help button home button Biophys. J.
HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS

Biophysical Journal 52: 717-728 (1987)
© 1987 the Biophysical Society

This Article
Right arrow Full Text (PDF)
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Similar articles in this journal
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Right arrow reprints & permissions
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Wendler, J.
Right arrow Articles by Holzwarth, A. R.
Right arrow Search for Related Content
PubMed
Right arrow Articles by Wendler, J.
Right arrow Articles by Holzwarth, A. R.

State Transitions in the Green Alga Scenedesmus Obliquus Probed by Time-Resolved Chlorophyll Fluorescence Spectroscopy and Global Data Analysis

Joachim Wendler and Alfred R. Holzwarth

ABSTRACT

Decay-associated fluorescence spectra of the green alga Scenedesmus obliquus have been measured by single-photon timing with picosecond resolution in various states of light adaptation. The data have been analyzed by applying a global data analysis procedure. The amplitudes of the decay-associated spectra allow a determination of the relative antenna sizes of the photosystems. We arrive at the following conclusions: (a) The fluorescence kinetics of algal cells with open PS II centers (F0 level) have to be described by a sum of three exponential components. These decay components are attributed to photosystem (PS) I ({tau} {approx} 85 ps, {lambda}maxem {approx} 695-700 nm), open PS II {alpha}-centers ({tau} {approx} 300 ps, {lambda}maxem = 685 nm), and open PS II ß-centers ({tau} {approx} 600 ps, {lambda}maxem = 685 nm). A fourth component of very low amplitude ({tau} {approx} 2.2-2.3 ns, {lambda}maxem = 685 nm) derives from dead chlorophyll. (b) At the Fmax level of fluorescence there are also three decay components. They originate from PS I with properties identical to those at the F0 level, from closed PS II {alpha}-centers ({tau} {approx} 2.2 ns, {lambda}maxem = 685 nm) and from closed PS ß-centers ({tau} {approx} 1.2 ns, {lambda}maxem = 685 nm). (c) The major effect of light-induced state transitions on the fluorescence kinetics involves a change in the relative antenna size of {alpha}- and ß-units brought about by the reversible migration of light-harvesting complexes between {alpha}-centers and ß-centers. (d) A transition to state II does not measurably increase the direct absorption cross-section (antenna size) of PS I. Our data can be rationalized in terms of a model of the antenna organization that relates the effects of state transitions and light-harvesting complex phosphorylation with the concepts of PS II {alpha},ß-heterogeneity. We discuss why our results are in disagreement with those of a recent lifetime study of Chlorella by M. Hodges and I. Moya (1986, Biochim. Biophys. Acta., 849:193-202).




This article has been cited by other articles:


Home page
Plant Physiol.Home page
J. Veerman, S. Vasil'ev, G. D. Paton, J. Ramanauskas, and D. Bruce
Photoprotection in the Lichen Parmelia sulcata: The Origins of Desiccation-Induced Fluorescence Quenching
Plant Physiology, November 1, 2007; 145(3): 997 - 1005.
[Abstract] [Full Text] [PDF]


Home page
ScienceHome page
D. Gust, T. A. Moore, A. L. Moore, S.-J. Lee, E. Bittersmann, D. K. Luttrull, A. A. Rehms, J. M. DeGraziano, X. C. Ma, F. Gao, et al.
Efficient Multistep Photoinitiated Electron Transfer in a Molecular Pentad
Science, April 13, 1990; 248(4952): 199 - 201.
[Abstract] [PDF]




HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
Copyright © 1987 by the Biophysical Society.