) along with two salt bridges (E11-R349 and E114-K334) are the most probable determinants for the binding direction of the CaMKK peptide to CaM.

Structural features of an influenza virus promoter and their implications for viral RNA synthesis.

The influenza A virus, a severe pandemic pathogen, has a segmented RNA genome consisting of eight single-stranded RNA molecules. The 5' and 3' ends of each RNA segment recognized by the influenza A virus RNA-dependent RNA polymerase direct both transcription and replication of the virus's RNA genome. Promoter binding by the viral RNA polymerase and formation of an active open complex are prerequisites for viral replication and proliferation. Here we describe the solution structure of this promoter as solved by multidimensional, heteronuclear magnetic resonance spectroscopy. Our studies show that the viral promoter has a significant dynamic nature and reveal an unusual displacement of an adenosine that forms a novel (A-A) x U motif and a C-A mismatch stacked in a helix. The characterized structural features of the promoter imply that the specificity of polymerase binding results from an internal RNA loop. In addition, an unexpected bending (46 +/- 10 degrees ) near the initiation site suggests the existence of a promoter recognition mechanism similar to that of DNA-dependent RNA polymerase and a possible regulatory function for the terminal structure during open complex formation.

Methods for sequential resonance assignment in solid, uniformly 13C, 15N labelled peptides: quantification and application to antamanide.

The application of adiabatic polarization-transfer experiments to resonance assignment in solid, uniformly 13C-15N-labelled polypeptides is demonstrated for the cyclic decapeptide antamanide. A homonuclear correlation experiment employing the DREAM sequence for adiabatic dipolar transfer yields a complete assignment of the C(alpha) and aliphatic side-chain 13C resonances to amino acid types. The same information can be obtained from a TOBSY experiment using the recently introduced P9(12)1 TOBSY sequence, which employs the J couplings as a transfer mechanism. A comparison of the two methods is presented. Except for some aromatic phenylalanine resonances, a complete sequence-specific assignment of the 13C and 15N resonances in antamanide is achieved by a series of selective or broadband adiabatic triple-resonance experiments. Heteronuclear transfer by adiabatic-passage Hartmann-Hahn cross polarization is combined with adiabatic homonuclear transfer by the DREAM and rotational-resonance tickling sequences into two- and three-dimensional experiments. The performance of these experiments is evaluated quantitatively.

Solid-phase synthesis of selectively labeled DNA: applications for multidimensional nuclear magnetic resonance spectroscopy.

The solid-phase chemical synthesis method has a strong advantage over the enzymatic method for preparing selectively labeled DNA oligomers. Atom-specific and fully labeled 2'-deoxynucleosides are economically prepared with routinely available isotope precursors using this synthetic route. Special DNA oligomers prepared by advanced labeling techniques are needed for advanced NMR applications, and chemical synthesis is the method of choice to respond to such demands. As a summary of this chapter, two tables are given. Table I lists the labeled nucleosides reported to be available by chemical syntheses. Table II lists the NMR studies using labeled DNA oligomers that were prepared by chemical syntheses.

[(13)C,(13)C]- and [(13)C,(1)H]-TROSY in a triple resonance experiment for ribose-base and intrabase correlations in nucleic acids.

A novel TROSY (transverse relaxation-optimized spectroscopy) element is introduced that exploits cross-correlation effects between (13)C-(13)C dipole-dipole (DD) coupling and (13)C chemical shift anisotropy (CSA) of aromatic ring carbons. Although these (13)C-(13)C effects are smaller than the previously described [(13)C,(1)H]-TROSY effects for aromatic (13)C-(1)H moieties, their constructive use resulted in further transverse relaxation-optimization by up to 15% for the resonances in a 17 kDa protein-DNA complex. As a practical application, two- and three-dimensional versions of the HCN triple resonance experiment for obtaining ribose-base and intrabase correlations in the nucleotides of DNA and RNA (Sklenar, V.; Peterson, R. D.; Rejante, M. R.; Feigon, J. J. Biomol. NMR 1993, 3, 721-727) have been implemented with [(13)C,(1)H]- and [(13)C,(13)C]-TROSY elements to reduce the rate of transverse relaxation during the polarization transfers between ribose (13)C1' and base (15)N1/9 spins, and between (13)C6/8 and N1/9 within the bases. The resulting TROSY-HCN experiment is user-friendly, with a straightforward, robust experimental setup. Compared to the best previous implementations of the HCN experiment, 2-fold and 5-fold sensitivity enhancements have been achieved for ribose-base and intrabase connectivities, respectively, for (13)C,(15)N-labeled nucleotides in structures with molecular weights of 10 and 17 kDa. TROSY-HCN experiments should be applicable also with significantly larger molecular weights. By using modified TROSY-HCN schemes, the origins of the sensitivity gains have been analyzed.

Slow motion in the CAA*TTG sequence of a DNA decamer duplex studied by NMR.

In DNA duplexes, pyrimidine-purine steps are believed to be flexible or conformationally unstable. Indeed, several DNA crystal structures exhibit a multitude of conformations for CpA*TpG steps. The question arises of whether this structural flexibility is accompanied by dynamical flexibility, i.e., a question pertaining to the energy barrier between conformations. Except for TpA steps, slow motions on the microsecond-to-millisecond time scale have not been detected in duplexes until now. In the present study, such slow motion was investigated by 1H, 13C, and 15N NMR relaxation measurements on a DNA decamer d(CATTTGCATC)*d(GATGCAAATG). The DNA decamer was enriched with 15% 13C and 98% 15N isotopes for each adenosine and guanosine residue. Three lines of evidence support the notion of slow motion in the CAA*TTG moiety. Analysis of (15)N relaxation showed that the order parameter, S2, of guanosine imino NH groups was about 0.8, similar to that of CH groups for this oligomer. The strong temperature dependence of guanosine NH S2 in the CAA*TTG sequence indicated the presence of a large-amplitude motion. Signals of adenosine H8 protons in the CAA*TTG sequence were broadened in 2D 1H NOESY spectra, which also suggested the existence of slow motion. As well as being smaller than for other adenine residues, the 1H T2 values exhibited a magnetic field strength dependence for all adenosine H8 signals in the ATTTG*CAAAT region, suggesting slow motions more pronounced at the first adenosine in the CAA*TTG sequence but extending over the CAAAT*ATTTG region. This phenomenon was further examined by the pulse field strength dependence of the 1H, 13C, and 15N T1rho values. 1H and 13C T1rho values showed a pulse field strength dependence, but 15N T1rho did not. Assuming a two-site exchange process, an exchange time constant of 20-300 micros was estimated for the first adenosine in the CAA sequence. The exact nature of this motion remains unknown.

H...N hydrogen bond lengths in double stranded DNA from internucleotide dipolar couplings.

The ratio of the internucleotide dipolar coupling and the corresponding one-bond imino 15N-1H dipolar coupling provides a measure for the N...H/H-N distance ratio. Measurements were carried out for a dodecamer, d(CGCGAATTCGCG)2, in which a C-G and an A-T basepair were uniformly enriched in 15N. When assuming H-bonds to be perfectly linear, dipolar data indicate time-averaged hydrogen bond lengths of 1.80 +/- 0.03 A for A-T and 1.86 +/- 0.02 A for C-G. When using H-bond orientations from high resolution X-ray data, H-bond lengths are about 0.1 A shorter.

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 (> or = 99% for all 2''-2H, > or = 98% for 2'-2H of A, C, and T, and > or = 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 phi(m) values of 26 degrees to 44 degrees, 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 JH1'H2' and JH1'H2'' 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 degrees distribution was obtained, respectively. The differences between these two motional models are discussed based on a simple simulation of J-coupling constants.

NMR structure of Streptomyces killer toxin-like protein, SKLP: further evidence for the wide distribution of single-domain betagamma-crystallin superfamily proteins.

A protein isolated from the culture supernatant of the soil bacterium, Streptomyces sp. F-287, exhibits cytocidal effects for both budding and fission yeasts, and causes morphological changes of yeasts and filamentous fungi. This protein, which was the first killer toxin-like protein for yeasts identified in the Streptomyces microorganism, was named SKLP (Streptomyces killer toxin-like protein). Since the amino acid sequence of the protein, as determined by sequential Edman degradations, seemed to be unique, we determined the structure by NMR spectroscopy. Although the actual target of SKLP in yeasts has not been determined yet, the structure might give us a clue to characterize the targets. The solution structure of SKLP determined by NMR, however, turned out to be a single-domain crystallin-like protein, with two Greek key motifs and a short extra beta-strand at the N terminus. The final ensemble of 20 NMR structures overlaid onto their mean coordinate with rmsd values of 0.32(+/-0.06) A for the backbone atoms involved in the secondary structure elements. As a yeast killer toxin, WmKT, isolated from the yeast strain Williopsis mrakii also has a Greek key beta-barrel fold, we have made a detailed comparison of the structural features of SKLP with the other crystallin superfamily proteins. It is very interesting that SKLP has a unique electrostatic potential distribution on the molecular surface. Namely, one surface of the beta-barrel fold in SKLP has a large negatively charged region, with an isolated positive charge of the Arg62 side-chain at the center. The edge of this surface is surrounded by positively charged residues, including Arg31, Arg65 and Arg74. The salient features of the charge distribution on this surface and the cluster of Arg residues might be related to the target binding of SKLP.

Synthesis of 5-substituted [N3-15N]-pyrimidine nucleosides: Developing model systems for NMR studies of substituent effects on the N-H...N hydrogen bond in duplex DNA.

The effects on various NMR parameters of substitutions, which may influence the hydrogen bond strengths of Watson-Crick-type base pairs, were investigated for DNA dodecamers containing 5-substituted-2'-deoxyuridine derivatives in oligomers, 5'-d(CGCGAATXCGCG)-3', where A and X were [ul-15N]-2'-deoxyadenosine and [3(-15)N]-2'-deoxyuridine derivatives. The substitution effects on the NMR parameters were linearly correlated with the pKa values of the 2'-deoxyuridine derivatives.

Reelin molecules assemble together to form a large protein complex, which is inhibited by the function-blocking CR-50 antibody.

Reelin is a key mediator of ordered neuronal alignment in the brain. Here, we demonstrate that Reelin molecules assemble with each other to form a huge protein complex both in vitro and in vivo. The Reelin-Reelin interaction clearly is inhibited by the function-blocking anti-Reelin antibody, CR-50, at a concentration known to inhibit Reelin function. This assembly is mediated by electrostatic interaction of the CR-50 epitope region. Recombinant CR-50 epitope fragments spontaneously constitute a soluble, string-like homopolymer with a regularly repeated structure composed of more than 40 monomers. Mutated Reelin, which lacks the CR-50 epitope region, cannot form a homopolymer and fails to induce efficient tyrosine phosphorylation of Disabled 1 (Dab1), which should occur to transduce the Reelin signal. These data suggest that Reelin exerts its biological function by composing a large protein assembly driven by the CR-50 epitope region, proposing a novel model of the Reelin signaling in neurodevelopment.

Three-dimensional structure determination of a uniformly labeled molecule by frequency-selective dipolar recoupling under magic-angle spinning.

The complete three-dimensional (3D) structure of a glycylisoleucine (Gly-Ile) molecule was determined by individually measuring six dihedral angles with a frequency-selective homonuclear dipolar recoupling method, R2TR (rotational resonance in the tilted rotating frame), using a powder sample of diluted uniformly 13C,15N-labeled Gly-Ile. Each dihedral angle was obtained by recoupling a dipolar interaction between three or four bonds distant spins concerned or observing a dipolar correlation 2D powder pattern. The 3D structure of a Gly-Ile molecule was also determined by X-ray crystallography, and a good agreement with the NMR result was obtained. The results demonstrate that the R2TR method in a uniformly labeled powder sample can provide the 3D structure without the need to prepare a lot of selectively labeled samples.

Solution structure of an RNA duplex including a C-U base pair.

The formation of the C-U base pair in a duplex was observed in solution by means of the temperature profile of (15)N chemical shifts, and the precise geometry of the C-U base pair was also determined by NOE-based structure calculation. From the solution structure of the RNA oligomer, r[CGACUCAGG].r[CCUGCGUCG], it was found that a single C-U mismatch preferred being stacked in the duplex rather than being flipped-out even in solution. Moreover, it adopts an irregular geometry, where the amino nitrogen (N4) of the cytidine and keto-oxygen (O4) of the uridine are within hydrogen-bonding distance, as seen in crystals. To further prove the presence of a hydrogen bond in the C-U pair, we employed a point-labeled cytidine at the exocyclic amino nitrogen of the cytidine in the C-U pair. The temperature profile of its (15)N chemical shift showed a sigmoidal transition curve, indicating the presence of a hydrogen bond in the C-U pair in the duplex.

Determination of h2J(NN) and h1J(HN) coupling constants across Watson-Crick base pairs in the Antennapedia homeodomain-DNA complex using TROSY.

This paper describes NMR measurements of 15N-15N and 1H-15N scalar couplings across hydrogen bonds in Watson-Crick base pairs, h2J(NN) and h1J(HN), in a 17 kDa Antennapedia homeodomain-DNA complex. A new NMR experiment is introduced which relies on zero-quantum coherence-based transverse relaxation-optimized spectroscopy (ZQ-TROSY) and enables measurements of h1J(HN) couplings in larger molecules. The h2JNN and h1J(HN) couplings open a new avenue for comparative studies of DNA duplexes and other forms of nucleic acids free in solution and in complexes with proteins, drugs or possibly other classes of compounds.

Simple suppression of spurious peaks in TROSY experiments.

In (1)H-(15)N TROSY experiments of proteins and nucleic acids, where the second coherence transfer delay time tau' has been fixed as 5.6 ms, 1/(2(1)J(NH)), in order to achieve complete spin-state selection, spurious negative peaks are observed along the (15)N axes. These peaks are often annoyingly large, especially for nucleic acids. A simple product operator calculation, however, indicated that the shortening of the second delay time tau', which is next to the t1 period, would efficiently suppress these spurious peaks, without sacrificing the sensitivities of the TROSY peaks too much. We have shown for three systems, two 11- and 17-kDa proteins and one 8-kDa DNA duplex, that these spurious peaks can be effectively suppressed with delay times of 3.3 ms for the two proteins and 2.3 ms for the DNA. These delay times, optimized by trial and error, for the spurious peak suppression did not depend on the magnetic field strength and the temperature very much. Although the shortened tau' delay times attenuate the TROSY peak intensities by about 10 and 20% for the two proteins and the DNA, respectively, this simple modification will be useful for the quantitative uses of TROSY peaks and will result in cleaner spectra for various TROSY-based multiple resonance experiments.

Structural comparison between wild-type and P25S human cystatin A by NMR spectroscopy. Does this mutation affect the alpha-helix conformation?

The effect of substituting Pro25, located in the alpha-helical region of the cystatin A structure, with Ser has been studied. The structures of wild type and P25S cystatin A were determined by multidimensional NMR spectroscopy under comparable conditions. These two structures were virtually identical, and the alpha-helix between Glu15-Lys30 exists with uninterrupted continuity, with a slight bend at residue 25. In order to characterize the possible substitution effects of Pro25 with Ser on the alpha-helix, the chemical shifts of the amide nitrogens and protons, the generalized order parameters obtained by the analyses of the 15N-1H relaxation data, the amide proton exchange rates, and the NOE networks among the alpha-helical and surrounding residues were carefully compared. None of these parameters indicated any significant static or dynamic structural differences between the alpha-helical regions of the wild-type and P25S cystatin A proteins. We therefore conclude that our previous structure of the wild-type cystatin A, in which the alpha-helix exhibited a sharp kink at Pro25, must be revised. The asymmetric distribution of hydrophobic interactions between the side-chain residues of the alpha-helix and the rolled beta-sheet surface, as revealed by NOEs, may be responsible for the slight bend of the alpha-helix in both variants and for the destabilized hydrogen bonding of the alpha-helical residues that follow Pro25/Ser25, as evidenced by increased amide exchange rates.