The solution structure of the Mu Ner protein reveals a helix-turn-helix DNA recognition motif.

BACKGROUND: The Mu Ner protein is a small (74 amino acids), basic, DNA-binding protein found in phage Mu. It belongs to a class of proteins, the cro and repressor proteins, that regulate the switch from the lysogenic to the lytic state of the phage life cycle. There is no significant sequence identity between Mu Ner and the cro proteins of other phages, despite their functional similarity. In addition, there is no significant sequence identity with any other DNA-binding proteins, with the exception of Ner from the related phage D108 and the Nlp protein of Escherichia coli. As the tertiary structures of Mu Ner and these two related proteins are unknown, it is clear that a three-dimensional (3D) structure of Mu Ner is essential in order to gain insight into its mode of DNA binding. RESULTS: The 3D solution structure of Mu Ner has been solved by 3D and 4D heteronuclear magnetic resonance spectroscopy. The structure consists of five alpha helices, two of which comprise a helix-turn-helix (HTH) motif. Analysis of line broadening and disappearance of crosspeaks in a 1H-15N correlation spectrum of the Mu Ner-DNA complex suggests that residues in these two helices are most likely to be in contact with the DNA. CONCLUSIONS: Like the functionally analogous cro proteins from phages lambda and 434, the Mu Ner protein possesses a HTH DNA recognition motif. The Ner protein from phage D108 and the Nlp protein from E. coli are likely to have very similar tertiary structures due to high amino-acid-sequence identity with Mu Ner.

Structure of Bam HI endonuclease bound to DNA: partial folding and unfolding on DNA binding.

The crystal structure of restriction endonuclease Bam HI complexed to DNA has been determined at 2.2 angstrom resolution. The DNA binds in the cleft and retains a B-DNA type of conformation. The enzyme, however, undergoes a series of conformational changes, including rotation of subunits and folding of disordered regions. The most striking conformational change is the unraveling of carboxyl-terminal alpha helices to form partially disordered "arms." The arm from one subunit fits into the minor groove while the arm from the symmetry related subunit follows the DNA sugar-phosphate backbone. Recognition of DNA base pairs occurs primarily in the major groove, with a few interactions occurring in the minor groove. Tightly bound water molecules play an equally important role as side chain and main chain atoms in the recognition of base pairs. The complex also provides new insights into the mechanism by which the enzyme catalyzes the hydrolysis of DNA phosphodiester groups.

DNA binding specificity of the Mu Ner protein.

Binding of purified phage Mu Ner protein to a series of DNA fragments was investigated in order to determine the length requirements for tight specific binding. Gel retardation experiments with wild-type 307 base pair (bp) Mu DNA and shorter, synthetic oligonucleotides were performed, and apparent dissociation constants (KappD) were determined from the half-saturation point. While Ner formed four complexes with the 307 bp DNA fragment, only one complex was observed with the shorter DNAs. The 50 and 30 bp fragments had KappD values of 5 and 20 nM, respectively. Ner binding was progressively weaker with decreasing size of the DNA fragments, with no binding observed for 12mers. The shortest DNA fragments which bound well were two 18 bp fragments for which KappD values were in the range of 50-100 nM. The stoichiometry of Ner complexes with the 30 and 18 bp fragments was determined using a modified Ferguson method. Ner was found to form a tetramer on the 30 bp DNA and a dimer on the 18 bp DNA, which makes the latter a good candidate for the study of a Ner-DNA complex by NMR. In order to clarify which DNA regions were important for Ner-DNA binding, hydroxyl radical footprinting was performed for a range of Ner concentrations from 30 to 500 nM. The footprint revealed that Ner contacts the DNA backbone every 12-13 bp, on both strands of the DNA. The order in which protected regions appeared with increasing protein concentration indicated that two Ner monomers bound to DNA simultaneously. A model of Ner binding to DNA is proposed on the basis of these results.

Crystallization and preliminary X-ray analysis of restriction endonuclease BamHI-DNA complex.

Restriction endonuclease BamHI from Bacillus amyloliquefaciens has been co-crystallized with a 12 bp DNA fragment that encompasses its recognition site. The co-crystals diffract to at least 1.95 A resolution and belong to space group P2(1)2(1)2(1). The unit cell parameters are a = 108.8 A, b = 81.9 A, c = 68.8 A, consistent with one complex in the crystallographic asymmetric unit. The direction of the DNA appears to be along the b axis. In order to achieve end to end stacking of DNA, the complex must lie on the screw axis along b. A self-rotation function has determined the directions of the non-crystallographic 2-fold axes.

Structure of restriction endonuclease bamhi phased at 1.95 A resolution by MAD analysis.

BACKGROUND: Type II restriction endonucleases recognize DNA sequences that vary between four to eight base pairs, and require only Mg2+ as a cofactor to catalyze the hydrolysis of DNA. Their protein sequences display a surprising lack of similarity, and no recurring structural motif analogous to the helix-turn-helix or the zinc finger of transcription factors, has yet been discovered. RESULTS: We have determined the crystal structure of restriction endonuclease BamHI at 1.95 A resolution. The structure was solved by combining phase information derived from multi-wavelength X-ray data by algebraic and maximum likelihood methods. The BamHI subunit consists of a central beta-sheet with alpha-helices on both sides. The dimer configuration reveals a large cleft which could accommodate B-form DNA. Mutants of the enzyme that are deficient in cleavage are located at or near the putative DNA-binding cleft. BamHI and endonuclease EcoRI share a common core motif (CCM) consisting of five beta-strands and two helices. It remains to be determined if other restriction enzymes also contain the CCM. CONCLUSIONS: The structure of BamHI provides the first clear evidence that there may be substantial structural homology amongst restriction enzymes, even though it is undetectable at the sequence level.

Structure of restriction endonuclease BamHI and its relationship to EcoRI.

Type II restriction endonucleases are characterized by the remarkable specificity with which they cleave specific DNA sequences. Surprisingly, their protein sequences are in most cases unrelated, and no recurring structural motif has yet been identified. We have determined the structure of restriction endonuclease BamHI at 1.95 A resolution. BamHI shows striking resemblance to the structure of endonuclease EcoRI (refs 3, 4), despite the lack of sequence similarity between them. We also observe some curious differences between the two structures, and propose an evolutionary scheme that may explain them. The active site of BamHI is structurally similar to the active sites of EcoRI and EcoRV (ref. 5), but the mechanism by which BamHI activates a water molecule for nucleophilic attack may be different.

Overexpression, purification and crystallization of BamHI endonuclease.

The type II restriction endonuclease BamHI has been expressed in E. coli, producing 100-fold more enzyme than the wild type Bacillus amyloliquefaciens H strain. This high yield has facilitated purification to homogeneity of large amounts of the enzyme, along with its crystallization in a form which diffracts to at least 1.9 A in X-ray analysis.

Phase transitions of concentrated DNA solutions in low concentrations of 1:1 supporting electrolyte.

Transitions between isotropic and liquid crystalline phases of concentrated solutions of DNA with an average contour length (500 A) near the persistence length were examined in 0.01 M supporting 1:1 electrolyte (predominantly NaCl). A quantitative phase diagram describing the transitions occurring over a DNA concentration range from 100 to 290 mg/mL and temperatures from 20 to 60 degrees C was constructed from solid-state 31P-nmr data and examination of the morphologies of the mesophases by polarized light microscopy. Three anisotropic phases were observed in solutions with DNA concentrations of 160-290 mg/mL: an unidentified, weakly birefringent phase termed "precholesteric," a true cholesteric phase with pitch approximately 2 microns, and a third, presumably more highly ordered phase. Comparison with previous studies showed that the critical concentration for anisotropic phase formation and the nature of the phases formed by these DNA molecules are not strongly affected by decreasing the supporting electrolyte concentration from approximately 0.2 M to 10 mM. There are, however, profound effects of decreasing the supporting electrolyte concentration on the width of the transition from isotropic to totally anisotropic solutions, and the nature of the transitions between phases. Decreasing the supporting electrolyte concentration significantly increases the concentration range of persistence of the isotrophic phase, and results in the formation of triphasic solutions (isotropic and two liquid crystalline phases). Values of the critical DNA concentrations for anisotropic phase formation from the theory of A. Stroobants et al. [(1986) Macromolecules 19, 2232 to 2238] were found to be significantly lower than the observed values for any reasonable estimate of the effective radius, probably because of the relatively short lengths of DNA fragments examined in the present study. Comparison of the experimentally determined DNA concentrations required for anisotropic phase formation with the values predicted from Flory's lattice statistics theory, which explicitly considers the rod length, permitted estimation of the effective DNA radius. The estimated radius was inconsistent with effective radii calculated from Poisson-Boltzmann (P-B) theory based on a supporting electrolyte concentration of 10 mM, but was in fair agreement with P-B theory assuming that Na+ DNA contributes approximately 0.24 Na+ counterions/nucleotide to the effective free sodium ion concentration.

A 23Na-NMR study of sodium-DNA interactions in concentrated DNA solutions at low-supporting electrolyte concentration.

Aqueous solutions of DNA fragments with a contour length (500 A) near the persistence length at DNA concentrations ranging from 10 to 290 mg/mL solvent and a constant supporting electrolyte concentration of 0.01 M (predominantly NaCl) were examined by 23Na-nmr spectroscopy at temperatures of 20, 40, and 60 degrees C. Over the higher portion of this concentration range (greater than 100 mg/ml) the DNA solutions undergo a complex series of transitions between different anisotropic, liquid crystalline phases (T. E. Strzelecka and R. L. Rill, Biopolymers, in press). Counterions in solutions of strong polyelectrolytes are usually described in terms of a two-state model as free or "bound" (influenced by the electrostatic field of the polyanion). The longitudinal relaxation rate (R1 = 1/T1) at all DNA concentrations decreased with increasing temperature, demonstrating fast exchange between free and bound counterions. R1 increased nearly linearly with increasing DNA phosphate/sodium ratio in the isotropic domain until the onset of anisotropic phase formation, in agreement with similar nmr studies conducted at low DNA concentrations. The value of R1,b = 194 +/- 7 Hz obtained for the isotropic phase from 10 to 100 mg DNA/mL at 20 degrees C was in agreement with values reported previously. A nonlinear increase in R1 with DNA concentration was observed upon onset of anisotropic phase formation, indicating an increase in the product of the fraction of bond ions times their relaxation rate (r.R1,b). The spectral lineshape of all isotropic samples was Lorentzian. Spectra of anisotropic samples exhibited low magnitude quadrupole splitting of less than or equal to 400 Hz correlated with appearance of a cholesteric phase with pitch approximately 2 microns. The magnitude of the quadrupole splitting decreased with increasing DNA concentration at low temperatures and increased with concentration at high temperatures. At all concentrations the quadrupole splitting decreased then increased with temperature. These temperature- and concentration-dependent changes in quadrupole splitting are consistent with an angle between the DNA helix axis and the principal component (VZZ) of the local electric field gradient tensor near the "magic angle" of 54.7 degrees.

Multiple liquid crystal phases of DNA at high concentrations.

DNA packaging in vivo is very tight, with volume concentrations approaching 70% w/v in sperm heads, virus capsids and bacterial nucleoids. The packaging mechanisms adopted may be related to the natural tendency of semi-rigid polymers to form liquid crystalline phases in concentrated solutions. We find that DNA forms at least three distinct liquid crystalline phases at concentrations comparable to those in vivo, with phase transitions occurring over relatively narrow ranges of DNA concentration. A weakly birefringent, dynamic, 'precholesteric' mesophase with microscopic textures intermediate between those of a nematic and a true cholesteric phase forms at the lowest concentrations required for phase separation. At slightly higher DNA concentrations, a second mesophase forms which is a strongly birefringent, well-ordered cholesteric phase with a concentration-dependent pitch varying from 2 to 10 micron. At the highest DNA concentrations, a phase forms which is two-dimensionally ordered and resembles smectic phases of thermotropic liquid crystals observed with small molecules.

Semiconductor properties of natural melanins.

Basic semiconductor characteristics of natural melanins isolated from bovine eye, human dark hair, and banana peel were obtained by means of the dc dark conductivity experiments and optical absorption measurements. The results were compared with results obtained for synthetic melanin. Specific conductivity in natural melanins is of the order 10(-11) omega -1 cm-1 and in synthetic melanin 10(-8) omega -1 cm-1. Thermal activation energies in the range 298-333 degrees K are eye melanin, 0.93 eV; hair melanin, 1.01 eV; banana melanin, 1.04 eV; whereas synthetic melanin has two values of activation energy: up to 311 degrees K, 0.1 eV; above 313 degrees K, 0.78 eV. Optical gaps are: in eye melanin, 1.73 eV; in hair melanin, 1.35 eV; in banana melanin, 1.55 eV; and in synthetic melanin, 1.40 eV. The observed differences between natural melanins and the synthetic one could be explained by either the presence of protein residues in natural melanins or the influence of the isolation method on their electrical properties.

A band model for synthetic dopa-melanin.

To determine a band model for synthetic melanin obtained by autooxidation of L-dopa (3,4-dihydroxyphenyl-L-alanine), dependence of dark current on temperature in the range 298-333 degrees K was measured as well as dependence of optical absorption coefficient on wave-length in the range 250-800 nm. It was found that up to 311 degrees K thermal activation energy equals 0.1 eV and above 313 degrees K it equals 0.78 eV. The first value is connected with the band of localized states at the Fermi level. Optical gap, determined from optical absorption measurements is equal to 1.40 eV. The estimated value of sigma o, assuming the value of thermal coefficient of activation-energy to be gamma = 5 X 10(-4) eV/degrees K, is 2 X 10(-6) omega -1 cm-1 for 0.1 eV and 5 X 10(2) omega -1 cm-1 for 0.78 eV. Density of states in the valence band is N(EV) = 8 X 10(21)/cm3 X eV, and in the band of localized states at the Fermi level N(EF) = 3 X 10(13)/cm3 X eV.

A hypothetical structure of melanin and its relation to biology.

Measurements of optical absorption of synthetic and natural melanins during their degradation in sodium hydroxide establish that from the "optical" point of view these polymers consist of two different parts. An explanation of this result and its possible relation to the biological role of melanin is given.