The intracellular pupil mechanism and photoreceptor signal: noise ratios in the fly Lucilia cuprina

The function of the intracellular pupil mechanism is examined by comparing the responses of photoreceptors in normal flies with those from white-eyed flies that lack the pupil. In white-eyed flies the response to an intensity increment of fixed contrast decreases at high background intensities. There is a smaller decrease in noise amplitude so that the signal:noise ratio falls. The intensity dependence of the photoreceptor signal:noise ratio fits a simple model in which activated photopigment molecules compete for 3 X 10(4) transduction units. The signal:noise ratio decreases at high intensities because the transduction units are saturated. This model is supported by a noise analysis, which provides three estimates of the number of events generating photoreceptor responses. In white-eyed flies the event number saturates at high background intensities, suggesting that a maximum of 2 X 10(4) events can be simultaneously active. Wild-type flies do not exhibit saturation effects over the range of intensities studied. The signal:noise ratio rises with intensity to reach a stable asymptote, close to the maximum observed for white-eyed flies. Pupil attenuation is calculated from measurements of signal:noise ratio in white-eyed and wild-type flies. The pupil is progressively activated over a two log unit intensity range and when fully closed attenuates the effective intensity by 99%. The threshold of this pupil effect coincides with the threshold of pupil activation measured optically. We conclude that the intracellular pupil attenuates the light flux to prevent receptor saturation and to extend the range of intensities at which fly photoreceptors operate close to their maximum signal:noise ratio. This upper limit is determined by the number of transduction units generating a cell's response.     

Novel optical solid-state glucose sensor using immobilized glucose oxidase

Meso-tetra(4-carboxyphenyl)porphine (CTPP(4)) binds reversibly to immobilized glucose oxidase (GOD), resulting in an absorbance peak for the CTPP(4)-GOD complex at 427nm. The absorbance intensity of the 427nm peak is reduced upon exposure to glucose, which causes the dissociation of CTPP(4) from GOD. The change in absorbance at 427nm shows linear dependence on glucose concentration from 20 to 200mg/dL (1.1-11.1mM).     

The kinetic relationship between the C-550 absorbance change, the reduction of Q(delta A320) and the variable fluorescence yield change in chloroplasts at room temperature.

The light minus dark difference spectrum and the kinetics of the indicator pigment C-550 have been measured at room temperature in isolate, envelope-free chloroplasts in the presence of 3-(3' ,4'-dichlorophenyl)-1,1-dimethylurea (DCMU). The C-550 spectrum indicates a band shift with peaks at 540 and 550 nm and has an isobestic point at 545 nm. On the assumption of 400 chlorophyll molecules per electron transfer chain the differentaial extinction coefficient delta epsilon (540-550) is calculated to be approximately 5 mM-1 . CM-1. The kinetics of the C-550 absorbance change, occurring upin the onset of continuous illumination, are shown to be biphasic and strictly correlated with the kinetics of the complementary area measured from the fluorescence induction curve under identical cinditions and with those of the absorbance increase at 320 nm due to photoreduction of Q. The lighted-induced change in these three parameters can be described as a function of the variable fluorescence yield change occurring under the same conditions. Such functions are non-linear and reveal a heterogeneous dependence of the variable fluorescence yield on the fraction of closed System II reaction centers. It is concluded that for every molecule of the primary electron acceptor Q of Photosystem II that is photochemically reduced there corresponds an equivalent change in the absorbance of the indicator pigment C-550 and in the size of the complementary area. Ths, C-550 and area are two valid parameters for monitoring the primary photochemical activity of System II at the room temperature.     

Light and dark adaptation of halorhodopsin

Dark incubation of envelope vesicles derived from a strain of Halobacterium halobium that lacks bacteriorhodopsin but contains halorhodopsin and a third rhodopsin-like pigment caused a decrease in the flash yield [the amplitude of a transient absorbance change of flash reactive component(s) by flash] of halorhodopsin but not the rhodopsin-like pigment. The flash yield decreased to reach a low steady level after incubation for about 4 days in the dark. The flash yield of halorhodopsin at any stage of dark incubation was increased by actinic illumination of the vesicles. The flash yield at 490 nm (absorbance increase) was found to be approximately proportional to that at 590 nm (absorbance decrease). These results indicate that halorhodopsin in the envelope vesicles has two forms, dark and light adapted, and that the halorhodopsin phototransient absorbing at 490 nm is originated from the light-adapted form. A difference spectrum between these two forms of halorhodopsin shows that the light-adapted halorhodopsin was red-shifted from the dark-adapted form. The light-induced membrane potential was measured by tetraphenylphosphonium uptake. The uptake by the dark-adapted vesicles was slower than that by the light-adapted vesicles, suggesting that only the light-adapted halorhodopsin has ion-transporting activity.     

The kinetic relationship between the C-550 absorbance change,the reduction of Q(ΔA320) and the variable fluorescence yield change in chloroplasts at room temperature

The light minus dark difference spectrum and the kinetics of the indicator pigment C-550 have been measured at room temperature in isolated, envelopefree chloroplasts in the presence of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea (DCMU). The C-550 spectrum indicates a band shift with peaks at 540 and 550 nm and has an isosbestic point at 545 nm. On the assumption of 400 chlorophyll molecules per electron transfer chain the differential extinction coefficient Δ?(540–550) is calculated to be approximately 5 mM^?1 · cm^?1. The kinetics of the C-550 absorbance change, occurring upon the onset of continuous illumination, are shown to be biphasic and strictly correlated with the kinetics of the complementary area measured from the fluorescence induction curve under identical conditions and with those of the absorbance increase at 320 nm due to photoreduction of Q. The light-induced change in these three parameters can be described as a function of the variable fluorescence yield change occurring under the same conditions. Such functions are non-linear and reveal a heterogeneous dependence of the variable fluorescence yield on the fraction of closed System II reaction centers.It is concluded that for every molecule of the primary electron acceptor Q of Photosystem II that is photochemically reduced there corresponds an equivalent change in the absorbance of the indicator pigment C-550 and in the size of the complementary area. Thus, C-550 and area are two valid parameters for monitoring the primary photochemical activity of System II at room temperature.     

Spectrophotometric detection of pentachlorophenol (PCP) in water using immobilized and water-soluble porphyrins

The spectrophotometric properties of porphyrins are altered upon interaction with chlorophenols and other organochlorine pollutants. Meso-tetra(4-sulfonatophenyl)porphyrin (TPPS), zinc meso-tetra(4-sulfonato phenyl)porphyrin (Zn-TPPS), monosulfonate-tetraphenylporphyrin (TPPS1), meso-tri(4-sulfonatophenyl)mono(4-carboxyphenyl)porphyrin (C1TPP), meso-tetra(4-carboxyphenyl)porphyrin (C4TPP), and copper meso-tetra(4-carboxyphenyl)porphyrin (Cu-C4TPP) in solution exhibit a broad absorbance in the range 400-450 nm Soret region. The interaction of the above mentioned porphyrins in solution with pentachlorophenol (PCP) induces a red shift in the Soret spectrum with absorbance losses at 413, 418, 403, 405, 407, and 404 nm, respectively, and the appearance of new peaks at 421, 427, 431, 416, 417, and 416 nm, respectively. The intensity of the Soret spectral change is proportional to the pentachlorophenol concentration with a detection limit of 1, 0.5, 1.16, 1, 0.5, and 0.5 ppb, respectively. The interaction of (C4TPP) and (Cu-C4TPP) in solution with PCP shows to concentration dependent for concentrations less than 4 ppb the dependence was log-linear. However, for concentrations greater than 4 ppb the relation was linear. Monosulfonate-tetraphenylporphyrin immobilized as a monolayer on a Kimwipe tissue exhibits an absorbance peak in the Soret region at 422 nm. The interaction of the porphyrin with PCP induces a red shift in the Soret spectrum with absorbance loss at 419 nm and the appearance of new peaks at 446 nm. The intensity of the Soret spectral change is proportional to the log of PCP concentration. The detection limit with immobilized TPPS1 for PCP is 0.5 ppb. These results suggest the potential for development of spectrophotometric chemosensor for PCP residues in water with detection limits less than US EPA maximum contaminate level (MCL) of 1 ppb. The immobilized TPPS1 on the Kimwipe will make it possible to develop a wiping sensors to monitor the PCP or other pesticides residues on the vegetables or wood products.     

Characterization of a Rhodobacter capsulatus reaction center mutant that enhances the distinction between spectral forms of the initial electron donor

A large scale mutation of the Rhodobacter capsulatus reaction center M-subunit gene, sym2-1, has been constructed in which amino acid residues M205-M210 have been changed to the corresponding L subunit amino acids. Two interconvertable spectral forms of the initial electron donor are observed in isolated reaction centers from this mutant. Which conformation dominates depends on ionic strength, the nature of the detergent used, and the temperature. Reaction centers from this mutant have a ground-state absorbance spectrum that is very similar to wild-type when measured immediately after purification in the presence of high salt. However, upon subsequent dialysis against a low ionic strength buffer or the addition of positively charged detergents, the near-infrared spectral band of P (the initial electron donor) in sym2-1 reaction centers is shifted by over 30 nm to the blue, from 852 to 820 nm. Systematically varying either the ionic strength or the amount of charged detergent reveals an isobestic point in the absorbance spectrum at 845 nm. The wild-type spectrum also shifts with ionic strength or detergent with an isobestic point at 860 nm. The large spectral separation between the two dominant conformational forms of the sym2-1 reaction center makes detailed measurements of each state possible. Both of the spectral forms of P bleach in the presence of light. Electrochemical measurements of the P/P+ midpoint potential of sym2-1 reaction centers show an increase of about 30 mV upon conversion from the long-wavelength form to the short-wavelength form of the mutant. The rate constant of initial electron transfer in both forms of the mutant reaction centers is essentially the same, suggesting that the spectral characteristics of P are not critical for charge separation. The short-wavelength form of P in this mutant also converts to the long-wavelength form as a function of temperature between room temperature and 130 K, again giving rise to an isobestic point, in this case at 838 nm for the mutant. A similar, though considerably less pronounced spectral change with temperature occurs in wild-type reaction centers, with an isobestic point at about 855 nm, close to that found by titrating with ionic strength or detergent. Fitting the temperature dependence of the sym2-1 reaction center spectrum to a thermodynamic model resulted in a value for the enthalpy of the conformational interconversion between the short- and long-wavelength forms of about -6 kJ/mol and an entropy of interconversion of about -35 J/(K mol). Similar values of enthapy and entropy changes can be used to model the temperature dependence in wild-type. Thus, much of the temperature dependence of the reaction center special pair near-infrared absorbance band can be described as an equilibrium shift between two spectrally distinct conformations of the reaction center.     

Intracellular calcium changes in Balanus photoreceptor. A study with calcium ion-selective electrodes and Arsenazo III

Intracellular Ca2+ concentration (Cai) in the dark and during light stimulation, was measured in Balanus photoreceptors with Ca2+ ion-selective electrodes (Ca-ISE) and Arsenazo III absorbance changes (AIII). The average basal Cai of 17 photoreceptors in darkness was 300 +/- 160 nM determined with liquid ion-exchanger (t-HDOPP) Ca-ISE. Ca-ISE measurements indicated that light increased Cai by 700 nM (average), whereas AIII indicated an average change of 450 nM. The time course of AIII absorbance changes matched the time course of changes in the receptor potential more closely than did the Ca-ISE. Changes in Cai were graded with light intensity but the change in Cai was much greater for a decade change in intensity at high light intensity than at low intensity. The peak light induced conductance change of voltage clamped cells had a relationship to light intensity similar to that of the change in Cai. The peak Cai level measured with Ca-ISE was in good agreement with the free Ca2+ concentration of injected buffer solutions. Control Cai levels were usually restored within 5 min following injection of Ca2+ buffers. Injection of Ca2+ buffers with free Ca2+ of 0.6 microM produced a membrane depolarization. Larger increases in Cai (greater than microM) produced by injection of CaCl2 or release of Ca2+ from injected buffers by acidifying the cell, produced a pronounced membrane hyperpolarization. Increasing Cai with all of these techniques reduced the amplitude of the receptor potential. The time course of the receptor potential recovery was usually similar to that of Cai recovery.     

Adapting-bump model for eccentric cells of Limulus

Light-evoked intracellular voltage noise records have been obtained from Limulus eccentric cells, from threshold light intensity to an intensity .10(5) times threshold. These data are analyzed in terms of a simple "adapting-bump" noise model. It is shown how the model yields a data reduction procedure that slightly generalizes the familiar use of Campbell's theorem for Poisson shot noise: the correlative effect of adaptation amends Campbell's theorem by a single multiplicative factor, which may be estimated directly from the power spectrum of the noise data. The model also permits direct estimation of the bump shape from the power spectrum. The bump shape estimated from noise at dim light is in excellent agreement with the average shape of bumps observed directly in the dark. The data yield a bump rate that is linear with light up through about 50 times threshold intensity but that falls short of linearity by a factor of 35 at the brightest light. The bump height decreases as the -0.4 power of light intensity across the entire range. Bump duration decreases by a factor of 2 across the entire range, and the adaptation correlation factor descends from unity to about one-third. The modest change of the adaptation correlation shows that naive application of Campbell's theorem to such data is adequate for rough estimation of the model's physiological parameters. This simple accounting for all the data gives support to the adapting-bump model.     

Action spectra of the light-growth response of Phycomyces

The light-growth response of Phycomyces blakesleeanus (Burgeff) is a transient change in elongation rate of the sporangiophore caused by a change in light intensity. Previous investigators have found that the light-growth response has many features in common with phototropism; the major difference is that only the light-growth response is adaptive. In order to better understand the light-growth response and its relationship to phototropism, we have developed a novel experimental protocol for determining light-growth-response action spectra and have examined the effect of the reference wavelength and intensity on the shape of the action spectrum. The null-point action spectrum obtained with broadband-blue reference light has a small peak near 400 nm, a flat region from 430 nm to 470 nm, and an approximately linear decline in the logarithm of relative effectiveness above 490 nm. The shape of the action spectrum is different when 450-nm reference light is used, as has been shown previously for the phototropic-balance action spectrum. However, the action spectrum of the light-growth response differs from that for phototropic balance, even when the same reference light (450 nm) is used. Moreover, for the light-growth response, the relative effectiveness of 383-nm light decreases as the intensity of the 450-nm reference light increases; this trend is the opposite of that previously found for phototropic balance. The dependence of the lightgrowth-response action spectrum on the reference wavelength, its difference from the phototropic-balance action spectrum, and the reference-intensity dependence of the relative effectiveness at 383 nm may be attributable to dichroic effects of the oriented photoreceptor(s), and to transduction processes that are unique to the light-growth response.I dedicated to Masaki Furuya on the occasion of his 65th birthdayThis work was supported by a grant from the National Institutes of Health (GM29707) to E.D. Lipson. Anuradha Palit, Promod Pratap, and Benjamin Horwitz participated in the early phases of this work. We thank Leonid Fukshansky and Benjamin Horwitz for helpful discussions, David Durant for computer programming, and Steven Block for providing us with a C-language program of Reinsch's procedure for cubic spline interpolation. One of us (R.S.) gratefully acknowledges a junior faculty fellowship leave from the Department of Physics at Yale University.     

Spectral effects of the pupil in fly photoreceptors

Summary Photoreceptors of flies contain pigment granules which upon illumination of the receptors migrate towards the rhabdomere and act as a longitudinal pupil. Data in the literature concerning the effect of the pupil on the spectral sensitivity are contradictory. Therefore spectral sensitivity ofMusca photoreceptors upon light adaptation was reinvestigated.The change in spectral sensitivity of fly photoreceptors upon light adaptation as measured by Hardie (1979) was confirmed. Taking into account waveguide optics this change was explained from absorbance spectra of pupillary granules, measured by microspectrophotometry in squash preparations. Furthermore the pupil absorbance spectrum determined in vivo (Stavenga et al. 1973) was interpreted. The absence of a change in spectral sensitivity upon light adaptation measured by pupillary reflexion (Bernard and Stavenga 1979) is explained by a local-triggering of the pupil.     

Le contrôle automatique du flux lumineux dans l'oeil composé des Diptères

In the compound eye of the fly Musca, tiny pigment granules move within the cytoplasm of receptor cells Nos. 1–6 and cluster along the wall of the rhabdomeres under light adaptation, thus attenuating the light flux to which the visual pigment is exposed (Kirschfeld and Franceschini, 1969). Two recently developed optical methods (the neutralization of the cornea and the deep pseudopupil) combined with antidromic and orthodromic illumination of the eye (Fig. 1) make it possible to analyse the properties of the mechanism at the level of the single cell, in live and intact insects (Drosophila and Musca). The mechanism is shown to be an efficient attenuator in the spectral range (blue-green) where cells Nos. 1–6 have been reported to be maximally sensitive (Figs. 4c and d, 5b and 11b). In spite of the fact that the granules do not penetrate into the rhabdomere, the attenuation spectrum they bring about closely matches the absorption spectrum of the substance of which they are composed (ommochrome pigment, dotted curve in Fig. 11b). The dramatic increase in reflectance of the receptors after light adaptation (Figs. 3, 4b, 5a and 11a) can be explained as a mere by-product of the high absorption index of the ommochrome pigment, especially if one takes into account the phenomenon of anomalous dispersion (Chapter 8). The vivid green or yellow colour of the rhabdomeres would thus have a physical origin comparable to a metallic glint. Contrasting with the lens eye in which the pupillary mechanism is a common attenuator for both receptor types (rods and cones), the compound eye of higher Diptera is equiped with two types of pupils adapted respectively to both visual subsystems. A scotopic pupil is present in each of the six cells (Nos. 1–6) whose signals are gathered in a common cartridge of the first optic ganglion. This pupil comes into play at a moderate luminance (0,3 cd/m² in Drosophila; 3 to 10 cd/m² in Musca. Figs 13, 14, 15, 16). A photopic pupil is present in the central cell No. 7 whose signal reaches one column of the second optic ganglion. Attenuating the light flux for both central cells 7 and 8, the photopic pupil has its threshold about two decades higher than the scotopic pupil, just at the point where the latter reaches saturation (Fig. 3b, e-State II of Figs. 6b and 15). The photopic pupil itself saturates at a luminance one to two decades higher still (Fig. 3c, f=State III of Figs. 6c and 15). The two-decades-shift in threshold of these pupil-mechanisms supports the view that receptors 1–6 are a scotopic subsystem, receptors 7 and 8 a photopic subsystem of the dipteran eye. The luminance-threshold of the scotopic pupil (as determined with the apparatus described in Fig. 2) appears to be located at least 3.5 decades (Drosophila) or even 5 decades (Musca) higher than the absolute threshold of movement perception (Fig. 16). After a long period (1 hr) of darkness a light step of high intensity can close the scotopic pupil within about 10 sec (time constant 2 sec as in Fig. 9) and the photopic pupil within no less than 30–60 sec. Some mutants of Drosophila possess only a scotopic pupil (w , Figs. 4 and 5) whereas ommochrome deficient mutants lack both types of pupil (v, cn, see Fig. 7c, d). Comparable reflectance changes, accomplished within about 60 sec of light adaptation, are described for two insects having fused rhabdomes: the bee and the locust (Fig. 17).     

A stopped-flow study of the reaction between mercuric reductase and NADPH

The reaction of the FAD-containing enzyme, mercuric reductase, with NADPH has been studied by stopped-flow kinetic methods at 25 degrees C, pH 7.3. The results suggest that the reaction involves at least three steps. The first step is very rapid and is essentially complete within the dead time of the stopped-flow apparatus. This step is associated with decreasing absorbances at 340 nm (NADPH) and 455 nm (FAD), whereas there is little formation of the absorbance at 530 nm characterizing 2-electron-reduced enzyme subunits (EH2). The second step involves an increase of the absorbance at 530 nm. The third step results in an increase of the intensity of the long-wavelength band and a change of its shape. A second equivalent of NADPH per FAD is required for this step. It is proposed that the product is an EH2-NADPH complex. In addition to these rapid steps, slow absorbance changes are also observed.     

Optical solid-state detection of organophosphates using organophosphorus hydrolase

We have developed a sensor surface for optical detection of organophosphates based on reversible inhibition of organophosphorus hydrolase (OPH) by copper complexed meso-tri(4-sulfonato phenyl) mono(4-carboxy phenyl) porphyrin (CuC1TPP). OPH immobilized onto glass microscope slides retains catalytic activity for more than 232 days. CuC1TPP is a reversible, competitive inhibitor of OPH, binding at the active site of the immobilized enzyme. The absorbance spectrum of the porphyrin-enzyme complex is measured via planar waveguide evanescent wave absorbance spectroscopy using a blue LED as a light source and an Ocean Optics USB2000 as the spectrophotometer. The characteristics of the absorbance spectrum of CuC1TPP are specific and different when the porphyrin is bound to the enzyme or is bound non-specifically to the surface of the slide. Addition of a substrate of OPH such as one of the organophosphates paraoxon, coumaphos, diazinon, or malathion displaces the porphyrin from the enzyme resulting in reduced absorbance intensity at 412 nm. Absorbance changes at 412 nm show log-linear dependence on substrate concentration. Paraoxon concentrations between 7 parts per trillion (ppt) and 14 parts per million (ppm) were investigated and a 3:1 S/N detection limit of 7 ppt was determined. Concentrations of 700 ppt to 40 ppm were investigated for diazinon, malathion, and coumaphos with detection limits of 800 ppt, 1 part per billion, and 250 ppt, respectively. This optical technique does not require the addition of reagents or solutions other than the sample and absorbance spectra can be collected in less than 6 s.     

Diffuse reflectance spectroscopy of fibrous proteins

UV-visible diffuse reflectance (DR) spectra of the fibrous proteins wool and feather keratin, silk fibroin and bovine skin collagen are presented. Natural wool contains much higher levels of visible chromophores across the whole visible range (700-400?nm) than the other proteins and only those above 450?nm are effectively removed by bleaching. Both oxidative and reductive bleaching are inefficient for removing yellow chromophores (450-400?nm absorbers) from wool. The DR spectra of the four UV-absorbing amino acids tryptophan, tyrosine, cystine and phenylalanine were recorded as finely ground powders. In contrast to their UV-visible spectra in aqueous solution where tryptophan and tyrosine are the major UV absorbing species, surprisingly the disulphide chromophore of solid cystine has the strongest UV absorbance measured using the DR remission function F(R)(∞). The DR spectra of unpigmented feather and wool keratin appear to be dominated by cystine absorption near 290?nm, whereas silk fibroin appears similar to tyrosine. Because cystine has a flat reflectance spectrum in the visible region from 700 to 400?nm and the powder therefore appears white, cystine absorption does not contribute to the cream colour of wool despite the high concentration of cystine residues near the cuticle surface. The disulphide absorption of solid L: -cystine in the DR spectrum at 290?nm is significantly red shifted by ~40?nm relative to its wavelength in solution, whereas homocystine and lipoic acid showed smaller red shifts of 20?nm. The large red shift observed for cystine and the large difference in intensity of absorption in its UV-visible and DR spectra may be due to differences in the dihedral angle between the crystalline solid and the solvated molecules in solution.     

Potential of phenothiazine as a thin film dosimeter for UVA exposures.

The research reported in this paper on the changes in absorbance and the calibration of a proposed UVA (320-400 nm) dosimeter have established the phenothiazine-mylar combination as a potential UVA dosimeter for population studies of UVA exposures. The change in optical absorbance at 370 nm was employed to quantify the UVA exposures. This change starts to saturate at a change in absorbance of approximately 0.3. This relates to solar UVA exposures at a sub-tropical site on a horizontal plane of approximately three to four hours. The shape of this calibration curve varies with the season. This can be overcome in the same manner as for polysulfone where the dosimeter is calibrated for the conditions that it will be employed to measure the UVA exposures.     

The light-induced carotenoid absorbance changes in Rhodopseudomonas sphaeroides: an analysis and interpretation of the band shifts.

An analysis has been made of the spectrum of the carotenoid absorption band shift generated by continuous illumination of chromatophores of the GlC-mutant of Rhodopseudomonas sphaeroides at room temperature by means of three computer programs. There appears to be at least two pools of the same carotenoid, only one of which, comprising about 20% of the total carotenoid content, is responsible for the light-induced absorbance changes. The 'remaining' pool absorbs at wavelengths which were about 5 nm lower than those at which the 'changing' pool absorbs. This difference in absorption wavelength could indicate that the two pools are influenced differently by permanent local electric fields. The electrochromic origin of the absorbance changes has been demonstrated directly; the isosbestic points of the absorption difference spectrum move to shorter wavelengths upon lowering of the light-induced electric field. Band shifts up to 1.7 nm were observed. A comparison of the light-induced absorbance changes with a KCl-valinomycin-induced diffusion potential has been used to calibrate the electrochromic shifts. The calibration value appeared to be 137 +/- 6 mV per nm shift.     

Plumage reflectance is not affected by preen wax composition in red knots Calidris canutus

It has recently been shown that sandpipers (Scolopacidae) abruptly switch the chemical composition of their preen gland secretions from mono- to diester waxes just before the period of courtship. The timing and context of the shift suggested that diesters could provide a visible quality signal during mate choice. We used captive red knots Calidris canutus to test whether mono- and diester preen waxes affect the light reflectance ("colour") of the plumage. We also determined light absorbance spectra of the two wax types. The reflectance of breast feathers of the breeding plumage was measured with spectrophotometry when birds secreted monoesters and six weeks later when they secreted diester preen waxes. Light reflectance was also measured after removing the mono- and diester waxes from the plumage with a solvent. The results show that: (1) diester preen waxes absorb more light, especially ultraviolet (UV), than monoester preen waxes, but that (2) the compositional shift in the preen waxes did not change plumage reflectance and, (3) the removal of preen waxes did not change the reflectance of the plumage within the light spectrum assumed visible to birds (320–700 nm). This is not consistent with the idea that compositional shifts in the preen waxes of red knots have a visual function.     

Characterization of reductant-induced, tryptophan fluorescence changes in cytochrome oxidase

We have measured the steady-state tryptophan fluorescence spectrum of cytochrome oxidase in its oxidized and fully reduced states. Reduction of the oxidized enzyme by sodium dithionite causes an apparent shift in the fluorescence emission maximum from 328 nm, in the oxidized enzyme, to 348 nm, in the reduced enzyme. This spectroscopic change has been observed previously and assigned to a redox-linked, conformational change in cytochrome oxidase [Copeland, R. A., Smith, P. A., & Chan, S. I. (1987) Biochemistry 26, 7311-7316]. When dithionite-reduced enzyme sits in an open cuvette, the enzyme returns to the oxidized state, and the fluorescence maximum shifts back to 328 nm. However, the time course of the fluorescence change does not follow the redox state of the enzyme, monitored spectrophotometrically at 445,605, and 820 nm, but follows the disappearance of dithionite, which absorbs at 315 nm. Moreover, when the fluorescence emission spectrum of the dithionite-reduced enzyme is corrected for the absorbance due to dithionite, the fluorescence maximum is found 2 nm blue shifted, relative to that of the oxidized enzyme, at 326 nm. This dithionite-induced, red-shifted steady-state tryptophan fluorescence is also seen with the non-heme-containing enzyme carboxypeptidase A. The tryptophan emission spectrum of untreated carboxypeptidase A is at 332 nm, whereas in the presence of dithionite the emission spectrum of carboxypeptidase A is at 350 nm. When corrected for the absorbance of dithionite, the tryptophan emission maximum is at 332 nm. We have also used the photoreductant 3,10-dimethyl-5-deazaisoalloxazine (deazaflavin) to reduce cytochrome oxidase.(ABSTRACT TRUNCATED AT 250 WORDS)     

Conformational change of the heme moiety of the ferrous cytochrome P-450scc-phenyl isocyanide complex upon binding of reduced adrenodoxin

Reduction of cytochrome P-450scc(SF) (SF, substrate free) purified from bovine adrenocortical mitochondria with sodium dithionite (Na2S2O4) or with beta-NADPH mediated by catalytic amounts of adrenodoxin and adrenodoxin reductase in the presence of phenyl isocyanide produced a ferrous cytochrome P-450scc(SF)-phenyl isocyanide complex with Soret absorbance maximum at 455 nm having a shoulder at 425 nm. On the other hand, when a preformed cytochrome P-450scc(SF)-adrenodoxin complex was reduced chemically or enzymatically under the same conditions, the absorbance spectrum showed drastic changes, i.e., an increase in intensity at 425 nm and a concomitant decrease in intensity at 455 nm. Similar spectral changes could be produced by addition of the same amount of reduced adrenodoxin afterward to the ferrous cytochrome P-450scc(SF)-phenyl isocyanide complex. Titration experiments with adrenodoxin showed that (1) a 1:1 stoichiometric saturation of the spectral change was obtained for both the absorbance increase at 425 nm and the absorbance decrease at 455 nm, (2) there was no spectral change in the presence of 0.35 M NaCl, and (3) there was no spectral change for cytochrome P-450scc(SF) whose Lys residue(s) essential to the interaction with adrenodoxin had been covalently modified with PLP. These results suggest that ternary complex formation of ferrous cytochrome P-450scc(SF)-phenyl isocyanide with reduced adrenodoxin caused a conformational change around the ferrous heme moiety. By analysis of temperature and pH dependencies of the spectral change of the ternary complex, it was suggested that this conformational change may reflect the essential step for electron transfer from reduced adrenodoxin to the ferrous-dioxygen complex of cytochrome P-450scc.