Studies on pig serum lipoproteins. V. Optical properties of low density lipoproteins.

The circular dichroism (CD), optical rotatory dispersion (ORD), and fluorescence emission spectra of two subfractions of pig serum low density lipoproteins (LDL1 and LDL2) were compared. The contribution of the carbohydrate moiety to the CD and ORD spectra was estimated on the basis of data obtained from isolated glycopeptides and the constituent monosaccharides. The carbohydrate moiety had no effect on the conformation of the protein moieties of LDL1 and LDL2 (apoLDL1 and apoLDL2). However, the intensities of the observed extrema in the CD and ORD spectra of the glycopeptides were greater than those expected from the monosaccharide composition. This suggests the existence of secondary structure in the carbohydrate moiety. In contrast to the carbohydrate moiety, the contribution of the lipid moiety to the CD and ORD spectra could not be neglected. When the effect of the lipid moiety was subtrated from the CD and ORD spectra, the spectra due to apoLDL1 and apoLDL2 were quite similar. Delipidation in the presence of sodium dodecyl sulfate (SDS) induced an increase in the content of disordered structure and alpha-helix accompanied by a decrease in the beta-structure. In the presence of SDS, marked quenching occurred in the fluorescence emission spectra with a blue shift of the maximum emission wavelength from 332 to 326 nm. ApoLDL1 and apoLDL2 showed quite similar SDS-induced conformational transitions. The secondary structures of apoLDL1 and apoLDL2 in the native lipoproteins were stable to changes of pH and temperature. However, this stability was lost in the presence of SDS. These results suggest the importance of the lipid moiety in maintaining the native secondary structures of LDL1 and LDL2. From the overall similarity of the optical properties of apoLDL1 and apoLDL2, we conclude that the secondary structures of apoLDL1 and apoLDL2 are identical.     

Total optical activity of agarose: relation to observable transitions in the vacuum ultraviolet

The changes in optical activity that accompany and characterize the coil-helix and helix-coil transitions of agarose in aqueous solutions and gels have been investigated by combined quantitative analysis of data from vacuum ultraviolet circular dichroism (VUCD) and optical rotary dispersion (ORD). VUCD of agarose in the high-temperature coil state shows a single accessible Gaussian band centered at ～183 nm. In the helix state this band is blue-shifted by ～9 nm, and the intensity is increased by a factor of ～2.6. Spectra at intermediate temperatures can be fitted to within experimental error by linear combination of coil and helix spectra, the relative proportions required providing an index of the extent of conformational ordering. ORD spectra throughout the conformational transition have a common form and differ only in absolute magnitude. The temperature course of conformational ordering derived from ORD intensity is in close agreement with the values obtained from VUCD. In both the coil and helix states the accessible VUCD band is positive, while the overall ORD is negative, indicating strong negative CD activity at lower wavelength. The ORD contribution corresponding to the positive VUCD band was calculated by Kronig–Kramers transform, and it was subtracted from the total ORD to give the residual ORD from all other optically active transitions of the molecule. In both the coil and helix states, this residual ORD could be fitted to within experimental error by a single Gaussian CD band at ～149 nm. A negative band at this wavelength has been reported previously for agarose films, but the observed intensity, relative to that of the lower energy positive band, is substantially smaller than the fitted value under hydrated conditions. In both the coil and helix states the total optical activity of agarose, characterized by observed ORD spectra, can be matched to within experimental error by Kronig-Kramers transform of the 149-nm negative band and the smaller positive band at higher wavelength, with no necessary involvement of deeper-lying transitions. The significance of this conclusion for fundamental understanding of carbohydrate optical activity is discussed.     

Nanosecond optical rotatory dispersion spectroscopy: application to photolyzed hemoglobin-CO kinetics.

A standard technique for static optical rotatory dispersion (ORD) measurements is adapted to the measurement of ORD changes on a nanosecond (ns) time scale, giving approximately a million-fold improvement in time-resolution over conventional instrumentation. The technique described here is similar in principle to a technique recently developed for ns time-resolved circular dichroism (TRCD) spectroscopy, although the time-resolved optical rotatory dispersion (TRORD) technique requires fewer optical components. As with static ORD, TRORD measurements may be interpreted by empirical comparisons or may be transformed, via the Kramers-Kronig relations, to more easily interpreted TRCD spectra. TRORD can offer experimental advantages over TRCD in studying kinetic processes effecting changes in the chiral structures of biological molecules. In particular, the wider dispersion of ORD bands compared with the corresponding CD bands means that ORD information may often be obtained outside of absorption bands, a signal-to-noise advantage for multichannel measurements. Demonstration of the technique by its application to ns TRORD and the transform-calculated TRCD of carboxy-hemoglobin (Hb-CO) after laser photolysis is presented.     

Optical rotatory dispersion and circular dichroism of carbanilyl polysaccharides

Measurements of optical rotatory dispersion (ORD) and circular dichroism (CD) have been made in the range of 600-210 mμ for the β-glycan carbanilates as for instance, 2,3,6-tricarbanilylcellulose (I), 2,3,6-tricarbanilylmannan (II), 2,3-dicarbanilylcellulose (III), and octacarbanilylcellobiose (IV) and also for the α-glycan carbanilates, such as 2,3,6-tricarbanilylamylose (V), tricarbanilylpullulan (VI), 2,3-dicarbanilylamylose (VII), and octacarbanilylmaltose (VIII). Furthermore, the 2,3,4,6-tetracarbanilyl-α-methyl-glucopyranoside (IX) and the 1,2,3,4,6-pentacarbanilylglucose (X) have been measured in dioxane at 20°C. For the β-glycans a small negative CD in the region of 238–240 mμ and nearly symmetrical ORD curve with a crossover point at 238–240 mμ are found; this indicates a simple negative Cotton effect. In the case of α-glycosides, a strong negative CD with a maximum at 240–242 mμ and a strong positive CD with a maximum at 223–225 mμ were found; the ORD curves are asymmetrical and cross the abscissa in two places, at 241–243 and 220–222 mμ. With 2,3,4,6-tetracarbanilyl-α-methylglucoside (IX) no CD and ORD in the ultraviolet region and with 1,2,3,4,6-pentacarbanilyl-glucopyranoside (X) the ORD, but not the CD, could be measured. The ORD curve is nearly symmetrical, like those of the β-glycans but is of opposite sign. It seems impossible to discuss the striking difference of the CD and ORD spectra between the α-and the β-glycans in terms of contributions of single independant chromophores influenced by their individual different steric arrangements and their spatial relation to the glycosidic bond in C₁. The exciton theory of Moffitt, which is suitable for explaining the ORD and CD spectra of helical polymers, has been applied to α- and β-glycans. A structure with helical parts is proposed for the α-glycans while a nearly planar arrangement is assumed for the β-glycans.     

Effect of counterions on the conformation of hyaluronic acid.

To study the effect of metal ions on the conformation of hyaluronic acid, circular dichroism (CD) and optical rotatory dispersion (ORD), along with viscosity measurements of the Na, Li, Ca, and Mg salts of the polymer, were carried out. With divalent cations, the results show a decrease in CD minima at 210 nm and an increase in ORD troughs at 220 nm, as compared to monovalent ions. To account for this behavior, the ORD in the visible range corresponding to the observed CD bands was directly calculated from the Moscowitz equation using Kronig-Kramer's transform. The background rotation was found to be more levorotatory in bivalent than in monovalent cations. The ORD spectra of various metal hyaluronates differ significantly from each other in the far ultraviolet region, especially at lower pH values. The values of intrinsic viscosities of these hyaluronates, on the other hand, are almost the same in the pH range of 1–3. These results indicate a local conformation variation rather than any appreciable change in the chain conformation of the molecule in the presence of different counterions.     

Diamide model for the optical activity of collagen and polyproline I and II

A diamide, N-acetyl-L -proline-N,N-dimethylamide (AcProDMA), in water solution has optical rotatory dispersion (ORD) and circular dichroism (CD) spectra very similar to those of poly-L -proline II and the fibrous protein collagen. In contrast, AcProDMA in cyclohexane solution has optical activity resembling that of poly-L -proline I. Conformational analysis shows that AcProDMA is confined by steric constraints to either of two narrow regions of conformational space. The trans isomer of AcProDMA assumes conformations near those of polyproline II and collagen nearest neighbors, while cis-AcProDMA assumes conformations near that of polyproline I nearest neighbors. Nuclear magnetic resonance (NMR) experiments show that an equilibrium mixture of the cis and trans isomers of AcProDMA is present in solution. The trans isomer predominates in aqueous solution, but the equilibrium shifts to favor the cis isomer in nonpolar organic solvents such as cyclohexane. Analysis of the ORD spectra in terms of two basic spectra reveals a solvent dependent isomerization which parallels that observed by NMR. The optical activity of the pure isomers of AcProDMA can be derived from the ORD, CD and NMR data. A comparison of component cotton effects confirms the similarity in optical activity of trans-AcProDMA, polyproline II, and collagen on the one hand, and of cis-AcProDMA and Polyproline I on the other.     

Fast generation of nonresonant and resonant optical rotatory dispersion curves with the help of circular dichroism calculations and Kramers-Kronig transformations

It can be computationally expensive to compute smooth, well resolved, optical rotation (OR) dispersion (ORD) curves from first principles theory. Instead of computing the OR at a large number of frequency points, similar results can be obtained by combined use of a computed circular dichroism (CD) spectrum along with a few OR calculations by using subtractive Kramers-Kronig transformations. We have tested various subtractive schemes for simulated (analytical) CD/ORD and for time-dependent density functional computations for dimethyloxirane, fenchone, and [4]triangulane. Nonresonant ORD can be obtained with as few as two OR and one CD calculation. For resonant ORD we found that between 7 and 15 OR computations plus the CD spectrum were typically sufficient, depending on the number of excitations within the frequency window of interest.     

Kramers-Kronig transformation of experimental electronic circular dichroism: application to the analysis of optical rotatory dispersion in dimethyl-L-tartrate

When a limited region of the experimental electronic circular dichroism (ECD) spectrum is subjected to Kramers-Kronig (KK) transformation, the resulting optical rotatory dispersion (ORD) may or may not reproduce the experimentally measured ORD in the long-wavelength nonresonant region. If the KK transform of experimentally measured ECD in a limited wavelength region reproduces the experimentally measured ORD in the long-wavelength nonresonant region, then that observation indicates that the ORD in the long-wavelength nonresonant region should be satisfactorily predicted from the correspondingly limited number of electronic transitions in a reliable quantum mechanical calculation. On the other hand, if the KK transform of experimentally measured ECD in a limited region does not reproduce the experimentally measured ORD in the long-wavelength nonresonant region, then it should be possible to identify the ECD bands in the shorter wavelength region that are responsible for the differences between experimentally observed ORD and KK-transformed ECD. This approach helps to identify the role of ECD associated with higher energy-excited states in the nature of ORD in the long-wavelength nonresonant region. These concepts are demonstrated here by measuring the experimental ECD and ORD for dimethyl-L-tartrate in different solvents. While ECD spectra of dimethyl-L-tartrate in different solvents show little variation, ORD spectra in the long-wavelength nonresonant region show marked solvent dependence. These observations are explained using the difference between experimental ORD and KK-transformed ECD. Quantum mechanical predictions of ECD and ORD are also presented for isolated (R, R)-dimethyl tartrate at the B3LYP/aug-cc-pVDZ level.     

Far-ultraviolet optical activity of saccharide derivatives. II. Dextran,amylose, and mycodextran acetes; dextran and amylose xanthates

The ultraviolet ORD and CD spectra of amylose, dextran, and mycodextran acetates and some of thier oligomers were recorded in trifluoroethanol solution in the 300–185nm wavelength range. Similarly, the spectra of amylose and dextran xanthates in water solution were obtained in the 400–200 nm range. In the amylose acetate series, the monomer and dimer both show a normal acetyl n → π* transition in CD, while the trimer and the polymer both exhibit an additional, shorter wavelength peak. The latter is presumed to arise from a helical conformation of the amylose chain. This interpretation is substantiated by a helix–coil type transition of the CD spectra of amylose triacetate at elevated temperatures and a reversion of the anomalous CD to the normal CD upon partial deacetylation. By contrast, neither dextran acetates nor mycodextran acetate exhibit any conformational effects. The CD of dextran acetates is quite sensitive to β-1,6 and branch linkages. The ORD and CD of amylose xanthate are complex, suggesting the presence of organized structure in solution. The dextran xanthate shows only a simple ORD spectrum and no observable CD.     

Correlation between conformation distortion of the DNA sugar-phosphate backbone and high optical activity of its compact form

Different physico-chemical methods (CD, ORD, small-angle X-ray diffraction, etc) were used for investigating the properties of the DNA compact particles formed in PEG-containing water-salt solutions. It has been shown that small-angle reflection, characteristic of the DNA compact particles, changes from 36.8 A (CPEG = 140 mg/ml) to 25 A (CPEG = 300 mg/ml). The maximal optical activity (the intense negative CD-band and optical rotation [alpha] = 60 000 degrees) are inherent properties of the DNA compact particles formed at CPEG 120--180 mg/ml. The high optical activity points to the twist of DNA chromophores through the DNA molecule resulting in a long-rang pitch (P approximately 2000A).Such macroscopic superhelical structure (diameter 40--30 A) is due to conformational distortion of the DNA double-helix with alternating "left" and "right" orientation of chromophoes. Disappearance of conformation distortion is accompanied by disappearance of the high optical activity of the DNA compact particles and results in a small-angle reflection of 25 A. Taking into account the reasons of formation of the optically-active DNA compact particles conditions are suggested to conserve high optical activity at CPEG equal to 400 mg/ml.     

Optical rotatory dispersion and circular dichroism of silver(I):Polyribonucleotide complexes

Optical rotatory dispersion (ORD) and circular dichroism (CD) spectra of single- and multistranded polyribonucleotides undergo extensive changes on binding of the silver ion. These changes are consistent with the proposition that Ag(I) binds to the heterocyclic bases and not to the phosphate groups of polynucleotides. ORD and CD of silver complexes of poly(A)·poly(U) and double-helical rice dwarf viral RNA display negative Cotton effects when there is more than one Ag(I) per two nucleotide residues in solution. These observations suggest a significant distortion of the double-helical conformation as a result of Ag(I) binding. Silver(I) binding sites of pyrimidine polynucleotides are apparently saturated when there is one Ag(I) per two nucleotide residues and those of purine polynucleotides at one Ag(I) per nucleotide in solution. These data are consistent with the supposition that some Ag(I) binding sites exist on the pyrimidine ring and additional sites on the imidazole ring of polynucleotides. The sedimentation coefficient of poly(A) increases by severalfold when one Ag(I) is present per nucleotide residue. Silver(I) may introduce intra- and interstrand cross-links (through bidentate chelates) in single-stranded polynucleotides, resulting in structures with high sedimentation coefficients. Among the polynucleotides studied, poly(U) was an exception. Silver(I) did not affect the optical properties (absorbance, ORD, and CD) of poly(U) at neutral pH.     

CDSpecTech: A single software suite for multiple chiroptical spectroscopic analyses

The program CDSpecTech was developed to facilitate the analysis of chiroptical spectra, which include the following: vibrational circular dichroism (VCD) and corresponding vibrational absorption (VA) spectra; vibrational Raman optical activity (VROA) and corresponding vibrational Raman spectra; electronic circular dichroism (ECD) and corresponding electronic absorption (EA) spectra. In addition, the program allows for generating optical rotatory dispersion (ORD) as the Kramers–Kronig transform of ECD spectra. The simulation of theoretical spectra from transition strengths can be achieved using different bandshape profiles. The experimental and simulated theoretical spectra can be visually compared by displaying them together. A unique feature of CDSpecTech is performing spectral analysis using the ratio spectra; i.e., the dimensionless dissymmetry factor (DF) spectrum, which is the ratio of CD to absorption spectra, and the dimensionless circular intensity difference (CID) spectrum, which is the ratio of VROA to vibrational Raman spectra. The quantitative agreement between experimental and simulated theoretical spectra can also be assessed from the numerical similarity overlap between them. Two different similarity overlap methods are available. The program uses a graphical user interface which allows for ease of use and facilitates the analysis. All these features make CDSpecTech a valuable tool for the analysis of chiroptical spectra. The program is freely available on the World Wide Web.     

Preparation and study of chiral magnesium porphyrin-amino acid complexes

Mixtures of magnesium protoporphyrin or magnesium mesoporphyrin with a variety of chiral amino acids (L-histidine, D- and L-proline, L-serine and L-threonine) produce prominent induced Cotton effects in the UV-visible region. By contrast magnesium deuteroporphyrin mixtures exhibit no optical rotatory dispersion (ORD)/circular dichroism (CD) spectra. It is proposed that the species producing the Cotton effects are six-coordinate species of the type Mg (porphyrin) (amino acid)₂. For L-histidine and L-threonine CD spectra have shown that complexes of the opposite chirality can be obtained for different samples of magnesium protoporphyrin. For D- and L-proline such a change in sign of spectra was not found for the same magnesium porphyrin samples. Reasons for these observations are presented together with proposals regarding structural details of the six-coordinate complexes. It is also suggested that racemic samples of such amino acid-magnesium porphyrin mixtures could yield optical resolution of products on irradiation with circularly polarised light. Details of a study of this type are presented.     

The conformation of poly-L-alanine in hexafluoroisopropanol

High-molecular-weight poly-L -alanine dissolved in hexafluoroisopropanol exhibits infrared, ultraviolet, circular dichroism, and optical rotatory dispersion spectra which are unique and unlike any other previously reported polypeptide spectra. Strong evidence that a helical conformation is present is shown by the high degree of hypochromism in the 187mμ absorption peak and by the positions of the amide infrared bands. The CD and ORD spectra are also similar to those of α-helical polypeptides, though important qualitative and qualitative differences are observed. To explain the novel spectra, which are not mixtures of the spectra of previously reported polypeptide conformations, a new α-helix-like conformation is proposed. The postulated conformation (a doubly hydrogen-bonded helix) is a distorted α-helix in which the peptide carbonyl groups point slightly out from the helix axis and are hydrogen bonded simul taneously both to the NH of the fourth peptide residue to the carboxyl terminal side (as in the classical α-helix), as well as to a solvent molecule's hydroxyl hydrogen.     

Conformational changes in the progesterone binding globulin-progesterone complex.

An improved purification procedure for the progesterone-binding globulin (PBG) of the pregnant guinea pig has been developed utilizing sulfopropyl Sephadex, a strong cation exchanger, in the first step. The method exploits the low pI (2.8) and favorable acid stability of the glycoprotein. Subsequent chromatographies on DEAE-cellulose and Sephadex G-200 afford a highly purified PBG that exhibits the previously observed polydispersity (R.M. Burton et al. (1974), Biochemistry 13, 3554-3561). Circular dichroism, optical rotatory dispersion, and difference uv spectra all indicate the purified protein to undergo a conformational transition upon forming a complex with a steroid ligand. The CD and ORD spectra cannot be interpreted in terms of tertiary structure probably due to carbohydrate contributions. However, the difference spectra indicate strong perturbation of both a tryptophan residue and the steroid chromophore in the complex.     

Optical activity of simple peptides. I. Glycine oligopeptides with internal L-alanyl or L-glutamyl residues

Oligopeptides containing glycine and one or two L -alanyl or L -glutamyl residues have been studied by circular dichroism (CD) and optical rotatory dispersion (ORD) in aqueous solution at pH 1.0, pH 6.0, and pH 10.0 and in aqueous ethanol. Two glycyl residues are required to remove effects of α-carboxyl or amino titration on the optical activity of the internal alanyl or glutamyl residues. The CD spectra of the alanyl and protonated glutamyl residues are similar, having two regions of negative ellipticity around 215 nm resulting in a spectrum reassembling that of poly-α-L -glutamic acid (PGA) at high pH. Another large positive band below 190 nm was observed for gly₂-glu₂-gly₂ in water at pH 6 and 10 and for several peptides in aqueous ethanol. Residue ellipticities were approximately additive in every case except for peptides containing intrenal glutamyl residu at pH 6.0.     

Conformational aspects of polypeptides. XXIX. Conformational assignments for some aromatic polypeptides by far-UV Cotton effects. New results

Recent improvements in apparatus permit the examination of circular dichroism (CD) and optical rotatory dispersion (ORD) spectra to 185 mμ. In addition, new solvents which are transparent to 185 mμ have become available for synthetic polypeptides. The spectral region 185–250 mμ is extremely important for the amide (peptide) chromophore, because of the presence at these wavelengths of the n–π* and π–π* bands,¹ and of another transition, the assignment of which remains unsettled.²     

Solution studies on heme proteins. Circular dichroism and optical rotation of Glycera dibranchiata hemoglobins

Circular dichroism (CD) and optical rotatory dispersion (ORD) spectra of several liganded derivatives of the monomer and polymer hemoglobin components of the marine annelid, Glycera dibranchiata were measured over the wavelength range 650--195 nm. The differences observed between the monomer and polymer components for the heme dichroic bands in the visible, Soret and ultraviolet wavelength regions seem to result from changes in the heme environment, geometry and coordination state of the central heme iron in these proteins. Within the Soret region, the liganded derivatives of the monomer hemoglobin exhibit predominantly negative circular dichroic bands. The heme band at 260 nm is also absent for the monomer hemoglobin. The ORD and CD spectra in the far-ultraviolet, peptide absorbing region suggest also differences in the alpha-helix content of the monomer and polymer hemoglobins. The values for the single-chain G. dibranchiata hemoglobin are in the expected range (about 70% alpha-helix) as predicted by the X-ray structure of this protein. The lower estimates of the alpha-helix content for the polymer hemoglobin (approx. 50%), may reflect the differences in amino acid composition, primary structure and polypeptide chain foldings. Changes in oxidation state and ligand binding appears to have no pronounced effect on the helicity of either the monomer or polymer hemoglobins. The removal of the heme moiety from the monomer hemoglobin did result in a major decrease in its helix content similar to the loss of heme from myoglobin.     

Oligonucleotide studies: optical rotatory dispersion of normal and 2'-O-methylated diribonucleoside monophosphates

The optical rotatory dispersion (ORD) of several diribonucleoside monophosphates (NpN) and the corresponding 2′-O-methyl substituted dinucleoside monophosphates containing 2′-O-methyl ribosyl 3′-nucleotide and a 5′-nucleoside (NmpN) were measured at pH 1, 7, and 11.2, at 0.1 ionic strength in order to examine the role of the 2′-hydroxyl group of the ribose in the conformation of the oligoribonucleotides. The optical measurements are reported from 210 to 340 mμ. The pH effect on the ORD spectra of NpN as well as NmpN are large. No dramatic changes are seen in the shapes of the ORD spectra of the NmpN to the corresponding NpN at pH 7. However, a decrease in the amplitude is seen in most of the NmpN over that of the corresponding NpN ranging from 7 percent in the case of UmpG to 46 percent in AmpA. The differences seen in the NpN and the corresponding NmpN ORD results are best explained as a consequence of a change in the ribosyl conformation on 2′-O-methylation, rather than the involvement of the 2′-hydroxyl group in intramolecular hydrogen bonding in the ribo dimmer. The NmpN behave like NpN and not dNpdN, suggesting that the geometry of the stack in NpmN and NpN depends on the oxygen at the 2′-carbon and not on what is attached to it.     

Simultaneous measurement of optical rotation dispersion and absorption spectra for chiral substances

We present a new method based on optical null methods for simultaneously measuring the optical rotatory dispersion (ORD) and absorption spectra of chiral substances. The optical rotation angle at a specific wavelength can be obtained from the optical nulls of the Malus curves with and without the sample. We use the optical nulls of the two curves as benchmark points and the readings to the right of the benchmark points by a certain angular offset to eliminate the influence of the analyzer on the light intensity and obtain the absorbance of the chiral substance at a specific wavelength. The 4096 pixels of the line scan CCD can measure multiple wavelengths simultaneously so that continuous ORD and absorption spectra can be obtained. The experimental results show that the standard deviation of the specific optical rotation is 0.11 deg mL g⁻¹ dm⁻¹, the standard deviation of the maximum absorption wavelength is 0.45 nm, and that absorbance of the sample varies linearly with the concentration. This method is helpful for simplifying the experiment and has a profound influence on the analysis of the contents and molecular configurations of chiral substances in the future.