Circular dichroism of films of polynucleotides

The CD spectra of films of the lithium salt of E. coli and calf thymus DNA, and alternating d-AT : AT were measured as a function of relative humidity. Films of the ammonium acetate salt of DNA were also measured. The ammonium films yield the previously reported A-form CD spectra. A possible explanation for the small magnitude of the 260-nm band of the A-form film spectra compared to double-stranded RNA spectra is that the film DNA is in a different conformation than RNA within the A family of conformations. At relative humidities of 92% or lower, a negative nonconservative CD spectrum with negative minima near 270 and 210 nm is observed with the lithium films. The magnitude of the minima varies from film to film. In films of DNA the magnitude ranges from a delta epsilon of ?5 to ?35; d-AT : AT films show magnitudes to ?300. CD spectra of this type are designated Ψ spectra. Similar spectra have been reported from reconstituted complexes of DNA and polylysine or f-1 histone. If the origins of the film and protein–DNA complex spectra are similar, the complex spectra are not the result of specific secondary structural changes induced in the DNA by the protein fraction. Theoretical analysis suggests that Ψ spectra are not the result of changes in the secondary or tertiary structure of DNA. Instead, the previously proposed explanation based on liquid crystals is favored. The DNA could form asymmetric structures with long-range periodicity. It is likely that the observed CD spectra of f-1 complexes are artifacts of DNA aggregation. The possibility that some other previously published spectra of protein–DNA complexes also reflect artifacts is suggested.     

Circular dichroism of polynucleotides: A general method applied to dimers

A method is described which relates the circular dichroism of a polymer to its conformation. The method takes into account near and accidental degeneracies and eliminates the artificial distinction between degenerate and nondegenerate systems. Comparison of this method with perturbation theory indicates that the errors inherent in nondegenerate perturbation theory tend to cancel when a circular dichroism spectrum is calculated. The method is applied to dinucleoside phosphates.     

Circular dichroism of polynucleotides: A simple theory

A particularly simple theory of circular dichroism is described and applied to the polynucleotides. It works surprisingly well and predicts the conservative spectrum of DNA and the more intense nonconservative spectrum of RNA. The anomalously low intensity of the CD of the nucleic acids is shown to be a natural consequence of the cancellation of the rotational strengths of the many CD bands. The theory's many successes and predictions as well as its weaknesses are discussed.     

Circular dichroism of helices formed by purine monomers with pyrimidine polynucleotides

The CD spectra of a number of helical complexes formed by purine monomers and complementary pyrimidine polyribonucleotides have been observed over the range 200–400 nm. Each of these spectra is quite similar to that of the corresponding polymer–polymer helix. The spectra are evidently determined by the geometry of the asymmetric array of bases, largely unperturbed by the ribose–phosphate backbone. The helix structure (A-form), on the other hand, is determined by the backbone of the pyrimidine homopolymer. Data on the monomer–polymer complexes support the conclusion that the CD spectra of ribohomopolymer helices depend primarily on interastrand interactions of the same transition within a given base and are relatively unaffected by transitions of the complementary base.     

Circular dichroism of adenine and thymine containing synthetic polynucleotides

Circular dichroism (CD) spectra of poly(dA), poly(dT), poly(dA)·poly(dT), and poly[d(A-T)]·poly[d(T-A)] have been measured as a function of temperature. From these data difference spectra have been calculated by subtracting the spectrum measured at low temperature from the spectra measured at higher temperatures. The CD difference spectra obtained upon melting of the two double-stranded polymers are very similar. From a comparison of these difference spectra with calculated ones it is shown that optical transitions near 272 nm (on A) and 288 nm (most probably on T) are present. The premelting changes of the CD spectrum of poly[d(A-t)]·poly[d(T-A)] are due to a change in conformation in which the secondary structure goes from a C- to B-type spectrum by increasing the A-type nature of the polymer. Such a change is not observed for poly(dA)·poly(dT). Instead, a transition between two different B-type geometries occurs.     

Circular dichroism calculations for double-stranded polynucleotides of repeating sequence

Optical property calculations are presented for poly(A·U), poly[(A-U)·(A-U)], poly(G·C), and poly[(G-C)·(G-C)] in RNA, B-DNA, and C-DNA conformations. An all-order classical coupled oscillator polarizability theory was used, and an effective dielectric constant of 2 was assumed. The calculated CD spectra were found to be sensitive to both geometry and sequence. Agreement with the measured CD spectra of poly(A·U), poly(G·C), and poly(dG·dC) is very good. Calculations for other sequences and geometries are less satisfactory and are particularly poor for poly[(G-C)·(G-C)] in RNA geometry and poly(A·T) in B-DNA geometry. Attempts to improve agreement with measured spectra by varying monomer properties have been only partially successful for these calculations, but they illustrate the types of changes that may prove to be necessary. Calculations using other published X-ray coordinates for certain deoxypolynucleotides of simple sequence, some of which are quite different from B-DNA coordinates, did not result in better agreement with measured spectra. Finally, the dependence of the calculated CD on chain length is examined. Results show that non-nearest neighbor interactions can be important when runs of 3 or more identical base pairs appear in a given sequence.     

Circular dichroism of polynucleotides: dimers as a function of conformation

Working within the restrictions of a model, we have calculated the circular dichroism of the dinucleoside phosphates ApA, CpC, and CpA for various conformations. Comparing the calculated curves with those measured in aqueous solution we find agreement for (1) ApA as a right-handed helix with both bases either as in B-form DNA, or else rotated 180° around the glycosidic bond, (2) CpC as the right-handed conformation with both bases as in DNA, (3) ApC as either the right-handed conformation with both bases as in DNA, or else as a left-handed helix with both bases rotated 180°, and (4) CpA as either a left-handed helix with both bases in a left-handed DNA, or else in the right-handed conformation with both bases rotated 180°. In addition, we have investigated circular dichroism as a measure of unstacking. We find that opening the bases to a 90° total angle (base planes perpendicular) reduces the intensity of the calculated bands to 20% of their original value. Further, we find that allowing the sliding of one base past the other does not lead to a temperature dependence consistent with experiment.     

The linear dichroism of oriented helical and superhelical polymers

Expressions are derived to relate the linear dichroism of oriented helical and super-helical polymers to the vector equation describing a transition moment in a reference frame based on the position of a single monomer unit in a simple helix and the super-helix tilt angle β. The reduced dichroism of a perfectly oriented superhelical polymer, (Δε/ε)₀, is related to the reduced dichroism of a perfectly oriented helical polymer, (Δε/ε)₁, by the expression (Δε/ε)₀ = ½ (Δε/ε)₁(3 cos² β ? 1). Hence the linear dichroism of a helical polymer can be significantly altered by supercoiling. The application of the general expressions is illustrated by the derivation of specific equations which relate the dichroism of helical and superhelical DNA to the tilt and twist of the DNA bases, the directions of the transition moments within the base planes, and the superhelix tilt angle. Calculations of the reduced dichroism of perfectly oriented, non-super-helical DNA in the A and B configurations suggest that it will be difficult to distinguish between these two forms on the basis of dichroism measurements.     

Matrix-method calculation of linear and circular dichroism spectra of nucleic acids and polynucleotides

Calculations of the optical properties (absorption, linear dichroism, circular dichroism, and anisotropic components of the CD) are presented for polynucleotides of random or regular sequence within the formalism of the matrix method using a set of parameters that includes only the ππ* transitions of the aromatic bases. Experimental solution spectra agree favorably with calculated CD spectra for A-RNA, A-DNA, and B-DNA, when coordinates derived from x-ray studies on fibers are used. Excessive hypochromicity is predicted when parameters intended to reproduce the vacuum-uv absorption of the chromophores are included in the calculations, but total elimination of these parameters leads to an insufficient hypochromicity for the long-wavelength absorption band. Using alternative conformations for DNA in low-salt aqueous solution did not improve the agreement between experimental and calculated spectra, but some features of the optical properties predicted for these variant structures suggest that the tilt of the bases with respect to the helical axis may be larger than that of the fiber B-form. In the case of polynucleotides with regular structure, which have been traditionally less easy to understand in terms of the standard nucleic acid conformations, a series of alternative structures has been examined. Unexpectedly, the calculated spectrum for the Z-DNA structure compares almost quantitatively with the experimental spectrum of poly(dGC·dGC) in low salt. This result, which confirms a recent report [Vasmel, H. & Greve, J. (1981) Biopolymers 20 , 1329–1332], is in contrast with the current identification of Z-DNA with the high-salt form of poly(dGC·dGC). Finally, the optical properties of single-stranded polyribonucleotides appear to be better explained when alternative structures [9₁-helix for poly(rA) and 6₁-helix for poly(rC)] are introduced instead of the A-RNA form.     

Circular dichroism studies on helical structure preferences of amino acid residues of proteins caused by sodium dodecyl sulfate

The extent of helical structure of 19 intact proteins and of 15 proteins with no disulfide bridges in the absence and presence of 10 mM sodium dodecyl sulfate (SDS) was determined using the curve-fitting method of circular dichroic spectra. The change in helicity caused by the addition of SDS was examined as a function of each amino acid fraction. An increase in the helicity upon the addition of SDS occurred in most of the proteins with no disulfide bridges (C proteins) and containing more than 0.06 Lys fraction. In most of the intact proteins (B proteins), most of which contained disulfide bridges, helicity in SDS decreased with an increase in Lys fraction. The helicity of the C proteins in SDS also tended to increase with an increase in the Leu and Phe fractions, while it decreased with an increase in the Gly fraction. For the helicity of the B proteins in SDS, there was a tendency to increase with increased Asn fraction and decrease with increased His fraction. On the other hand, amino acids were divided into eight groups according to their side-chain properties and the conformational preference for each of the amino acid groups of C proteins was calculated using a simple assumption.     

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.     

Study of coenzyme reorientation in the active center of tryptophanase by linear dichroism method

Tryptophanase from E.coli was oriented in a compressed slab of polyacrylamide gel and its linear dichroism (LD) and absorption spectra were measured. The free enzyme displays four LD bands at 305, 340, 425 and 490 nm. Two bands at 340 and 425 nm belong to the internal coenzyme-lysine aldimine. The 305 nm band apparently belongs to an aromatic amino acid residue; the sign and form of this band are changed upon the enzyme reaction with substrate analogs. The 490 nm band is present in the LD spectra of holo- and apoenzyme and disappears after treatment with NaBH4. It is suggested that the 490 nm band belongs to a quinoid enzyme subform. The reaction of tryptophanase with threo-beta-phenyl-DL-serine and L-threonine leads to formation of the external aldimine with a strong absorption band at 420-425 nm. The reduced LD (delta A/A) in this band is one order of magnitude greater than that in the 420 nm of the free enzyme. The complex with D-alanine is characterized by an intermediate LD value in the 425 nm band. In the presence of indole this complex displays the same LD as that observed with beta-phenylserine. The reaction of tryptophanase with L-alanine and oxindolyl-L-alanine leads to formation of the quinoid intermediate with a 500 nm absorption band. The LD value in this band differs from those in the absorption bands of the free enzyme. It is concluded that reorientations of the coenzyme occur in the course of the tryptophanase reaction.     

Circular dichroism of the parallel β helical proteins pectate lyase C and E

The pectate lyases, PelC and PelE, have an unusual folding motif, known as a parallel β-helix, in which the polypeptide chain is coiled into a larger helix composed of three parallel β-sheets connected by loops having variable lengths and conformations. Since the regular secondary structure consists almost entirely of parallel β-sheets these proteins provide a unique opportunity to study the effect of parallel β-helical structure on circular dichroism (CD). We report here the CD spectra of PelC and PelE in the presence and absence of Ca²⁺, derive the parallel β-helical components of the spectra, and compare these results with previous CD studies of parallel β-sheet structure. The shape and intensity of the parallel β-sheet spectrum is distinctive and may be useful in identifying other proteins that contain the parallel β-helical folding motif. © 1995 Wiley-Liss, Inc.     

Circular dichroism as a detection method in the screening of enantioselective catalysts

The combination of liquid chromatography (HPLC), UV/Vis-spectroscopy and circular dichroism (CD) can be used to construct a high-throughput screening system to determine the enantioselectivity of enzyme- or metal-catalyzed reduction of acetophenone with formation of (S)- and (R)-1-phenylethanol. Prerequisite for the viability of this system is the experimental finding that the anisotropy factor g is linearly related to the enantiomeric excess (ee) and that it is independent of concentration, thereby excluding possible aggregation effects.     

Circular dichroism of superhelical DNA

The circular dichroism (CD) spectra of a number of superhelical DNA's have been measured. The introduction of negative superhelical turns causes an increase in magnitude of the positive band around 280 mμ, while the trough around 250mμ is little affected. For two samples of λb2b5c DNA (20 Mdalton) containing different number of negative superhelical turns, the magnitude of the positive band relative to that of the nicked control increases with increasing number of superhelical turns. In 2M NaCl, the small (1.45 Mdalton) superhelical DNA from E. coli 15 shows an unusually large difference in CD compared with that of the same DNA with a few single-chain scissions per molecule. This large difference is not observed in a medium containing p. 0.11M NaCl. These results indicate that the double helix in a superhelical DNA is perturbed somewhat due to the bending and torsional forces in such a molecule. The magnitude of such structural alteration seems to depend on the number of superhelical turns per unit length, the size of the DNA molecule, as well as the ionic medium.