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Regional Basic Professional Training Course in Korea

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schematically <strong>in</strong> Fig. (2.7).<br />

❙ 77 ❙<br />

2. Radiation Protection<br />

As a charged particle passes through the gas it ionizes atoms and forms with<strong>in</strong> the<br />

chamber, ion pairs composed of the residual positively charged atoms and the negatively<br />

charged electrons. The positive and negative charges thus produced have a force applied<br />

to them by the voltage; positively charged particles tend to move toward the chamber<br />

walls and negatively charged particles toward the central electrode, because, of course,<br />

opposite charges attract. The central electrode is often referred to as the collector.<br />

The ma<strong>in</strong> differences among the three types of gas‐filled detectors lie <strong>in</strong> the gas used, the<br />

pressure at which that gas is ma<strong>in</strong>ta<strong>in</strong>ed with<strong>in</strong> the chamber, and the voltage level that is<br />

ma<strong>in</strong>ta<strong>in</strong>ed between the central electrode and walls of the chamber. Fig. (2.8) is a graph<br />

of the voltage versus the amount of ionization that occurs.<br />

Fig. (2.7) A Gas‐Filled Detector. The <strong>in</strong>com<strong>in</strong>g ioniz<strong>in</strong>g A enters the detector B and causes<br />

ionization. The residual positive ions move toward the chamber walls D, which are<br />

negatively charged, and thus form the cathode. The electrons (negative ions) move<br />

toward the central wire E, which is positively charged and thus forms the anode or<br />

collector. The central wire and the chamber walls are electrically isolated from each<br />

other by the <strong>in</strong>sulat<strong>in</strong>g material F. The voltage level V is ma<strong>in</strong>ta<strong>in</strong>ed by the power<br />

source P. The resistor R capacitor C circuit <strong>in</strong>tegrates <strong>in</strong>dividual pulses from the<br />

electrons.

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