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Chlorophyll Fluorescence
> Continuous Excitation
How does a Continuous Excitation Chlorophyll Fluorimeter Measure Chlorophyll
Fluorescence?
A continuous excitation fluorimeter is designed to measure the Kautsky Induction
or Fast Chlorophyll Fluorescence Induction (Kautsky and Hirsch, 1931*).
The chlorophyll fluorimeter uses focussed, high intensity light from red LED's
to induce a fast chlorophyll fluorescence response from a dark adapted sample.
Continuous systems require the use of a special leafclip system. This is a
multi-purpose tool which provides dark adaptation for the sample (required for
the measurement of maximum photochemical efficiency), defines the measurement
area on the sample and prevents ambient light leakage into the highly sensitive
photodiode used by the instrument for chlorophyll fluorescence detection.
The Kautsky Fluorescence Induction.
If a sample is dark adapted the PSII electron acceptor pool is gradually
re-oxidised to a point where all of the PSII reaction centres are capable of
undertaking photochemistry. If that sample is then suddenly illuminated with a
high intensity light source, a rapid (approx. 1 s) polyphasic rise in
chlorophyll fluorescence may be observed which is subsequently followed by a
slow (approx. 2 min) decline in fluorescence intensity to a steady state level
of fluorescence. This induction phenomena is often referred to as the Kautsky
Induction (Kautsky and Hirsch, 1931*).
Kautsky Induction curves must be plotted on a logarithmic axis in order to
observe the polyphasic rise to the maximum chlorophyll fluorescence value. This
is due to the reactions causing the different kinetics occur typically in the
first 300 msecs of illumination.
The kinetics of the induction curve appear universally in photosynthetic
organisms including microalgae and cyanobacteria. It is therefore possible to
label the individual elements of the fluorescence rise as shown in the graph
above. The peaks are denoted by the letters O, J, I, P (please refer to the
OJIP Analysis section of the Parameters page for further details).
Fo (Fluorescence Origin) and Fm (Fluorescence Maximum) are parameters which have
long been used in measurements of chlorophyll fluorescence. From these 2
absolute values, the parameter of Fv (Variable Fluorescence) may be calculated
as the difference between the Fm and Fo levels. In turn, the Fm value may be
displayed as a function of the Fv parameter in order to give the parameter
Fv/Fm.
Fv/Fm has been used and widely accepted for many years as an indication of the
maximum efficiency of Photosystem II. It is a highly effective and sensitive
parameter which may be used as an indicator of sample stress.
The animation below represents the reaction centre states at different stages of
the Kautsky fluorescence induction. Click on the Advance Image button below to
display to the next stage in the kinetic.
Measuring the Fast Fluorescence Induction.
Chlorophyll fluorescence measurements are not absolute. The fluorescence emitted
depends upon the light intensity and the response of the plant to the new light
conditions. Many of the commonly used comparative fluorescence parameters are
ratios. It is therefore important that measurements are made in truly comparable
circumstances if data is to be used for comparison. The use of a fluorometer to
make measurements is only one aspect of good experimental design and procedure.
If Fo and Fm cannot be determined accurately, all calculated values will be
inaccurate. The accurate determination of Fo depends upon instrument design. The
measuring device should be capable of rapidly recording the fluorescence signal
induced by illumination.
Hansatech Instruments produce 2 types of continuous excitation fluorimeter,
Handy PEA and the new Pocket PEA.
Both of these systems utilise a fast data acquisition system capable of
recording every 10 microseconds. An algorithm is then used to determine a line
of best fit through the data points recorded immediately after the start of
illumination. This line is extrapolated back to time zero when illumination
commenced in order to derive Fo.
It is vitally important that the illumination should not vary in intensity
during measurement otherwise the Fo and peak fluorescence will have been
determined using different light levels and therefore cannot be compared.
The illumination must also be at full measuring intensity before measurements
commence, otherwise the early data points are recorded at varying light
intensities. This is the advantage of using LED’s as they almost instantaneously
rise to full intensity when illuminated.
In order that the maximum fluorescence signal obtained can be regarded as Fm,
the sample should be dark adapted and the light must be of sufficient intensity
to saturate the plant, so that the addition of more light would not cause
additional fluorescence. If the light is not of saturating intensity, the
fluorescence will reach a peak value, but this peak will not be the maximum
possible fluorescence signal (Fm) and should not be used for calculations of
Fv/Fm ratios.
Saturating intensities will vary from species to species, and with the period of
dark adaptation and the environmental conditions in which the plant is growing.
It is important to ensure that saturation is achieved by measuring at various
light intensities after a range of dark adaptation periods to check that the
Fv/Fm ratio cannot be increased by using higher light levels.
* Kautsky, H. and A. Hirsch (1931). Chlorophyllfluoreszenz und
Kohlensäureassimilation. Naturwissenschaften, 19, 964.
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