Differential scattering of incident left and right circularly polarized light can be an important contribution to the circular dichroism of macromolecules. In principle both differential absorption and differential scattering of circularly polarized light contribute to circular dichroism, but differential scattering is increasingly important for particles whose dimensions are greater than 1/20th the wavelength of light. The scattering contribution is probably not important for unaggregated proteins and nucleic acids in solution. It can be very important for viruses, membranes, and other protein-nucleic acid complexes. Outside the absorption bands of the scattering, chiral particle, only differential scattering contributes to the circular dichroism. The sign and magnitude of the differential scattering is quantitatively related to the relative orientations and the distances between the scattering units of the particle. The interpretation of the circular differential scattering depends on a simple, classical method. Thus, in understanding a measured circular dichroism, it often will be easier to relate the differential scattering to the structure of a particle (such as a virus) than it is to relate the differential absorption to the structure. CD and optical rotatory dispersion (ORD) studies have been helpful in providing useful knowledge about the structure of biological macromolecules. These methods were limited originally to homogeneous solutions of macromolecules. More recently, they also have been applied to increasingly complex systems such as viruses (1, 2), erythrocytes (3, 4), nucleohistones (5, 6), DNA-polylysine complexes (7,8), DNA aggregates (9), chloroplasts (10), etc. (11). A remarkable common feature of many of these systems was the presence of anomalies in their CD and optical rotatory dispersion spectra. The CD spectra presented: (i) apparent differential absorption of circularly polarized light outside of the absorption bands (the CD signal at long wavelengths was slowly varying but non-zero; this longwavelength "tail" could be positive or negative); (ii) signals sensitive to the distance of the photomultiplier from the sample; and (iii) CD values 1 or 2 orders of magnitude larger than normal. Fig. 1 Recently, a new quantitative understanding of differential scattering of circularly polarized light has been obtained. We were able to relate the difference in scattering efficiency for incident left and right circularly polarized light to the detailed structure of the scattering particle (20-24). We have measured the angular dependence of this circular intensity differential scattering for a helix of known structure and obtained good agreement with theory (25). Thus, we now can explain the "anomalous" behavior of chiral macromolecules and aggregates. We find that the scattering "artifacts" can provide valuable information about the configuration (left-or right-handed) of the component particles.Here we will show how the differential scattering of left and right circularly polarized light ...