Trends in Plant Science
OpinionA quantitative model of the domain structure of the photosynthetic membrane
Section snippets
Structure from electron microscopy
The photosynthetic membrane (also named the thylakoid membrane) consists of a system of paired membranes enclosing between them the lumen and separating it from the surrounding stroma of the chloroplast. In addition to the asymmetry across the membrane, there is also a lateral asymmetry such that one can distinguish between different domains with different biochemical composition and function 1 (Fig. 1).
The grana are stabilized by ‘stacking’ forces between the outer surface of thylakoids in the
Fragmentation and separation analysis
One way to study the organization and structure of a complex biological object is to disintegrate it, separate the components, determine their composition and properties and then try to construct a model of the original object. When applied to the thylakoid membrane this approach has given us important knowledge about its components and their organization and function in the membrane. Press treatment or sonication gives rise to membrane vesicles that originate from the different parts of the
More quanta are captured by photosystem I than photosystem II
A fundamental question in photosynthesis is how the light quanta captured by the pigments are distributed between the two photosystems. Because the separation of thylakoid vesicles is quantitative, it is possible to determine the distribution of chlorophyll and carotenoid between PSI and PSII (Refs 6, 7). It turns out that there is more chlorophyll associated with PSI than with PSII, the excess being in the range 14–20% (i.e. per 100 chlorophyll molecules 57–60 are associated with PSI and 40–43
A model for the thylakoid membrane
According to the model (Fig. 2), 80% of the membrane is in the form of grana and 20% as stroma lamellae. Linear electron transport (Box 1) occurs in the grana where PSII, localized in the appressed core of the grana, cooperates with PSI in the margin, which forms an annulus (ring) surrounding the grana core. The margin covers 40% of the circular grana disc to accommodate ∼40% of the chlorophyll localized in a grana disc, which is associated with PSIα (Table 1).
PSII of the appressed grana and
Why are photosystem I and photosystem II laterally segregated in the thylakoid membrane?
This is a frequently asked question. One can answer ‘Why not?'It has been known for many years that macromolecules do not readily mix in solutions; mixing is the exception rather than the rule in polymer mixtures, both in water and in organic solvents 19. This is because of the large size of macromolecules, resulting in a domination of the interaction between the macromolecules over the entropy of mixing. If the interaction between like molecules is more attractive than between unlike
What is the functional advantage with patches of photosystem II that form grana stacks?
This question has been discussed ever since grana were discovered. It has been suggested that grana can facilitate light harvesting and its regulation 17, 21, protect against photodamage 17 and prevent quanta captured by PSII from ending up in PSI (Ref. 22).
A feature of the present model is that the formation of grana prevents competition between linear and cyclic electron transport. The grana and the stroma lamellae should complement each other and not compete when carrying out their
Light-induced protein phosphorylation
What has been written above holds for conditions when light is limiting. Dramatic changes occur when light intensity increases 25: PSII is down regulated, its functional antenna decreases, oxygen evolution becomes eventually saturated, the antenna of PSI might increase, cyclic electron transport increases relative to the linear, several proteins are phosphorylated, photosystems are damaged and repaired.
The net result is that the excess of quanta captured by PSI becomes even larger than under
Acknowledgements
My thanks to John F. Allen and Jonathan Park for critically reading the manuscript.
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