TEMPERATURE DEPENDENCE OF DELAYED LIGHT EMISSION IN THE 6 to 340 MICROSECOND RANGE AFTER A SINGLE FLASH IN CHLOROPLASTS

Abstract. The delayed light emission decay rate (up to 120 μs) and the rise in chlorophyll a fluorescence yield (from 3 to 35 μs) in isolated chloroplasts from several species, following a saturating 10 ns flash, are temperature independent in the 0–35°C range. However, delayed light in the 120–340 μs range is temperature dependent. Arrhenius plots of the exponential decay constants are: (a) linear for lettuce and pea chloroplasts but discontinuous for bush bean (12–17°C) and spinach (12–20°C) chloroplasts; (b) unaffected by 3-(3,4 dichlorophenyl)-1,1-dimethylurea (inhibitor of electron flow), gramicidin D (which eliminates light-induced membrane potential) and glutaraldehyde fixation (which stops gross structural changes).
The discontinuities, noted above for bush bean and spinach chloroplasts, are correlated with abrupt changes in (a) the thylakoid membrane lipid fluidity (monitored by EPR spectra of 12 nixtroxide stearate, 12NS) and (b) the fluidity of extracted lipids (monitored by differential calorimetry and EPR spectra of 12 NS). However, no such discontinuity was observed in (a) chlorophyll a fluorescence intensity of thylakoids and (b) fluorescence of tryptophan residues of delipidated chloroplasts.
Microsecond delayed light is linearly dependent on light intensity at flash intensities as low as one quantum per 2 times 10⁴ chlorophyll molecules. We suggest that this delayed light could originate from a one quantum process in agreement with the hypothesis that recombination of primary charges leads to this light emission. A working hypothesis for the energy levels of Photosystem II components is proposed involving a charge stabilization step on the primary acceptor side, which is in a lipid environment.
Finally, the redox potential of P680 (the reaction center for chlorophyll of system II) is calculated to be close to 1.0–1.3 V.     

ACTION SPECTRA FOR BIOSYNTHESIS OF CHLOROPHYLLS a AND b AND β-CAROTENE

Abstract— Action spectra for the formation of chlorophyll b and β-carotene were determined with etiolated wheat leaves and compared with the action spectrum for the formation of chlorophyll a determined for the same samples. The action spectra were measured with etiolated leaves which had been pre-illuminated for 10 min and incubated in the dark for 4 h to eliminate induction of pigments. The action spectra for chlorophyll b and for β-carotene accorded with the action spectrum for chlorophyll a and with the absorption spectrum of protochlorophyllide in intact etiolated leaves. It is postulated from this result with chlorophyll b that this pigment is formed from protochlorophyllide through chlorophyll a or some intermediates to chlorophyll a. Complexing between chlorophylls and β-carotene and proteins is postulated to interpret the action spectrum for β-carotene. It is assumed that the low concentration of chlorophylls formed photochemically limits the rate of complexing, and that consumption of β-carotene for the complexing induces formation of new β-carotene.     

OPTICAL SPECTROSCOPY OF BILAYER MEMBRANES

Abstract— The absorption and fluorescence spectroscopy of natural and model bilayer lipid membranes is reviewed. Basic structural features of biological membranes and the relative advantages of black lipid membranes (BLM) and of liposomes are discussed. Theoretical considerations show that the wavelengths of absorption maxima are affected by the refractive index and dielectric constant of the medium surrounding the chromophore. Techniques of obtaining photoelectric action spectra, direct absorption spectra, and reflection spectra of BLM are described. Polarized spectra can give information about the orientation of membrane constituents and show, for example, that the porphyrin ring of chlorophyll in BLM is tilted at 45 ± 5° to the membrane surface. Absorption maxima of chlorophyll in BLM are compared with solution spectra of various chlorophyll adducts and aggregates. It is concluded that chlorophyll in BLM exists largely as solvated monomer and dimer (or oligomer), depending on concentration, and is not coordinated with water. From the theory of fluorescence spectroscopy it follows that aggregation and the polarity of the environment affect the fluorescence yield and lifetime of a membrane component, and also the wavelength of its emission maximum. The microviscosity of the membrane matrix affects the anisotropy of fluorescence. Techniques of steady-state fluorescence spectroscopy and of fluorescence lifetime measurements are reviewed. Examples of the use of fluorescent probes in membrane studies are given. Certain probes such as anilinonaphthalene sulfonate (ANS) preferentially bind to membrane proteins. The location of a probe in a particular membrane region can be pinpointed from its fluorescence yield and emission maximum. The orientation of the hydrocarbon chains of membrane lipids has been found, from fluorescence polarization of certain probes, to be normal to the membrane surface as postulated a priori on the basis of the lipid bilayer model. Anisotropy of fluorescence shows that elongated probe molecules rotate rapidly about their long axes when surrounded by phospholipids but become immobilized when bound to proteins. Changes in intensity and anisotropy of fluorescence as function of temperature have demonstrated the existence of phase transitions and phase equilibria of membrane lipids. Excimer fluorescence has been used as a measure of the available lipid core volume of membranes. Mechanisms of energy transfer between membrane components are reviewed. The theoretical dependence of energy transfer on distance and orientation for several rigid and fluid membrane models is discussed in terms of the structural information it can provide. Fluorescence sensitization resulting from energy transfer within and across bilayer membranes has been demonstrated in various systems. Quantitative measurement of energy transfer efficiency in BLM has shown that such transfer is about five times more efficient than in solutions at comparable donor-acceptor distances. Lipid membranes can be viewed as structures which maintain their components at high concentrations, in a reactive state, and at favourable orientations.     

SPECTROSCOPY OF CHLOROPHYLL IN BIOLOGICAL AND SYNTHETIC SYSTEMS*

Abstract. –This review discusses recent spectroscopic studies aimed at discovering the structure, orientation, and function of chlorophyll in vivo. In plant membranes there appear to be at least two distinct types of chlorophyll a. The greater part, over 99%, is antenna chlorophyll which absorbs and transfers radiant energy to a few specialized chlorophyll molecules in a reaction center where the actual charge separation occurs. A dimer-oligomer model for antenna chlorophyll has been proposed on the basis of comparative studies of the absorption spectra of chlorophyll in various dry solvents and in vivo. Unfortunately a similarity between essentially structureless broad spectra is very weak evidence for their original identity. Also the requirement of an anhydrous environment for most of the chlorophyll in biological material is an unlikely postulate. A cross-linked, linear polymer model of chlorophyll in vivo has also been proposed. Recent Resonance Raman spectroscopic results appear to rule out, in large part, either polymer model and once again suggest that it is the various attachments of chlorophyll to proteins which determine its function as antenna pigment in vivo. Circular dichroism measurements of chlorophyll in various plant materials have also led to the conclusion that antenna chlorophyll has strong interaction with protein. However, some doubt still exists as to the interpretation of these CD results. New studies of fluorescence, polarized fluorescence and Resonance Raman spectroscopy of various plant species corroborate the original proposition, based upon deconvolution of absorption spectra, that antenna chlorophyll occurs in vivo in at least five discrete pools, and that each pool is likely to be located in the same environment in different plants. A new model-systems approach to simulating chlorophyll in vivo has come through the use of lipid bilayers and liposomes. Charge transfer has been observed between chlorophyll in a lipid phase and phycobiliproteins or cytochrome c. The most promising, newly synthesized model for the reaction center, P700, is a covalently bound dimeric derivative of pyrochlorophyllide a. Its properties are similar to P700 in several respects except for reversible photooxidation which has not yet been observed. By detergent treatments chlorophyll-protein complexes having about 20–40 chlorophyll a molecules for every P700 have been isolated from different plants, and their spectroscopic properties are under investigation in several laboratories. The several hypotheses to explain the shape of the oxidized minus reduced absorption difference spectrum of P700 have not yet been reconciled. The nature of the photosystem II reaction center chlorophyll, P680, is also a subject of active investigation. Its absorption difference spectrum appears to have two kinetic components.     

ENERGY TRANSFER FROM CHLOROPHYLL b TO CHLOROPHYLL a IN A HYDROPHOBIC MODEL SYSTEM

Abstract— Chlorophyll a and chlorophyll b purified by high-performance liquid chromatography (HPLC) were subsequently adsorbed on the surface of a pellicular reverse phase packing normally used in HPLC. The granule surface is reacted with octadecyl groups and furnishes an hydrophobic substrate for pigment adsorption. Reflectance spectra of chlorophyll a and chlorophyll b , each adsorbed at average spacings of about 11 nm² per molecule, had red region maxima at 664 and 643nm respectively. Fluorescence excitation spectra for 740nm emission from these surfaces peaked at about 420nm for chlorophyll a and 460nm for chlorophyll b. Adsorbed pigments excited at either of the two wave lengths had a single fluorescence emission peak at 683nm for chlorophyll a and at 664nm for chlorophyll b. A surface having both pigments adsorbed in approximately equal amounts with an overall average spacing of about 5.6nm² per molecule also had peaks at 420 and 460nm in the excitation spectrum. However, excitation of adsorbed molecules on this (latter) surface, at either 420 or 460nm, produced emission with the single chlorophyll a peak at 683nm. It is concluded that, under the conditions of our experiment, exciting adsorbed chlorophyll b contributes strongly to emission from adsorbed chlorophyll a.     

CHLOROPHYLL PHOTOSENSITIZED ELECTRON TRANSFER IN PHOSPHOLIPID VESICLE SYSTEMS: COMPARISON OF INSIDE-OUTSIDE ASYMMETRY BETWEEN LARGE AND SMALL UNILAMELLAR VESICLES*

Abstract— We have determined the chlorophyll triplet quenching efficiencies, the chlorophyll cation radical yields and the conversion efficiencies of chlorophyll triplet to radical in large and small unilamellar phosphatidylcholine vesicles (LUV and SUV, respectively) in the presence of electrically-charged electron acceptors (ferricyanide and oxidized cytochrome c) located in either the inner or outer aqueous compartments of the vesicles. Both types of vesicles displayed inside-outside asymmetry, although the properties were reversed. Triplet quenching in SUV was more efficient when ferricyanide was located within the vesicle interior, whereas the reverse was true in LUV. When ferricyanide was located on the outside of the vesicles, the extent of triplet quenching in LUV was about two times that in SUV and the amount of cation radical formed in LUV was about two times that in SUV. Under these conditions, the conversion efficiencies of chlorophyll triplet to radical were 12.2% for LUV and 8.5% for SUV. With cytochrome c as an electron acceptor in negatively charged vesicles (25 mol per cent dixhexadecylphosphate incorporated) similar results were obtained. Again, the triplet quenching and radical yield inside-outside asymmetry properties were reversed between the two types of vesicles, and radical formation efficiencies when cyt c was located outside the vesicles were higher in LUV (11.7%) than in SUV (4.2%). We conclude that the inside-outside asymmetric photochemical behavior of unilamellar phosphatidylcholine vesicles is influenced by factors in addition to the difference in radius of curvature between the inside and outside surfaces. It is suggested that transmembrane electrostatic potentials may be involved. Furthermore, in the present system the properties of LUV were more favorable to photochemical electron transfer product formation than those of SUV.     

RESOLUTION ENHANCEMENT AND DECONVOLUTION INTO VIBRONIC BANDS OF THE FLUORESCENCE AND ABSORPTION SPECTRA IN THE RED REGION OF DILUTE SOLUTIONS OF CHLOROPHYLL a IN VARIOUS SOLVENTS

Abstract— The fluorescence spectra of chlorophyll a in less than 10–⁶ mol dm^-3 solutions of benzene, toluene, tetrahydrofurane, EPA and ethanol were determined at both room temperature and at 77 K. Resolution enhancement using Fourier transform methods revealed the presence of vibronic bands with essentially solvent-invariant separation between their origins; this was confirmed by the quantitative deconvolution of the spectra into Gaussian bands. It was concluded that the fluorescence is due to a single spectroscopically distinct species. The absorption spectra in the above solvents include a band absent from the fluorescence spectra which, from its position and intensity, may be identified as the longest wavelength X-polarized electronic transition of chlorophyll a. Differences observed between the shapes of the low-and high-temperature absorption spectra may be attributed primarily to the narrowing of bandwidths with decreasing temperature and to intensity redistribution within the bands; the apparent increase in the integrated intensity on cooling the solutions appears to be due largely to the increase in the volume concentration of the solute as a result of solvent contraction.     

LONG-LIVED AFTERGLOW OF PHOTOSYNTHETIC PIGMENTS IN SOLUTION: PHOTOCHEMILUMINESCENCE

Abstract —Our recent research on photochemiluminescence (PCL) of pigments in solutions is reviewed. PCL was observed in the course of photooxidation by oxygen of chlorophyll a , bacteriochlorophyll, protochlorophyll, their analogs, synthetic dyes and aromatic hydrocarbons. The PCL of chlorophyll was studied in detail. It depends on oxygen concentration, intensity of exciting light, pH, nature of pigments, solvents etc. The thermochemiluminescence was observed after illumination of liquid and solid pigment solutions at low temperature (down to - 170C). The excitation spectra of PCL coincide with the pigment absorption spectra. The PCL emission spectra in most cases differ from those of pigment fluorescence. Electron acceptors, electron donors, radical inhibitors and β-carotene quench PCL. The quenching efficiency of electron acceptors is similar to their action on the chlorophyll triplet state. The quenching effect of radical inhibitors and β-carotene correlates with their activity in reaction with singlet oxygen. The effect of quenchers on the chlorophyll fluorescence, photobleaching and pigment sensitized oxygenation was studied. Analysis of experimental data allowed the assumption that chemiluminescence accompanies the decomposition of labile pigment peroxides. The accumulation of peroxides is probably due to the reaction in the complex of pigment and singlet oxygen, formed as a result of energy transfer from photoexcited (triplet) pigment molecules to oxygen. The terminal chemiluminescence emission proceeds from the singlet excited states of molecules of pigments and products of their oxidation.     

FLUORESCENCE PROPERTIES OF ISOTROPICALLY AND ANISOTROPICALLY EMBEDDED FLAVINS

Abstract— On the basis of corrected fluorescence excitation and emission spectra, flavin photo-processes in anisotropically vesicle-bound flavins have been studied. By means of aliphatic C₁₈H₃₇-chains at positions 3, 7 and 10, the flavin nucleus can be variously anchored within the membrane/water interface (amphiflavin), thereby mimicking the various positions and microenvironments of the isoalloxazine ring in flavoproteins. From polarization spectra, the angles between the different electronic transition moments of isotropically dissolved or membrane-bound flavins have been obtained. Polarization and angle spectra of isotropically and various anisotropically embedded flavins exhibit strong differences, reflecting the specific interaction with the matrices. Based on a slightly modified theory, originally developed by Perrin and Weber, using the concentration dependence of fluorescence polarization, it is found that the radiative flavin-flavin interaction (selfcontact) on the membrane is by a factor of 25 to 54 smaller than in isotropic solution. This is taken as further justification to study anisotropic flavin chemistry on the basis of flavin-loaded vesicles.     

LOW-TEMPERATURE FLUORESCENCE SPECTRA OF CHLOROPHYLL a SOLUTIONS

Abstract Fluorescence and fluorescence polarization spectra of chlorophyll a dissolved in ethanol, n -propanol, EM (ethanol-methanol, 4:1) and EPE (ether, n -pentane, ethanol, 5:5:2) were measured at 77 K. An emission band ('shoulder') between the two usual fluorescence bands appears in such spectra of dilute solutions (concentration ˜ 10^-5 M ) of chlorophyll a (except in EPE). The position, intensity and half-width of this band were calculated using a computer. The correlation between electronic transitions of chlorophyll a and these emission bands is discussed.     

GENETIC VARIATIONS AND LINOLENIC ACID INDUCED CHANGES IN THE ORIENTATION PATTERN OF CHLOROPHYLL a IN THYLAKOID MEMBRANES

Abstract Orientation pattern of the Q_y absorption and emission dipoles of chlorophyll a were studied in wild type Scenedesmus obliquus and in mutants deficient in chlorophyll b and carotenoids. Fluorescence polarization ratio at –140°C and linear dichroism at 25°C were measured in whole cells and thylakoids aligned in polyacrylamide gel. Unlike normal thylakoids, mutants displayed fluorescence polarization ratios significantly lower than 1.0 and showed a negative LD signal around 672 nm, indicating the tendency of the Q_y dipoles to tilt out from the membrane plane. Such an orientation pattern can also be artificially induced by treating normal thylakoids with linolenic acid.     

IS ZEAXANTHIN CAPABLE OF ENERGY TRANSFER TO CHLOROPHYLL a IN PARTIALLY GREENED LEAVES? A STUDY OF FLUORESCENCE EXCITATION SPECTRA DURING VIOLAXANTHIN DEEPOXIDATION

Absorbance spectra and excitation spectra of chlorophyll a fluoresence were recorded during the light-induced deepoxidation of violaxauthin to zeaxanthin in bean leaves (Phaseolus coccineus) greened under intermittent light. Light minus dark fluorescence excitation difference spectra showed distinct minima at 440, 465, and 500 nm corresponding to maxima in the absorbance difference spectra. Both difference spectra were prevented by the deepoxidase inhibitor dithiothreitol and were inverted when zeaxanthin was epoxidized. The fluorescence excitation difference spectra were successfully modeled by considering the absorbance differences between violaxanthin and zeaxanthin, assuming no energy transfer from the two pigments to chlorophyll a, and accounting for light-induced scattering changes. The pigment stoichiometry and the scattering changes of the simulation were in accordance with experimental data. The results indicate that, in the early stage of leaf development, light absorbed by the cycle pigments violaxanthin and zeaxanthin is not transferred to chlorophyll.     

ACTION SPECTRA FOR PHOTOREACTIONS I AND II OF PHOTOSYNTHESIS IN THE BLUE-GREEN ALGA ANACYSTIS NIDULANS

Abstract— Action spectra for photoreactions I and II of photosynthesis were obtained for Anacystis nidulans and three of its variants which had altered chlorophyll/phycocyanin ratios. The spectra are properly scaled to each other. They provide information on contributions of phycocyanin and chlorophyll to initial absorption and final distribution of excitation energy to reaction centers I and II. In normally pigmented cells the light harvesting pigments for photoreaction I include about 40% of the phycocyanin and 84% of the chlorophyll. Both in normal cells and in cells with altered pigmentation excitation energy from phycocyanin is delivered to photoreaction II via a small number of chlorophylls. In response to alterations in chlorophyll/phycocyanin ratio Action I spectra showed large variations whereas Action II spectra were essentially invariant. The result is taken to mean that alteration in chlorophyll components in Anacystis is attended by a special restriction: there are only small changes in amount of chlorophyll accessible to photoreaction II in the face of large changes in amount committed to photoreaction I.     

A FLASH PHOTOLYSIS STUDY OF INTERMEDIATES IN PHOTOCHEMICAL REACTIONS OF CHLOROPHYLL

Abstract— The photochemical reactions of chlorophyll intermediates in vitro have been studied by the flash photolysis method. The flash excitation of pigment solutions has been shown to involve the population of a chlorophyll triplet state where the oxidation-reduction processes occur. The mechanism and kinetics of pigment triplet decay have been investigated from 20°to — 50°C and the ability of chlorophyll molecules to carry out triplet-triplet energy transfer has been established. The latter phenomenon has been used to show up the role of chlorophyll triplets in the reversible photooxidation reaction with P -quinone. There have been studied initial products of pigment photoreduction with ascorbic acid and phenylhydrazine. Experimental data of the mechanism of the initial oxidation and reduction in chlorophyll photosensitized reactions have been analysed. There have been also obtained the differential spectra of chlorophyll triplets and radicals. A calculation has been made of rate constants for a few elementary reactions.     

ON THE FORMATION OF PHOTOSYNTHETIC MEMBRANES IN BEAN PLANTS*

Abstract— The formation of lamellar chlorophyll-protein complexes I and II, solubilized by sodium dodecyl sulfate, was studied by hydroxylapatite column chromatography during greening of etiolated Phaseohis vulgaris leaves.
The protein moiety of both complexes preexists in the prolamellar body of etiolated tissue. The complex II to complex I protein ratio is of the order of 0.5. During greening in intermittent illumination the 'proto'-chloroplast is agranal, and contains 'primary' thylakoids and chlorophyll a (Chl a ). At this stage the complex II to complex I protein ratio increases only slightly. Further greening of the plant tissue in continuous illumination results in grana, Chi b (chlorophyll b ) and more Chl a formation. The complex II to complex I protein ratio in unfractionated thylakoids is now of the order of 2.5, while in grana it is of the order of 4.0.
The binding of chlorophyll formed during greening to the protein moiety of the two complexes is found to be selective. The Chi a selectively formed under intermittent illumination is more strongly bound to the complex I protein. The Chi b and Chl a formed in continuous illunination are found bound to both complex I and complex II proteins.
Analysis by hydroxylapatite column chromatography of subchloroplast fractions obtained by different fractionation procedures have shown that these two chlorophyll-protein complexes are most probably derived from the PSI (photosystem I) and PSII (photosystem II) particles of the photosynthetic membrane. These findings suggest that PSI units are assembled ahead of PSII units. Moreover, they indicate that the complex I protein is the main protein component in the prolamellar body membranes, the 'primary' thylakoids. and the stroma lamellae, while in the grana membranes the major protein is the complex II protein. Finally our results show that formation of the photosynthetic membranes is a multi-step process.     

PREPARATION AND PROPERTIES OF CHLOROPHYLL/WATER-SOLUBLE MACROMOLECULAR COMPLEXES IN WATER. STABILIZATION OF CHLOROPHYLL AGGREGATES IN THE WATER-SOLUBLE MACROMOLECULE

Abstract— As an artificial model compound of the chlorophyll-protein complex in vivo , the chlorophyll/water-soluble macromolecular complexes were prepared by using synthetic linear polymers of polyvinylpyrrolidone (PVP), polyvinyl alcohol (PVA), polyethylene glycol (PEG), and a natural polymer of bovine serum albumin (BSA). By the method described here, it is possible to prepare an aqueous chlorophyll (Chl)-macromolecular complex solution of a desired Chi aggregate, such as: Chi a (670), Chi a (740) and Chi b ; and with a desired relative content and concentration. These procedures for preparing such complexes will have wide applicability for technical use in Chi studies. For example, extremely diluted aqueous complex solutions of at least 1 × 10^-4% wt Chi a (670 or 740)-macromolecular complex / wt can be obtained without changing the spectral features. From viscosity measurements, the structures of the complexes were inferred: (1) for a linear macromolecular (PVA or PVP) complex, a Chi species is tightly surrounded by a chain of the polymer causing shrinkage of the chain; (2) globular BSA molecules surround Chi species to form a large complex. The mechanism of stabilization of Chi aggregates in thylakoid membrane was discussed concerning an analogy to the complexes studied here.     

ZERO FIELD OPTICAL DETECTION OF MAGNETIC RESONANCE OF TRIPLET STATE OF CHLOROPHYLL a IN LIPID BILAYER VESICLES

Abstract The zero-field ODMR of triplet state of chlorophyll a incorporated in phosphatidylcholine (PC) vesicles (Chi a : PC = 1:100) has been carried out. The zero-field ODMR frequencies and intersystem crossing rate constants have been measured at various fluorescence wavelengths. The ODMR data suggest that the chlorophyll is present in mono- and biligated species. The nature of the ligand and the role of the medium (phospholipid) are also discussed.     

PHOTO-EXCITED TRIPLET STATE OF DIMERIC CHLOROPHYLL a IN 3-METHYLPENTANE RIGID MATRIX AT 77 K STUDIED BY FLASH PHOTOLYSIS

Abstract— Flash photolysis studies of dimeric and monomeric chlorophyll a were carried out at 77 K. The triplet-triplet absorption spectrum of the dimeric chlorophyll a in 3-methylpentane at 77 K is interpreted as a sum of the spectra of chlorophyll a in the ground and triplet states. The dimeric chlorophyll a in the triplet state is considered to have the half-excited structure at 77 K without photodisaggregation owing to high viscosity of the solvent.     

FOURIER-TRANSFORM INFRARED SPECTROSCOPIC STUDY OF THE STRUCTURE OF CHLOROPHYLL a and CHLOROPHYLL b IN HIGHLY DILUTE WATER-SATURATED CARBON TETRACHLORIDE SOLUTIONS

Abstract— Fourier-transform (FT) infrared (IR) absorption spectra have been measured for chlorophyll a (Chi a ), chlorophyll b (Chi b ), pheophytin a (Pheo a ), and pheophytin b (Pheo b ) in highly dilute (10^-5-10^-6 M ) water-saturated carbon tetrachloride solutions. Frequencies of IR bands due to C=O stretching modes of the 9-keto group indicate that Chi a assumes largely a dimeric structure in the concentrated (10^-2-10^-3 M ) water-saturated carbon tetrachloride solutions but it remains mostly a monomer with one or two coordinated water molecules in dilute (10^-5-10^-6 M ) solutions. Although it seems that Chi b also assumes predominantly dimeric form in concentrated solutions and monomelic form in dilute solutions, the relative intensity change of two C=O stretching bands ascribed to the free and coordinated 3-aldehyde groups with decreasing concentration suggests that the aldehyde group is also involved in formation of the dimer. The relative intensity of two C=O stretching bands due to the free and coordinated aldehyde groups changes significantly for Pheo b in water-saturated carbon tetrachloride solutions. This observation suggests that some of Pheo b also assume dimeric form via the aldehyde group in concentrated solutions.     

PHOTOELECTRON TRANSFER BETWEEN A CHARGED DERIVATIVE OF CHLOROPHYLL AND FERRICYANIDE AT THE LIPID BILAYER-WATER INTERFACE

Abstract— Flash illumination of a lipid bilayer containing a positively charge pigment: chlorophyll b cholyl hydrazone and separating two salt solutions, one of which contained ferricyanide, resulted in a photovoltage of ∼20mV, acceptor side negative. The positive charge on the pigment resulted in several novel effects. (1) The photo-emf is twice that of chlorophyll a and five times that of chlorophyll b at a given concentration. A higher surface concentration of the charged derivative is the likely cause of this effect. (2) The pheophytin of chlorophyll b cholyl hydrazone produces about one-half the photo emf of the magnesium derivative whereas pheophytin a or b produced only one-tenth the signal. This may be a reflection of the changed redox potential of the cation chlorophyll b cholyl hydrazone. (3) A voltage drop of 100 mV across the membrane, the acceptor side negatively biased, causes a 3–4-fold increase in the charge recombination rate. Biasing the acceptor side 100 mV positive has no effect. Chlorophyll a or b do not show this field effect. This asymmetric effect is explained as a movement of the more polar chlorophyll dication towards the water interface, leading to more rapid reaction with donor. Thus the kinetics of the charge reversal are a sensitive and specific probe of the polar interfacial region of the lipid bilayer-water interface.