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handbook of modern sensors

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17.5 Complex Sensors 515<br />

Fig. 17.12. Simplified configuration <strong>of</strong> an optical CO 2 sensor.<br />

The slots allow CO 2 to diffuse into the chamber. The bottom parts <strong>of</strong> the chambers<br />

are made <strong>of</strong> glass. Both wafers, A and B, form optical waveguides. The test chamber<br />

is filled with a reagent, and the reference chamber is not. The sample part <strong>of</strong> the<br />

sensor monitors the optical absorbency <strong>of</strong> a pH indicator in a dilute solution, where<br />

the optical absorbency changes in accordance with the Beer–Lambert law:<br />

I = I 0 exp [−α (λ, pH) dC] , (17.12)<br />

where I is the transmitted intensity, I 0 is the source intensity, a is the molar absorptivity,<br />

λ is the wavelength, C is the concentration, and d is the optical path length.<br />

Ambient CO 2 equilibrates with the bicarbonate ion buffer system in the reagent,<br />

as it is done in the traditional Severinghaus–Stow CO 2 electrode. Equilibrium among<br />

CO 2 ,H 2 CO 3 , and HCO 3 produces a change in the pH <strong>of</strong> the solution. The solution<br />

contains a pH indicator Chlorophenol Red, which exhibits a sharp, nearly linear<br />

change in the optical absorbency at 560 nm from pH 5 to pH 7. The buffer concentration<br />

can be selected to exhibit pH changes in the range for partial CO 2 pressures from<br />

0 to 140 torr. Because the buffer pH varies linearly with the log <strong>of</strong> the partial pressure<br />

<strong>of</strong> carbon dioxide (pCO 2 ), changes in optical absorbency can also be expected to vary<br />

linearly with the log <strong>of</strong> pCO 2 .<br />

The LED common for both halves <strong>of</strong> the sensor transmits light through the pHsensitive<br />

sample to a test photodiode (PD1). The second photodiode (PD2) is for<br />

reference purposes to negate variations in the light intensity <strong>of</strong> the LED. For temperature<br />

stability, the sensor should operate in a thermally stable environment.<br />

Fiber-optic chemical <strong>sensors</strong> (Fig. 17.13) use a chemical reagent phase to alter<br />

the amount or wavelength <strong>of</strong> light reflected by, absorbed by, or transmitted through<br />

a fiber waveguide (see also Fig. 4.17A <strong>of</strong> Chapter 4). A fiber-optic sensor typically<br />

contains three parts: a source <strong>of</strong> incident (pilot) light, an optrode, and a transducer<br />

(detector), to convert the changing photonic signal to an electrical signal. It is the optrode<br />

that contains the reagent phase membrane or indicator whose optical properties<br />

are affected by the analyte [19].<br />

The location <strong>of</strong> the reagent, and the specific optical characteristic that is affected<br />

by it, vary from one type <strong>of</strong> optical sensor to another. Simple polymer-coated fibers

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