A study on the energy-dependent quenching of chlorophyll fluorescence by means of photoacoustic measurements

The mechanism of energy-dependent quenching (q_E) of chlorophyll fluorescence was studied employing photoacoustic measurements of oxygen evolution and heat release. It is shown that concomitant to the formation of q_E the yield of open reaction centers _p decreases indicating that q_E quenching originates from a process being competitive to fluorescence as well as to photochemistry. The analysis of heat release (rate of thermal deactivation) shows: 1. The competitive process is not given by a still unknown energy storing process. 2. If the competitive process would be a futile cycle the life-times of the involved intermediates had to be faster than 50 s.The results of the photoacoustic measurements are in line with the idea that q_E quenching originates from an increased probability of thermal deactivation of excited chlorophylls.Abbreviations F actual fluorescence - F_m fluorescence yield with all PS II reaction centers closed in a light adapted state - F₀ fluorescence yield with all PS II reaction centers open in a light adapted state - PS Photosystem - _p intrinsic photochemical yield - q_E energy-dependent quenching - q_I photoinhibition quenching - q_N non-photochemical quenching - q_P photochemical quenching - q_T state transition quenching     

Xanthophyll cycle and energy-dependent fluorescence quenching in leaves from pea plants grown under intermittent light

The possible role of zeaxanthin formation and antenna proteins in energy-dependent chlorophyll fluorescence quenching (qE) has been investigated. Intermittent-light-grown pea (Pisum sativum L.) plants that lack most of the chlorophyll a/b antenna proteins exhibited a significantly reduced qE upon illumination with respect to control plants. On the other hand, the violaxanthin content related to the number of reaction centers and to xanthophyll cycle activity, i.e. the conversion of violaxanthin into zeaxanthin, was found to be increased in the antenna-protein-depleted plants. Western blot analyses indicated that, with the exception of CP 26, the content of all chlorophyll a/b-binding proteins in these plants is reduced to less than 10% of control values. The results indicate that chlorophyll a/b-binding antenna proteins are involved in the energy-dependent fluorescence quenching but that only a part of qE can be attributed to quenching by chlorophyll a/b-binding proteins. It seems very unlikely that xanthophylls are exclusively responsible for the qE mechanism.Abbreviations CAB chlorophyll a/b-binding - Chl chlorophyll - F_V variable fluorescence - IML intermittent light - LHC light harvesting complex - PFD photon flux density - qP photochemical quenching of chlorophyll fluoresence - qN non-photochemical quenching - qE energy-dependent quenching - qI photoinhibitory quenching - qT quenching by state transition     

Action potential in a plant cell lowers the light requirement for non-photochemical energy-dependent quenching of chlorophyll fluorescence

This study deals with effects of membrane excitation on photosynthesis and cell protection against excessive light, manifested in non-photochemical quenching (NPQ). In Chara corallina cells, NPQ and pericellular pH displayed coordinated spatial patterns along the length of the cell. The NPQ values were lower in H(+)-extruding cell regions (external pH approximately 6.5) than in high pH regions (pH approximately 9.5). Generation of an action potential by applying a pulse of electric current caused NPQ to increase within 30-60 s. This effect, manifested as a long-lived drop of maximum chlorophyll fluorescence (F(m)'), occurred at lower photosynthetic flux densities (PFD) in the alkaline as compared to acidic cell regions. The light response curve of NPQ shifted, after generation of an action potential, towards lower PFD. The release of NPQ by nigericin and the rapid reversal of action potential-triggered NPQ in darkness indicate its relation to thylakoid DeltapH. Generation of an action potential shortly after darkening converted the chloroplasts into a latent state with the F(m) identical to that of unexcited cells. This state transformed to the quenched state after turning on weak light that was insufficient for NPQ prior to membrane excitation of the cells. The ionophore, A23187, shifted NPQ plots similarly to the action potential effect, consistent with a likely role of a rise in the cytosolic Ca(2+) level in the action potential-induced quenching. The results suggest that a rapid electric signal, across the plasma membrane, might exert long-lived effects on photosynthesis and chlorophyll fluorescence through ion flux-mediated pathways.     

Action potential in a plant cell lowers the light requirement for non-photochemical energy-dependent quenching of chlorophyll fluorescence

This study deals with effects of membrane excitation on photosynthesis and cell protection against excessive light, manifested in non-photochemical quenching (NPQ). In Chara corallina cells, NPQ and pericellular pH displayed coordinated spatial patterns along the length of the cell. The NPQ values were lower in H⁺-extruding cell regions (external pH ∼ 6.5) than in high pH regions (pH ∼ 9.5). Generation of an action potential by applying a pulse of electric current caused NPQ to increase within 30-60 s. This effect, manifested as a long-lived drop of maximum chlorophyll fluorescence (F_m′), occurred at lower photosynthetic flux densities (PFD) in the alkaline as compared to acidic cell regions. The light response curve of NPQ shifted, after generation of an action potential, towards lower PFD. The release of NPQ by nigericin and the rapid reversal of action potential-triggered NPQ in darkness indicate its relation to thylakoid ΔpH. Generation of an action potential shortly after darkening converted the chloroplasts into a latent state with the F_m identical to that of unexcited cells. This state transformed to the quenched state after turning on weak light that was insufficient for NPQ prior to membrane excitation of the cells. The ionophore, A23187, shifted NPQ plots similarly to the action potential effect, consistent with a likely role of a rise in the cytosolic Ca²⁺ level in the action potential-induced quenching. The results suggest that a rapid electric signal, across the plasma membrane, might exert long-lived effects on photosynthesis and chlorophyll fluorescence through ion flux-mediated pathways.     

Tryptophan at position 181 of the D2 protein of photosystem II confers quenching of variable fluorescence of chlorophyll: implications for the mechanism of energy-dependent quenching.

The lumenal CD loop region of the D2 protein of photosystem II contains residues that interact with a reaction center chlorophyll and the redox-active Tyr(D). Using combinatorial mutagenesis, photoautotrophic mutants of Synechocystis sp. PCC 6803 have been generated with multiple amino acid changes in this region. The CD loop mutations were transferred into a photosystem I-less Synechocystis strain to facilitate characterization of photosystem II properties in the mutants. Most of the combinatorial photosystem I-less mutants obtained had a high yield of variable fluorescence, F(V). However, in three mutants, which shared a replacement of Phe181 by Trp, the F(V) yield was dramatically reduced although a high rate of oxygen evolution was maintained. A site-directed F181W D2 mutant shared similar properties. Picosecond time-resolved fluorescence measurements revealed that in the combinatorial F181W mutants the fluorescence lifetimes in closed and open photosystem II centers were essentially identical and were similar to the fluorescence lifetime in open centers of the control strain. These results are explained by quenching of variable fluorescence in the mutants by charge separation between Trp181 and excited reaction center chlorophyll. This reaction competes efficiently with fluorescence and nonradiative decay in closed photosystem II centers, where the lifetime of the excitation in the chlorophyll antenna is long. Thermodynamic considerations favor the formation of oxidized tryptophan and reduced chlorophyll in the quenching reaction, presumably followed by charge recombination. A possible role of tryptophan-chlorophyll charge separation in the mechanism of energy-dependent quenching of excitations in photosynthesis is discussed.     

Properties of energy-dependent calcium transport by rat liver microsomal fraction as revealed by initial-rate measurements.

Measurements of the initial rate of Ca2+ transport by rat liver microsomal preparations reveal the existence of two phases of transport activity. The first, a phase of rapid transport, is complete by 3-5 min, at which time the second (slower) phase begins; this remains linear for up to at least 40 min. The initial phase is minimal in the absence of MgATP. The initial rate of Ca2+ transport reaches values as high as 25 nmol/min per mg of protein; the Km for Ca2+total is 1-2 micrometer and that for MgATPtotal about 500 micrometer. Ruthenium Red (3-5 nmol/mg of protein) has little effect on the initial rate of transport, whereas tributylin (2 micrometer) inhibits equally in a KC1- or a KNO3-containing medium. Compunds that collapse components of the proton electrochemical gradient in mitochondria (valinomycin and carbonyl cyanide m-chlorophenylhydrazone) each inhibit by 70-80% the initial rate of microsomal Ca2+ transport.     

Effect of concentration quenching on fluorescence recovery after photobleaching measurements.

Standard analysis of fluorescence recovery after photobleaching (FRAP) data is valid only if the quantum yield of unphotobleached fluorophores is independent of concentration, yet close molecular packing in two-dimensional systems may lead to significant fluorescence concentration quenching. Using total internal reflection fluorescence, we quantified the surface concentration dependence of the relative quantum yield of fluorescein isothiocyanate-labeled proteins adsorbed to polymeric surfaces before performing measurements of fluorescence recovery after pattern photobleaching. Adsorbed layers of FITC-labeled ribonuclease A displayed significant concentration quenching, and thus the standard FRAP analysis method was unacceptable. We present an extended FRAP analysis procedure that accounts for the changing quantum yield of diffusing fluorophores in systems that are influenced by concentration quenching. The extended analysis shows that if concentration quenching conditions prevail, there may be significant error in the transport parameters obtained from FRAP measurements by using the standard procedures.     

Chlorpheniramine binding to human serum albumin by fluorescence quenching measurements.

The binding of chlorpheniramine to human serum albumin has been studied by fluorescence quenching, as a function of temperature; the experimental data could only be fitted to the Stern-Volmer modified equation. A statistical analysis of the results was performed in order to determine the significance of the constants calculated by this equation, as well as their thermodynamic parameters. The chlorpheniramine binding to human serum albumin accounts for almost half of the binding of this antihistaminic agent to human plasma proteins.     

Investigation of conformational changes in yeast enolase using dynamic fluorescence and steady-state quenching measurements

Conformational changes in yeast enolase were investigated using steady state quenching and dynamic (fluorescence decay and fluorescence anisotropy decay) measurements. The tryptophan fluorescence rotational correlation time increases from 24 to 38 ns on subunit association. The acrylamide quenching constant decreases two-fold when the subunits associate. The conformational metal ion effect suggests a more compact molecule. Under conditions of catalysis, the correlation time decreases 25%, though the sedimentation constant does not change (Holleman, 1973). The enzyme may undergo a hinge-bending motion during catalysis.     

Evidence for energy-dependent change in phosphate binding for mitochondrial oxidative phosphorylation based on measurements of medium and intermediate phosphate-water exchanges.

Characteristics of the exchange reactions catalyzed by beef heart submitochondrial particles give new insight into energy transducing steps of oxidative phosphorylation. The uncoupler-insensitive portion of the total Pi in equilibrium HOH exchange in presence of ATP, ADP, and Pi is the intermediate Pi in equilibrium HOH exchange, that is the exchange occurring with Pi formed by hydrolysis of ATP prior to release of Pi from the catalytic site. The exchange of medium Pi with HOH is as sensitive to uncouplers as the Pi in equilibrium ATP exchange and net oxidative phosphorylation, demonstrating a requirement of an uncoupler-sensitive energized state, probably a transmembrane potential or proton gradient, for bringing medium Pi to the reactive state. The covalent bond forming and breaking step at the catalytic site (ADP + Pi in equilibrium ATP + HOH) appears relatively insensitive to uncouplers. Thus to the extent that uncouplers dissipate transmembrane proton-motive force, it is unlikely that such a force is used to drive ATP formation by direct protonations of Pi oxygens. When only Pi and ADP are added and formation of ATP from added ADP by adenylate kinase and subsequent ATP hydrolysis are adequately blocked, no Pi in equilibrium HOH exchange can be observed, demonstrating a requirement of energization by ATP binding and cleavage for such an exchange. This uncoupler-insensitive energization is suggested to represent a conformationally energized state that can be used reversibly to develop a transmembrane protonmotive force accompanying ADP and Pi release. Rates of various exchanges as estimated by improved procedures are compatible with all oxygen exchanges occurring by dynamic reversal of ATP hydrolysis at the catalytic site.     

PO2 measurements in the microcirculation using phosphorescence quenching microscopy at high magnification

In phosphorescence quenching microscopy (PQM), the multiple excitation of a reference volume produces the integration of oxygen consumption artifacts caused by individual flashes. We analyzed the performance of two types of PQM instruments to explain reported data on Po2 in the microcirculation. The combination of a large excitation area (LEA) and high flash rate produces a large oxygen photoconsumption artifact manifested differently in stationary and flowing fluids. A LEA instrument strongly depresses Po2 in a motionless tissue, but less in flowing blood, creating an apparent transmural Po2 drop in arterioles. The proposed model explains the mechanisms responsible for producing apparent transmural and longitudinal Po2 gradients in arterioles, a Po2 rise in venules, a hypothetical high respiration rate in the arteriolar wall and mesenteric tissue, a low Po2 in lymphatic microvessels, and both low and uniform tissue Po2. This alternative explanation for reported paradoxical results of Po2 distribution in the microcirculation obviates the need to revise the dominant role of capillaries in oxygen transport to tissue. Finding a way to eliminate the photoconsumption artifact is crucial for accurate microscopic oxygen measurements in microvascular networks and tissue. The PQM technique that employs a small excitation area (SEA) together with a low flash rate was specially designed to avoid accumulated oxygen photoconsumption in flowing blood and lymph. The related scanning SEA instrument provides artifact-free Po2 measurements in stationary tissue and motionless fluids. Thus the SEA technique significantly improves the accuracy of microscopic Po2 measurements in the microcirculation using the PQM.     

The fluorescence quenching resolved spectra and red-edge excitation fluorescence measurements of human alpha 1-proteinase inhibitor

The human alpha 1-proteinase inhibitor (alpha 1-PI) and its reactive site modified form (alpha 1-PI*) have been examined using the fluorescence quenching resolved spectra method. The red-edge excitation measurements were applied for the study of structural differences between these forms. The crystallographic data of alpha 1-PI* structure have shown that its polypeptide chain includes only two tryptophan residues. The fluorescence quenching data have indicated that the conversion of the intact inhibitor molecule into its nicked form is accompanied by changes in the tryptophan environments. The red-edge excitation measurements have proved that the dipolar relaxation process around the Trp-194 residue is much bigger in alpha 1-PI* form than in the nicked one.     

Recovery of radial PO(2) profiles from phosphorescence quenching measurements in microvessels

Work by previous investigators has indicated that a substantial amount of oxygen diffuses from the precapillary circulation. These losses imply that there should be radial gradients of oxygen tension (PO(2)) in arterioles, leading to a non-uniform distribution of oxygen within these microvessels. We have employed the phosphorescence quenching method to measure oxygen, allowing us to evaluate the heterogeneity of PO(2) inside short segments of microvessels. The phosphorescence decay curve contains information about the distribution of oxygen within the excited volume and the distribution can be represented as a histogram, by decomposing the decay curve into several components with weights proportional to the volume fraction of plasma with different PO(2), under the condition of a high signal-to-noise ratio. Furthermore, the histogram can be converted into a radial profile of PO(2), based on the assumptions of a circular vascular lumen, axisymmetric distribution of oxygen and monotonic PO(2) profile. Albumin-bound Pd-porphyrin phosphor was infused into the circulation of hamsters and excited by flash illumination at 10 Hz, with a square region of excitation light just covering the entire lumen, (i.e. width of region equaled luminal diameter) of microvessels in the hamster mesentery. A set of 50 curves (5 s of data) was averaged to obtain a decay curve with low noise. Curves were analyzed with the above histogram procedure, and this analysis allowed us to distinguish between PO(2) values originating from intra and extravascular subvolumes. The intravascular PO(2) in these microvessels was very heterogeneous, which could be explained by the existence of significant radial PO(2) gradients. The radial PO(2) gradients were estimated to be approximately 1 mmHg/microm.     

Characterization of the tryptophan environments of interleukins 1 alpha and 1 beta by fluorescence quenching and lifetime measurements

The tryptophan environments of interleukins 1 alpha and 1 beta, immunomodulatory proteins with similar biological activities but only 25% sequence homology, were characterized by steady-state and dynamic fluorescence measurements. Both proteins exhibited similar emission maxima, but the emission intensity of IL-1 beta was greatly enhanced by increasing the ionic strength of the medium, whereas that of IL-1 alpha was unaffected. The two cytokines were also similarly quenched by the polar quencher acrylamide, but differences were observed for the ionic quenchers iodide and cesium. The fluorescence intensity decays of both cytokines were characterized by two (long and short) component lifetimes. However, the average lifetime of IL-1 beta (4.4 ns) was much longer than that of IL-1 alpha (1.93 ns). Taken together with the results of steady-state measurements, we suggest that the single tryptophan of IL-1 beta is statically quenched by neighboring charged residues, whereas the tryptophan fluorescence of IL-1 alpha is unaffected by ionic strength, and that the tryptophans of the two proteins have different accessibilities to ionic quenchers. The results are discussed in terms of similarities and differences in the tryptophan environments of the two proteins.