In situ kinetics of cytochromes c1 and c2

In Rhodobacter sphaeroides chromatophores, cytochromes (cyt) c(1) and c(2) have closely overlapping spectra, and their spectral deconvolution provides a challenging task. As a result, analyses of the kinetics of different cytochrome components of the bc(1) complex in purple bacteria usually report only the sum cyt c(1) + cyt c(2) kinetics. Here we used newly determined difference spectra of individual components to resolve the kinetics of cyt c(1) and c(2) in situ via a least-squares (LS) deconvolution. We found that the kinetics of cyt c(1) and c(2) are significantly different from those measured using the traditional difference wavelength (DW) approach, based on the difference in the absorbance at two different wavelengths specific for each component. In particular, with the wavelength pairs previously recommended, differences in instrumental calibration led to kinetics of flash-induced cyt c(1) oxidation measured with the DW method which were faster than those determined by the LS method (half-time of approximately 120 micros vs half-time of approximately 235 micros, in the presence of antimycin). In addition, the LS approach revealed a delay of approximately 50 micros in the kinetics of cyt c(1) oxidation, which was masked when the DW approach was used. We attribute this delay to all processes leading to the oxidation of cyt c(1) after light activation of the photosynthetic reaction center, especially the dissociation of cyt c(2) from the reaction center. We also found that kinetics of both cyt c(1) and c(2) measured by the DW approach were significantly distorted at times longer than 1 ms, due to spectral contamination from changes in the b hemes. The successful spectral deconvolution of cyt c(1) and c(2), and inclusion of both cytochromes in the kinetic analysis, significantly increase the data available for mechanistic understanding of bc(1) turnover in situ.     

Simultaneous determination of hemes a, b, and c from pyridine hemochrome spectra

Two procedures for analyzing overlapping optical spectra of mixtures of pyridine hemochromes are described, and extinction coefficients of pyridine hemochromes are provided for use with these methods. In the first procedure, absorbance is measured at a number of wavelengths equal to the number of components to be analyzed. This is the minimum amount of spectral data from which the concentration of each species can be calculated. In the second procedure, absorbance is measured at a number of wavelengths greater than the number of components to be analyzed. This redundancy of information makes it impossible to fit spectra which contain contributions from additional components, unless the spectra of the additional components are equal to linear combinations of the spectra of the species being analyzed. These two procedures are generally applicable to analyses of absolute or difference spectra of mixtures of components obeying Beer's law. The sensitivity to error in the absorbance measurements is only slightly greater than that for measuring a pure component at a single wavelength.     

Spectral analysis of the bc(1) complex components in situ: beyond the traditional difference approach

The cytochrome (cyt) bc(1) complex (ubiquinol: cytochrome c oxidoreductase) is the central enzyme of mitochondrial and bacterial electron-transport chains. It is rich in prosthetic groups, many of which have significant but overlapping absorption bands in the visible spectrum. The kinetics of the cytochrome components of the bc(1) complex are traditionally followed by using the difference of absorbance changes at two or more different wavelengths. This difference-wavelength (DW) approach has been used extensively in the development and testing of the Q-cycle mechanism of the bc(1) complex in Rhodobacter sphaeroides chromatophores. However, the DW approach does not fully compensate for spectral interference from other components, which can significantly distort both amplitudes and kinetics. Mechanistic elaboration of cyt bc(1) turnover requires an approach that overcomes this limitation. Here, we compare the traditional DW approach to a least squares (LS) analysis of electron transport, based on newly determined difference spectra of all individual components of cyclic electron transport in chromatophores. Multiple sets of kinetic traces, measured at different wavelengths in the absence and presence of specific inhibitors, were analyzed by both LS and DW approaches. Comparison of the two methods showed that the DW approach did not adequately correct for the spectral overlap among the components, and was generally unreliable when amplitude changes for a component of interest were small. In particular, it was unable to correct for extraneous contributions to the amplitudes and kinetics of cyt b(L). From LS analysis of the chromophoric components (RC, c(tot), b(H) and b(L)), we show that while the Q-cycle model remains firmly grounded, quantitative reevaluation of rates, amplitudes, delays, etc., of individual components is necessary. We conclude that further exploration of mechanisms of the bc(1) complex, will require LS deconvolution for reliable measurement of the kinetics of individual components of the complex in situ.     

Transient intermediates in the folding of dihydrofolate reductase as detected by far-ultraviolet circular dichroism spectroscopy

The kinetics of the reversible folding and unfolding of Escherichia coli dihydrofolate reductase have been studied by stopped-flow circular dichroism in the peptide region at pH 7.8 and 15 degrees C. The reactions were induced by concentration jumps of a denaturant, urea. The method can detect various intermediates transiently populated in the reactions although the equilibrium unfolding of the protein is apparently approximated by a two-state reaction. The results can be summarized as follows. (1) From transient circular dichroism spectra measured as soon as the refolding is started, a substantial amount of secondary structure is formed in the burst phase, i.e., within the dead time of stopped-flow mixing (18 ms). (2) The kinetics from this burst-phase intermediate to the native state are multiphasic, consisting of five phases designated as tau 1, tau 2, tau 3, tau 4, and tau 5 in increasing order of the reaction rate. Measurements of the kinetics at various wavelengths have provided kinetic difference circular dichroism spectra for the individual phases. (3) The tau 5 phase shows a kinetic difference spectrum consistent with an exciton contribution of two aromatic residues in the peptide CD region. The absence of the tau 5 phase in a mutant protein, in which Trp 74 is replaced by leucine, suggests that Trp 74 is involved in the exciton pair and that the tau 5 phase reflects the formation of a hydrophobic cluster around Trp 74. From the similarity of the kinetic difference spectrum to the difference between the native spectra of the mutant and wild-type proteins, it appears that Trp 47 is the partner in the exciton pair and that the structure formed in the tau 5 phase persists during the later stages of folding. (4) The later stages of folding show kinetic difference spectra that can be interpreted by rearrangement of secondary structure, particularly the central beta sheet of the protein. The pairwise similarities in the spectrum between the tau 3 and tau 4 phases, and between the tau 1 and tau 2 phases, also suggest the presence of two parallel folding channels for refolding. (5) The unfolding kinetics show three to four phases and are interpreted in terms of the presence of multiple native species. The total ellipticity change in kinetic unfolding reaction, however, agrees with the ellipticity difference between the native and unfolding states, indicating the absence of the burst phase in unfolding.(ABSTRACT TRUNCATED AT 400 WORDS)     

High frequency components in the spectrum of the visual evoked potential

The occurrence of short term high frequency components in the spectra of the VEP is usually overshadowed by larger amplitude slow waves which occur simultaneously with the high frequency waves. The high frequency components become evident when the time varying power spectra of short duration (250 ms) segments of the VEP are examined. Two types of short duration time varying power spectra are considered: one is obtained directly from overlapping time segments of the average VEP; and, the other is obtained by computing the spectra from the average autocorrelation functions of overlapping time segments of the data following each stimulus. The first yields the time varying properties for the spectra of the stimulus-synchronized data while, the latter shows the time varying properties of both the synchronized and unsynchronized data present.     

Modified Light-Induced Absorbance Changes in dim Y Photoresponse Mutants of Trichoderma

A brief pulse of blue light induces the common soil fungus Trichoderma harzianum to sporulate. Photoresponse mutants with higher light requirements than the wild type are available, including one class, dim Y, with modified absorption spectra. We found blue-light-induced absorbance changes in the blue region of the spectrum, in wild-type and dim Y mutant strains. The light-minus-dark difference spectra of the wild type and of several other strains indicate photoreduction of flavins and cytochromes, as reported for other fungi and plants. The difference spectra in strains with normal photoinduced sporulation have a prominent peak at 440 nm. After actinic irradiation, this 440 nanometer difference peak decays rapidly in the dark. In two dim Y photoresponse mutants, the difference spectra were modified; in one of these, LS44, the 440 nanometer peak was undetectable in difference spectra. Detailed study of the dark-decay kinetics in LS44 and the corresponding control indicated that the 440 nanometer difference peak escaped detection in LS44 because it decays faster than in the control. The action spectrum of the 440 nm difference peak is quite different from that of photoinduced sporulation. The light-induced absorbance changes are thus unlikely to be identical to the primary photochemical reaction triggering sporulation. Nevertheless, these results constitute genetic evidence that physiologically relevant pigments participate in these light-induced absorbance changes in Trichoderma.     

M?ssbauer characterization of the tetraheme cytochrome c3 from Desulfovibrio baculatus (DSM 1743). Spectral deconvolution of the heme components.

M?ssbauer spectroscopy was used to study the tetraheme cytochrome c3 from Desulfovibrio baculatus (DSM 1743). Samples with different degrees of reduction were prepared using a redoxtitration technique. In the reduced cytochrome c3, all four hemes are reduced and exhibit diamagnetic M?ssbauer spectra typical for low-spin ferrous hemes (S = 0). In the oxidized protein, the hemes are low-spin ferric (S = 1/2) and exhibit overlapping magnetic M?ssbauer spectra. A method of differential spectroscopy was applied to deconvolute the four overlapping heme spectra and a crystal-field model was used for data analysis. Characteristic M?ssbauer spectral components for each heme group are obtained. Hyperfine and crystal-field parameters for all four hemes are determined from these deconvoluted spectra.     

Interaction between proteins and detergents which contain a hydrocarbon chain longer than 16 carbon atoms. II. Difference spectra of various proteins in cetyldimethyl-benzylammonium chloride.

The detergents which contain a hydrocarbon side chain longer than 16 cabron atoms were used as a perturbant for the study of protein structure. ta low concentration of cetyldimethylbenzylammonium chloride (CDBA) caused difference spectra for Ac-Trp-OEt and AC-Tyr-OEt. The delta e values at their difference maxima became constant above 30 mM of cetyldimethylbenzylammonium chloride, 1430 at 294 nm for Ac-Trp-OEt and 450 at 288 nm for Ac-Tyr-OEt. These delta e values are higher than any other delta e values resulting from solvent effects by such a remarkably low concentration of organic reagents described in the literature so far. The absence of denaturation blue shift in the difference spectra and the fact that the optical rotatory dispersion of the proteins examined in the present study was not changed significantly by cetyldimethylbenzylammonium chloride indicate that the secondary and tertiary structures of the proteins were not destroyed by cetyldimethylbenzylammonium chloride. These characteristics, together with small overlapping of their difference spectra at 288 and 294 nm were advantageous in the determination of tryptophan and tyrosine residues exposed in glucagon, insulin and alcohol dehydrogenase from yeast. No tyrosine residues in ribonuclease A was accessible to cetyldimethylbenzylammonium chloride. Unusual difference spectrum with a peak at 298 nm was observed for lysozyme which is known to contain tryptophan residues in special environments. Ovalbumin gave a novel unusual difference spectrum with a peak at 290 nm and a shoulder at 298 nm, showing the existence of unusual tryptophan and probably tyrosine residues in the molecule.     

Circular dichroism studies of the B goes to A conformational transition in seven small DNA restriction fragments containing the Escherichia coli lactose control region.

The B goes to A conformational transition caused by high ethanol concentrations was studied for seven DNA restriction fragments with overlapping and known sequences. Since the DNAs are homogeneous and range in GC content from 44-63%, they permit an evaluation of the influence of DNA sequence and base composition on the B goes to A transition. Moreover, their small size (80-301 bp) minimizes precipitation artifacts. The B- form spectra (in low salt) and the transition toward the C- form (in ethanol concentrations below the B goes to A transition) agree with prior measurements on chromosomal DNAs and are similar for all seven DNAs. At higher ethanol concentrations (80%), all fragments undergo a transition to the A- form as judged by the large increase of the positive CD band at 270 nm. Difference spectra among the fragments reveal minor differences between the A- form spectra. The ethanol concentration necessary to cause this transition is 72 +/- 2% for all fragments, thus excluding a preference of the CAP-, E. coli RNA polymerase-, or lac repressor-binding sequences for the A- form. The kinetics of the B goes to A transition in 80% ethanol are biphasic; the initial rapid transition is an intramolecular B goes to A form shift and the slower transition is an aggregation (but not precipitation) of the DNA     

Removal of sodium channel inactivation in squid giant axons by n-bromoacetamide

The group-specific protein reagents, N-bromacetamide (NBA) and N- bromosuccinimide (NBS), modify sodium channel gating when perfused inside squid axons. The normal fast inactivation of sodium channels is irreversibly destroyed by 1 mM NBA or NBS near neutral pH. NBA apparently exhibits an all-or-none destruction of the inactivation process at the single channel level in a manner similar to internal perfusion of Pronase. Despite the complete removal of inactivation by NBA, the voltage-dependent activation of sodium channels remains unaltered as determined by (a) sodium current turn-on kinetics, (b) sodium tail current kinetics, (c) voltage dependence of steady-state activation, and (d) sensitivity of sodium channels to external calcium concentration. NBA and NBS, which can cleave peptide bonds only at tryptophan, tyrosine, or histidine residues and can oxidize sulfur- containing amino acids, were directly compared with regard to effects on sodium inactivation to several other reagents exhibiting overlapping protein reactivity spectra. N-acetylimidazole, a tyrosine-specific reagent, was the only other compound examined capable of partially mimicking NBA. Our results are consistent with recent models of sodium inactivation and support the involvement of a tyrosine residue in the inactivation gating structure of the sodium channel.     

Studies on the subsite structure of amylases. I. Interaction of glucoamylase with substrate and analogues studied by difference-spectrophotometry.

Studies were made on the ultraviolet difference-spectra of glucoamylase from Rhizopus niveus [EC 3.2.1.3] specifically produced by the substrate maltose and the inhibitors, glucose, glucono-1: 5-lactone (gluconolactone), methyl beta-D-glucoside, cellubiose, and cyclohexa-, and cyclohepta-amyloses. Of these, maltose and gluconolactone produced characteristic difference spectra with a trough near 300 nm. Based on studies with a model compound for a tryptophan residue, Ac-Trp, this trough was attributed to the effect of a negative charge upon the tryptophan residue. From the concentration dependency of the difference spectra, the dissociation constants of the complexes between the enzyme and maltose, glucose, and gluconolactone were evaluated to be 1.2 mM, 51 mM, and 1.5 mM, respectively. These values are in good agreement with the values of Km or K1 obtained from the steady-state kinetics. The difference-spectrophotometric data suggested that referring to the values of subsite affinities of glucoamylase, maltose, and gluconolactone occupy mainly Subsite 1, where the non-reducing-end glucose residue of a substrate is bound in a productive form and that a tryptophan residue with shows a trough near 300 nm in difference spectra is located in this subsite.     

Electron spin echo studies on chloroplasts. Spectral characteristics of electron transport components and light-induced transients

Electron-spin resonance echoes are used to study the complex overlapping ESR spectra of whole chloroplasts. By varying the repetition rate of the microwave pulse sequence, delay time, and pulse width, signals with different longitudinal and transverse relaxation times were extracted. We have identified the echo signals due to plastocyanin and ferredoxins. In addition, we have found a strong signal at g = 4.3, that possibly arises from distorted cytochrome, and weak signals in the region g = 6-9. The strong echo signal at g = 2.0047 (Signal II), is made up of at least three "dark" components that differ in their relaxation times. Upon illumination at 1.2 K several of the echo signals including Signal II show reversible light-induced components. The kinetics of these transients depend on the addition of 3(3,4-dichlorophenyl)-1,1-dimethyl urea. Part of the transients are believed to arise from cyclic electron flow around Photosystem I.     

Changes in conformation and nucleotide binding of Ca, Mn, or MgG-actin upon removal of the bound divalent cation. Studies of ultraviolet difference spectra and optical rotation

The ultraviolet difference spectra of EDTA-induced denaturation of dithiothreitoltreated actin prepared with either Ca²⁺, Mn²⁺, or Mg²⁺ as the strongly bound cation showed no appreciable difference, nor could any difference be found in the change of optical rotation. However, at different wavelengths the changes in the spectra have different rates and these rates do differ significantly depending on the bivalent cation bound to G-actin. The nucleotide and the cation appear to be removed simultaneously and at the fastest rate; about 50–80% is released within 1 min. The spectral changes have two phases: a fast change whose detailed kinetics have not been investigated in this paper, followed by a slower rate with first-order kinetics. The changes of optical rotation follow a single-phase first-order kinetics. The rates depend on the divalent cation, the sequence being Mn²⁺ > Ca²⁺ > Mg²⁺. ATP release is partially reversible upon Ca²⁺ addition; the reversibility is diminished as the time of incubation with EDTA is increased. On rebinding of ATP and Ca²⁺, the spectral and optical rotatory changes are not reversed, but no further changes occur. Such an EDTA-treated actin is polymerizable after addition of Ca²⁺, and the G-actin obtained after polymerization and depolymerization shows the same spectral change on a second addition of EDTA as the original actin. On the basis of these observations a scheme is suggested for the denaturation of G-actin.     

The Application of Gaussian Mixture Models for Signal Quantification in MALDI-ToF Mass Spectrometry of Peptides

Matrix assisted laser desorption/ionization time-of-flight (MALDI-TOF) coupled with stable isotope standards (SIS) has been used to quantify native peptides. This peptide quantification by MALDI-TOF approach has difficulties quantifying samples containing peptides with ion currents in overlapping spectra. In these overlapping spectra the currents sum together, which modify the peak heights and make normal SIS estimation problematic. An approach using Gaussian mixtures based on known physical constants to model the isotopic cluster of a known compound is proposed here. The characteristics of this approach are examined for single and overlapping compounds. The approach is compared to two commonly used SIS quantification methods for single compound, namely Peak Intensity method and Riemann sum area under the curve (AUC) method. For studying the characteristics of the Gaussian mixture method, Angiotensin II, Angiotensin-2-10, and Angiotenisn-1-9 and their associated SIS peptides were used. The findings suggest, Gaussian mixture method has similar characteristics as the two methods compared for estimating the quantity of isolated isotopic clusters for single compounds. All three methods were tested using MALDI-TOF mass spectra collected for peptides of the renin-angiotensin system. The Gaussian mixture method accurately estimated the native to labeled ratio of several isolated angiotensin peptides (5.2% error in ratio estimation) with similar estimation errors to those calculated using peak intensity and Riemann sum AUC methods (5.9% and 7.7%, respectively). For overlapping angiotensin peptides, (where the other two methods are not applicable) the estimation error of the Gaussian mixture was 6.8%, which is within the acceptable range. In summary, for single compounds the Gaussian mixture method is equivalent or marginally superior compared to the existing methods of peptide quantification and is capable of quantifying overlapping (convolved) peptides within the acceptable margin of error.     

Spectroscopic forms of carbonmonoxi-cytochrome oxidase.

A systematic study of the errors of low-temperature recording of kinetics of the cytochrome oxidase-CO reaction had identified the classic devitrification process of Keilin & Hartree [(1950) Nature (London)165, 504-505]. The methodology described here minimizes this effect, and the computation methods afford appropriate ways of detecting a residual effect. Thus it has been possible to identify that absorption difference spectra and kinetics of the reaction of fully reduced or half-reduced cytochrome oxidase with CO indicate only one spectroscopic form of the respective carbonmonoxi-cytochrome oxidase.     

Spectral networks: a new approach to de novo discovery of protein sequences and posttranslational modifications

Significant technological advances have accelerated high-throughput proteomics to the automated generation of millions of tandem mass spectra on a daily basis. In such a setup, the desire for greater sequence coverage combines with standard experimental procedures to commonly yield multiple tandem mass spectra from overlapping peptides-typical observations include peptides differing by one or two terminal amino acids and spectra from modified and unmodified variants of the same peptides. In a departure from the traditional spectrum identification algorithms that analyze each tandem mass spectrum in isolation, spectral networks define a new computational approach that instead finds and simultaneously interprets sets of spectra from overlapping peptides. In shotgun protein sequencing, spectral networks capitalize on the redundant sequence information in the aligned spectra to deliver the longest and most accurate de novo sequences ever reported for ion trap data. Also, by combining spectra from multiple modified and unmodified variants of the same peptides, spectral networks are able to bypass the dominant guess/confirm approach to the identification of posttranslational modifications and alternatively discover modifications and highly modified peptides directly from experimental data. Open-source implementations of these algorithms may be downloaded from peptide.ucsd.edu.     

Vibrational spectroscopy of biopolymers under mechanical stress: processing cellulose spectra using bandshift difference integrals

Mechanical stretching of covalent bonds, for example when a fibrous polymer is loaded in tension, results in their stretching vibrational bands in the infrared or Raman spectrum being shifted to lower frequency. Conversely stretching a hydrogen bond shifts the stretching vibrational mode of the donor covalent X-H bond to higher frequency. These band shifts are small and difficult to detect in complex regions of the spectrum where differently affected bands overlap. This paper describes a method of integrating the difference spectra (spectrum under tensile strain minus spectrum at zero tensile strain) to recover the shape of the bands that are shifted and the spectral variation in bandshift. The application of this method to two sets of vibrational spectra of cellulose under tension is described. In one example, C-O-C stretching bands of highly crystalline tunicate cellulose were observed to shift to lower frequency under axial strain. In the other example, a group of overlapping O-D stretching bands in partially deuterated cellulose showed varied bandshifts under axial strain, some bandshifts being positive as expected due to extension of axially oriented hydrogen bonds while others were negative. The possibility of constructing spectral plots of bandshift has the potential to clarify the interpretation of overlapped, shifting bands in the vibrational spectra of polymers under tension.     

Blind spectral decomposition of single-cell fluorescence by parallel factor analysis

Simultaneous measurement of multiple signaling molecules is essential to investigate their relations and interactions in living cells. Although a wide variety of fluorescent probes are currently available, the number of probes that can be applied simultaneously is often limited by the overlaps among their fluorescence spectra. We developed the experimental system to measure and analyze many overlapping fluorescent components in single cells. It is based on the recording of two-dimensional single-cell fluorescence spectra and on the blind spectral decomposition of fluorescence data by method of parallel factor analysis. Because this method does not require any preknowledge about the shapes of individual component spectra, it can be applied to the specimens that contain fluorescent components with unknown spectra. By examining the performance using the mixture solutions of fluorescent indicators, it was confirmed that >10 largely overlapping spectral components could be easily separated. The effectiveness in the physiological experiments was proven in the applications to the temporal analysis of intracellular Ca(2+) concentration and pH, as well as the intrinsic fluorescent components, in single mouse oocytes.     

S-state dependent Fourier transform infrared difference spectra for the photosystem II oxygen evolving complex

Vibrational spectroscopy provides a means to investigate molecular interactions within the active site of an enzyme. We have applied difference FTIR spectroscopy coupled with a flash turnover protocol of photosystem II (PSII) to study the oxygen evolving complex (OEC). Our data show two overlapping oscillatory patterns as the sample is flashed through the four-step S-state cycle that produces O(2) from two H(2)O molecules. The first oscillation pattern of the spectra shows a four-flash period four oscillation and reveals a number of new vibrational modes for each S-state transition, indicative of unique structural changes involved in the formation of each S-state. Importantly, the first and second flash difference spectra are reproduced in the 1800-1200 cm(-)(1) spectral region by the fifth and sixth flash difference spectra, respectively. The second oscillation pattern observed is a four-flash, period-two oscillation associated with changes primarily to the amide I and II modes and reports on changes in sign of these modes that alternate 0:0:1:1 during S-state advance. This four-flash, period-two oscillation undergoes sign inversion that alternates during the S(1)-to-S(2) and S(3)-to-S(0) transitions. Underlying this four-flash period two is a small-scale change in protein secondary structure in the PSII complex that is directly related to S-state advance. These oscillation patterns and their relationships with other PSII phenomena are discussed, and future work can initiate more detailed vibrational FTIR studies for the S-state transitions providing spectral assignments and further structural and mechanistic insight into the photosynthetic water oxidation reaction.     

Highly purified microsomal P-450: the oxyferro intermediate stabilized at low temperature.

The oxyferro intermediate of highly purified microsomal P-450 from rabbit liver was formed and stabilized at ?30°C in a mixture of aqueous buffer and glycerol ($\text{1}\text{1}$). Absolute and difference (Fe^2·+O₂-Fe³⁺) spectra of this intermediate appear to be very similar to those obtained under either steady state kinetics or stopped flow conditions on the same cytochrome as well as on bacterial P-450_cam. (Absolute and difference spectra present maxima at 420 and 557–558 nm and a broad maximum at 442 nm respectively). As temperature increases the oxyferro intermediate autoxidizes and ferric cytochrome P-450 is restored. This reaction appears to follow biphasic first order kinetics. The rate constant of both phases decreases with temperature and increases with protons concentrations.