Photosynthetic activities of sections of intact tobacco leaves ( Nicotina tabacum L. var. Xanthi) were monitored by the photoacoustic effect. A reference signal was obtained using brief simultaneous illumination of the leaf with continuous light of saturating intensity. 1. The effect of the direct continuous light depends on the modulation frequency: A decrease in the photoacoustic signal, ‘negative effect’, is observed at low frequency (under approx. 200 Hz) and an increase of the photoacoustic signal, ‘positive effect’, at high frequency (above approx. 200 Hz). Both effects are reversible. 2. When leaves are water-infiltrated only a ‘positive effect’: of the direct continuous light is observed, at any frequency. Leaves infiltrated with aqueous DCMU solution (50 μM) do not show any direct continuous light effect. 3. The ‘negative effect’ develops, as the leaf is illuminated, in parallel to the (low frequency) photoacoustic signal itself which increases gradually after an initial lag period. This transient phenomenon takes a few minutes under our conditions. The differential increase of the signal during the induction period matches the size of the negative effect obtained by applying the direct continuous light at various times during the induction or in the steady state. 4. In a similar way, the ‘positive effect’ increases during the induction period, due to a transient decrease of the photoacoustic signal measured at high frequency. This change in the ‘positive effect’ is less noticeable, as a sizeable effect is already observed in a dark-adapted leaf, upon illumination, and the extent of the photoacoustic transient is relatively small. 5. No photoacoustic transients are observed when direct continuous light is used continuously. 6. It is concluded that the photoacoustic signal is due to two contributions: At low frequency there is a considerable contribution from modulated oxygen evolution, which tends to zero as the direct continuous light is applied. At high frequency the main contribution is from the conversion of photon energy to heat, and direct continuous light effects reflect mainly photochemical energy storage. Both low and high frequency photoacoustic transients reflect the induction period of photosynthesis. 7. Preliminary calculations on the relative damping of modulated oxygen evolution and thermal photoacoustic contributions with the modulation frequency, are consistent with the above model, taking into account diffusion and the rate-limiting step in O 2 evolution. 8. Photoacoustic data were used to construct a relative quantum yield spectrum for both oxygen evolution and photochemical energy storage.
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