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216    CHAPTER 16 Nuclear plant instrumentation















                         FIG. 16.3
                         A self-powered neutron detector.

                            Since the appearance of the beta particle in a self-powered detector must wait for
                         radioactive decay of the emitter, the measurement is not instantaneous. So, the mea-
                         surement experiences a time lag that depends on the half-life of the emitter. Also, the
                         sensor calibration changes as the absorber is consumed by neutron absorptions.


                         16.2.1.4 Scintillation detectors
                         Scintillation detectors contain material that emits light upon absorbing a neutron (see
                         Fig. 16.4). The sensor monitors the light intensity and converts that signal into
                         neutron flux.

                         16.2.1.5 Gamma thermometers
                         Fig. 16.5 shows the general layout of a gamma thermometer.
                            The sensor contains a differential thermocouple that measures the temperature
                         difference between two locations inside the sensor. One location is insulated and
                         the other is un-insulated. Heat deposited (mainly by gamma rays) inside the sensor
                         causes the temperatures at the two locations to be different because of different heat
                         transfer resistances. Following equations describe the principle of a gamma
                         thermometer.



















                         FIG. 16.4
                         A scintillation detector.
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