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biologia - Studia

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CHLOROPHYLL FLUORESCENCE IN STATE TRANSITIONS<br />

0.8<br />

F0 Fm Fv<br />

0.7<br />

Fluorescence<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

M V1 V2 V3 V4 V5 V6<br />

Fig. 1. Evolution of minimal, maximal and variable fluorescence in the conditions of<br />

photosystems’ state 1 and 2. M= control; V 1 -V 6 (see material and method)<br />

The photochemical efficiency (F v /F m ) as well as the quantum yield of the<br />

photosynthetic electrons transport chain have decreased significantly in both redox<br />

states of the photosystems, highlighting the photoinhibition of the closed reaction<br />

centers (fig. 2). In state 1 in the presence of DBMIB inhibitor it was recorded a slight<br />

recovery of the photochemical activity, although DBMIB inhibits the linear electron<br />

flow (Joët et al., 2002). This recovery is assigned to the cyclic electron current around<br />

PS I. The close numeric values for photochemical effieciency and quantum yield in<br />

all variants emphasized the lack of energized state in the thylakoidal membrane. In<br />

the state transitions, a decrease in the photochemical efficiency and quantum yield is<br />

due greatly to inhibitor effects of low temperature.<br />

Low light exposure produces reversible decrease of photochemical efficiency<br />

because photoinhibition appears. The extent of the photoinhibition depends on the<br />

capacity of energy usage in photochemical reactions or in thermal dissipation, processes<br />

which are used for decreasing the excitation energy for the purpose of decreasing the<br />

photosystem’s vulnerability to photoinhibition (Kornyeyev et al., 2002). The lack of<br />

balance between synthesis and degradation of D 1 protein produces an inhibition of<br />

the PS IIs’ electrons transport during photoinhibition (Briantais et al., 1988).<br />

85

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