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Circadian rhythms are endogenous cellular programs that time metabolic and behavioral events to occur at optimal times in the daily cycle. Light and dark cycles synchronize the endogenous clock with the external environment through a process called entrainment. Previously, we identified the bacteriophytochrome-like circadian input kinase CikA as a key factor for entraining the clock in the cyanobacterium Synechococcus elongatus PCC 7942. Here, we present evidence that CikA senses not light but rather the redox state of the plastoquinone pool, which, in photosynthetic organisms, varies as a function of the light environment. Furthermore, CikA associates with the Kai proteins of the circadian oscillator, and it influences the phosphorylation state of KaiC during resetting of circadian phase by a dark pulse. The abundance of CikA varies inversely with light intensity, and its stability decreases in the presence of the quinone analog 2,5-dibromo-3-methyl-6-isopropyl-p-benzoquinone (DBMIB). The pseudo-receiver domain of CikA is crucial for sensitivity to DBMIB, and it binds the quinone directly, a demonstration of a previously unrecognized ligand-binding role for the receiver fold. Our results suggest that resetting the clock in S. elongatus is metabolism-dependent and that it is accomplished through the interaction of the circadian oscillator with CikA.

Circadian oscillators are endogenous biological systems that generate the approximately 24 hour temporal pattern of biological processes and confer a reproductive fitness advantage to their hosts. The cyanobacterial clock is the simplest known and the only clock system for which structural information for core component proteins, in this case KaiA, KaiB and KaiC, is available. SasA, a clock-associated histidine kinase, is necessary for robustness of the circadian rhythm of gene expression and implicated in clock output. The N-terminal domain of SasA (N-SasA) interacts directly with KaiC and likely functions as the sensory domain controlling the SasA histidine kinase activity. N-SasA and KaiB share significant sequence similarity and, thus, it has been proposed that they would be structurally similar and may even compete for KaiC binding. Here, we report the NMR structure of N-SasA and show it to be different from that of KaiB. The structural comparisons provide no clear details to suggest competition of SasA and KaiB for KaiC binding. N-SasA adopts a canonical thioredoxin fold but lacks the catalytic cysteine residues. A patch of conserved, solvent-exposed residues is found near the canonical thioredoxin active site. We suggest that this surface is used by N-SasA for protein-protein interactions. Our analysis suggests that the structural differences between N-SasA and KaiB are the result of only a few critical amino acid substitutions.

Circadian clocks are widespread endogenous mechanisms that control the temporal pattern of diverse biological processes, including gene transcription. KaiA is the positive element of the cyanobacterial clock because KaiA overexpression elevates transcription levels of clock components. Recently, we showed that the structure of KaiA is that of a domain-swapped homodimer. The N-terminal domain is a pseudo-receiver; thus, it is likely to be involved in signal transduction in the clock-resetting pathway. The C-terminal domain of KaiA is structurally novel and enhances the KaiC autokinase activity directly. Here, we report the NMR structure of the C-terminal domain of KaiA (ThKaiA180C) in complex with a KaiC-derived peptide from the cyanobacterium Thermosynechococcus elongatus BP-1. The protein-peptide interface is revealed to be different from a model that was proposed earlier, is stabilized by a combination of hydrophobic and electrostatic interactions, and includes many residues known to produce a circadian-period phenotype upon substitution. Although the structure of the monomeric subunit of ThKaiA180C is largely unchanged upon peptide binding, the intersubunit dimerization angle changes. It is proposed that modulation of the C-terminal KaiA domain dimerization angle regulates KaiA-KaiC interactions.

Trans-hydrogen-bond deuterium isotope effects of Watson-Crick A:U and A:T base pairs of 10 homologous RNA and DNA duplexes are compared. The isotope effect at 13C2 of adenosine residues due to deuterium/protium substitution at the imino H3 site, 2hDelta13C2, is larger in RNA than in DNA. The virtually consistent larger isotope effects in RNA suggest that the N1...N3 hydrogen bonds of A:U base pairs of RNA are stronger than those of the A:T base pairs of DNA.

The circadian clock found in Synechococcus elongatus, the most ancient circadian clock, is regulated by the interaction of three proteins, KaiA, KaiB, and KaiC. While the precise function of these proteins remains unclear, KaiA has been shown to be a positive regulator of the expression of KaiB and KaiC. The 2.0-A structure of KaiA of S. elongatus reported here shows that the protein is composed of two independently folded domains connected by a linker. The NH(2)-terminal pseudo-receiver domain has a similar fold with that of bacterial response regulators, whereas the COOH-terminal four-helix bundle domain is novel and forms the interface of the 2-fold-related homodimer. The COOH-terminal four-helix bundle domain has been shown to contain the KaiC binding site. The structure suggests that the KaiB binding site is covered in the dimer interface of the KaiA "closed" conformation, observed in the crystal structure, which suggests an allosteric regulation mechanism.

The chemical shifts of (13)C2 of adenosine residues of DNA were observed to experience a through-space or trans-hydrogen bond isotope effect as a result of deuterium substitution at the imino hydrogen site of base-paired thymidine residues. NMR measurements of several self-complementary DNA duplexes at natural abundance (13)C in 50% H(2)O, 50% D(2)O solvent mixtures yielded an average trans-hydrogen bond isotope effect, (2h)Delta(13)C2, of -47 ppb. The data suggest that stronger hydrogen bonds have more negative (2h)Delta(13)C2 values, which means that A:T N1.H3 hydrogen bonds increase the anharmonicity of the effective vibrational potential of H3. However, (2h)Delta(13)C2 values do not correlate with intra-residue (2)Delta(13)C4 values of thymidine observed here and earlier (Vakonakis et al., 2003), which suggests that (2h)Delta(13)C2 is not determined entirely by hydrogen bond strength. Instead, the variations observed in (2h)Delta(13)C2 values suggest that they may also be sensitive to base pair geometry.

KaiA is a two-domain circadian clock protein in cyanobacteria, acting as the positive element in a feedback loop that sustains the oscillation. The structure of the N-terminal domain of KaiA is that of a pseudo-receiver, similar to those of bacterial response regulators, which likely interacts with components of the clock-resetting pathway. The C-terminal domain of KaiA is highly conserved among cyanobacteria and enhances the autokinase activity of KaiC. Here we present the NMR structure of the C-terminal domain of KaiA from the thermophilic cyanobacterium Thermosynechococcus elongatus BP-1. This domain adopts a novel all alpha-helical homodimeric structure. Several mutations known to affect the period of the circadian oscillator are shown to be located at an exposed groove near the dimer interface. This NMR structure and a 21-A-resolution electron microscopy structure of the hexameric KaiC particle allow us to postulate a mode of KaiA-KaiC interaction, in which KaiA binds a linker region connecting two globular KaiC domains.

Internal motions of d-ribose selectively 2H-labeled at the 2' position were measured using solid state 2H NMR experiments. A sample of d-ribose-2'-d was prepared in a hydrated, non-crystalline state to eliminate effects of crystal-packing. Between temperatures of -74 and -60 degrees C the C2'-H2' bond was observed to undergo two kinds of motions which were similar to those of C2'-H2'/H2" found previously in crystalline deoxythymidine (Hiyama et al. (1989) J. Am. Chem. Soc., 111, 8609-8613): (1) Nanosecond motion of small angular displacement with an apparent activation energy of 3.6+/-0.7 kcal mol(-1), and (2) millisecond to microsecond motion of large amplitude with an apparent activation energy > or =4 kcal mol(-1). At -74 degrees C, the slow, large-amplitude motion was best characterized as a two-site jump with a correlation time on the millisecond time scale, whereas at -60 degrees C it was diffusive on the microsecond time scale. The slow, large-amplitude motions of the C2'-H2' bond are most likely from interconversions between C2'-endo and C3'-endo by way of the O4'-endo conformation, whereas the fast, small-amplitude motions are probably librations of the C2'-H2' bond within the C2'-endo and C3'-endo potential energy minima.

Deuterium isotope effects and fractionation factors of N1.H3-N3 hydrogen bonded Watson-Crick A:T base pairs of two DNA dodecamers are presented here. Specifically, two-bond deuterium isotope effects on the chemical shifts of (13)C2 and (13)C4, (2)delta(13)C2 and (2)delta(13)C4, and equilibrium deuterium/protium fractionation factors of H3, Phi, were measured and seen to correlate with the chemical shift of the corresponding imino proton, delta(H3). Downfield-shifted imino protons associated with larger values of (2)delta(13)C2 and (2)delta(13)C4 and smaller Phi values, which together suggested that the effective H3-N3 vibrational potentials were more anharmonic in the stronger hydrogen bonds of these DNA molecules. We anticipate that (2)delta(13)C2, (2)delta(13)C4 and Phi values can be useful gauges of hydrogen bond strength of A:T base pairs.

In the cyanobacterium Synechococcus elongatus (PCC 7942) the proteins KaiA, KaiB, and KaiC are required for circadian clock function. We deduced a circadian clock function for KaiA from a combination of biochemical and structural data. Both KaiA and its isolated carboxyl-terminal domain (KaiA180C) stimulated KaiC autophosphorylation and facilitated attenuation of KaiC autophosphorylation by KaiB. An amino-terminal domain (KaiA135N) had no function in the autophosphorylation assay. NMR structure determination showed that KaiA135N is a pseudo-receiver domain. We propose that this pseudo-receiver is a timing input-device that regulates KaiA stimulation of KaiC autophosphorylation, which in turn is essential for circadian timekeeping.

The human metalloregulatory transcription factor, metal-response element (MRE)-binding transcription factor-1 (MTF-1), contains six TFIIIA-type Cys(2)-His(2) motifs, each of which was projected to form well-structured betabetaalpha domains upon Zn(II) binding. In this report, the structure and backbone dynamics of a fragment containing the unusual C-terminal fingers F4-F6 has been investigated. (15)N heteronuclear single quantum coherence (HSQC) spectra of uniformly (15)N-labeled hMTF-zf46 show that Zn(II) induces the folding of hMTF-zf46. Analysis of the secondary structure of Zn(3) hMTF-zf46 determined by (13)Calpha chemical shift indexing and the magnitude of (3)J(Halpha-HN) clearly reveal that zinc fingers F4 and F6 adopt typical betabetaalpha structures. An analysis of the heteronuclear backbone (15)N relaxation dynamics behavior is consistent with this picture and further reveals independent tumbling of the finger domains in solution. Titration of apo-MTF-zf46 with Zn(II) reveals that the F4 domain binds Zn(II) significantly more tightly than do the other two finger domains. In contrast to fingers F4 and F6, the betabetaalpha fold of finger F5 is unstable and only partially populated at substoichiometric Zn(II); a slight molar excess of zinc results in severe conformational exchange broadening of all F5 NH cross-peaks. Finally, although Cd(II) binds to apo-hMTF-zf46 as revealed by intense S(-)-->Cd(II) absorption, a non-native structure results; addition of stoichiometric Zn(II) to the Cd(II) complex results in quantitative refolding of the betabetaalpha structure in F4 and F6. The functional implications of these results are discussed.

The concept of using a dynamic base-pairing nucleobase as a mode for degenerate recognition presents a unique challenge to analysis of DNA structure. Proton and phosphorus NMR studies are reported for two nine-residue DNA oligodeoxyribonucleotides, d(CATGGGTAC).d(GTACNCATG) (1) and d(CATGTGTAC).(GTACNCATG) (2), which contained 1-(2'-deoxy-beta-D-ribofuranosyl)-1,2,4-triazole-3-carboxamide (N) in the center of the helix at position 14. The duplexes were compared to the canonical Watson-Crick duplexes, d(CATGGGTAC).d(GTACCCATG) (3) and d(CATGTGTAC).d(GTACACATG) (4). Two-dimensional NOESY spectra of 1-4 in H(2)O and D(2)O solutions collected at 5 degrees C allowed assignment of the exchangeable and nonexchangeable protons for all four oligodeoxyribonucleotides. Thermodynamic and circular dichroism data indicated that 1-4 formed stable, B-form duplexes at 5 degrees C. Two-dimensional (1)H-(31)P correlation spectra indicated that there were minor perturbations in the backbone only near the site of the triazole base. Strong NOESY cross-peaks were observed between the H5 and H1' of N14 in 1 and, unexpectedly, 2, which indicated that, in both duplexes, N14 was in the syn(chi)() conformation about the glycosidic bond. NOESY spectra of 1 and 2 recorded in 95% H(2)O, 5% D(2)O indicated that the imino proton of the base opposite N14, G5, or T5, formed a weak hydrogen bond with N14. These conformations place the polar carboxamide functional group in the major groove with motional averaging on the intermediate time scale.

The three-dimensional structures of two DNA duplexes d(CATGAGTAC). d(GTACXCATG) (1) and d(CATGAGTAC).d(GTACTCATG) (2), where X represents 1-(2'-deoxy-beta-D-ribofuranosyl)-3-nitropyrrole, were solved using high resolution nuclear magnetic resonance spectroscopy and restrained molecular dynamics. Good convergence was observed between final structures derived from A- and B-form starting geometries for both 1 and 2. Structures of 1 and 2 are right-handed duplexes within the B-form conformational regime. Furthermore, the structures of 1 and 2 are highly similar, with differences in the structures localized to the vicinity of residue 14 (X versus T). The pyrrole group of 1 is in the syn conformation and it is displaced towards the major groove. Furthermore, unlike T14 in 2, the base of X14 has reduced pi-pi stacking interactions with C13 and C15 and the nitro group of X14 is pointing out of the major groove. The structures presented here establish the basis of the thermal data of DNA duplexes containing X and should be informative during the design of improved wild card nucleobase analogs.

We report the solution structure of the chemotactic cytokine (chemokine) vMIP-II. This protein has unique biological activities in that it blocks infection by several different human immunodeficiency virus type 1 (HIV-1) strains. This occurs because vMIP-II binds to a wide range of chemokine receptors, some of which are used by HJV to gain cell entry. vMIP-II is a monomeric protein, unlike most members of the chemokine family, and its structure consists of a disordered N-terminus, followed by a helical turn (Gln25-Leu27), which leads into the first strand of a three-stranded antiparallel beta-sheet (Ser29-Thr34; Gly42-Thr47; Gln52-Asp56). Following the sheet is a C-terminal alpha-helix, which extends from residue Asp60 until Gln68. The final five residues beyond the C-terminal helix (Pro70-Arg74) are in an extended conformation, but several of these C-terminal residues contact the first beta-strand. The structure of vMIP-II is compared to other chemokines that also block infection by HIV-1, and the structural basis of its lack of ability to form a dimer is discussed.

Encoded by Kaposi's sarcoma-associated herpesvirus, viral macrophage-inflammatory protein-II (VMIP-II) is unique among CC chemokines in that it has been shown to bind to the CXC chemokine receptor CXCR4 as well as to a variety of CC chemokine receptors. This unique binding ability allows vMIP-II to block infection by a wide range of human immunodeficiency virus type I (HIV-1) strains, but the structural and dynamic basis for this broad range of binding is not known. 15N T1, T2 and 15N[-HN] nuclear Overhauser effect (NOE) values of vMIP-II, determined through a series of heteronuclear multidimensional nuclear magnetic resonance (NMR) experiments, were used to obtain information about the backbone dynamics of the protein. Whereas almost all chemokine structures reveal a dimer or multimer, vMIP-II has a rotational correlation time (tauc) of 4.7 +/- 0.3 ns, which is consistent with a monomeric chemokine. The rotational diffusion anisotropy, D parallel/D perpendicular, is approximately 1.5 +/- 0.1. The conformation of vMIP-II is quite similar to other known chemokines, containing an unstructured N-terminus followed by an ordered turn, three beta-strands arranged in an antiparallel fashion, and one C-terminal alpha-helix that lies across the beta-strands. Most of the protein is well-ordered on a picosecond time scale, with an average order parameter S2 (excluding the N-terminal 13 amino acids) of 0.83 +/- 0. 09, and with even greater order in regions of secondary structure. The NMR data reveal that the N-terminus, which in other chemokines has been implicated in receptor binding, extends like a flexible tail in solution and possesses no secondary structure. The region of the ordered turn, including residues 25-28, experiences conformational exchange dynamics. The implications of these NMR data to the broad receptor binding capability of vMIP-II are discussed.

Chemokines (chemotactic cytokines) are a family of immune system proteins, several of which have been shown to block human immunodeficiency virus (HIV) infection in various cell types. While the solved structures of most chemokines reveal protein dimers, evidence has accumulated for the biological activity of individual chemokine monomers, and a debate has arisen regarding the biological role of the chemokine dimer. Concurrent with this debate, several N-terminal truncations and modifications in the CC subfamily of chemokines have been shown to have functional significance, in many cases antagonizing their respective receptors and in some cases retaining the ability to block HIV entry to the cell. As the dimer interface of CC chemokines is located at their N-terminus, a structural study of N-terminally truncated chemokines will address the effect that this type of mutation has on the dimer-monomer equilibrium. We have studied the structural consequences of N-terminal truncation in macrophage inflammatory protein 1 beta (MIP-1 beta), a CC chemokine that has been shown to block HIV infection. Examination of nuclear magnetic resonance (NMR) spectra of a series of N-terminally truncated MIP-1 beta variants reveals that these proteins possess a range of ability to dimerize. A mutant beginning at amino acid Asp6 [termed MIP(6)] has near wild-type dimer properties, while further truncation results in weakened dimer affinity. The mutant MIP(9) (beginning with amino acid Thr9) has been found to exist solely as a folded monomer. Relaxation measurements yield a rotational correlation time of 8.6 +/- 0.1 ns for wild-type MIP-1 beta and 4.5 +/- 0.1 ns for the MIP(9) mutant, consistent with a wild-type dimer and a fully monomeric MIP(9) variant. The presence of physiological salt concentration drastically changes the monomer-dimer equilibrium for both wild-type and most mutant proteins, heavily favoring the dimeric form of the protein. These results have implications for structure-function analysis of existing chemokine mutants as well as for the larger debate regarding the biological existence and activity of the chemokine dimer.

Hydrogen bonds stabilize protein and nucleic acid structure, but little direct spectroscopic data have been available for characterizing these critical interactions in biological macromolecules. It is demonstrated that the electric field gradient at the nucleus of an amide hydrogen can be determined residue-specific by measurement of 15N NMR relaxation times in proteins dissolved in D2O, and uniformly enriched with 13C and 15N. In D2O, all backbone amide protons can be exchanged with solvent deuterons, and the T1 relaxation rate of a deuteron is dominated by its quadrupole coupling constant (QCC), which is directly proportional to the electric field gradient at the nucleus. 2HN T1 relaxation can be measured quantitatively through its effect on the T2 relaxation of its directly attached 15N. QCC values calculated from 2HN T1 and previously reported spectral densities correlate with the inverse cube of the X-ray crystal structure-derived hydrogen bond lengths: QCC = 228 + Sigmai 130 cos alphai/ri3 kHz, where alpha is the N-H...Oi angle and r is the backbone-backbone (N-)H...Oi(=C) hydrogen bond distance in ângstroms.