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Photosynthesis consists of light absorption, primary electron transfer, energy stabilization, and the synthesis and transport of photosynthetic products1. Understanding each step is vital to guide efforts to increase crop photosynthetic efficiency. Light affects the rate of photosynthesis, requiring balancing energy supply, in the form of photons, with demand for reducing equivalents. When supply exceeds demand, for example under high-light or during reduced CO2 fixation caused by stomatal closure, build-up of reducing power increases the probability of reactive oxygen species formation with the potential to damage the photosynthetic apparatus and impair electron transport. Therefore, to prevent damage, plants have developed several photo-protective mechanisms, including detoxification of reactive oxygen species and non-photochemical quenching of the excited chlorophyll states (NPQ)2.
Maintaining high rates of photosynthesis is challenging under a field environment. Seasonal and diurnal changes, along with environmental fluctuations such as wind-induced leaf movements and transient cloud cover, cause shifts in the amount and intensity of light received by plants for photosynthesis3. NPQ dissipates excess light energy and can help prevent photo-damage while allowing for sustained rates of photosynthesis at high-light4. However, prolonged NPQ during high- to low-light transitions continues to dissipate energy that could be used for carbon reduction5. As a result, speeding up the relaxation of NPQ can increase the efficiency of photosynthesis6, making NPQ relaxation an attractive target for crop improvement.
Pulse amplitude modulated chlorophyll fluorescence (PAM) analysis can be used to calculate NPQ from measurable parameters (Supplementary Table 1 and Supplementary Table 2)7,8,9. This article focuses on determining NPQ relaxation rates in field-grown plants for the purpose of screening natural variation in germplasm. However, PAM chlorophyll fluorometry analysis can also be used for a wide variety of purposes, applied to species ranging from algae to higher plants, and is reviewed elsewhere7,8,9.
In a dark-adapted leaf or cell, photosystem II (PSII) reaction centers are open to receive electrons and there is no NPQ. Switching on a low-intensity measuring light elicits chlorophyll fluorescence while avoiding electron transport through PSII. The recorded minimum fluorescence in this dark-adapted state is described by the parameter Fo. Applying a high-intensity light pulse to a dark-adapted leaf can rapidly reduce the first stable electron acceptor pool of quinones bound to the quinone A site. This temporarily blocks electron transfer capacity in PSII reaction centers, which are then said to be closed and unable to receive electrons from water-splitting. By using a short pulse duration, there is insufficient time to stimulate NPQ. The resulting chlorophyll fluorescence is equivalent to the maximum value obtainable in the absence of NPQ, or maximum fluorescence, Fm. The difference between minimal and maximal fluorescence is referred to as variable fluorescence, Fv. The maximum photochemical quantum yield of photosystem II (Fv/Fm) is calculated from these two parameters using the following equation:
Fv/Fm = (Fm-Fo)/Fm
This can provide an important indicator of photosystem function and stress. Turning on an actinic (photosynthetic) light stimulates non-photochemical quenching, and subsequent application of a saturating flash allows for the measurement of light-adapted maximal fluorescence, Fm'. By comparing the difference between dark and light-adapted maximum fluorescence, NPQ can be calculated according to the Stern-Volmer equation10:
NPQ = Fm/Fm' - 1
In higher plants, NPQ has been described as consisting of at least five distinct components, including qE, qT, qZ, qI and qH. The precise mechanisms involved in NPQ are not fully understood; however, qE is considered to be the major component of NPQ in most plants. Crucial factors for full engagement of qE have been found to include the build-up of a proton gradient across the thylakoid membrane, the activity of photosystem II subunit S11,12, and de-epoxidated xanthophylls, antheraxanthin, lutein, and in particular zeaxanthin13. qE relaxes the fastest of any NPQ component (< 2 min)14, and reversible activation of qE is therefore particularly important for adaptation to shifting light intensities. A second slower phase of NPQ relaxation (~2-30 min) encompasses both qT, related to state transitions, and qZ, involving interconversion of zeaxanthin to violaxanthin15. Slow relaxing (> 30 min) of NPQ may include both photoinhibitory quenching (qI)16 and processes independent of photodamage17,18, such as qH, which is sustained quenching in the peripheral antennae of PSII mediated by a plastid lipocalin protein19,20.
NPQ increases during exposure to high light. Subsequent transfer to low light can result in downregulation of NPQ. The decay of fast, intermediate, and slow relaxing phases can be captured in the parameters of a bi-exponential function15,21,22,23
NPQ = Aq1(-t/τ1) + Aq2(-t/τ2) + Aq3
The theoretical basis for the bi-exponential function is based on the assumption of first-order utilization of hypothetical quenchers, including qE (Aq1), the combined relaxation of qZ and qT (Aq2), with the corresponding time-constants τq1 and τq2, and long-term NPQ, which includes qI and photodamage independent processes (Aq3). As such, the bi-exponential function provides a more realistic representation of the multiple connected biological processes involved in quenching chlorophyll fluorescence compared to a simpler Hill equation which lacks a theoretical basis24.
NPQ can be measured using a variety of commercially available PAM fluorometers25,26, from simple hand-held devices27 to more advanced closed systems28. However, a limitation of several of these approaches is a relatively low throughput, which makes screening large collections of plants challenging without multiple devices and a team of researchers. To address this issue, McAusland et al. developed a procedure based on excised leaf tissue and used it to identify differences in chlorophyll fluorescence between two wheat cultivars29. The attraction of this approach is that imaging leaf disks, taken from multiple plants with a single device, can facilitate screening hundreds of genotypes within a day. This makes it possible to assess variation in NPQ relaxation as part of genome wide association studies, or for screening breeding populations with the potential to increase crop photosynthetic efficiency and ultimately yield.
Building on the findings of McAusland et al.29, we use PAM chlorophyll fluorescence analysis of leaf disks for high-throughput screening of NPQ relaxation rates in Glycine max (G. max; soybean). This protocol uses the CF Imager25, which is comparable to other commercially available closed-PAM systems, such as the popular FluorCam26. With a dark room for adaptation of samples, users can image 96-well plates, Petri dishes, and small plants. The key advantage of this approach is the increase in throughput afforded by using leaf disks compared to sequential analysis of individual plants. Herein we present representative results, and a method for sampling, measuring, and analysis of NPQ in field-grown plants.