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 Encyclopedia of Physical Science and Technology  EN012C-562  July 26, 2001  15:30







              Photoacoustic Spectroscopy                                                                   11

                                                                This was the first time such quantitative information on
                                                                the amount of energy transfer between PS I  and PS II  was
                                                                provided. All these measurements were made with 650 nm
                                                                modulated light.
                                                                  In order to understand these changes in the spectral
                                                                range of photosynthetically active radiation, spectra were
                                                                recorded under state 1 and state 2 conditions (Fig. 10). The
                                                                photochemical activity remains the same in both state 1
                                                                and state 2 between 580 and 700 nm, but it is lower in state
                                                                2 between 400 and 580 nm. Both PS I and PS II activities
                                                                change significantly due to the migration of LHC II . The
                                                                amplitude of LHC II coupling-induced change is the same
                                                                in both PS I and PS II between 580 and 700 nm, but it is
                                                                less in PS I than in PS II between 400 and 580 nm, which
                                                                explains the lower photochemical activity of the leaf in
                                                                state 2 than in state 1. This is due to the decrease in energy
                                                                transfer efficiency of the carotenoids to chlorophylls in
                                                                LHC II when it is associated with PS I .

















              FIGURE  9  Photoacoustic  signal  from  sugar  maple  leaf  in  the
              course of time during state 1 (A) and state 2 (B).


              the direct evidence for the migration of LHC II  between PS I
              and PS II . Energy storage of both systems changes during
              state transitions. The fraction of energy gained by PS I  is
              nearly equal to that lost by PS II  during transition to state 2
              andviceversainstate1.Thisfractionamountstoabout5%
              of absorbed light, 19% of total energy stored, 34% of PS II
              energy stored, and 43% of PS I  energy stored in state 2.


                                                       , and
              TABLE I  ES T  , ES PS I  , and ES PS II  , Ratio of ES PS I  /ES PS II
              Light Distribution between PS I  (α) and PS II  (β) during State 1–
              State 2 Transition in Sugar Maple Leaves
                           State 1   State 2   (State 2 − State 1)
              ES T  (%)   27.3 ± 3.7  26.9 ± 3.4   −0.4
                 (%)       6.7 ± 4.0  11.8 ± 4.3   +5.1
              ES PS I
                  (%)     20.6 ± 5.5  15.1 ± 5.8   −5.5
              ES PS II
                            3.1       1.3          −1.8
              ES PS I  /ES PS II
              α             0.24      0.44         +0.19        FIGURE 10 Energy storage of both photosystem I and II to-
                                                                gether (squares), photosystem I (open circles), and photosystem
              β             0.75      0.56         −0.19
                                                                II (closed circles) of sugar maples leaves.
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