Local conformational changes induced in B-DNA by ethidium intercalation

Structural effects of binding the intercalating drug ethidium bromide (EtBr) to 160 base pair (bp) fragments of nucleosomal calf thymus DNA have been probed by the method of Raman difference spectroscopy. With the use of a near-infrared (NIR) laser source to excite the Raman spectrum at 752 nm, vibrational signatures of both the EtBr intercalant and DNA target have been identified in spectra of the drug-DNA complexes. Analysis of the results obtained on complexes consisting of 1 EtBr bound/10 bp leads to the following conclusions: (i) Raman markers diagnostic of DNA phosphodiester conformation are converted from the B type to the A type with EtBr binding, commensurate with the proportion of ethidium-bound nucleotides in the complex. (ii) Ethidium binding converts deoxynucleoside sugar puckers from the C2'-endo to the C3'-endo conformation, also consistent with binding stoichiometry. Both pyrimidine and purine deoxynucleoside sugar puckers are perturbed by the phenanthridinium ring intercalation. (iii) Phenanthridinium insertion between bases is accomplished with no apparent change in hypochromicities of purine or pyrimidine Raman markers, indicating that base-phenanthridinium interactions provide compensatory hypochromic effects. (iv) Novel Raman markers of helix unwinding have been identified and assigned primarily to methylene deformation modes of the deoxyribosyl C2'H(2) and C5'H(2) groups. The present study provides new insights into drug-DNA recognition in solution and demonstrates the feasibility of NIR-Raman spectroscopy for structural studies of highly chromophoric DNA complexes.     

Polarized Raman spectra of oriented fibers of A DNA and B DNA: anisotropic and isotropic local Raman tensors of base and backbone vibrations.

Polarized Raman spectra of oriented fibers of calf thymus DNA in the A and B conformations have been obtained by use of a Raman microscope operating in the 180 degrees back-scattering geometry. The following polarized Raman intensities in the spectral interval 200-1800 cm-1 were measured with both 514.5 and 488.0 nm laser excitations: (1) Icc, in which the incident and scattered light are polarized parallel to the DNA helical axis (c axis); (2) Ibb, in which the incident and scattered light are polarized perpendicular to c; and (3) Ibc and Icb, in which the incident and scattered light are polarized in mutually perpendicular directions. High degrees of structural homogeneity and unidirectional orientation were confirmed for both the A and B form fibers, as judged by comparison of the observed Raman markers and intensity anisotropies with measurements reported previously for oligonucleotide single crystals of known three-dimensional structures. The fiber Raman anisotropies have been combined with solution Raman depolarization ratios to evaluate the local tensors corresponding to key conformation-sensitive Raman bands of the DNA bases and sugar-phosphate backbone. The present study yields novel vibrational assignments for both A DNA and BDNA conformers and also confirms many previously proposed Raman vibrational assignments. Among the significant new findings are the demonstration of complex patterns of A form and B form indicator bands in the spectral intervals 750-900 and 1050-1100 cm-1, the identification of highly anisotropic tensors corresponding to vibrations of base, deoxyribose, and phosphate moieties, and the determination of relatively isotropic Raman tensors for the symmetrical stretching mode of phosphodioxy groups in A and B DNA. The present fiber results provide a basis for exploitation of polarized Raman spectroscopy to determine DNA helix orientation as well as to probe specific nucleotide residue orientations in nucleoproteins, viruses, and other complex biological assemblies.     

Orientations of Tyr 21 and Tyr 24 in the capsid of filamentous virus Ff determined by polarized Raman spectroscopy

The capsid of filamentous virus Ff is assembled from approximately 2750 copies of a 50-residue alpha-helical subunit, the two tyrosines of which (Tyr 21 and Tyr 24) are located within a hydrophobic sequence that constitutes the subunit interface. We have determined the side chain orientations of Tyr 21 and Tyr 24 by polarized Raman microspectroscopy of oriented Ff fibers, utilizing a novel experimental approach that combines site-specific mutation and residue-specific deuteration of capsid subunits. The polarized Raman signature of Tyr 21 was obtained by incorporating C(delta 1),C(delta 2),C(epsilon 1),C(epsilon 2)-tetradeuteriotyrosine at position 21 in an Ff mutant in which Tyr 24 is replaced with methionine. Similarly, the polarized Raman signature of Tyr 24 was obtained by incorporating C(delta 1),C(delta 2),C(epsilon 1),C(epsilon 2)-tetradeuteriotyrosine at position 24 in the analogous Tyr 21 --> Met mutant. Polarizations of the corresponding C-D stretching bands in the 2200-2400 cm(-1) interval of the Raman spectrum were measured and interpreted using tensors transferred from a polarized Raman analysis of L-tyrosine-2,3,5,6-d(4) single crystals. Polarized Raman analysis was extended to the bands of Ff near 642 and 855 cm(-1), which originate from vibrational modes of the tyrosine phenolic ring. The results indicate the following: (i) For both Tyr 21 and Tyr 24, the phenolic 2-fold axis (C(1)-C(4) line) is inclined at 41 +/- 5 degrees from the virion axis and the normal to the plane of the phenolic ring is inclined at 71 +/- 5 degrees from the virion axis; (ii) the mutation of Tyr 24, but not the mutation of Tyr 21, perturbs Raman markers of the subunit tryptophan (Trp 26), suggesting interdependence of Tyr 24 and Trp 26 orientations in native Ff; and (iii) polarization anisotropies observed for Raman markers of Ff DNA bases are unperturbed by mutation of either Tyr 21 or Tyr 24, indicating that nonrandom base orientations of packaged Ff DNA are independent of the mutation of either Tyr 21 or Tyr 24. A molecular model consistent with these findings is proposed.     

A 2H-NMR study of the A-DNA conformation in films of oriented Na-DNA: evidence of a disordered B-DNA contribution

Solid-state ²H-nmr spectra have been obtained from folded films of oriented Li- and Na-DNA molecules with the purine bases selectively deuterium labeled at the 8 position. From line shape simulations, we find that the Na-DNA sample at 75% relative humidity (rh) contains both A-DNA and surprisingly large amounts of B-DNA

1 Here, B-DNA refers to “B-DNA family” (i.e. B- or C-DNA).

(57%). For the A-DNA component the average base tilt is 23°, and the total distribution width of tilt angles and helix axis orientations is ～ 4° (standard deviation). In the B-DNA component the base tilt is ～ 0° and the total distribution width is ～ 20°. In contrast, films of Li-DNA only exhibit the B-form line shape, consistent with a base tilt of ～ 0° and a total distribution width of base tilt angles and helix axis orientations of 9°. The nmr results that demonstrate the presence of large amounts of B-DNA in the Na-DNA sample contrast with the x-ray diffraction measurements that indicated mainly A-form. The nmr spectra are used to monitor the B-DNA content in the Na-films and to evaluate procedures for increasing the A-DNA fraction.     

Polarized Raman spectroscopy of double-stranded RNA from bacteriophage phi6: local Raman tensors of base and backbone vibrations

Raman tensors for localized vibrations of base (A, U, G, and C), ribose and phosphate groups of double-stranded RNA have been determined from polarized Raman measurements on oriented fibers of the genomic RNA of bacteriophage phi6. Polarized Raman intensities for which electric vectors of both the incident and scattered light are polarized either perpendicular (I[bb]) or parallel (I[cc]) to the RNA fiber axis have been obtained by Raman microspectroscopy using 514.5-nm excitation. Similarly, the polarized Raman components, I(bc) and I(cb), for which incident and scattered vectors are mutually perpendicular, have been obtained. Spectra collected from fibers maintained at constant relative humidity in both H2O and D2O environments indicate the effects of hydrogen-isotopic shifts on the Raman polarizations and tensors. Novel findings are the following: 1) the intense Raman band at 813 cm(-1), which is assigned to phosphodiester (OPO) symmetrical stretching and represents the key marker of the A conformation of double-stranded RNA, is characterized by a moderately anisotropic Raman tensor; 2) the prominent RNA band at 1101 cm(-1), which is assigned to phosphodioxy (PO2-) symmetrical stretching, also exhibits a moderately anisotropic Raman tensor. Comparison with results obtained previously on A, B, and Z DNA suggests that tensors for localized vibrations of backbone phosphodiester and phosphodioxy groups are sensitive to helix secondary structure and local phosphate group environment; and 3) highly anisotropic Raman tensors have been found for prominent and well-resolved Raman markers of all four bases of the RNA duplex. These enable the use of polarized Raman spectroscopy for the determination of purine and pyrimidine base residue orientations in ribonucleoprotein assemblies. The present determination of Raman tensors for dsRNA is comprehensive and accurate. Unambiguous tensors have been deduced for virtually all local vibrational modes of the 300-1800 cm(-1) spectral interval. The results provide a reliable basis for future evaluations of the effects of base pairing, base stacking, and sequence context on the polarized Raman spectra of nucleic acids.     

Raman spectroscopy of DNA-metal complexes. I. Interactions and conformational effects of the divalent cations: Mg, Ca, Sr, Ba, Mn, Co, Ni, Cu, Pd, and Cd.

Interactions of divalent metal cations (Mg2+, Ca2+, Ba2+, Sr2+, Mn2+, Co2+, Ni2+, Cu2+, Pd2+, and Cd2+) with DNA have been investigated by laser Raman spectroscopy. Both genomic calf-thymus DNA (> 23 kilobase pairs) and mononucleosomal fragments (160 base pairs) were employed as targets of metal interaction in solutions containing 5 weight-% DNA and metal:phosphate molar ratios of 0.6:1. Raman difference spectra reveal that transition metal cations (Mn2+, Co2+, Ni2+, Cu2+, Pd2+, and Cd2+) induce the greatest structural changes in B-DNA. The Raman (vibrational) band differences are extensive and indicate partial disordering of the B-form backbone, reduction in base stacking, reduction in base pairing, and specific metal interaction with acceptor sites on the purine (N7) and pyrimidine (N3) rings. Many of the observed spectral changes parallel those accompanying thermal denaturation of B-DNA and suggest that the metals link the bases of denatured DNA. While exocyclic carbonyls of dT, dG, and dC may stabilize metal ligation, correlation plots show that perturbations of the carbonyls are mainly a consequence of metal-induced denaturation of the double helix. Transition metal interactions with the DNA phosphates are weak in comparison to interactions with the bases, except in the case of Cu2+, which strongly perturbs both base and phosphate group vibrations. On the other hand, the Raman signature of B-DNA is largely unperturbed by Mg2+, Ca2+, Sr2+, and Ba2+, suggesting much weaker interactions of the alkaline earth metals with both base and phosphate sites. A notable exception is a moderate perturbation by alkaline earths of purine N7 sites in 160-base pair DNA, with Ca2+ causing the greatest effect. Correlation plots demonstrate a strong interrelationship between perturbations of Raman bands assigned to ring vibrations of the bases and those of bands assigned to exocyclic carbonyls and backbone phosphodiester groups. However, strong correlations do not occur between the Raman phosphodioxy band (centered near 1092 cm-1) and other Raman bands, suggesting that the former is not highly sensitive to the structural changes induced by divalent metal cations. The structural perturbations induced by divalent cations are much greater for > 23-kilobase pair DNA than for 160-base pair DNA, as evidenced by both the Raman difference spectra and the tendency toward the formation of insoluble aggregates. In the presence of transition metals, aggregation of high-molecular-weight DNA is evident at temperatures as low as 11 degrees C.(ABSTRACT TRUNCATED AT 400 WORDS)     

Structural details of the thermophilic filamentous bacteriophage PH75 determined by polarized Raman microspectroscopy

The filamentous virus PH75, which infects the thermophile Thermus thermophilus, consists of a closed DNA strand of 6500 nucleotides encapsidated by 2700 copies of a 46-residue coat subunit (pVIII). The PH75 virion is similar in composition to filamentous viruses infecting mesophilic bacteria but is distinguished by in vivo assembly at 70 degrees C and thermostability to at least 90 degrees C. Structural details of the PH75 assembly are not known, although a fiber X-ray diffraction based model suggests that capsid subunits are highly alpha-helical and organized with the same symmetry (class II) as in the mesophilic filamentous phages Pf1 and Pf3 [Pederson et al. (2001) J. Mol. Biol. 309, 401-421]. This is distinct from the symmetry (class I) of phages fd and M13. We have employed polarized Raman microspectroscopy to obtain further details of PH75 architecture. The spectra are interpreted in combination with known Raman tensors for modes of the pVIII main chain (amide I) and Trp and Tyr side chains to reveal the following structural features of PH75: (i) The average pVIII peptide group is oriented with greater displacement from the virion axis than peptide groups of fd, Pf1, or Pf3. The data correspond to an average helix tilt angle of 25 degrees in PH75 vs 16 degrees in fd, Pf1, and Pf3. (ii) The indolyl ring of Trp 37 in PH75 projects nearly equatorially from the subunit alpha-helix axis, in contrast to the more axial orientations for Trp 26 of fd and Trp 38 of Pf3. (iii) The phenolic rings of Tyr 15 and Tyr 39 project along the subunit helix axis, and one phenoxyl engages in hydrogen-bonding interaction that has no counterpart in either fd or Pf1 tyrosines. Also, in contrast to fd, Pf1, and Pf3, the packaged DNA genome of PH75 exhibits no Raman anisotropy, suggesting that DNA bases are not oriented unidirectionally within the nucleocapsid assembly. The structural findings are discussed in relation to intrasubunit and intersubunit interactions that may confer hyperthermostability to the PH75 virion. A refined molecular model is proposed for the PH75 capsid subunit.     

Joint interaction of ethidium bromide and methylene blue with DNA. The effect of ionic strength on binding thermodynamic parameters

Large amount of data of experimental and theoretical studies have shown that ethidium bromide (EtBr) and methylene blue (MB) may bind to nucleic acids via three modes: intercalation between two adjacent base pairs, insertion into the plane between neighboring bases in the same strand (semi-intercalation), and outside binding with negatively charged backbone phosphate groups. The aim of the given research is to examine the behavior of these two ligands at both separate and joint DNA binding. The obtained experimental data show that the effect of simultaneous binding of EtBr and MB on double-stranded DNA has a non-additive effect of separate binding. The analyses of the melting thermodynamic parameters of DNA complexes with two bound ligands suggest competitive mechanism of interaction.     

Viscometric analysis of the interaction of bisphenanthridinium compounds with closed circular supercoiled and linear DNA.

The interaction with closed circular supercoiled and linear DNA of bisphenanthridinium compounds substituted through both the meta and para positions of the 6-phenyl group, along with appropriate monomer intercalators as controls, has been investigated by viscometric titration. When CPK models for the phenanthridinium rings of the three bis-compounds are oriented in a parallel manner as a model for intercalation, their ring plane to ring plane distances are approximately 7 to 8 A (SR 2430), 11 A (SR 2193), and 15 A (SR 2166). In SR 2430 the two phenanthridines are linked through the para positions of the 6-phenyl group; this chain allows intercalation of the two rings at adjacent binding sites in DNA, but is not long enough to accommodate an excluded site. The viscometric titrations with both superhelical and linear DNA clearly indicate that SR 2430 gives results close to those of the monomer control compounds while SR 2193 and SR 2166 have approximately twice the unwinding angle and DNA length increase on binding to DNA as the monomer compounds. These phenanthridinium compounds, therefore, are capable of bisintercalation only if their linking groups are of sufficient length to allow an excluded binding site between base pairs. This conclusion is supported by DNA thermal denaturation experiments in the presence of these compounds.     

HU protein employs similar mechanisms of minor-groove recognition in binding to different B-DNA sites: demonstration by Raman spectroscopy

The sequence isomers d(CGCAAATTTGCG) and d(TCAAGGCCTTGA) form self-complementary duplexes that present distinct targets for binding of the homodimeric architectural protein HU of Bacillus stearothermophilus (HUBst). Raman spectroscopy shows that although each duplex structure is of the B-DNA type, there are subtle conformational dissimilarities between them, involving torsion angles of the phosphodiester backbone and the arrangements of stacked bases. Each DNA duplex forms a stable stoichiometric (1:1) complex with HUBst, in which the structure of the HUBst dimer is largely conserved. However, the Raman signature of each DNA duplex is perturbed significantly and similarly with HUBst binding, as reflected in marker bands assigned to localized vibrations of the phosphodiester moieties and base residues. The spectral perturbations identify a reorganization of the DNA backbone and partial unstacking of bases with HUBst binding, which is consistent with non-sequence-specific minor-groove recognition. Prominent among the HUBst-induced perturbations of B-DNA are a conversion of approximately one-third of the alpha/beta/gamma torsions from the canonical g(-)/t/g(+) conformation to an alternative conformation, an equivalent conversion of deoxyadenosyl moieties from the C2'-endo/anti to the C3'-endo/anti conformation, and appreciable unstacking of purines. The results imply that each solution complex is characterized by structural perturbations extending throughout the 12-bp sequence. Comparison with previously studied protein/DNA complexes suggests that binding of HUBst bends DNA by approximately 70 degrees.     

Anthracycline-DNA interactions studied with linear dichroism and fluorescence spectroscopy

DNA-binding geometry and dynamics of a number of anthracyclines, including adriamycin and 4-demethoxydaunorubicin, interacting with DNA have been studied by means of linear dichroism and fluorescence techniques. The anthracycline chromophore is found to be approximately parallel to the plane of the DNA bases and to have a restricted mobility, as would be expected for an intercalative binding mode, but there are variations between different directions in the chromophore as well as between the drugs. From dichroic spectra of adriamycin in an anisotropic host of poly(vinyl alcohol), absorption components corresponding to transitions with mutually orthogonal polarizations have been resolved. These can be exploited to determine the orientations of the two chromophore axes in the DNA complex relative to the DNA helix axis. In a certain binding regime the long axis of the bound anthracycline chromophores (with the exception of 4-demethoxydaunorubicin) is found to be approximately 10 degrees closer to perpendicular to the helix axis than are the DNA bases. This demonstrates that the average base tilt is at least 10 degrees. By contrast, the short axis of the aglycon moiety is found to be tilted some 20-30 degrees from perpendicular. This may be because it is probing a base direction with a more pronounced, static or dynamic, inclination than the average in DNA. The drug orientation and the DNA orientation (reflecting flexibility) are observed to vary differently and nonmonotonically with binding ratio, suggesting specific binding and varying site geometries.(ABSTRACT TRUNCATED AT 250 WORDS)     

Characterization of DNA structures by laser Raman spectroscopy

Oriented fibers drawn from aqueous gels of calf-thymus DNA were maintained at constant relative humidites of 75 and 92% to yield canonical A-DNA and B-DNA structures, respectively. Raman spectra of the two forms of DNA were recorded over the spectral range 300–4000 cm^?1. The authenticated DNA fibers were deuterated in hygrostatic cells containing D₂O at appropriate relative humidities, and the corresponding spectra of deuterated DNAs were also obtained. The spectra reveal all of the Raman scattering frequencies and intensities characteristic of A- and B-DNA structures in both nondeuterated and deuterated froms, as well as the frequencies and intensities of adsorbed solvent molecules from which the hydration content of DNA fibers can be calculated. Numerous conformation-sensitive vibrational modes of DNA bases and phosphate groups have been identified throughout the 300–1700-cm^?1 interval. Evidence has also been obtained for conformation sensitivity of deoxyribosyl CH stretching modes in the 2800–3000-cm^?1 region. Raman lines of both the backbone and the bases are proposed as convenient indicators of A- and B-DNA structures. The results are extended to Z-DNA models investigated previously. Some implications of these findings for the determination of DNA or RNA structure from Raman spectra of nucleoproteins and viruses are considered.     

Raman spectra of single crystals of r(GCG)d(CGC) and d(CCCCGGGG) as models for A DNA, their structure transitions in aqueous solution, and comparison with double-helical poly(dG).poly(dC)

The self-complementary oligonucleotides [r(CGC)d(CGC)]2 and [d(CCCCGGGG)]2 in single-crystal and solution forms have been investigated by Raman spectroscopy. Comparison of the Raman spectra with results of single-crystal X-ray diffraction and with data from polynucleotides permits the identification of a number of Raman frequencies diagnostic of the A-helix structure for GC sequences. The guanine ring frequency characteristic of C3'-endo pucker and anti base orientation is assigned at 668 +/- 2 cm-1 for both dG and rG residues of the DNA/RNA hybrid [r(GCG)d(CGC)]2. The A-helix backbone of crystalline [r(GCG)d(CGC)]2 is altered slightly in the aqueous structure, consistent with the conversion of at least two residues to the C2'-endo/anti conformation. For crystalline [d(CCCCGGGG)]2, the Raman and X-ray data indicate nucleosides of alternating 2'-endo-3'-endo pucker sandwiched between terminal and penultimate pairs of C3'-endo pucker. The A-A-B-A-B-A-A-A backbone of the crystalline octamer is converted completely to a B-DNA fragment in aqueous solution with Raman markers characteristic of C2'-endo/anti-G (682 +/- 2) and the B backbone (826 +/- 2 cm-1). In the case of poly(dG).poly(dC), considerable structural variability is detected. A 4% solution of the duplex is largely A DNA, but a 2% solution is predominantly B DNA. On the other hand, an oriented fiber drawn at 75% relative humidity reveals Raman markers characteristic of both A DNA and a modified B DNA, not unlike the [d-(CCCCGGGG)]2 crystal. A comparison of Raman and CD spectra of the aqueous [d(CCCCGGGG)]2 and poly(dG).poly(dC) structures suggests the need for caution in the interpretation of CD data from G clusters in DNA.     

Circular dichroism of flow-oriented nucleic acids. II. Comparison between observed and calculated spectra.

The ultraviolet circular dichroism (CD) of oriented DNA and RNA molecules is calculated by an extension of Johnson and Tinoco's theory [(1969) Biopolymers 7 , 727–749] for unoriented molecules. The calculations are carried out for molecular models of A-DNA, B-DNA, planar B-DNA, C-DNA, and RNA-11-α. The calculated curves are compared to measured spectra [(1975) J. Mol. Biol. 92 , 449–466] Chung and Holzwarth, for oriented solutions of DNA in buffer, DNA in 6 M LiCl or in ethylene glycol, and double-stranded viral RNA. The calculation, which considers only base–base interactions, predicts that the CD of B-DNA, measured with light propagating parallel to the helix axis, should be large and semiconservative, whereas the CD for light propagating perpendicular to the helix axis should be nonconservative. These predictions agree qualitatively with the experimental observations for DNA in buffer; agreement improves if one assumes the bases to be exactly perpendicular to the helix axis. For the other geometries, agreement is less satisfactory, but qualitative agreement with experiment is obtained and the signs of the specific CD spectra are in accord with observations.     

Low-frequency dynamics and Raman scattering of crystals, of B-, A-, and Z-DNA, and fibers of C-DNA

Normal modes of vibration of DNA in the low-frequency region (10-300 cm-1 interval) have been identified from Raman spectra of crystals of B-DNA [d(CGCAAATTTGCG)], A-DNA [r(GCG)d(CGC) and d(CCCCGGGG)], and Z-DNA [d(CGCGCG) and d(CGCGTG)]. The lowest vibrational frequencies detected in the canonical DNA structures--at 18 +/- 2 cm-1 in the B-DNA crystal, near 24 +/- 2 cm-1 in A-DNA crystals, and near 30 +/- 2 cm-1 in Z-DNA crystals--are shown to correlate well with the degree of DNA hydration in the crystal structures, as well as with the level of hydration in calf thymus DNA fibers. These findings support the assignment [H. Urabe et al. (1985) J. Chem. Phys. 82, 531-535; C. Demarco et al. (1985) Biopolymers 24, 2035-2040] of the lowest frequency Raman band of each DNA to a helix mode, which is dependent primarily upon the degree of helix hydration, rather than upon the intrahelical conformation. The present results show also that B-, A-, C-, and Z-DNA structures can be distinguished from one another on the basis of their characteristic Raman intensity profiles in the region of 40-140 cm-1, even though all structures display two rather similar and complex bands centered within the intervals of 66-72 and 90-120 cm-1. The similarity of Raman frequencies for B-, A-, C-, and Z-DNA suggests that these modes originate from concerted motions of the bases (librations), which are not strongly dependent upon helix backbone geometry or handedness. Correlation of the Raman frequencies and intensities with the DNA base compositions suggests that the complex band near 90-120 cm-1 in all double-helix structures is due to in-plane librational motions of the bases, which involve stretching of the purine-pyrimidine hydrogen bonds. This would explain the centering of the band at higher frequencies in structures containing G.C pairs (greater than 100 cm-1) than in structures containing A.T pairs (less than 100 cm-1), consistent with the strengths of G.C and A.T hydrogen bonding.     

Static disorder and librational motions of the purine bases in films of oriented Li-DNA

Solid-state 2H nuclear magnetic resonance line shapes have been obtained from folded films of oriented Li-DNA molecules with the purine bases selectively labeled with deuterium at the 8-position. From line shape simulations, the static base tilts as well as the anisotropic motional amplitudes were determined as a function of hydration level and temperature. It was found that the average tilt angle of the bases is close to 0 degrees and at a hydration of ten water molecules per nucleotide the distribution width of tilt angles about this average cannot be larger than 9 degrees (standard deviation). A slightly increased distribution width is observed at low hydration levels. The motional amplitudes are hydration dependent, with the tilting motion ranging from 4 degrees for the driest, up to 15 degrees for the wettest sample, and slightly larger amplitudes are observed for the twisting motion. The amplitude of the twisting motion is unaffected by a temperature decrease down to -60 degrees C, in contrast to the tilting motion that is suppressed at low temperatures.     

Interactions of molecules with nucleic acids. XI. Generalization of techniques to generate nucleic acid structures with applications to intercalation sites and kinked structures

A generalized procedure to generate nucleic acid structures is presented. In this procedure, the bases of a base pair are oriented first for characterization of particular DNA receptor sites. The resultant sites are then used in the study of specific molecule–DNA interactions. For example, intercalation sites, kinked DNA, and twisted and tilted bases are envisioned. Alterations of structures via anti → syn orientations of bases, as well as crankshaft motion about collinear bonds, provide additional conformations without disrupting the overall backbone structure. These approaches to the generation of nucleic acid structures are envisioned as required in studies of the intercalation phenomenon, minor adjustments of DNA to accommodate denaturation, binding of carcinogens to DNA, complex formation of transition metals with DNA, and antitumor agents as ligands. For these base-pair and base orientations, backbone orientations are calculated by the AGNAS technique to yield physically meaningful conformations, namely, those conformations for which nonbonded contacts are favourable. A procedure is presented to generate dimer duplex units that are physically meaningful and to assemble these units into a polynucleotide duplex. Double helices that begin with B-DNA, undergo a transition to one of the above-mentioned receptor sites, and return to B-DNA can be assembled from a catalog of dimer duplexes. Stereographic projections of the various receptor sites already being used to model binding to DNA are presented.     

Coenzyme reorientations in the active sites of aspartate aminotransferase isoenzymes studied by linear dichroism method

Cytosolic and mitochondrial pig heart aspartate aminotransferases (cAspAT and mAspAT) and chicken heart cAspAT have been oriented in a compressed slab of polyacrylamide gel and their linear dichroism LD spectra have been recorded. The coenzyme's tilt angles in the active sites of chicken cAspAT and pig mAspAT and their quasisubstrate complexes imitating catalytic intermediates have been computed. The computations are based on reduced linear dichroism values (delta A/A), the known directions of the transition dipole moments in the coenzyme ring and atomic coordinates of the coenzyme obtained by X-ray crystallography. It has been found that formation of the enzyme complex with glutarate and protonation of the internal pyridoxal-lysine aldimine induce reorientations of the coenzyme. As a result of protonation, the coenzyme ring tilts by 27 degrees in cAspAT and 13 degrees in mAspAT. Formation of the external aldimine with 2-methylaspartate is accompanied by tilting of the coenzyme ring by 44 degrees in cAspAT and 39 degrees in mAspAT. For the quinonoid complex with erythro-3-hydroxyaspartate, the tilt angles were found to be 63 degrees in cAspAT and 53 degrees in mAspAT. It is inferred that the basic features of the active site dynamics are similar in the three AspAT's studied. The differences in the coenzyme tilt angles between cAspAT and mAspAT may be linked to catalytic and structural peculiarities of the isoenzymes.