| Literature DB >> 26010864 |
Mayank Anand Gururani1, Jelli Venkatesh2, Markkandan Ganesan3, Reto Jörg Strasser4, Yunjeong Han5, Jeong-Il Kim5, Hyo-Yeon Lee6, Pill-Soon Song6.
Abstract
Chlorophyll-a fluorescence analysis provides relevant information about the physiology of plants growing under abiotic stress. In this study, we evaluated the influence of cold stress on the photosynthetic machinery of transgenic turfgrass, Zoysia japonica, expressing oat phytochrome A (PhyA) or a hyperactive mutant phytochrome A (S599A) with post-translational phosphorylation blocked. Biochemical analysis of zoysiagrass subjected to cold stress revealed reduced levels of hydrogen peroxide, increased proline accumulation, and enhanced specific activities of antioxidant enzymes compared to those of control plants. Detailed analyses of the chlorophyll-a fluorescence data through the so-called OJIP test exhibited a marked difference in the physiological status among transgenic and control plants. Overall, these findings suggest an enhanced level of cold tolerance in S599A zoysiagrass cultivars as reflected in the biochemical and physiological analyses. Further, we propose that chlorophyll-a fluorescence analysis using OJIP test is an efficient tool in determining the physiological status of plants under cold stress conditions.Entities:
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Year: 2015 PMID: 26010864 PMCID: PMC4444231 DOI: 10.1371/journal.pone.0127200
Source DB: PubMed Journal: PLoS One ISSN: 1932-6203 Impact factor: 3.240
Formulae and glossary of terms used by the JIP-test (modified after Strasser et al. 2004).
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| Ft | fluorescence at time t after onset of actinic illumination |
| F50μs or F20μs | minimal reliable recorded fluorescence, at 50 μs with the PEA- or 20 μs with the Handy-PEA-fluorimeter |
| F300μs | fluorescence intensity at 300μs |
| FJ ≡ F2ms | fluorescence intensity at the J-step (2 ms) of OJIP |
| FI ≡ F30ms | fluorescence intensity at the I-step (30 ms) of OJIP |
| FP | maximal recorded fluorescence intensity, at the peak P of OJIP |
| tFM | time (ms) to reach the maximal fluorescence intensity FM |
| Area | total complementary area between the fluorescence induction curve and F = FM |
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| F0 ≅ F50μs or ≅ F20μs | minimal fluorescence (all PSII RCs are assumed to be open) |
| FM (= FP) | maximal fluorescence, when all PSII RCs are closed (equal to FP when the actinic light intensity is above 500 μmol photons m-2 s-1 and provided that all RCs are active as QA reducing) |
| Fυ≡ Ft-F0 | variable fluorescence at time t |
| FV ≡ FM-F0 | maximal variable fluorescence |
| Vt ≡ Fυ/FV ≡ (Ft-F0)/(FM-F0) | relative variable fluorescence at time t |
| M0 ≡ [(ΔF/Δt)0]/(FM-F50μs) ≡ 4 (F300μs-F50μs)/(FM- F50μs) | approximated initial slope (in ms-1) of the fluorescence transient normalised on the maximal variable fluorescence FV |
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| ABS /RC = M0 (1/VJ)(1/φPo) | absorption flux (of antenna Chls) per RC |
| TR0/RC = M0 (1/VJ) | trapped energy flux (leading to QA reduction) per RC |
| ET0/ RC = M0 (1/VJ)ψEo | electron transport flux (further than QA ⚿) per RC |
| RE0/RC = M0 (1/VJ)ψEo δRo | electron flux reducing end electron acceptors at the PSI acceptor side, per RC |
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| φPt ≡ TRt/ABS = [1-(Ft/FM)] = ΔFt/FM | quantum yield for primary photochemistry at any time t, according to the general equation of Paillotin (1976) |
| φPo ≡ TR0/ABS = [1-(F0/FM)] | maximum quantum yield for primary photochemistry |
| ψEo ≡ ET0/TR0 = (1-VJ) | efficiency/probability for electron transport (ET), i.e. efficiency/probability that an electron moves further than QA ⚿ |
| φEo ≡ ET0/ABS = [1-(F0/FM)]ψEo | quantum yield for electron transport (ET) |
| δRo ≡ RE0/ET0 = (1-VI)/(1-VJ) | efficiency/probability with which an electron from the intersystem electron carriers moves to reduce end electron acceptors at the PSI acceptor side (RE) |
| φRo ≡ RE0/ABS = [1-(F0/FM)]ψEo δRo | quantum yield for reduction of end electron acceptors at the PSI acceptor side (RE) |
| γRC = ChlRC/Chltotal = RC/(ABS+RC) | probability that a PSII Chl molecule functions as RC |
| RC/ABS = γRC/(1-γRC) = φPo (VJ/ M0) | QA-reducing RCs per PSII antenna Chl (reciprocal of ABS/RC) |
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| ABS/CS = | absorption per excited cross-section |
| TRo/CS = ΦPo·(ABS/CS) | trapping per excited cross-section |
| ETo/CS = ΦPo·Ψo·(ABS/CS) | electron transport per excited cross-section |
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| PIABS ≡ [γRC/(1-γRC)]. [φPo/(1- φPo)].[ψo/(1- ψo] | performance index (potential) for energy conservation from exciton to the reduction of intersystem electron acceptors |
| PItotal ≡ (PIABS).(δRo/1- δRo) | performance index (potential) for energy conservation from exciton to the reduction of PSI end acceptors |