The optical rotatory dispersion and circular dichroism of molecules containing interacting residues

We use a semiclassical formalism to derive expressions for the optical rotatory dispersion and circular dichroism associated with a dilute system of molecules represented as freely-rotating, rigid arrays of interacting residues. The relationship of the present approach to DeVoe's classical theory is discussed. Far from resonance, our results become equivalent to the equations of Moffitt, Fitts, and Kirkwood when the separation between adjacent residues is small compared to the wavelength of the light. In the resonance case, a calculation of the frequency-dependent circular dichroism per residue is carried out for a particular geometrical arrangement of the residues. These curves, for arrays both finite and infinite in extent, are compared with those obtained when a certain commonly used approximation to the orientational averaging is introduced. It is shown that this approximation is not always valid.     

FTIR measurements of optical rotatory dispersion and circular dichroism

FTIR methods for measuring optical rotatory dispersion (ORD) and circular dichroism (CD) were developed. The measurements of both phenomena are accomplished by means of various techniques. The study of ORD makes use of linearly polarized IR radiation while that of CD requires a circular polarizer (retarder) able to convert linearly polarized IR radiation into circularly polarized one. Examples of induced cholesteric solutions are shown.     

Optical rotatory dispersion and circular dichroism. LXXV. Circular dichroism of some aryl-amino acids

CD. curves have been recorded for α-aryl-α-amino acids, esters and amides related to α-phenylglycine, α-phenyl-alanine and their N-dimethyl derivatives, and for the corresponding α-cyclohexyl-α-amino acids and esters. Compounds with the (S)-configuration at the single asymmetric carbon atom give strong positive Cotton effects near 220 nm. The conformations of the acids are discussed and compared with those of other α-amino acids.     

Optical rotatory dispersion and circular dichroism studies of copoly(propyl-L-aspartate-benzyl-L-aspartate)

Copoly(propyl-L -aspartate-benzyl-L -aspartate)s with various compositions were synthesized by propylation of a parent poly(β-benzyl-L -Aspartate). The variation of helix sense of copolyaspartate obtained against a degree of propylation and temperature was examined by optical rotatory dispersion and circular dichroism method. Copolyaspartate of propylation less than about 70% is in a left-handed α helix conformation and its Moffitt parameter b₀ and molecular ellipticity [θ]₂₂₂ decreased gradually with increasing propylation. On the other hand, a different temperature dependence of b₀ and [θ]₂₂₂ was observed for copolyaspartate of propylation more than about 80%, i.e., the reversible transition of the helix sense from right- to left-handed α helix took place by temperature increasing. These features were basically similar to the variation in helix sense of copoly(ethyl-L -aspartate-benzyl-L -aspartate), although a slight difference was seen for copoly(propyl-L -aspartate-benzyl-L -aspartate). The thermodynamic treatment indicating larger entropy of right-handed α helix suggests much mobile side chain of the right-handed α helix than the left handed one.     

Optical rotatory dispersion and vacuum ultraviolet circular dichroism of poly[(R)-oxypropylene]

The circular dichroism (CD) spectrum of poly[(R)-oxypropylene] in a number of solvents has been measured in the vacuum ultraviolet region. Two CD bands were measured for cyclohexane, acetonitrile, and trifluoroethanol solutions. The CD spectrum was extended to 140 nm and three bands were measured in a 1,1,1,3,3,3-hexafluoro-2-propanol solution. The similarity of these four CD spectra in sign, shape, and intensity confirm that poly[(R)-oxypropylene] has similar conformations in all solvents studied, even though the optical rotatory dispersion (ORD) in the visible region is positive for the cyclohexane solution but negative for the alcohol solutions. A Kronig–Kramers transform of the two CD bands observed for the cyclohexane solution accounts for the observed positive ORD spectrum. In contrast, a third large and negative CD band centered below 160 nm is necessary to account for the negative ORD spectra observed for the alcohol solutions. Apparently the anomalous sign variation of the ORD curves observed in the visible region is due to subtle changes in the interplay of a large number of CD bands. Solvent interaction, observed as a blue shift of the first two CD bands for the alcohol solutions, could produce the subtle changes necessary to change the sign of the ORD curve in the visible region. The first two CD bands of poly[(R)-oxypropylene] are tentatively assigned as n? σ^* and the third as an n? 3s.     

An optical rotatory dispersion and circular dichroism investigation of the chloramidation of the triamine EnPYClNO2ClPtCl

Conclusions An optically active product from the chloramidation of (-)₅₈₉ EnPyClNO₂ClPtCl with the composition (+)₅₈₉ (NH₂C₂H₄NCl)·PyClNO₂ClPt has been isolated in the solid state for the first time. The optical activity of a solution of this compound in DMF has been investigated using CD and ORD. A sharp change in the spectrum of the optically active bands of the reagent takes place during chloramidation which is apparently not only associated with the change in the nature of the Pt-chelate bond but also with the appearance of a new chromophore (the chlorimido group), the absorption bands of which can become optically active as a result of the vicinal effect.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimieheskaya, No. 4, pp. 928–931, April, 1970.     

Ab initio optical rotatory dispersion and electronic circular dichroism spectra of (S)-2-chloropropionitrile

Coupled-cluster and density-functional methods have been used to determine specific rotations and electronic circular dichroism (ECD) rotational strengths for (S)-2-chloropropionitrile. Coupled-cluster specific rotations using both the length- and velocity-gauge representations of the electric-dipole operator, computed with basis sets of triple-zeta quality containing up to 326 functions, compare very well with recently reported gas-phase cavity-ring-down polarimetry data. ECD rotational strengths for the six lowest-lying excited states are found to vary in sign, and the second excited state, which has a larger rotational strength than the first by a factor of 4, was found to yield a much larger contribution (by a factor of 10) to the overall negative specific rotation observed both experimentally and theoretically. However, both valence and Rydberg states appear to make substantial contributions to the total rotation, often of opposite sign from the converged/linear-response result. Furthermore, the sum-over-states approach was found to be inadequate for reproducing the specific rotations derived from the linear-response approach, even when 100 excited states (well beyond the estimated ionization limit) were included in the summation. Density-functional specific rotations using the B3LYP functional with basis sets of quadruple-zeta quality containing up to 588 functions are found to be too large compared to experiment by approximately a factor of 2. This error appears to be related to both the underestimation of the electronic excitation energies, as well as concomitant overestimation of the corresponding ECD rotational strengths. Although earlier studies reported good agreement between density-functional specific rotations and experiment when electric-field-dependent functions were used in conjunction with a double-zeta-quality basis set, the results reported here, which are near the basis-set limit, suggest that this agreement may be fortuitous.     

Optical rotatory dispersion studies—CIV Low-temperature circular dichroism behavior of various chromophoric derivatives of alcohols and amines

The low-temperature circular dichroism behavior of various cyclic and alicyclic systems containing the methyl xanthato-, N,N-diethyl-N′-acylthioureyl-, N-phthalimido-, nitrito- and dithio-carbalkoxy- chromophores is discussed. Rotational strength (R₀^T) values are reported where possible and changes in this parameter upon variation of the temperature are interpreted, where relevant, in terms of the degree of steric inhibition to free rotation about the various bonds connected to the asymmetric center bearing (or nearest to) the chromophore moiety.     

Study of the conformation of the antibiotic A-128-OP and its derivatives by the methods of optical rotatory dispersion and circular dichroism

Summary 1. The optical rotatory dispersion and circular dichroism of the antibiotic A-128-OP and derivatives of it have been investigated in the wavelength range from 230 to 450 nm.2. On the basis of the ORD and CD characteristics and the results of biochemical tests, it has been concluded that the molecule of the antibiotic A-128-Op has a preferred conformation which is most favorable for its functioning.M. V. Lomonosov State University. Translated from Khimiya Prirodnykh Soedinenii, No. 5, pp. 640–645, September–October, 1974.     

Calculation of circular dichroism spectra from optical rotatory dispersion, and vice versa, as complementary tools for theoretical studies of optical activity using time-dependent density functional theory

A comparison of two theoretical methods based on time-dependent density functional theory for the calculation of the linear dispersive and absorptive properties of chiral molecules has been made. For this purpose, a recently proposed computational method for the calculation of circular dichroism (CD) spectra from the imaginary part of the optical rotation parameter has been applied to six rigid organic molecules. The results have been compared to the CD spectra obtained from the rotatory strengths and from the Kramers-Kronig transformation of optical rotatory dispersion (ORD) curves. We have also investigated a criterion based on the Kramers-Kronig integration formula to determine a number of excitations in truncated CD spectra which may yield a reasonable low frequency resonant ORD. It has been tested by calculating the ORD from the sum-over-states formula both in the nonresonant and resonant regions. Finally, we have applied these methods to model the resonant optical activity of proline at low pH.