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Geiger-Mueller detector detectors

Detectors include (1) Geiger-Mueller tube, (2) ionization chambers, (3) scintillation counters, (4) proportional counter, (5) electron-multiplier tubes, and (G) nondispersive detectors using cooled lithium-drifted Si detectors, See Fig. 3... [Pg.1759]

Radioisotope detection of P, 14C, and Tc was reported by Kaniansky et al. (7,8) for isotachophoresis. In their work, isotachophoretic separations were performed using fluorinated ethylene-propylene copolymer capillary tubing (300 pm internal diameter) and either a Geiger-Mueller tube or a plastic scintillator/photomultiplier tube combination to detect emitted fi particles. One of their reported detection schemes involved passing the radiolabeled sample components directly through a plastic scintillator. Detector efficiency for 14C-labeled molecules was reported to be 13-15%, and a minimum detection limit of 0.44 nCi was reported for a 212 nL cell volume. [Pg.61]

E. Because of the weak beta radiation, tritium is NOT readily measured by the Geiger-Mueller counter used with most fielded radiac instruments and requires wipe testing swipes and a liquid scintillation detector to determine the level of contamination. [Pg.106]

Hans Geiger worked in Ernest Rutherford s laboratory manually and meticulously counting a-particle scintillations for the famous experiments that led to the discovery of the nucleus. Because of this work, he developed an a-particle detector. After World War I, Geiger developed the modern Geiger-Mueller counter and worked until his death to increase its speed and sensitivity. [Pg.1082]

Gas-fllled detector systems collect and record the electrons freed from gaseous atoms and molecules by the interaction of radiation with these atoms and molecules. The systems have been classified into the primary categories of ionization chambers, proportional counters, and Geiger-Mueller (G-M) counters. The detectors have a variety of designs, but essentially consist of a chamber, which serves as the cathode, and a center wire, which serves as the anode. The electrical field is characterized by chamber shape and radius, the wire radius, and the applied voltage (Knoll 1989). The chamber is filled with a gas and a potential is applied between the two electrodes. The configuration of the system is shown in Fig. 2.10. [Pg.29]

Material around the source and detector, notably the detector housing, cause scattering into the detector. The opportunity for scattering into the detector increases when the source is more distant. This scattering adds a few percent to the count rate for end-window Geiger-Mueller (G-M) detectors when the sample is 2 cm or more distant (Zumwalt 1950), but little for gas-flow proportional counters with the sample only about 0.3 cm from a relatively large window. Scattering, attenuation. [Pg.139]

Geiger-Mueller (G-M) counter A gas-filled ionization detector operating in the Geiger-Mueller applied voltage region. [Pg.427]

The area radiation monitoring system i II system consisting of two Rack Units possible) measuring channels. Each me of a model DAl-6 GM detector assembly 8 electronic channel. Units needing radiation level and a local alarm also indicator. All units have a range of mR/hour and use a geiger-mueller detec radiation. These units will continue 1000 R/hour fields. [Pg.63]

Detector Geiger Mueller Radiation Detected gamma Alarm Set Points (mrem/hr) ... [Pg.66]

Scintillation Detector Ionization Chamber Geiger-Mueller tube... [Pg.451]

Which of the following best describes the reason for the high sensitivity of a Geiger-Mueller tube radiation detector ... [Pg.464]

Electronic Dosimeters — Electronic dosimeters have been available since the early 1980s. These devices use energy-compensated Geiger-Mueller tubes or solid-state detectors with supporting electronics in a package typically the size of a deck of playing cards. Features vary with respect to size, ruggedness, user control, display of accumulated dose and/or dose rate, alarm set point, battery life, computer interface, etc. f I i... [Pg.40]

The sulfur threshold detector is used to measure the integrated fast flux above 2.9 MeV. In Part B, the equation used to determine the fast flux is derived in conjunction with a phosphorus-pellet calibration of the Geiger-Mueller counter ... [Pg.633]

GeIger-Mueller tubes scintillation detectors semiconductor detectors... [Pg.250]

This chapter presents a description of difficulties with the detectors most frequently used in advanced nuclear spectrometry. Although a detector is directly, and sometimes Inseparably, connected to electronics, discussions on the behaviour and faults of electronic parts is avoided for this the reader should refer to Chapters 5 and 11. Furthermore, attention is devoted entirely to the high resolution detectors simple detectors, such as Geiger-Mueller or scintillation, are described in Chapter 11. Accordingly, the chapter starts with the high-resolution x-ray and gamma-ray detectors. [Pg.279]


See other pages where Geiger-Mueller detector detectors is mentioned: [Pg.162]    [Pg.179]    [Pg.1411]    [Pg.2322]    [Pg.257]    [Pg.66]    [Pg.155]    [Pg.340]    [Pg.341]    [Pg.288]    [Pg.92]    [Pg.376]    [Pg.464]    [Pg.222]    [Pg.203]    [Pg.621]    [Pg.627]    [Pg.258]   


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