Chlorophyll Fluorescence Measuring Methods OJIP - part 2
OJIP is a measurement method used to study chlorophyll fluorescence kinetics in detail, specifically the rapid initial rise in fluorescence during a saturating light pulse. This rise reveals information about energy fluxes and electron transport within the photosynthetic apparatus.
In Part 1 of our OJIP blog series, I explained which physiological processes cause this characteristic fluorescence increase. In Part 2, I will focus on the parameters that can be derived from the OJIP transient (JIP test). These parameters allow us to quantify the processes discussed earlier, turning the curve shape into measurable physiological indicators.
Schematic overview
JIP parameters focus on the pathway of energy through the photosynthetic system: they track the fate of light energy from the moment it is absorbed, showing whether it is used to drive photosynthesis or dissipated as heat or fluorescence. The parameters can be grouped into three categories: energy fluxes, quantum yields and efficiencies.
Energy fluxes
Flux parameters describe the amount of energy flow through the different steps of the electron transport chain:
(1) Absorption flux: Photons absorbed by the antenna pigments and creating excited chlorophyll.
(2) Trapping flux: Channeled energy from excited chlorophyll to the reaction center to be converted into the electron transport chain (QA reduction).
(3) Electron flux: Electron transport further than QA
(4) Reduction flux: Reduction of end electron acceptors at the PSI side of the electron transport chain.
(5) Dissipation flux: Energy that is dissipated as heat or fluorescence.

Quantum yields + efficiencies
Next to the energy fluxes, we can calculate the fraction of absorbed energy by PSII that is used for a specific photochemical event. These fractions are also known as the quantum yield. Furthermore, the efficiency of the the event (with trapped energy) can also be calculated:
- Quantum yield of primary photochemistry, reducing QA (φP₀, often expressed as Fv/Fm)
- Quantum yield of electron transport from QA → QB → PQ pool (φE₀)
- Quantum yield of electron transport to the final PSI acceptors (φR₀)
- Efficiency with which a trapped excitation moves an electron further than QA into the electron transport chain (ΨE₀)
- Efficiency with which electrons arriving at PSI reduce the end acceptors FA/FB, ferredoxin, or NADP⁺ (δR₀)
These parameters provide insight into the functioning of the photosynthetic apparatus and are valuable for studying, for example, the mode of action of various compounds or the effects of environmental stresses.
A parameter that combines multiple of these processes, and that is highly sensitive to stress is the Performance Index (PI).
Performance index
The Performance Index (PI) was introduced because the commonly used parameter for photosynthetic efficiency, Fv/Fm, is not always sensitive enough to detect early or subtle stress responses. PI integrates multiple components of the photosynthetic process into a single value (energy absorption, trapping and electron transport). It is widely used by plant physiologists to evaluate the effects of biotic and abiotic stresses, and it is also a powerful parameter for breeding programs to rapidly screen genotypes under conditions such as drought or salinity stress. PI is considered one of the most sensitive OJIP-derived parameters.
There are two Performance Index variants: PI_ABS and PI_TOTAL.
PI_ABS combines three components into a single value:
- The density of active reaction centres
- The efficiency of trapping (the probability that absorbed light energy closes QA)
- The efficiency of electron transport beyond QA
PI_TOTAL includes the three components of PI_ABS and adds a fourth:
4. The efficiency of electron transport to the final PSI acceptors
Because PI incorporates multiple steps in the photosynthetic electron transport chain, any disturbance affecting one of the components will be reflected in the PI value, making it more sensitive than individual parameters alone.
Literature review
To provide an overview of the JIP parameters and how they can be used, we performed a literature survey to assess how different types of stresses affect JIP parameters. The following stresses were included: salt stress, drought stress, heat stress, cold stress, and high-light stress.
In general, several JIP parameters consistently respond to stress across studies, but the direction of the response can vary: some parameters increase under stress in a certain species or conditions, while others decrease. The exact pattern depends on the plant species, or even cultivar, and the severity of the stress. An overview of the results is summarized in the table below.
How parameters from OJIP are often visualized and interpreted
The large number of available OJIP parameters can make interpretation challenging. However, it is valuable for researchers to view the full set of parameters, as each one reflects a different component of the photosynthetic apparatus. Effects in one part of the electron transport chain may not appear in another, so examining multiple parameters can reveal where specific changes or stress responses occur.
A useful way to visualize the complete dataset is through spider plots (Figure 1). These plots allow many parameters to be displayed simultaneously, making it easier to identify patterns, compare treatments, or detect stress-induced deviations.
In some studies, authors visualize the different energy fluxes (per cross‑section) using a leaf model, such as the one shown below (Figure 2). In this type of schematic, the width of the arrows represents the magnitude of each energy flux, with yellow indicating absorption flux, dark blue representing electron transport flux, light blue showing trapping flux, and red depicting dissipation flux. The black dots inside the central square illustrate the number of inactive or silent reaction centres.
This type of model is highly informative, as it summarizes the state of the photosynthetic apparatus in a single image. In the example shown above, two barley cultivars were compared under high‑light and low light conditions. From the flux pattern, it becomes clear that the cultivar ‘Arabi Aswad’ (left) is more capable of handling high light, having a larger electron transport flux, lower dissipation flux, and more active reaction centers. The cultivar ‘Arabi Abiad’ (right) is better adapted to low light.
The model can also be expressed as a membrane model, showing the fluxes per reaction center (RC). See image below. Here, the effect of heating on the membrane model is described by Strasser as:
• "Absorption per active reaction center increases due to the inactivation of some RCs"
• "The ratio of total dissipation to the amount of active RCs increases due to the high dissipation of the inactive RCs"
• "Electron transport per active reaction center increases due to a thermal activation of the dark reactions"
And on the leaf model (per cross section) as:
• "Decrease of electron transport per excited cross section due to the inactivation of reaction center complexes"
• "Decrease of the density of active reaction centers RC/CS (indicated as open circles)
• "Increase of the energy dissipation per excited cross section."
• Decrease of the energy absorbed per excited cross section ABS/CS."
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