pH-dependent interconvertible forms of mushroom tyrosinase with different kinetic properties

The lag in cresolase activity and inhibition by excess tyrosine of mushroom tyrosinase which was observed when assayed at pH 6.8 was found to be absent when assayed at pH 5.0. The absence of lag and inhibition by excess tyrosine of tyrosinase at pH 5.0 were brought about only after the enzyme was kept at pH 5.0, at 0-4 degrees C, for 1.5 h. The enzyme kept at pH 5.0 for 1.5-3 h at 0-4 degrees C when brought back to pH 6.8, acquires lag and inhibition by excess tyrosine when its activity was measured at pH 6.8. The pH-dependent changes in the kinetic properties of the mushroom tyrosinase are similar to the pH-dependent changes in the kinetic properties of tyrosinase from B-16 murine melanoma and human skin, and thus appear to be a general property of tyrosinase from diverse sources.     

Absorption and circular dichroism spectra of methylene blue bound to alginate

The addition of methylene blue to certain samples of Na alginate produces a complex succession of spectrally distinguishable aggregated (metachromatic) dye species. Three of these species are active in CD; they are interpreted as aggregates of dye, but probably dimers, bound in orientations characteristic of the constituent copolymer blocks of alginate to which they are tentatively assigned. The aggregates compete with divalent metal ions and hydrogen ion for the binding sites of the polymer. Other samples of alginate give a modified succession of aggregated spectral species, which are almost devoid of CD activity. Mild treatment with acid, insufficient for hydrolysis, converts forms of alginate with CD activity into modified forms without it, the absorption spectra of which resemble those of samples originally devoid of activity. It is implied, subject to confirmation, that the chiral properties of the binding sites of the native polysaccharide are diminished or lost by acid treatment during commercial preparation.     

Absorption flattening in the circular dichroism spectra of small membrane fragments

The inhomogeneous distribution of chromophore occurring in a particulate suspension can result in a reduction in the apparent molar ellipticity recorded in circular dichroism (CD) spectra. The possibility of such a systematic error has often been a matter of concern when CD spectra of cell membrane proteins are recorded. The recent publication of CD spectra for bacteriorhodopsin in native and sonicated membranes, in detergent-solubilized form, and reconstituted into small unilamellar vesicles [Mao, D., & Wallace, B. A. (1984) Biochemistry 23, 2667-2673] gives a unique opportunity to apply the theoretical analysis of Gordon and Holzwarth [Gordon, D. J., & Holzwarth, G. (1971) Arch. Biochem. Biophys. 142, 481-488] so as to provide a definitive answer to the question of whether absorption flattening is significant for membrane particles. We show here that the data of Mao and Wallace can be combined with the theoretical analysis of Gordon and Holzwarth to rule out significant absorption flattening effects over the range 200-240 nm for submicrometer-sized membranes. In addition, the results show that absorption flattening can be disregarded even at 190 nm for membranous material in the size range below 100 nm. The demonstration that there are no major flattening effects in the CD spectra of bacteriorhodopsin, particularly in the region of 200-240 nm, means that the experimental spectra are incompatible with the proposal that this transmembrane protein contains seven transmembrane helices.     

Circular dichroism and magnetic circular dichroism spectra of chlorophylls a and b in nematic liquid crystals. II. Magnetic circular dichroism spectra

Absorption and magnetic circular dichroism (MCD) spectra are reported for chlorophyll (Chl) a and Chl b dissolved in nematic liquid crystal solvents. The spectra were measured with the dye molecules oriented uniaxially along the direction of. the magnetic field and measuring light beam. It is significant that under such conditions the MCD spectra recorded in the wavelength region of the Q and Soret bands of the chlorophyll are essentially unchanged with respect to rotation of the sample cell around this axis, even though there is almost complete orientation of the chlorophyll molecules by the liquid crystals. The MCD spectra of Chl a and b in the nematic liquid crystal solvents used in this study are surprisingly similar to the spectra obtained under isotropic conditions. These results illustrate an important technique with which to examine the optical spectra of dyes oriented in liquid crystal matrices in which the anisotropic effects can be reduced the negligible proportions by the application of a strong magnetic field parallel to the direction of the measuring light beam. The first deconvolution calculations are reported that describe the deconvolution of pairs of absorption and MCD spectra, in the Q and B band regions, for both Chl a and b. The spectral analysis to obtain quantitative estimates of transition energies was accomplished by carrying out detailed deconvolution calculations in which the both the absorption and MCD spectral envelopes were fitted with the same number of components; each pair of components had the same hand centres and bandwidth values. This procedure resulted in an assignment of each of the main transitions in the absorption spectra of both Chl a and b. Chl a is clearly monomeric, with Qy, Qx, By and Bx located at 671, 582, 439 and 431 nm, respectively. Analysis of the spectral data for Chl b located Qy, By and Bx, at 662, 476 and 464 nm, respectively.     

Absorption spectra and magnetic circular dichroism of heme-containing proteins in nonequilibrium states. VI. Cytochrome c-oxidase

Low temperature (77 degrees K) absorption spectra of nonequilibrium states of cytochrome c oxidase produced by reduction of oxidases form protein by thermolysed electrons at 77 degrees K was studied. During reduction of cytochrome oxidase water-glycerol solution by thermolysed electrons at 77 degrees K a nonequilibrium reduced protein is formed. Low temperature (77 degrees K) absorption spectra of the nonequilibrium cytochrome oxidase differs from those reduced by ditionite. It was shown that the oxidation state of cytochrome a3 or addition of cytochrom c have no influence on these spectral changes. It is assumed, that the observed effects are conditioned by structural differences of reduced and oxidased cytochrome oxidase active center. Similar spectral changes were observed for cytochrome oxidase, bound to the mitochondrial membrane. At temperature increasing the low temperature reduced protein is relaxed to a corresponding equilibrium state. The spectral properties of bacterial cytochrome oxidase M. lysodeicticus do not depend on the way of reduction (by dytionite or thermolysed electrons at 77 degrees K).     

Deconvolution of the circular dichroism spectra of proteins: the circular dichroism spectra of the antiparallel beta-sheet in proteins.

A recently developed algorithm, called Convex Constraint Analysis (CCA), was successfully applied to determine the circular dichroism (CD) spectra of the pure beta-pleated sheet in globular proteins. On the basis of X-ray diffraction determined secondary structures, the original data set used (Perczel, A., Hollosi, M., Tusnady, G. Fasman, G.D. Convex constraint analysis: A natural deconvolution of circular dichroism curves of proteins, Prot. Eng., 4:669-679, 1991), was improved by the addition of proteins with high beta-pleated sheet content. The analysis yielded CD curves of the pure components of the main secondary structural elements (alpha-helix, antiparallel beta-pleated sheet, beta-turns, and unordered conformation), as well as a curve attributed to the "aromatic contribution" in the wavelength range of 195-240 nm. Upon deconvolution the curves obtained were assigned to various secondary structures. The calculated weights (percentages determining the contributions of each pure component curve in the measured CD spectra of a given protein) were correlated with the X-ray diffraction determined percentages in an assignment procedure and were evaluated. The Pearson product correlation coefficients (R) are significant for all five components. The new pure component curves, which were obtained through deconvolution of the protein CD spectra alone, are promising candidates for determining the percentages of the secondary structural components in globular proteins without the necessity of adopting an X-ray database. The CD spectrum of the CheY protein was interesting because it has the characteristic shape associated with the alpha-helical structure, but upon analysis yielded a considerable amount of beta-sheet in agreement with the X-ray structure.     

Determination of protein secondary structure from circular dichroism spectra. III. Protein-derived base spectra of circular dichroism for antiparallel and parallel beta-structures

Protein-derived basic CD spectra for alpha-helix, antiparallel and parallel beta-structures, beta-bends and irregular form of proteins have been determined from the experimental CD spectra of six (myoglobin, lysozyme, ribonuclease A, papain, lactate dehydrogenase, subtilisin BPN') or seven (glyceraldehyde-3-phosphate dehydrogenase added) reference proteins and the analysis of the X-ray data. The secondary structures of thirteen proteins (seven reference and six additional ones) have been analysed using the basic CD spectra thus obtained. The data obtained have been compared with the results of the X-ray data analysis. It is shown that the accuracy of determination of the beta-structure and beta-bends contents using our basic CD spectra is about 2-3 times better than using the basic spectra reported by Chang et al. (Analyt. Biochem. 91, 13-31, 1978).     

Vibrational circular dichroism spectra of unblocked proline oligomers.

Vibrational Circular Dichroism (VCD) spectra of unblocked L-proline oligopeptides, (Pro)n n = 3 to 7, dissolved in D2O are reported. For these oligomers, the VCD spectra can be attributed to a conformational dominance of the trans amide conformation with subunits interrelated by a left-handed twist, particularly for the longer oligomers. As a function of oligomer length, formation of this conformation starts at n = 3; and by n = 5 a spectrum closely resembling that of the poly-L-proline II helix in shape and magnitude is seen. The VCD data are compared with previous (Pro)n results using IR, CD, Raman and NMR spectroscopies, and reasons for the variations in interpretation are discussed.     

Heme-heme interactions in circular dichroism spectra

Using the theory of optical activity by Kirkwood and Tinoco, the CD spectra of the heme peptides in mono- and dimeric forms have been calculated according to the simple spectral model of heme of Simpson.     

Protein secondary structure from circular dichroism spectra

Circular dichroism spectra of proteins are extremely sensitive to secondary structure. Nevertheless, circular dichroism spectra should not be analyzed for protein secondary structure unless they are measured to at least 184 nm. Even if all the various types ofβ-turns are lumped together, there are at least 5 different types of secondary structure in a protein (α-helix, antiparallelβ-sheet, parallelβ-sheet,β-turn, and other structures not included in the first 4 categories). It is not possible to solve for these 5 parameters unless there are 5 equations. Singular value decomposition can be used to show that circular dichroism spectra of proteins measured to 200 nm contain only 2 pieces of information, while spectra measured to 190 nm contain about 4. Adding the constraint that the sum of secondary structures must equal 1 provides another piece of information, but even with this constraint, spectra measured to 190 nm simply do not analyze well for the 5 unknowns in secondary structure. Spectra measured to 184 nm do contain 5 pieces of information and we have used such spectra successfully to analyze a variety of proteins for their component secondary structures.     

Absorption and magnetic circular dichroism spectra of hemoproteins in nonequilibrium states. V. Cytochrome P450 and its substrate complex

It was shown that ferrocytochrome P450 forms a nonequilibrium state if ferrocytochrome P450 and its complexes are reduced in freezed water-glycerol solutions by thermolysed electrons, arising during gamma-radiolysis of the matrix at 77 degrees K. Unlike the equilibrium form of ferrocytochrome P450 with the heme iron at the high-spin state the reduced nonequilibrium form of the protein contains the heme iron at a low-spin state. The absorption spectrum of ferrocytochrome P450 in the nonequilibrium state is characterized by alpha and beta-bands at 562 and 534 nm, respectively, whereas the magnetic circular dichroism spectra exhibit type A effect at 562 nm. Upon temperature increasing the nonequilibrium state is relaxed to the equilibrium one. Type 1 substrates had practically no influence on the spectral characteristic of the nonequilibrium form of ferrocytochrome P450. Binding of type 2 substrates results in an essential decrease of the intensity ratio of the alpha- and beta-bands (A alpha/A beta) and is accompanied by a red-shift of the alpha-band and corresponding magnetic circular dichroism effect. It was shown that mercaptoethanol complex of hemoglobin, formed by reduction at 77 degrees K is spectrally similar to the nonequilibrium ferrocytochrome P450 complex with type 2 substrates. From analysis of experimental data one can conclude that (i) the ligand environment of heme iron in oxidased and reduced cytochrome P450 are different; (ii) the sixth axial ligand of the heme iron in the oxidised protein is probably a water molecule (OH-) attached by a hydrogen bond to the neighbouring histidine. It is assumed that a similar nonequilibrium form of cytochrome P450 can be formed in physiological conditions.     

Analyzing protein circular dichroism spectra for accurate secondary structures.

We have developed an algorithm to analyze the circular dichroism of proteins for secondary structure. Its hallmark is tremendous flexibility in creating the basis set, and it also combines the ideas of many previous workers. We also present a new basis set containing the CD spectra of 22 proteins with secondary structures from high quality X-ray diffraction data. High flexibility is obtained by doing the analysis with a variable selection basis set of only eight proteins. Many variable selection basis sets fail to give a good analysis, but good analyses can be selected without any a priori knowledge by using the following criteria: (1) the sum of secondary structures should be close to 1.0, (2) no fraction of secondary structure should be less than -0.03, (3) the reconstructed CD spectrum should fit the original CD spectrum with only a small error, and (4) the fraction of alpha-helix should be similar to that obtained using all the proteins in the basis set. This algorithm gives a root mean square error for the predicted secondary structure for the proteins in the basis set of 3.3% for alpha-helix, 2.6% for 3(10)-helix, 4.2% for beta-strand, 4.2% for beta-turn, 2.7% for poly(L-proline) II type 3(1)-helix, and 5.1% for other structures when compared with the X-ray structure.     

Analyses of circular dichroism spectra of membrane proteins

Circular dichroism (CD) spectroscopy is a valuable technique for the determination of protein secondary structures. Many linear and nonlinear algorithms have been developed for the empirical analysis of CD data, using reference databases derived from proteins of known structures. To date, the reference databases used by the various algorithms have all been derived from the spectra of soluble proteins. When applied to the analysis of soluble protein spectra, these methods generally produce calculated secondary structures that correspond well with crystallographic structures. In this study, however, it was shown that when applied to membrane protein spectra, the resulting calculations produce considerably poorer results. One source of this discrepancy may be the altered spectral peak positions (wavelength shifts) of membrane proteins due to the different dielectric of the membrane environment relative to that of water. These results have important consequences for studies that seek to use the existing soluble protein reference databases for the analyses of membrane proteins.     

Circular dichroism and magnetic circular dichroism spectra of chlorophylls in nematic liquid crystals. I. Electric and weak magnetic field effects on the dichroism spectra

Dichroism spectra of chlorophyll a, chlorophyll b and bacteriochlorophyll a in various nematic liquid crystals are reported. The initial orientation of chlorophylls in such a sample is determined by the interaction of the aggregate formed from the pigment and the liquid crystal molecules with the electrode surface on the cell windows. Reorientation is carried out by either an electric or magnetic field. The analysis of the circular dichroism spectra obtained from these samples on the basis of the Mueller matrix shows that the intensity is predominantly related to the texture of the sample. Chlorophyll molecules can be aggregated with liquid crystals in two ways: (1) through the chlorin magnesium atom, which results in the liquid crystal chain being almost perpendicular to the porphyrin ring, or (2) attached parallel to the line connecting the first and third pyrrole rings of the chlorin, the chlorin now lying in the plane of the liquid crystal chains. By comparing the dichroism spectra of various chlorophylls in the same liquid crystal we can draw conclusions concerning the preferred type of aggregation, not only with liquid crystals, but also with biological molecules. These liquid crystal systems are models of the orientation effects found for chlorophyll in lamellae. The model studied in this work is much simpler than the lamellar system but it does exhibit several common properties with the latter. Both systems are anisotropic and show much more intense dichroism signals, often of opposite sign, compared with those observed for photosynthetic pigments in isotropic solutions. Dichroism signals of organism fragments are much more complex than those of our model, which can either be related to the occurrence in the organism of several types of pigments or, for a given type of pigment, could be the result of exciton splitting. On the basis of our model it is shown that small changes in the anisotropy of the pigment in the surroundings have a strong influence on the sign and amplitude of the observed circular dichroism signal. Such effects may be responsible for the structure of the dichroism spectra observed for biological samples. Such structures can be partially related to the superposition of the dichroism signal from various ‘domains’ of chromophore which are different in both pigment arrangement and in the anisotropy of the surroundings of the pigment molecules themselves.     

Absorption, circular dichroism, magnetic circular dichroism and emission study of rat kidney Cd,Cu-metallothionein

Absorption, circular dichroism (CD), magnetic circular dichroism (MCD) and emission spectra of rat liver and rat kidney cadmium-, zinc- and copper-containing metallothioneins (MT) are reported. The absorption, CD and MCD data of native rat kidney Cd,Cu-MT protein closely resemble data recorded for the rat liver Cd,Zn-MT. This suggests that the major features in all three spectra of the native Cd,Cu-MT are dominated by cadmium-related bands. The CD spectrum of the Cd,Cu-MT recorded at pH 2.7 has the same band envelope that is observed for a Cd,Cu-MT formed in vitro by titration of Cd,Zn-MT with Cu(I), suggesting that the copper occupies the zinc sites in Cd,Cu-MT formed both in vivo and, at low molar ratios, in vitro. Remetallalion of the metallothionein from low pH in the presence of both copper and cadmium results in considerably less cadmium bound to the protein than was present in the native sample. It is suggested that this is due to the effect of the distribution of the copper amongst all available binding sites, thus inhibiting cluster formation by the cadmium. Emission spectra are reported for the first time for a cadmium- and copper-containing metallothionein. An emission band at 610 nm is shown to be a sensitive indicator of Cu(I) binding to metallothionein. Both the native Cd,Cu-MT and a Cd,Cu-MT formed in vitro exhibit an excitation spectrum with a band in the copper-thiolate charge-transfer region.     

The sequence dependence of circular dichroism spectra of DNA duplexes.

The three satellite DNAs of Drosophila virilis, that approximate to poly d(CAAACTA)-poly d(TAGTTTG), poly d(TAAACTA)-poly d(TAGTTTA), poly d(CAAATTA)-poly d(TAATTTG), the satellite DNA of Drosophila melanogaster that approximates to poly d(AATAT)-poly d(ATATT), the synthetic DNA duplexes, poly dG-poly dC, poly d(AT)-poly d(AT), poly d(AAT)-poly d(ATT), poly d(AAC)-poly d(GTT), poly d(TAC)-poly d(GTA) and the block copolymer d(C15A15)-d(T15G15) all have circular dichroism spectra consistent with the propositions that they have the same molecular geometry in solution and that it is the kind and frequency of nucleotide triplet sequences that determines their spectral characteristics. Poly dA-poly dT is apparently an exception.