Studies of the interaction of the fluorophores harmine and harmaline with calf thymus DNA.

The binding to calf thymus DNA of the hallucinogen harmine and one of its analogues harmaline was studied by absorption spectrophotometry and fluorescence quenching analysis. Viscosity measurements were also carried out. For both molecules, quenched and unquenched sites on DNA are present. For each type of binding site, the value of the product of the number of sites times the association constant was determined. Harmine is more strongly bound than harmaline. Viscosity measurements indicate intercalation in the case of harmine only.     

The interaction of ellipticine derivatives with nucleic acids studied by optical and 1H-nmr spectroscopy: Effect of size of the heterocyclic ring system

The DNA interaction of derivatives of ellipticine with heterocyclic ring systems with three, four, or five rings and a dimethylaminoethyl side chain was studied. Optical spectroscopy of drug complexes with calf thymus DNA, poly [(dA-dT) · (dA-dT)], or poly [(dG-dC) · (dG-dC)] showed a 10 nm bathochromic shift of the light absorption bands of the pentacyclic and tetracyclic compounds upon binding to the nucleic acids, which indicates binding by intercalation. For the tricyclic compound a smaller shift of 1–3 nm was observed upon binding to the nucleic acids. Flow linear dichroism studies show that the geometry of all complexes is consistent with intercalation of the ring system, except for the DNA and poly [(dG-dC) · (dG-dC)] complexes of the tricyclic compound, where the average angle between the drug molecular plane and the DNA helix axis was found to be 65°. One-dimensional ¹H-nmr spectroscopy was used to study complexes between d(CGCGATCGCG)₂ and the tricyclic and pentacyclic compounds. The results on the pentacyclic compound show nonselective broadening due to intermediate chemical exchange of most oligonucleotide resonances upon drug binding. The imino proton resonances are in slow chemical exchange, and new resonances with upfield shifts approaching 1 ppm appear upon drug binding, which supports intercalative binding of the pentacyclic compound. The results on the tricyclic compound show more rapid binding kinetics and very selective broadening of resonances. The data suggest that the tricyclic compound is in an equilibrium between intercalation and minor groove binding, with a preference to bind close to the AT base pairs with the side chain residing in the minor groove. © 1994 John Wiley & Sons, Inc.     

Orientation and linear dichroism characteristics of porphyrin-DNA complexes

The linear dichroism spectra of complexes of tetrakis(N-methyl-4-pyridinio)prophine (H2TMpyP) and its zinc(II) derivative (ZnTMpyP) with DNA oriented in a flow gradient have been investigated. The dichroism of H2TMpyP determined within the Soret band and the Qy band system is consistent with an intercalative conformation in which the plane of the porphyrin ring system is nearly parallel to the planes of the DNA bases. In the case of ZnTMpyP on the other hand, the porphyrin ring system is inclined at angles of 62-67 degrees with respect to the axis of the DNA helix. The pyridyl groups in both cases are characterized by a low degree of orientation with respect to the axis of the helix. In contrast to H2TMpyP which does not significantly affect the degree of alignment of the DNA in the flow gradient, the binding of ZnTMpyP causes a significant decrease (about 50% for a base pair/ZnTMpyP ratio of 20) in the intrinsic dichroism at 260 nm due to the oriented DNA bases; the binding of ZnTMpyP to DNA either gives rise to regions of higher flexibility or causes bends or kinks at the binding sites. Increasing the ionic strength has little influence on the linear dichroism of the ZnTMpyP-DNA complexes, but the number of molecules bound at intercalation sites diminishes in the case of the H2TMpyP-DNA complexes; the accompanying changes in the linear dichroism characteristics suggest that external H2TMpyP complexes are formed at the expense of intercalation complexes.(ABSTRACT TRUNCATED AT 250 WORDS)     

X-ray diffraction and infrared circular dichroism of DNA-violamycin B1 complexes

X-ray diffraction and infrared linear dichroism of oriented samples of DNA-violamycin B1 complexes have been studied at different antibiotic/DNA phosphate ratios (r) as a function of relative humidity. Violamycin B1 binds to DNA according to the intercalation as well as to the outside binding model. At low r values, where the intercalation predominates the unwinding angle of DNA helix is between 6 degrees and 12 degrees per intercalation site as followed from the dependence of the pitch of helix versus r. At r greater than or equal to 0.17 the intercalation sites are saturated and the outside binding becomes prevalent; however the violamycin B1 chromophore is still oriented in the plane of DNA bases. Conformational mobility of DNA in the violamycin B1 complexes is largely inhibited compared with pure DNA, but it is higher than that of the daunomycin complexes. At least 30% of DNA in violamycin complexes has A conformation at the medium humidities as followed by IR linear dichroism. In the case of x-ray diffraction the A conformation was not detected. The distance between DNA molecules in the complex is found to be 23.2 A, that is 2 A less than in pure DNA at the same conditions and it does not depend upon r.     

Transient and linear dichroism studies on bacteriorhodopsin: determination of the orientation of the 568 nm all-trans retinal chromophore

The orientation of the 568 nm transition dipole moment of the retinal chromophore of bacteriorhodopsin has been determined in purple membranes from Halobacterium halobium and in reconstituted vesicles. The angle between the 568 nm transition dipole moment and the normal to the plane of the membrane was measured in two different ways.In the first method the angle was obtained from transient dichroism measurements on bacteriorhodopsin incorporated into large phosphatidylcholine vesicles. Following flash excitation with linearly polarized light, the anisotropy of the 568 nm ground-state depletion signal first decays but then reaches a time-independent value. This result, obtained above the lipid phase transition, is interpreted as arising from rotational motion of bacteriorhodopsin which is confined to an axis normal to the plane of the membrane. It is shown that the relative amplitude of the time-independent component depends on the orientation of the 568 nm transition dipole moment. From the data an angle of 78 ° ± 3 ° is determined.In the second method the linear dichroism was measured as a function of the angle of tilt between the oriented purple membranes and the direction of the light beam. The results were corrected for the angular distribution of the membranes within the oriented samples, which was determined from the mosaic spread of the first-order lamellar neutron diffraction peak. In substantial agreement with the results of the transient dichroism method, linear dichroism measurements on oriented samples lead to an angle of 71 ° ± 4 °.No significant wavelength dependence of the dichroic ratio across the 568 nm band was observed, implying that the exciton splitting in this band must be substantially smaller than the recently suggested value of 20 nm (Ebrey et al., 1977).The orientation of the 568 nm transition dipole moment, which coincides with the direction of the all-trans polyene chain of retinal, is not only of interest in connection with models for the proton pump, but can also be used to calculate the inter-chromophore distances in the purple membrane.     

Flow linear dichroism spectra of four filamentous bacteriophages: DNA and coat protein contributions

In this study, we have separated the contributions of DNA and protein to the absorption and linear dichroism (LD) of each of four phages: fd, IKe, Pf1, and Pf3. We have found that the DNA packaged in each of the phages is hypochromic relative to the purified single stranded DNA, suggesting that bases are stacked in all of the phages. We have oriented the phages by flow and for the first time report the intrinsic LD from 320 to 190 nm for each of these phages. From the intrinsic LD of the phages and the isotropic absorption of the individual components, we have determined the reduced dichroism of the DNA within the phages and, subsequently, the maximum angle of inclination of the DNA bases (from the helix axis) for the packaged DNA. The maximum angles were 63° and 64° for the DNAs of class I phages fd and IKe, respectively. The angles were significantly less, 51° and 49°, for the DNAs of the class II phages Pf1 and Pf3, respectively. Thus, the two classes of phage differ in the structures of their packaged DNA, the DNA bases of the class II phages being more parallel to the long axis of the phage than are the DNA bases of the class I phages.     

Spectroscopic studies of 9-hydroxyellipticine binding to DNA

The binding of 9-hydroxyellipticine to calf thymus DNA, poly[d(A-T)]₂, and poly-[d(G-C)]₂ has been studied in detail by means of CD, linear dichroism, resonance light scattering, and molecular dynamics. The transition moment polarizations of 9-hydroxyelliptiycine were determined in polyvinyl alcohol stretched film. Spectroscopic solution studies of the DNA/drug complex are combined with theoretical CD calculations using the final 50 ps of a series of molecular dynamics simulations as input. The spectroscopic data shows 9-hydroxyellipticine to adopt two main binding modes, one intercalative and the other a stacked binding mode involving the formation of drug oligomers in the DNA major groove. Analysis of the intercalated binding mode in poly[d(A-T)]₂ suggests the 9-hydroxyellipticine hydroxyl group lies in the minor groove and hydrogen bonds to water with the pyridine ring protruding into the major groove. The stacked binding mode was examined using resonance light scattering and it was concluded that the drug was forming small oligomer stacks rather than extended aggregates. Reduced linear dichroism measurements suggested a binding geometry that precluded a minor groove binding mode where the plane of the drug makes a 45° angle with the plane of the bases. Thus it was concluded that the drug stacks in the major groove. No obvious differences in the mode of binding of 9-hydroxyellipticine were observed between different DNA sequences; however, the stacked binding mode appeared to be more favorable for calf thymus DNA and poly[d(G-C)]₂ than for poly[d(A-T)]₂, an observation that could be explained by the slightly greater steric hindrance of the poly[d(A-T)]₂ major groove. A strong concentration dependence was observed for the two binding modes where intercalation is favored at very low drug load, with stacking interactions becoming more prominent as the drug concentration is increased. Even at DNA : drug mixing ratios of 70:1 the stacked binding mode was still important for GC-rich DNAs. © 1998 John Wiley & Sons, Inc. Biopoly 46: 127–143, 1998     

Interaction of Topotecan,DNA Topoisomerase I Inhibitor,with Double-stranded Polydeoxyribonucleotides. 3. Binding at the Minor Groove

Interaction of topotecan (TPT) with calf thymus DNA, coliphage T4 DNA, and poly(dGdC) · poly(dG-dC) was studied by optical (linear flow dichroism, UV-vis spectroscopy) and quantum chemical methods. The linear dichroism signal of TPT bound to DNA was shown to have positive sign in the range 260–295 nm. This means that the plane of quinoline fragment (rings A and B) of TPT forms an angle less than 54° with the long axis of DNA, and hence the TPT molecule cannot intercalate between DNA base pairs. TPT was established to bind to calf thymus DNA as readily as to coliphage T4 DNA whose cytosines in the major groove were all glycosylated at the 5th position. Consequently, the DNA major groove does not participate in TPT binding. TPT molecule was shown to compete with distamycin for binding sites in the minor groove of DNA and poly(dG-dC) · poly(dG-dC). Thus, it was demonstrated for the first time that TPT binds to DNA at its minor groove.     

Amine group of guanine enhances the binding of norfloxacin antibiotics to DNA.

The binding mode of norfloxacin, a quinolone antibacterial agent, in the synthetic polynucleotides poly[d(G-C)2], poly[d(I-C)2] and poly[d(A-T)2] was studied using polarized light spectroscopy, fluorescence spectroscopy and melting profiles. The absorption, circular and linear dichroism properties of norfloxacin are essentially the same for all the complexes, and the angle of electric transition dipole moment I and II of norfloxacin relative to the DNA helix axis is measured as 68-75 degrees for all complexes. These similarities indicate that the binding mode of norfloxacin is similar for all the polynucleotides. The decrease in the linear dichroism (LD) magnitude at 260 nm upon binding norfloxacin, which is strongest for the norfloxacin-poly[d(G-C)2] complex, and the identical melting temperature of poly[d(A-T)2] and poly[d(I-C)2] in the presence and absence of norfloxacin rule out the possibility of classic intercalation and minor groove binding. However, the characteristics of the fluorescence emission spectra of norfloxacin bound to poly[d(A-T)2] and to poly[d(I-C)2] are similar but are different to that of norfloxacin bound to poly[d(G-C)2]. As the amine group of the guanine base protrudes to the minor groove, this result strongly suggests that norfloxacin binds in the minor groove of B-form DNA in a nonclassic manner.     

Orientation of reaction center and antenna chromophores in the photosynthetic membrane of rhodopseudomonas viridis

Whole cells of Rhodopseudomonas viridis were oriented in a magnetic field. The degree of orientation of the cells was determined by using a photoselection technique. In order to deduce the orientation of the antennae and chromophores of the reaction centers with respect to the membrane plane, we performed linear dichroism measurements of absolute spectra and light induced difference spectra linked to states P⁺I and PI^? on oriented cells. These measurements lead to the following conclusions:The antennae bacteriochlorophyll molecular plane is nearly perpendicular to the membrane. The Q_y and Q_x transitions moments of these molecules make respectively angles of 20 and 70°ith the membrane plane. The antenna carotenoid molecules make an angle of 45°ith the membrane.The primary electron donor possesses two transition moments centered respectively at 970 and 850 nm. The 970 nm transition moment is parallel to the membrane plane, the 850 nm transition is tilted out of the plane. Upon photooxidation of this primary electron donor, a monomer-like absorption band appears at 805 nm. Its transition makes an angle smaller than 25° with the membrane. The photooxidation of the dimer also induces an absorption band shift for the two other bacteriochlorophyll molecules of the reaction center. The absorption band shifts of the two bacteriochlorophyll molecules occur in opposite direction.One bacteriopheophytin molecule is photoreduced in state PI^?. This photoreduction induces an absorption band shift for only one bacteriochlorophyll molecule. Finally, the geometry of the dimeric primary donor seems to be affected by the presence of a negative charge in the reaction center.     

Aryl substituted ruthenium bis-terpyridine complexes: intercalation and groove binding with DNA

The non-covalent interaction of five novel ruthenium(II) bis-terpyridine complexes with calf thymus DNA and, where appropriate, with poly[d(G-C)](2) and poly[d(A-T)](2) is described. Each complex is functionalised with aryl tail groups in the 4' position of the terpyridine ligands ((i) 9-anthracenyl, (ii) 4,4'-biphenyl, (iii) beta-naphthyl, (iv) 9-phenanthrenyl, and (v) 1-pyrenyl). Circular dichroism and linear dichroism show that the binding of three of the complexes (phenanthrenyl, anthracenyl and pyrenyl) at low metal complex concentration is dominated by intercalation of the aryl tail groups between the DNA bases. The complex with the biphenyl tail predominantly exhibits groove binding with no significant tail intercalation. The naphthyl derivative binds both by intercalation and a non-intercalative mode even at low metal complex concentrations. At high metal complex concentrations, aggregation of the complexes on the DNA is observed. Resonance light scattering indicates that the aggregates are of low nuclearity along the groove.     

Mitochondrial dysfunction and biotransformation of β-carboline alkaloids,harmine and harmaline,on isolated rat hepatocytes

The cytotoxic effects and biotransformation of harmine and harmaline, which are known β-carboline alkaloids and potent hallucinogens, were studied in freshly isolated rat hepatocytes. The exposure of hepatocytes to harmine caused not only concentration (0–0.50 mM)- and time (0–3 h)-dependent cell death accompanied by the formation of cell blebs and the loss of cellular ATP, reduced glutathione, and protein thiols but also the accumulation of glutathione disulfide. Of the other analogues examined, the cytotoxic effects of harmaline and harmol (a metabolite of harmine) at a concentration of 0.5 mM were less than those of harmine. The loss of mitochondrial membrane potential and generation of oxygen radical species in hepatocytes treated with harmine were greater than those with harmaline and harmol. In the oxygen consumption of mitochondria isolated from rat liver, the ratios of state-3/state-4 respiration of these β-carbolines were decreased in a concentration-dependent manner. In addition, harmine resulted in the induction of the mitochondrial permeability transition (MPT), and the effects of harmol and harmaline were less than those of harmine. At a weakly toxic level of harmine (0.25 mM), it was metabolized to harmol and its monoglucuronide and monosulfate conjugates, and the amounts of sulfate rather than glucuronide predominantly increased with time. In the presence of 2,5-dichloro-4-nitrophenol (50 μM; an inhibitor of sulfotransferase), harmine-induced cytotoxicity was enhanced, accompanied by decrease in the amount of harmol-sulfate conjugate, due to an increase in the amount of unconjugated harmol and the inhibition of harmine loss. Taken collectively, these results indicate that (a) mitochondria are target organelles for harmine, which elicits cytotoxicity through mitochondrial failure related to the induction of the MPT, mitochondrial depolarization, and inhibition of ATP synthesis; and (b) the toxic effects of harmine are greater than those of either its metabolite harmol or its analogue harmaline, suggesting that the onset of harmine-induced cytotoxicity may depend on the initial and/or residual concentrations of harmine rather than on those of its metabolites.     

Shape,conformation and stability of fibronectin fragments determined by electron microscopy,circular dichroism and ultracentrifugation

Human plasma fibronectin digested with cathepsin D yields a number of fragments: an N-terminal fibrin-binding 30K³ fragment, a gelatin-binding 40K fragment, a 70K fragment containing the 30K and 40K domains, a central 95/105K fragment and a heparin-binding 140K fragment. The 140K fragment is linked by disulphide bonds and forms the C-terminal ends of the fibronectin. Electron microscopy of rotary-shadowed specimens revealed the 40K, 70K and 95/105K fragments as thin rods (diameter about 2.2 nm) with lengths of 13, 25 and 25 nm. respectively. These dimensions agree with the distances between flexible, proteasesusceptible regions in individual fibronectin strands determined previously. The 140K fragment appeared as a V-shaped structure with two arms 21.5 nm long emerging at a preferred angle of about 70 °. The distribution function of this angle was identical to that observed for the angle between the two arms of intact fibronectin. The free energy required for a distortion of this angle by 60 ° was estimated to be 8 kJ/mol. Reduced and alkylated fibronectin was visualized as single strands (about 55 nm long) with kinks of variable angles corresponding to sites of increased flexibility. The hydrodynamic shapes of the fragments in solution were similar to the shapes observed by electron microscopy, indicating that the individual domains of fibronectin maintain their native structure after proteolytic separation. This was also demonstrated by circular dichroism (c.d.) studies. The c.d. spectrum and the thermal melting curve of native fibronectin were well represented by a linear combination of the contributions of the fragments, indicating conformational independence of the domains. The data support earlier findings that fibronectin consists of two thin strands (length about 60 nm), which are composed of several domains separated by flexible and protease-susceptible intervening regions. This very extended structure agrees with the small sedimentation constant found for fibronectin under conditions where electrostatic interactions between domains are repulsive or depressed. Probably because of such interactions the sedimentation constant is larger at neutral pH and low ionic strength, but even under these conditions a very asymmetric shape is still maintained.     

Interaction of topotecan,DNA topoisomerase I inhibitor,with double-stranded polydeoxyribonucleotides. III. Binding at the minor groove

Interaction of topotecan (TPT) with calf thymus DNA, coliphage T4 DNA, and poly(dG-dC). poly(dG-dC) was studied by optical (linear flow dichroism, UV-vis spectroscopy) and quantum chemical methods. The linear dichroism (LD) signal of TPT bound to DNA was shown to have positive sign in the range 260-295 nm. This means that the plane of quinoline fragment (rings A and B) of TPT molecule form an angle lower 54 degrees with the long axis of DNA, and hence TPT molecule can not intercalate between DNA base pairs. TPT was established to bind to calf thymus DNA as readily as to coliphage T4 DNA whose all cytosines in the major groove were glycosylated at the 5th position. Consequently, the DNA major groove does not participate in TPT binding. TPT molecule was shown to compete with distamycin for binding sites in the minor groove of DNA and poly(dG-dC). poly(dG-dC). Thus, it was demonstrated for the first time that TPT binds to DNA at its minor groove.     

Circular dichroism of cattle rhodopsin and bathorhodopsin at liquid nitrogen temperatures

The photoevent in vision has been considered to be the conversion of rhodopsin to bathorhodopsin, which is caused by photoisomerization of the chromophoric retinal. Recently some objections were raised to this hypothesis. The reliability of the hypothesis was verified by measurement of circular dichroism of bathorhodopsin.The measurement of circular dichroism of rhodopsin extract (containing 66% or 75% of glycerol) at liquid nitrogen temperatures (?195°C) by a conventional spectropolarimeter induced an extraordinary large signal, owing to linear dichroism originated from conversion of rhodopsin to bathorhodopsin by the measuring light. The similar linear dichroism can be induced by irradiation of rhodopsin extract at ?195°C with polarized light or natural light. At photosteady state the linear dichroism disappeared.Circular dichroism spectrum of cattle rhodopsin displayed two positive peaks ([θ]_max = 80 800 degrees at 335 nm, and [θ]_max = 42 600 degrees at 500 nm) at ?195°C, whereas, bathorhodopsin displayed a positive peak ([θ]_max = 43 100 degrees at 334 nm) and a negative peak ([θ]_max = 163 000 degrees at 540 nm).The change of the positive sign to negative one at α-band of circular dichroism spectrum supports the hypothesis that the conversion of rhodopsin is due to rotation of the chromophoric retinal about C-11—12 double bond (‘photoisomerization model’).     

Solution conformation of DNA

Optical observations on linear B-form DNA by the method of electric linear dichroism show that the value of the limiting reduced dichroism is molecular weight-dependent, increasing with molecular weight to a limit of about ?1.41 ± 0.02 in aqueous solution. These data and the rotational relaxation times obtained from the decay of the dichroism when the orienting field is instantaneously removed, imply the existence of a non-linear tertiary equilibrium structure for DNA. The data indicate that the essential B-form parameters of the double-stranded DNA are retained in this tertiary structure, and are not consistent with a DNA structure in which the base-pairs have a 34 ° propeller-like twist (Hogan et al., 1978). The interpretation of the dichroism data is supported by a clear demonstration that the magnitude of dichroism change in ethanol corresponds to that expected for the B to A-form structural transition as determined from X-ray diffraction. We propose that the tertiary structure of B-DNA is a helical coil and suggest the limits of the structural parameters of the coil consistent with the observations.     

Flow dichroism of deoxyribonucleic acid solutions

The flow dichroism of dilute DNA solutions (A₂₆₀ ≈ 0.1) has been studied in a Couette-type apparatus with the outer cylinder rotating and with the light path parallel to the cylinder axis. Shear gradients in the range of 5–160 sec.^?1 were studied. The DNA samples were whole, “half,” and “quarter” molecules of T4 bacteriophage DNA, and linear and circular λb₂b₅c, DNA. For the linear molecules, the fractional flow dichroism is a linear function of molecular weight. The dichroism for linear λ DNA is about 1.8 that of the circular molecule. For a given DNA, the dichroism is an approximately linear function of shear gradient, but with a slight upward curvature at low values of G, and some trend toward saturation at larger values of G. The fractional dichroism increases as the supporting electrolyte concentration decreases.     

Ultraviolet circular dichroism of polyproline and oriented collagen

The ultraviolet absorption, linear dichroism, circular dichroism, and oriented circular dichroism of collagen are reported and the spectra are resolved into a self-consistent set of bands in accord with exciton theory. The parallel band at 200 nm has 40% of the π → π* intensity; the perpendicular band is placed at 189 nm yielding a splitting of 2700 cm^?1. The circular dichroism is resolved into two Gaussians at λ_∥ and λ_τ (rotational strengths +14 × 10^?40 and ?32 × 10^?40 esu². cm²) plus a large non-Gaussian (“helix”) band with ampplitude ?25,000° at 201 nm. These data appear to be in reasonably good accord with recent calculations. Measurements of the absorption, linear dichroism and circular dichroism of polyproline I and II are also reported and are resolved into their component bands. Polyproline I is in good accord with exciton theory, whereas polyproline II remains unsatisfactory.     

Quinacrine: Spectroscopic properties and interactions with polynucleotides

The acridine dye quinacrine and its interactions with calf thymus DNA, poly(dA-dT) · poly (dA-dT), and poly (dG-dC) · poly(dG-dC) were studied by light absorption, linear dichroism, and fluorescence spectroscopy. The transition moments of quinacrine give rise to absorption bands polarized along the short axis (400–480-nm band), and the long axis (345-nm and 290-nm bands) of the molecule, respectively. Linear dichroism studies show that quinacrine intercalates into calf thymus DNA as well as into the polynucleotides, displaying fairly homogeneous binding to poly (dA-dT) · poly (dA-dT), but more than one type of intercalation site for calf thymus DNA and poly (dG-dC) · poly(dG-dC). Fluorescence spectroscopy shows that for free quinacrine the pK = 8.1 between the mono- and diprotonated states also remains unchanged in the excited state. Quinacrine bound to calf thymus DNA and polynucleotides exhibits light absorption typical for the intercalated diprotonated form. The fluorescence enhancement of quinacrine bound to poly (dA-dT) · poly(dA-dT) may be due to shielding from water interactions involving transient H-bond formation. The fluorescence quenching in poly(dG-dC) · poly(dG-dC) may be due to excited state electron transfer from guanine to quinacrine. © 1993 John Wiley & Sons, Inc.     

Linear dichroism characteristics of ethidium-and proflavine-supercoiled DNA complexes

A flow linear dichroism technique is utilized to study the unwinding of supercoiled DNA induced by the binding of ethidium bromide (EB) and proflavine (PF) at different ratios r (drug added/DNA base). In the case of either EB or PF bound to linear calf thymus DNA, the reduced linear dichroism signals LD/A (LD: linear dichroism; A: absorbance, both measured at the same wavelength), determined at 258, and 520 or 462 nm (corresponding to contributions predominantly from the partially oriented DNA bases, intercalated EB, or PF, respectively) are nearly independent of drug concentration. In the case of supercoiled DNA, the magnitude of LD/A at 258 nm first increases to a maximum value near r = 0.04-0.05, and then decreases as r is increased further, mimicking the behavior of the sedimentation coefficients, viscosities, and gel electrophoresis patterns measured by other workers at similar values of r. However, LD/A at 520 nm, which is due to DNA-bound EB molecules, is constant within the range of r values of 0.02-0.06 in which the magnitude of LD/A determined at 258 nm due to the DNA bases exhibits a pronounced maximum. In contrast, in the case of PF, the magnitudes of LD/A determined at 258 or 462 nm are characterized by similar dependencies on r, both exhibiting pronounced maxima at r = 0.05; this parallel behavior is expected according to a simple intercalation model in which the DNA bases and drug molecules are stacked on top of one another, and in which both are oriented to similar extents in the flow gradient. The unexpected differences in the dependencies of (LD/A)258 and (LD/A)520 on r in the case of EB bound to supercoiled DNA, are attributed to differences in the net overall alignment of the EB molecules and DNA bases in the flow gradient. The magnitude of the LD signal at 258 nm reflects the overall degree of orientation of the supercoiled DNA molecules that, in turn, depends on their hydrodynamic shapes and sizes; the LD signals characterizing the bound EB molecules may reflect this orientation also, as well as the partial alignment of individual DNA segments containing bound EB molecules.(ABSTRACT TRUNCATED AT 400 WORDS)