Study on the binding nature of acridine orange to DNA by means of flow dichroism

Linear dichroism spectroscopy of nucleic acids

This review will consider solution studies of structure and interactions of DNA and DNA complexes using linear dichroism spectroscopy, with emphasis on the technique of orientation by flow. The theoretical and experimental background to be given may serve, in addition, as a general introduction into the state of the art of linear dichroism spectroscopy, particularly as it is applied to biophysical problems.

Fluorescence polarization of stretched polytene chromosomes stained with acridine orange

The molecules of the fluorescent dye acridine orange (AO) bind to DNA in such a way that the absorption and emission dipoles lie on a plane perpendicular to the DNA axis. For this reason, definite fluorescence polarization should correspond to each mode of spatial DNA packing. A chromosome, considered as an axially symmetrical ensemble of DNA, was characterized by two experimental parameters, P parallel and P perpendicular, i.e., by polarizations of fluorescence excited by light polarized parallel and perpendicular to the symmetry axis. In view of the sequential order in the packing levels of DNA fiber in a chromosome, it was suggested that, under mechanical stretching, the highest level is disrupted first, then the others, in the order of their sequence. Isolated chromosomes of Chironomus thummi were stained with AO and stretched with needles of a micromanipulator. From the changes of P parallel and P perpendicular measured during stretching it was concluded the polytene chromosome bands have three, at least, DNA packing levels, tentatively described as 100 A fiber, 250 A coil and chromomere.

Flow dichroism, flow polarized fluorescence and viscosity of the DNA acridine complexes

The strong binding of various acridine dyes to DNA has been studied by the measurements of flow dichroism, flow polarized fluorescence and viscosity. Negative flow dichroism and percentage change in polarized fluorescence intensity show that intercalated dye molecules are oriented rather perpendicularly to the main axis of the DNA helix, like base pairs. On the other hand, viscosity measurements show that the increase of the contour length of DNA depends on the dye structure, being much smaller in the case of dyes with bulky substituents compared to that of the other dyes. This may be attributed to the formation of the outside bound complex. Further, the introduction of bulk substituents to the acridine ring leads to a little smaller values of the reduced dichroism and intensity change of polarized fluorescence. The results may be qualitatively understood if we assume that the outside bound dye lies in the groove of the DNA helix and the plane of the dye tilts from the perpendicular direction relative to the main axis of the helix.

Changes in superhelical density of closed circular deoxyribonucleic acid by intercalation of anti-R-plasmid drugs and primaquine

The following compounds, which possess anti-R-plasmid activity (Hahn and Ciak, 1976) in decreasing order, were shown by viscometric titration to change systematically the superhelical density of closed circular PM2 deoxyribonucleic acid in the manner of intercalators: ethidium bromide, quinacrine, acridine orange, quinine, chlorpromazine, chloroquine, and methylene blue. The same effect was caused by the antimalarial drug primaquine, which has not been tested for antiplasmid activity.