12 Automatic Analysers in Oenology 651
12.2.1.2 The Peristaltic Pump
The peristaltic pump is at the heart of the FIA analyser; containing 20–30 channels
in general, it regulates all liquid movements in the analytical circuit. Each channel
is constituted of a tube, composed generally of PVC which is pressed by a series
of rotating rollers against a circular surface to create pressurised flow. The flow
rate within each tube depends on its internal diameter which varies from 0.005 to
0.110cm. In this way the rhythm of introduction of the sample and different reagents
may be controlled with a high degree of precision.
12.2.1.3 The Analytical Cassette
This component contains all the elements of the analytical circuit. It is here that the
sample may be subjected to different treatments according to the requirements of
the analysis, i.e.
Dilution
Dialysis
Addition of reagent
Mixing
Distillation
Passage through a water bath (variable temperature and duration)
Part of the circuit may be thermostatted
From the time it exits the pump the liquid flow in the analytical circuit is seg-
mented regularly by air bubbles every 1 or 2cm; these bubbles are formed when
the needle passes from the rinsing vial to the sample vial. Due to surface tension
forces, the air bubbles prevent the diffusion of compounds in solution from one
section of the liquid column formed between two air boluses and the preceding or
succeeding column. In addition, the air bubble wipes the internal wall of the glass
or PVC tube, thus minimising the problem sample-to-sample cross contamination.
A second generation of FIA technology has been proposed, based on micro-flow
techniques which obviates the need for segmentation. This technology has remained
rather marginal due to problems with clogging of the tubes which can be difficult
to clear. Otherwise, the analytical principles remain the same as for segmentation-
based instruments.
12.2.1.4 The Detector
The most widely-used detectors in FIA methods are colorimetric.
12.2.1.5 The Recorder
A property of an analyte in the sample is converted by the detector into a signal
whose intensity is proportional to the analyte’s concentration. The signal is recorded
in the form of peaks whose height is proportional to the concentration.