Circular dichroism spectra of cytochrome c oxidase

Circular dichroism spectra of bovine heart aa(3)-type cytochrome c oxidase have been studied with a major focus on the Soret band π → π* transitions, B(0(x,y)), in the two iron porphyrin groups of the enzyme. The spectra of the fully reduced and fully oxidized enzyme as well as of its carbon monoxide and cyanide complexes have been explored. In addition, CD spectra of the reduced and oxidized ba(3)-type cytochrome c oxidase from Thermus thermophilus were recorded for comparison. An attempt is made to interpret the CD spectra of cytochrome c oxidase with the aid of a classical model of dipole-dipole coupled oscillators taking advantage of the known 3D crystal structure of the enzyme. Simultaneous modeling of the CD and absorption spectra shows that in the bovine oxidase, the dipole-dipole interactions between the hemes a and a(3), although contributing significantly, cannot account either for the lineshape or the magnitude of the experimental spectra. However, adding the interactions of the hemes with 22 aromatic amino acid residues located within 12 ? from either of the two heme groups can be used to model the CD curves for the fully reduced and fully oxidized oxidase with reasonable accuracy. Interaction of the hemes with the peptide bond transition dipoles is found to be insignificant. The modeling indicates that the CD spectra of cytochrome oxidase in both the reduced and oxidized states are influenced significantly by interaction with Tyr244 in the oxygen-reducing center of the enzyme. Hence, CD spectroscopy may provide a useful tool for monitoring the redox/ionization state of this residue. The modeling confirms wide energy splitting of the orthogonal B(x) and B(y) transitions in the porphyrin ring of heme a.     

Circular dichroism and DNA secondary structure.

The change in average rotation of the DNA helix has been determined for the transfer from 0.05 M NaCl to 3.0 M CsCl, 6.2 M LiCl and 5.4 M NH4Cl. This work, combined with data at lower salt from other laboratories, allows us to relate the intensity of the CD of DNA at 275 nm directly to the change in the number of base pairs per turn. The change in secondary structure for the transfer of DNA from 0.05 M NaCl (where it is presumably in the B-form) to high salt (where the characteristic CD has been interpreted as corresponding to C-form geometry) is found to be -0.22 (+/- 0.02) base pairs per turn. In the case of mononucleosomes, where the CD indicates the "C-form", the change in secondary structure (including temperature effects) would add -0.31 (+/- 0.03) turns about the histone core to the -1.25 turns estimated from work on SV40 chromatin. Accurate winding angles and molar extinction coefficients were determined for ethidium.     

Circular dichroism spectroscopy of fluorescent proteins

Circular dichroism (CD) spectra have been obtained from several variants of green fluorescent protein: blue fluorescent protein (BFP), enhanced cyan fluorescent protein (CFP), enhanced green fluorescent protein (GFP), enhanced yellow fluorescent protein (YFP), all from Aequorea victoria, and the red fluorescent protein from the coral species Discosoma (DsRed). We demonstrate that CD spectra in the spectral fingerprint region of the chromophore yield spectra that after normalization are not coincident with the normalized absorbance spectra of GFP, YFP and DsRed. On the other hand, the CD spectra of BFP and CFP coincide with the absorbance spectra. The resolution of absorption and CD spectra into Gaussian bands confirmed the location of the different electronic band positions of GFP and YFP as reported in the literature using other techniques. In the case of BFP and CFP the location of Gaussian bands provided information of the vibrational progression of the electronic absorption bands. The CD spectrum of DsRed is anomalous in the sense that the major CD band has a clear excitonic character. Far-UV CD spectra of GFP confirmed the presence of the high beta-sheet content of the polypeptide chain in the three-dimensional structure.     

Circular dichroism studies on proteins in films and in solution: estimation of secondary structure by g-factor analysis

Estimates of the secondary structure of a protein in solution are made by mathematical analyses of its circular dichroism (CD) spectrum below 240 nm. All current procedures require accurate determination of the concentration of the protein sample. Insoluble proteins, such as prions or amyloid, are examined as thin films or gels, but concentrations cannot be precisely defined. The ratio of a sample's CD and absorbance signals is the g-factor, an intensive property. The g-factor spectra of 19 soluble, unconjugated proteins of known structures were measured and used to derive basis spectra, characteristic of the four major structural elements, helix, sheet, turn, and remainder. Using these, the g-factor spectra of other unconjugated proteins, measured in solution or as films, can be analyzed by linear regression to give good estimates of their secondary structures when protein concentration cannot be determined.     

Circular dichroism spectroscopy has intrinsic limitations for protein secondary structure analysis

Secondary structure content (SSC) cannot be calculated accurately from circular dichroism (CD) spectra for the majority of proteins whose three-dimensional structures have been solved. “Reliable” SSC that is significantly different from random SSC can be calculated from CD spectra only for all-α proteins and all-β proteins with canonical β-strand geometry.     

Circular dichroism of cytochrome oxidase, cytochrome b566, and cytochrome c in beef heart mitochondrial membrane fragments

1. Circular dichroism spectra of the cytochromes in membrane fragments derived from sonicated beef heart mitochondria have been obtained in the wavelength region 400–480 nm in which the major absorbance maxima of the heme prosthetic groups are found.

2. 2. Cytochrome oxidase in the mitochondrial membrane fragments has a band of positive ellipticity at 426 nm in the oxidized form and a pronounced band of positive ellipticity at 445 nm in the reduced form. The reduced-minus-oxidized difference molar ellipticity at 445 nm, Δ[θ]₄₄₅ is 3.0·10⁵ degree·cm⁻²·dmole⁻¹ heme a for membrane-bound oxidase compared to 1.6·10⁵ degree·cm⁻²·dmole⁻¹ heme a for the purified oxidase. The membrane-bound oxidase in the reduced form also appears to have a band of negative ellipticity at 426 nm not found in the purified oxidase.

3. 3. When reduced with succinate in the presence of cyanide and oxygen, cytochrome oxidase in the membrane fragments has a positive band at 442 nm very similar to that observed with the purified oxidase.

4. 4. Cytochrome c, which has a positive band at 426 nm in the purified form when reduced, appears to have a negative band at this wavelength in the mito-chondrial membrane fragments which contributes to the pronounced negative band at 426 nm observed in the membrane fragments reduced with succinate in anaerobiosis. There is no evidence for a contribution to the CD spectra of the membrane fragments from cytochrome c₁ or from cytochrome b₅₆₁ in either the oxidized or the reduced form.

5. 5. Cytochrome b₅₆₆ in the mitochondrial membrane fragments has no detectable CD spectrum in the oxidized form, but has a small positive band at 427 nm and a small negative band at 436 nm in the reduced form. The same CD spectrum is observed with cytochrome b₅₆₆ reduced with succinate in the presence of antimycin A or 2-heptyl-4-hydroxyquinoline-N-oxide. The same increase in positive ellipticity is observed at 427 nm in the mitochondrial membrane fragments, treated with oligomycin to restore energy coupling, when cytochrome b₅₆₆ is reduced with succinate in the energized membrane, as is observed in the inhibitor-treated membrane fragments. The absence of a pronounced conformational change in cytochrome b₅₆₆ on energization, as revealed by its CD spectrum, favors the concept that its reduction by succinate in the energized state is due to reversed electron transport rather than an intrinsic shift in the cytochrome's midpoint redox potential.

Secondary structure and dosage of soluble and membrane proteins by attenuated total reflection Fourier-transform infrared spectroscopy on hydrated films

Attenuated total reflection Fourier-transform infrared spectroscopy of thin hydrated films of soluble and membrane protein included in a phospholipid bilayer is shown to provide useful information as to the secondary structure of the protein. The analysis of the amide I band of deuterated samples by Fourier self-deconvolution followed by a curve fitting was performed by a new procedure in which all the input parameters are generated by the computer rather than by the investigator. The results of this analysis provide a correct estimation of the alpha-helix and beta-sheet structure content with a standard deviation of 8.6% when X-ray structures are taken as a reference. We also show that the orientation of the different secondary structures resolved by the Fourier self-deconvolution/curve-fitting procedure and of the phospholipid acyl chains can be simultaneously evaluated for membrane proteins reconstituted in a lipid bilayer. Of special interest for reconstitution of membrane proteins, the lipid/protein ratio can be accurately and quickly determined from the infrared spectrum.     

Predicted secondary structure of bovine prothrombin fragment 1 and related proteins in different environments by circular dichroism spectroscopy.

Circular dichroism spectroscopy was used to investigate the structure of bovine prothrombin fragment 1 (BF1) and related proteins in several environments. The conformational change induced in BF1 by the addition of Mg[II] ions was found to be different from that induced by Ca[II] or Sr[II]. The Ca[II] and Sr[II] conformations appear to differ only slightly from the apo-metal conformation. The conformation of the 1-45 fragment of prothrombin, however, is markedly different than the conformation of the same fragment in the presence of either Ca[II] of Mg[II]; both of the latter structures differ substantially from one another. The presence of phospholipids has almost no effect on the structure of either BF1 or the 1-45 fragment; in the presence of both phospholipids and Ca[II] a structural change is seen for the 1-45 fragment but not BF1 (relative to the protein alone). The addition of phospholipids to the Mg[II]/BF1 structure did not induce a CD-detectable conformational change, while the addition of phospholipids to the Ca[II]/BF1 or Sr[II]/BF1 structures induced a change to a conformation similar in secondary structure composition to the relative apometal structures.     

Quantitation of secondary structure in ATR infrared spectroscopy

Polarized attenuated total reflection infrared spectroscopy of aligned membranes provides essential information on the secondary structure content and orientation of the associated membrane proteins. Quantitation of the relative content of different secondary structures, however, requires allowance for geometric relations of the electric field components (E(x), E(y), E(z)) of the evanescent wave, and of the components of the infrared transition moments, in combining absorbances (A() and A( perpendicular)) measured with radiation polarized parallel with and perpendicular to, respectively, the plane of incidence. This has hitherto not been done. The appropriate combination for exact evaluation of relative integrated absorbances is A() + (2E(z)(2)/E(y)(2) - E(x)(2)/E(y)(2))A( perpendicular), where z is the axis of ordering that is normal to the membrane plane, and the x-axis lies in the membrane plane within the plane of incidence. This combination can take values in the range approximately from A() - 0.4A( perpendicular) to A() + 2.7A( perpendicular), depending on experimental conditions and the attenuated total reflection crystal used. With unpolarized radiation, this correction is not possible. Similar considerations apply to the dichroic ratios of multicomponent bands, which are also treated.     

Synchrotron radiation circular dichroism spectroscopy of proteins: secondary structure, fold recognition and structural genomics

Recent developments in instrumentation and bioinformatics show that the technique of synchrotron radiation circular dichroism spectroscopy can provide novel information on protein secondary structures and folding motifs, and has the potential to play an important role in structural genomics studies, both as a means of target selection and as a high-throughput, low-sample-requiring screening method. This is possible because of the additional information content in the low-vacuum ultraviolet wavelength data obtainable with intense synchrotron radiation light sources, compared with that present in spectra from conventional lab-based circular dichroism instruments.     

The optimization of protein secondary structure determination with infrared and circular dichroism spectra.

We have used the circular dichroism and infrared spectra of a specially designed 50 protein database [Oberg, K.A., Ruysschaert, J.M. & Goormaghtigh, E. (2003) Protein Sci. 12, 2015-2031] in order to optimize the accuracy of spectroscopic protein secondary structure determination using multivariate statistical analysis methods. The results demonstrate that when the proteins are carefully selected for the diversity in their structure, no smaller subset of the database contains the necessary information to describe the entire set. One conclusion of the paper is therefore that large protein databases, observing stringent selection criteria, are necessary for the prediction of unknown proteins. A second important conclusion is that only the comparison of analyses run on circular dichroism and infrared spectra independently is able to identify failed solutions in the absence of known structure. Interestingly, it was also found in the course of this study that the amide II band has high information content and could be used alone for secondary structure prediction in place of amide I.     

Time-resolved magnetic circular dichroism spectroscopy of photolyzed carbonmonoxy cytochrome c oxidase (cytochrome aa3).

Nanosecond time-resolved magnetic circular dichroism (TRMCD) and time-resolved natural circular dichroism (TRCD) measurements of photolysis products of the CO complex of eukaryotic cytochrome c oxidase (CcO-CO) are presented. TRMCD spectra obtained at 100 ns and 10 microseconds after photolysis are diagnostic of pentacoordinate cytochrome a3Fe2+, as would be expected for simple photodissociation. Other time-resolved spectroscopies (UV-visible and resonance Raman), however, show evidence for unusual Fea3(2+) coordination after CO photolysis (Woodruff, W. H., O. Einarsdóttir, R. B. Dyer, K. A. Bagley, G. Palmer, S. J. Atherton, R. A. Goldbeck, T. D. Dawes, and D. S. Kliger. 1991. Proc. Nat. Acad. Sci. U.S.A. 88:2588-2592). Furthermore, time-resolved IR experiments have shown that photodissociated CO binds to CuB+ prior to recombining with Fea3(2+) (Dyer, R. B., O. Einarsdóttir, P. M. Killough, J. J. López-Garriga, and W. H. Woodruff. 1989. J. Am. Chem. Soc. 111:7657-7659). A model of the CcO-CO photolysis cycle which is consistent with all of the spectroscopic results is presented. A novel feature of this model is the coordination of a ligand endogenous to the protein to the Fe axial site vacated by the photolyzed CO and the simultaneous breaking of the Fe-imidazole(histidine) bond.