Interaction of lambda cro repressor with synthetic operator OR3 studied by competition binding with minor groove binders.

In the present work, we employ a combination of CD spectroscopy and gel retardation technique to characterize thermodynamically the binding of lambda phage cro repressor to a 17 base pair operator OR3. We have found that three minor groove-binding antibiotics, distamycin A, netropsin and sibiromycin, compete effectively with the cro for binding to the operator OR3. Among these antibiotics, sibiromycin binds covalently to DNA in the minor groove at the NH2 of guanine, whereas distamycin A and netropsin interact preferentially with runs of AT base pairs and avoid DNA regions containing guanine bases in the two polynucleotide strands. Only subtle DNA conformation changes are known to take place upon binding of these antibiotics. Both the CD spectral profiles and the results of the gel retardation experiments indicate that distamycin A and netropsin can displace cro repressor from the operator OR3. The binding of cro repressor to the OR3 is accompanied by considerable changes in CD in the far-UV region which appear to be attributed to a DNA-dependent structural transition in the protein. Spectral changes are also induced in the wavelength region of 270-290 nm. The CD spectral profile of the cro-OR3 mixture in the presence of distamycin A can be represented as a sum of the CD spectrum of the repressor-operator complex and spectrum of distamycin-DNA complex at the appropriate molar ratio of the bound antibiotic to the operator DNA (r). When r tends to the saturation level of binding the CD spectrum in the region of 270-360 nm approaches a CD pattern typical of complexes of the antibiotic with the free DNA oligomer. This suggests that simultaneous binding of cro repressor and distamycin A to the same DNA oligomer is not possible and that distamycin A and netropsin can be used to determine the equilibrium affinity constant of cro repressor to the synthetic operator from competition-type experiments. The binding constant of cro repressor to the OR3 is found to be (6 +/- 1).10(6)M-1 at 20 degrees C in 10 mM sodium cacodylate buffer (pH 7.0) in the presence of 0.1 M NH4F.     

Solution conformations of DNAs containing binding sites of the catabolite gene activator protein and lac repressor protein: characterization by Raman spectroscopy

Raman spectra from three subfragments of the Escherichia coli lactose promoter region were obtained in 0.1 M NaCl. The three DNAs are 21, 40, and 62 bp in length. The 21 and 62 bp DNAs contain the binding site for the catabolite gene activator protein (CAP). The 40 bp DNA contains the binding site for the lac repressor. A quantitative analysis of Raman band characteristics indicates an overall B-type conformation for these gene regulatory sites. Bands which correspond to A-family (807 cm-1) and B-family (834 cm-1) deoxyribose phosphate vibrations have the same intensities as bands found in heterogeneous DNAs. The spectra of the 21 bp CAP site have, however, a small band at 867 cm-1 and several other small differences similar to some characteristics observed in C-DNA spectra. Several dG nucleosides in the CAP site appear to be altered from the conventional C2'-endo/anti conformation. At 45 degrees C, well below the melting region of these DNAs, small changes occur in the spectra of the 40 bp lac repressor site which are not observed in the other DNAs. A weak band occurs at 705 cm-1, and intensity changes are observed at 497, 682, and 792 cm-1. The changes suggest that the conformations of several dG nucleosides are altered and that a small region may exist with characteristics of an A-family backbone. This conformational change at 45 degrees C coincides with previous NMR observations indicating an enhanced imino proton exchange rate at a GTG sequence within the lac operator site.     

The absence of non-local conformational changes in OR3 operator DNA on complexing with the cro repressor

The Interaction of the cro protein of lambda phage with a synthetic OR3 operator having 17 base pairs in length and with its 9 bp fragment has been studied using the circular dichroism (CD) method. In both cases, a considerable change in the CD of the samples was found in the region 260-300 nm upon the addition of the cro protein. The stoichiometry obtained by the CD titration was identical for OR3 and its 9 bp fragment: one duplex per dimeric cro. NaCl addition makes the complexes dissociate so that the 9 bp fragment becomes free at [NaCl] greater than 0.2 M while the whole OR3 becomes free at [NaCl] greater than 0.5 M. The CD spectra of both the free duplexes show a typical B-form conservative pattern with a positive CD band (270 nm) and a negative one (250 nm). The specific complexing of both the duplexes results in a substantial CD depression in the positive band. The most pronounced effect occurs at 280 nm. This spectral change is quite distinct from those in the B to A transition and in the non-cooperative winding of the DNA within the B-family of forms. The interaction of the cro protein with the non-operator DNAs, calf thymus DNA and a synthetic 10 bp duplex, reveals no visible CD changes at all. An inference is drawn that the CD change in the specific complexes is mainly due to the induced CD in tyr-26 upon its interaction with a specific base pair in the operator or its fragment, the operator DNA conformation being conserved in a B-like form as a whole.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effect of the G.T mismatch on backbone and sugar conformations of Z-DNA and B-DNA: analysis by Raman spectroscopy of crystal and solution structures of d(CGCGTG) and d(CGCGCG)

The Z-DNA crystal structures of d(CGCGTG) and d(CGCGCG) are compared by laser Raman spectroscopy. Raman bands originating from vibrations of the phosphodiester groups and sensitive to the DNA backbone conformation are similar for the two structures, indicating no significant perturbation to the Z-DNA backbone as a result of the incorporation of G.T mismatches. Both Z structures also exhibit Raman markers at 625 and 670 cm-1, assigned respectively to C3'-endo/syn-dG (internal) and C2'-endo/syn-dG conformers (3' terminus). Additional Raman intensity near 620 and 670 cm-1 in the spectrum of the d(CGCGTG) crystal is assigned to C4'-exo/syn-dG conformers at the mismatch sites (penultimate from the 5' terminus). A Raman band at 1680 cm-1, detected only in the d(CGCGTG) crystal, is assigned to the hydrogen-bonded dT residues and is proposed as a definitive marker of the Z-DNA wobble G.T pair. For aqueous solutions, the Raman spectra of d(CGCGTG) and d(CGCGCG) are those of B-DNA, but with significant differences between them. For example, the usual B-form marker band at 832 cm-1 in the spectrum of d(CGCGTG) is about 40% less intense than the corresponding band in the spectrum of d(CGCGCG), and the former structure exhibits a companion band at 864 cm-1 not observed for d(CGCGCG). The simplest interpretation of these results is that the conventional B-form OPO geometry occurs for only 6 of the 10 OPO groups of d(CGCGTG). The remaining four OPO groups, believed to be those at or near the mismatch site, are in an "unusual B" conformation which generates the 864 cm-1 band.(ABSTRACT TRUNCATED AT 250 WORDS)     

Right- and left-handed helixes of poly[d(A-T)].poly[d(A-T)] investigated by infrared spectroscopy

The secondary structures of double-stranded poly[d(A-T)].poly[d(A-T)] in films have been studied by IR spectroscopy with three different counterions (Na+, Cs+, and Ni2+) and a wide variety of water content conditions (relative humidity between 100 and 47%). In addition to the A-, B-, C-, and D-form spectra, a new IR spectrum has been obtained in the presence of nickel ions. The IR spectra of Ni2+-poly[d(A-T)].poly[d(A-T)] films are analyzed by comparison with previously assigned IR spectra of left-handed poly[d(G-C)].poly[d(G-C)] and poly[d(A-C)].poly[d(G-T)], and it is possible to conclude that they reflect a Z-type structure for poly[d(A-T)].poly[d(A-T)]. The Z conformation has been favored by the high polynucleotide concentration, by the low water content of the films, and by specific interactions of the transition metal ions with the purine bases stabilized in a syn conformation. A structuration of the water hydration molecules around the double-stranded Ni2+-poly[d(A-T)].poly[d(A-T)] is shown by the presence of a strong sharp water band at 1615 cm-1.     

A-like guanine-guanine stacking in the aqueous DNA duplex of d(GGGGCCCC)

We have used CD spectroscopy, NMR spectroscopy and unrestrained molecular dynamics to study conformational properties of a DNA duplex formed by the self-complementary octamer d(GGGGCCCC). Its unusual CD spectrum contains features indicating A-like stacking of half of the bases, whereas the other half stack in a B-like fashion. Unrestrained molecular dynamics simulations converged to a stable B-like double-helix of d(GGGGCCCC). However, the double-helix contained a central hole whose size was half of that occurring in structure A. In the canonical structure B, the hole does not exist at all because the base-pairs cross the double-helix centre. The cytosine bases were stacked in the duplex of d(GGGGCCCC) as in structure B, while stacking of the guanine bases displayed features characteristic for structure A. NMR spectroscopy revealed that the A-like guanine-guanine stacking was accompanied by an increased tendency of the deoxyribose rings attached to the guanine bases to be puckered in an A-like fashion. Otherwise, the duplex of d(GGGGCCCC) showed no clash, no bend and no other significant deviation from structure B. The present analysis demonstrates a remarkable propensity of the guanine runs to stack in an A-like fashion even within the B-DNA framework. This property explains why the oligo(dG). oligo(dC) tracts switch into structure A so easily. Secondly, this property may influence replication, because structure A is replicated more faithfully than structure B. Thirdly, the oligo(dG) runs might have played an important role in early evolution, when DNA took on functions that originally evolved on RNA. Fourthly, the present study extends the vocabulary of DNA secondary structures by the heteronomous duplex of d(GGGGCCCC) in which the B-like strand of oligo(dC) is bound to the A-like strand of oligo(dG).     

He—Ne激光诱变白细胞DNA的拉曼光谱研究

报道了Ｈｅ—Ｎｅ激光对白细胞ＤＮＡ诱变的拉曼光谱研究。Ｈｅ—Ｎｅ激光辐射前,白细胞ＤＮＡ主链振动区域出现二条强的Ａ,Ｃ构型特征线８１２ｃｍ－１和８７２ｃｍ－１,以及弱的Ｂ型语线１０９２ｃｍ－１。辐射后,Ａ型特征线８１２ｃｍ－１消失,代之是与Ｂ型结构有关的二条强的语线８００ｃｍ－１和１０９０ｃｍ－１。试验结果表明,Ｈｅ—Ｎｅ激光可诱变ＤＮＡ构型（ＡＭ－Ｂ型）。在碱基振动区域,辐射前其拉曼谱出现强而宽的Ｃ＝０伸长振动谱线１６８０ｃｍ－１,这是与酮基结构有关的谱线,辐射后该谱线强度大大减弱。实验结果提示,Ｈｅ一Ｎｅ激光有可能使碱基发生互变异构。     

Rotation of periphery methylpyridine of meso-tetrakis(n-N-methylpyridiniumyl)porphyrin (n = 2, 3, 4) and its selective binding to native and synthetic DNAs

By utilizing circular and linear dichroism, the binding mode of meso-tetrakis(n-N-methylpyridiniumyl)porphyrin (n = 2, 3, 4) to various DNAs was studied in this work. 2-N-(methylpyridiniumyl)porphyrin(o-TMPyP), in which rotation of the periphery pyridinium ring is prevented, exhibits similar spectral properties when bound to DNA, poly[d(G-C)(2)] and poly[d(A-T)(2)], suggesting a similar binding mode. Close analysis of the spectral properties led us to conclude that o-TMPyP sits in the major groove. However, both 3-N- and 4-N-(methylpyridiniumyl)porphyrin (m- and p-TMPyP), of which the periphery pyridinium ring is free to rotate, intercalate between the basepairs of DNA and poly[d(G-C)(2)]. In the presence of poly[d(A-T)(2)], m-TMPyP exhibits a typical bisignate excitonic CD spectrum in the Soret band, while p-TMPyP shows two positive CD bands. The excitonic CD spectrum of the m-TMPyP-poly[d(A-T)(2)] complex and the positive CD band of the o-TMPyP-poly[d(A-T)(2)] complex were not affected by the presence of the minor groove binding drug, 4',6-diamidino-2-phenylindole (DAPI), indicating that this porphyrin is bound in the major groove. In contrast, two positive CD bands of the p-TMPyP-poly[d(A-T)(2)] complex altered in the presence of DAPI. From the changes in CD spectrum and other spectral properties, a few possible binding modes for p-TMPyP to poly[d(A-T)(2)] are suggested.     

Coupled energetics of lambda cro repressor self-assembly and site-specific DNA operator binding II: cooperative interactions of cro dimers

The bacteriophage lambda relies on interactions of the cI and cro repressors which self assemble and bind the two operators (O(R) and O(L)) of the phage genome to control the lysogenic to lytic switch. While the self assembly and O(R) binding of cI have been investigated in detail, a more complete understanding of gene regulation by phage lambda also requires detailed knowledge of the role of cro repressor as it dimerizes and binds at O(R) sites. Since dimerization and operator binding are coupled processes, a full elucidation of the regulatory energetics in this system requires that the equilibrium constants for dimerization and cooperative binding be determined. The dimerization constant for cro has been measured as a prelude to these binding studies. Here, the energetics of cro binding to O(R) are evaluated using quantitative DNaseI footprint titration techniques. Binding data for wild-type and modified O(R) site combinations have been simultaneously analyzed in concert with the dimerization energetics to obtain both the intrinsic and cooperative DNA binding energies for cro with the three O(R) sites. Binding of cro dimers is strongest to O(R)3, then O(R)1 and lastly, O(R)2. Adjacently bound repressors exhibit positive cooperativity ranging from -0.6 to -1.0 kcal/mol. Implications of these, newly resolved, energetics are discussed in the framework of a dynamic model for gene regulation. This characterization of the DNA-binding properties of cro repressor establishes the foundation on which the system can be explored for other, more complex, regulatory elements such as cI-cro cooperativity.     

ATP-Induced phosphorylation of the sarcoplasmic reticulum Ca2+ ATPase: molecular interpretation of infrared difference spectra.

Time-resolved infrared difference spectra of the ATP-induced phosphorylation of the sarcoplasmic reticulum Ca2+-ATPase have been recorded in H2O and 2H2O at pH 7.0 and 1 degrees C. The reaction was induced by ATP release from P3-1-(2-nitro)phenylethyladenosine 5'-triphosphate (caged ATP) and from [gamma-18O3]caged ATP. A band at 1546 cm-1, not observed with the deuterated enzyme, can be assigned to the amide II mode of the protein backbone and indicates that a conformational change associated with ATPase phosphorylation takes place after ATP binding. This is also indicated between 1700 and 1610 cm-1, where bandshifts of up to 10 cm-1 observed upon protein deuteration suggest that amide I modes of the protein backbone dominate the difference spectrum. From the band positions it is deduced that alpha-helical, beta-sheet, and probably beta-turn structures are affected in the phosphorylation reaction. Model spectra of acetyl phosphate, acetate, ATP, and ADP suggest the tentative assignment of some of the bands of the phosphorylation spectrum to the molecular groups of ATP and Asp351, which participate directly in the phosphate transfer reaction: a positive band at 1719 cm-1 to the C==O group of aspartyl phosphate, a negative band at 1239 cm-1 to the nuas(PO2-) modes of the bound ATP molecule, and a positive band at 1131 cm-1 to the nuas(PO32-) mode of the phosphoenzyme phosphate group, the latter assignment being supported by the band's sensitivity toward isotopic substitution in the gamma-phosphate of ATP. Band positions and shapes of these bands indicate that the alpha- and/or beta-phosphate(s) of the bound ATP molecule become partly dehydrated when ATP binds to the ATPase, that the phosphoenzyme phosphate group is unprotonated at pH 7.0, and that the C==O group of aspartyl phosphate does not interact with bulk water. The Ca2+ binding sites seem to be largely undisturbed by the phosphorylation reaction, and a functional role of the side chains of Asn, Gln, and Arg residues was not detected.     

Spectroscopic analysis of the interaction of Escherichia coli DNA-dependent RNA polymerase with T7 DNA and synthetic polynucleotides.

We have studied the circular dichroism and ultraviolet difference spectra of T7 bacteriophage DNA and various synthetic polynucleotides upon addition of Escherichia coli RNA polymerase. When RNA polymerase binds nonspecifically to T7 DNA, the CD spectrum shows a decrease in the maximum at 272 but no detectable changes in other regions of the spectrum. This CD change can be compared with those associated with known conformational changes in DNA. Nonspecific binding to RNA polymerase leads to an increase in the winding angle, theta, in T7 DNA. The CD and UV difference spectra for poly[d(A-T)] at 4 degrees C show similar effects. At 25 degrees C, binding of RNA polymerase to poly[d(A-T)] leads to hyperchromicity at 263 nm and to significant changes in CD. These effects are consistent with an opening of the double helix, i.e. melting of a short region of the DNA. The hyperchromicity observed at 263 nm for poly[d(A-T)] is used to determine the number of base pairs disrupted in the binding of RNA polymerase holoenzyme. The melting effect involves about 10 base pairs/RNA polymerase molecule. Changes in the CD of poly(dT) and poly(dA) on binding to RNA polymerase suggest an unstacking of the bases with a change in the backbone conformation. This is further confirmed by the UV difference spectra. We also show direct evidence for differences in the template binding site between holo- and core enzyme, presumably induced by the sigma subunit. By titration of the enzyme with poly(dT) the physical site size of RNA polymerase on single-stranded DNA is approximately equal to 30 bases for both holo- and core enzyme. Titration of poly[d(A-T)] with polymerase places the figure at approximately equal to 28 base pairs for double-stranded DNA.     

Raman spectroscopy of cytoplasmic muscle fiber proteins. Orientational order.

The polarized Raman spectra of glycerinated and intact single muscle fibers of the giant barnacle were obtained. These spectra show that the conformation-sensitive amide I, amide III, and C-C stretching vibrations give Raman bands that are stronger when the electric field of both the incident and scattered radiation is parallel to the fiber axis (Izz). The detailed analysis of the amide I band by curve fitting shows that approximately 50% of the alpha-helical segments of the contractile proteins are oriented along the fiber axis, which is in good agreement with the conformation and composition of muscle fiber proteins. Difference Raman spectroscopy was also used to highlight the Raman bands attributed to the oriented segments of the alpha-helical proteins. The difference spectrum, which is very similar to the spectrum of tropomyosin, displays amide I and amide III bands at 1,645 and 1,310 cm-1, respectively, the bandwidth of the amide I line being characteristic of a highly alpha-helical biopolymer with a small dispersion of dihedral angles. A small dichroic effect was also observed for the band due to the CH2 bending mode at 1,450 cm-1 and on the 1,340 cm-1 band. In the C-C stretching mode region, two bands were detected at 902 and 938 cm-1 and are both assigned to the alpha-helical conformation.     

Aggregation of chymotrypsinogen: portrait by infrared spectroscopy.

Changes in the secondary structure and aggregation of chymotrypsinogen were investigated by infrared difference spectroscopy in conjunction with temperature and pressure tuning IR spectroscopy; both the amide I' band and side chain bands were studied. A prominent component of the amide I' band in the difference spectrum obtained upon cooling a chymotrypsinogen solution, or increasing the hydrostatic pressure, was observed in the region between 1627 and 1622 cm-1. Under denaturing conditions a white gel was formed, which is attributed to irreversible self-association or aggregation. This process was accompanied by the appearance of two new amide I' bands in the infrared spectrum of the protein: a very strong band at 1618 cm-1 and a weak band at 1685 cm-1. These bands are assigned to peptide segments with anti-parallel aligned beta-strands.     

Infrared spectra of carbon monoxide bound to mitochondria from diverse species and tissues reveal structurally similar cytochrome c oxidase dioxygen reaction sites

Infrared bands for CO bound to mitochondria from bovine and porcine hearts, bovine brain, rat kidney, and blowfly flight muscle and to intact blowfly flight muscle have been measured in the carbon-oxygen stretch region. Each spectrum contains a narrow band near 1963 cm-1 similar to the major band found earlier for the carbonyl cytochrome c oxidase purified from bovine heart. A second band near 1959 cm-1 ascribed to a less stable conformer of the purified oxidase carbonyl is also detected in mitochondria. These spectra support very similar CO (and O2) binding sites among all the oxidases examined whether the enzyme is purified or is still within mitochondria or intact tissue and therefore suggest that the reduced heme A ligand binding site has been highly conserved during evolution.     

Conformation of d(GGGATCCC)2 in crystals and in solution studied by X-ray diffraction, Raman spectroscopy and molecular modelling.

In the crystal, d(GGGATCCC)2 forms an A-DNA double helix as known from a single crystal X-ray diffraction study. Accordingly, in the Raman spectra of crystals the A-family marker bands at 664, 705, 807 and 1101 cm-1 and the spectral characteristics in the region 1200 to 1500 cm-1 clearly demonstrate the A-form as the dominant conformation. Bands at 691, 850, and 1080 cm-1, however, indicate that a minor fraction of the octamer molecules in the crystal is in an unusual, still not unequivocally identified conformation possibly belonging to the B-family. In solution, the octamer is in B-like conformation as shown by the presence of B-DNA Raman marker bands at 685, 837, 1094 and 1421 cm-1. Molecular modelling techniques lead to three structures with slightly different B-form geometries as the lowest energies models when a sigmoidal dielectric function with the bulk dielectric constant epsilon = 78 and the value q = -0.5e for the effective phosphate charges was used in the calculations. An A-form structure bearing a strong resemblance to the experimentally determined crystal structure becomes the lowest energy model structure when the electrostatic parameters are changed to epsilon = 30 and q = -0.25e, respectively.     

Specificity of the interaction between lambda cro repressor protein and operator DNA fragments

Cro repressor protein is known to interact with specific sites in the operator DNA. The cro protein of lambda phage was isolated and the mode of its interaction with three different DNA fragment, lambda-OR3 17mer, phi 80-OR2 19mer and CAP binding site 22-mer, were examined by the use of proton NMR. Some of the imino proton resonances of lambda-OR3 shifted and were broadened remarkably on addition of lambda-cro protein, which indicated the induction of conformational change with complexation. In the spectrum of phi 80-OR2 which has a six base pair sequence common to lambda-OR3 the signals of the common base pairs revealed slight shifts on addition of lambda-cro protein. The imino proton signals of the CAP site DNA, however, did not show any change at all on mixing with lambda-cro. Combining the data of photo CIDNP of lambda-cro, we could postulate the mode of interaction between lambda-cro repressor and operator DNA.     

lambda Phage cro repressor interaction with DNA

We present here the complete identification of the resonances from the aromatic region of the 1H NMR spectrum of the cro repressor of the Escherichia coli lysogenic phage lambda. This was accomplished by the use of two-dimensional NMR analysis as well as specifically deuterated tyrosines. Not surprisingly, it shows that the published resonance assignment approached by more conventional methods by others includes substantial errors. The effect of complex formation with DNA was examined in the 1H NMR spectrum as well as in 19F NMR spectra from 3-fluorophenylalanine- or 3-fluorotyrosine-substituted cro repressors. The fluoro analogues show the practicality of using a structural gene cloned into an inducible system as a starting point to obtain both material and specific nuclear spin incorporation for NMR spectroscopy. The NMR data offer direct support for the speculative models of cro repressor-DNA complexes proposed from x-ray structure analysis on the protein alone.     

Characteristics and variations of B-type DNA conformations in solution: a quantitative analysis of Raman band intensities of eight DNAs

Raman spectra were obtained from four bacterial DNAs varying in GC content and four periodic DNA polymers in 0.1 M NaCl at 25 degrees C. A curve fitting procedure was employed to quantify and compare Raman band characteristics (peak location, height, and width) from 400 to 1600 cm-1. This procedure enabled us to determine the minimum number of Raman bands in regions with overlapping peaks. Quantitative comparison of the Raman bands of the eight DNAs provided several new results. All of the DNAs examined required bands near 809 (+/- 7) and 835 (+/- 5) cm-1 to accurately reproduce the experimental spectra. Since bands at these frequencies are associated with A-family and B-family conformations, respectively, this result indicates that all DNAs in solution have a mixture of conformations on the time scale of the Raman scattering process. Band characteristics in the 800-850-cm-1 region exhibited some dependence on CG content and base pair sequence. As previously noted by Thomas and Peticolas [Thomas, G. A., & Peticolas, W. L. (1983) J. Am. Chem. Soc. 105, 993], the poly[d(A)].poly[d(T)] spectra were qualitatively distinct in this region. The A-family band is clearly observed at 816 cm-1. The intensity of this band and that of the B-family band at 841 cm-1 were similar, however, to intensities in the natural DNA spectra. Three bands at 811, 823, and 841 cm-1 were required to reproduce the 800-850-cm-1 region of the poly[d(A-T)].poly[d(A-T)] spectra. This may indicate the presence of three backbone conformations in this DNA polymer. Analysis of intensity vs. GC content for 42 Raman bands confirmed previous assignments of base and backbone vibrations and provided additional information on a number of bands.