PS II model based analysis of transient fluorescence yield measured on whole leaves of Arabidopsis thaliana after excitation with light flashes of different energies

Our recently presented PS II model (Belyaeva et al., 2008) was improved in order to permit a consistent simulation of Single Flash Induced Transient Fluorescence Yield (SFITFY) traces that were earlier measured by Steffen et al. (2005) on whole leaves of Arabidopsis (A.) thaliana at four different e...

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Published inBioSystems Vol. 103; no. 2; pp. 188 - 195
Main Authors Belyaeva, N.E., Schmitt, F.-J., Paschenko, V.Z., Riznichenko, G.Yu, Rubin, A.B., Renger, G.
Format Journal Article
LanguageEnglish
Published Ireland Elsevier Ireland Ltd 01.02.2011
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Abstract Our recently presented PS II model (Belyaeva et al., 2008) was improved in order to permit a consistent simulation of Single Flash Induced Transient Fluorescence Yield (SFITFY) traces that were earlier measured by Steffen et al. (2005) on whole leaves of Arabidopsis (A.) thaliana at four different energies of the actinic flash. As the essential modification, the shape of the actinic flash was explicitly taken into account assuming that an exponentially decaying rate simulates the time dependent excitation of PS II by the 10ns actinic flash. The maximum amplitude of this excitation exceeds that of the measuring light by 9 orders of magnitude. A very good fit of the SFITFY data was achieved in the time domain from 100ns to 10s for all actinic flash energies (the maximum energy of 7.5×1016 photons/(cm2flash) is set to 100%, the relative energies of weaker actinic flashes were of ∼8%, 4%, ∼1%). Our model allows the calculation and visualization of the transient PS II redox state populations ranging from the dark adapted state, via excitation energy and electron transfer steps induced by pulse excitation, followed by final relaxation into the stationary state eventually attained under the measuring light. It turned out that the rate constants of electron transfer steps are invariant to intensity of the actinic laser flash. In marked contrast, an increase of the actinic flash energy by more than two orders of magnitude from 5.4×1014 photons/(cm2flash) to 7.5×1016 photons/(cm2flash), leads to an increase of the extent of fluorescence quenching due to carotenoid triplet (3Car) formation by a factor of 14 and of the recombination reaction between reduced primary pheophytin (Phe−) and P680+ by a factor of 3 while the heat dissipation in the antenna complex remains virtually constant. The modified PS II model offers new opportunities to compare electron transfer and dissipative parameters for different species (e.g. for the green algae and the higher plant) under varying illumination conditions.
AbstractList Our recently presented PS II model (Belyaeva et al., 2008) was improved in order to permit a consistent simulation of Single Flash Induced Transient Fluorescence Yield (SFITFY) traces that were earlier measured by Steffen et al. (2005) on whole leaves of Arabidopsis (A.) thaliana at four different energies of the actinic flash. As the essential modification, the shape of the actinic flash was explicitly taken into account assuming that an exponentially decaying rate simulates the time dependent excitation of PS II by the 10 ns actinic flash. The maximum amplitude of this excitation exceeds that of the measuring light by 9 orders of magnitude. A very good fit of the SFITFY data was achieved in the time domain from 100 ns to 10s for all actinic flash energies (the maximum energy of 7.5 × 10¹⁶ photons/(cm²flash) is set to 100%, the relative energies of weaker actinic flashes were of ∼8%, 4%, ∼1%). Our model allows the calculation and visualization of the transient PS II redox state populations ranging from the dark adapted state, via excitation energy and electron transfer steps induced by pulse excitation, followed by final relaxation into the stationary state eventually attained under the measuring light. It turned out that the rate constants of electron transfer steps are invariant to intensity of the actinic laser flash. In marked contrast, an increase of the actinic flash energy by more than two orders of magnitude from 5.4×10¹⁴ photons/(cm²flash) to 7.5×10¹⁶ photons/(cm²flash), leads to an increase of the extent of fluorescence quenching due to carotenoid triplet (³Car) formation by a factor of 14 and of the recombination reaction between reduced primary pheophytin (Phe(-)) and P680(+) by a factor of 3 while the heat dissipation in the antenna complex remains virtually constant. The modified PS II model offers new opportunities to compare electron transfer and dissipative parameters for different species (e.g. for the green algae and the higher plant) under varying illumination conditions.
Our recently presented PS II model (Belyaeva et al., 2008) was improved in order to permit a consistent simulation of Single Flash Induced Transient Fluorescence Yield (SFITFY) traces that were earlier measured by Steffen et al. (2005) on whole leaves of Arabidopsis (A.) thaliana at four different energies of the actinic flash. As the essential modification, the shape of the actinic flash was explicitly taken into account assuming that an exponentially decaying rate simulates the time dependent excitation of PS II by the 10ns actinic flash. The maximum amplitude of this excitation exceeds that of the measuring light by 9 orders of magnitude. A very good fit of the SFITFY data was achieved in the time domain from 100ns to 10s for all actinic flash energies (the maximum energy of 7.5×1016 photons/(cm2flash) is set to 100%, the relative energies of weaker actinic flashes were of ∼8%, 4%, ∼1%). Our model allows the calculation and visualization of the transient PS II redox state populations ranging from the dark adapted state, via excitation energy and electron transfer steps induced by pulse excitation, followed by final relaxation into the stationary state eventually attained under the measuring light. It turned out that the rate constants of electron transfer steps are invariant to intensity of the actinic laser flash. In marked contrast, an increase of the actinic flash energy by more than two orders of magnitude from 5.4×1014 photons/(cm2flash) to 7.5×1016 photons/(cm2flash), leads to an increase of the extent of fluorescence quenching due to carotenoid triplet (3Car) formation by a factor of 14 and of the recombination reaction between reduced primary pheophytin (Phe−) and P680+ by a factor of 3 while the heat dissipation in the antenna complex remains virtually constant. The modified PS II model offers new opportunities to compare electron transfer and dissipative parameters for different species (e.g. for the green algae and the higher plant) under varying illumination conditions.
Our recently presented PS II model (Belyaeva et al., 2008) was improved in order to permit a consistent simulation of Single Flash Induced Transient Fluorescence Yield (SFITFY) traces that were earlier measured by Steffen et al. (2005) on whole leaves of Arabidopsis (A.) thaliana at four different energies of the actinic flash. As the essential modification, the shape of the actinic flash was explicitly taken into account assuming that an exponentially decaying rate simulates the time dependent excitation of PS II by the 10 ns actinic flash. The maximum amplitude of this excitation exceeds that of the measuring light by 9 orders of magnitude. A very good fit of the SFITFY data was achieved in the time domain from 100 ns to 10 s for all actinic flash energies (the maximum energy of 7.5 x 10 super(16) photons/(cm super(2) flash) is set to 100%, the relative energies of weaker actinic flashes were of [inline image]8%, 4%, [inline image]1%). Our model allows the calculation and visualization of the transient PS II redox state populations ranging from the dark adapted state, via excitation energy and electron transfer steps induced by pulse excitation, followed by final relaxation into the stationary state eventually attained under the measuring light. It turned out that the rate constants of electron transfer steps are invariant to intensity of the actinic laser flash. In marked contrast, an increase of the actinic flash energy by more than two orders of magnitude from 5.4 x 10 super(14) photons/(cm super(2) flash) to 7.5 x 10 super(16) photons/(cm super(2) flash), leads to an increase of the extent of fluorescence quenching due to carotenoid triplet ( super(3)Car) formation by a factor of 14 and of the recombination reaction between reduced primary pheophytin (Phe super(-)) and P680 super(+) by a factor of 3 while the heat dissipation in the antenna complex remains virtually constant. The modified PS II model offers new opportunities to compare electron transfer and dissipative parameters for different species (e.g. for the green algae and the higher plant) under varying illumination conditions.
Author Paschenko, V.Z.
Riznichenko, G.Yu
Renger, G.
Rubin, A.B.
Belyaeva, N.E.
Schmitt, F.-J.
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Issue 2
Keywords PQ
HL
Chl
Electron transfer
F0, FmSTF
Photosystem II
HS
Phe
PQH2
SFITFY
kZ
PS II
ΔΨ
QA and QB
PPFD
Model simulation
YZ
kHD
FL, FL(t)
Single turnover flash
Dissipative energy losses
WOC
LED
ET
kP680+, k3Car
RC
kPhe
Fluorescence yield
3Car
P680
kL(t)
kF
Triplet carotenoid quenching
Language English
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Snippet Our recently presented PS II model (Belyaeva et al., 2008) was improved in order to permit a consistent simulation of Single Flash Induced Transient...
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SubjectTerms Algae
Arabidopsis - metabolism
Arabidopsis thaliana
Computer Simulation
Dissipative energy losses
Electron transfer
Electron Transport - physiology
Fluorescence
Fluorescence yield
Kinetics
Model simulation
Models, Biological
Photosystem II
Photosystem II Protein Complex - metabolism
Plant Leaves - metabolism
Single turnover flash
Triplet carotenoid quenching
Title PS II model based analysis of transient fluorescence yield measured on whole leaves of Arabidopsis thaliana after excitation with light flashes of different energies
URI https://dx.doi.org/10.1016/j.biosystems.2010.09.014
https://www.ncbi.nlm.nih.gov/pubmed/20951762
https://search.proquest.com/docview/847432219
https://search.proquest.com/docview/907149280
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