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Page Title: Figure 14 Simple Ionization Circuit
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IONIZATION CHAMBER
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Instrumentation and Control 2 of 2
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Figure 15   Recombination and Ionization Regions

Radiation Detectors IONIZATION CHAMBER Figure 14 illustrates a simple ionization circuit consisting of two parallel plates of metal with an air space between them.   The plates are connected to a battery which is connected in series with a highly sensitive ammeter. Figure 14   Simple Ionization Circuit If  a  radioactive  source  that  is  an  emitter  of  beta  particles  is  placed  near  the  detector,  the  beta particles will pass between the plates and strike atoms in the air.  With sufficient energy, the beta particle causes an electron to be ejected from an atom in air.   A single beta particle may eject 40 to 50 electrons for each centimeter of path length traveled.   The electrons ejected by the beta particle  often  have  enough  energy  to  eject  more  electrons  from  other  atoms  in  air.    The  total number of electrons produced is dependent on the energy of the beta particle and the gas between the plates of the ionization chamber. In general, a 1 MeV beta particle will eject approximately 50 electrons per centimeter of travel, while a 0.05 MeV beta particle will eject approximately 300 electrons.   The lower energy beta ejects more electrons because it has more collisions.  Each electron produced by the beta particle, while traveling through air, will produce thousands of electrons.   A current of 1 micro-ampere consists of about 1012  electrons per second. If 1 volt is applied to the plates of the ionization chamber shown in Figure 14, some of the free electrons  will  be  attracted  to  the  positive  plate  of  the  detector.    This  attraction  is  not  strong because 1 volt does not create a strong electric field between the two plates.   The free electrons will tend to drift toward the positive plate, causing a current to flow, which is indicated on the ammeter.   Not all of the free electrons will make it to the positive plate because the positively charged  atoms  that  resulted  when  an  electron  was  ejected  may  recapture  other  free  electrons. Therefore, the ammeter will register only a fraction of the number of free electrons between the plates. Rev. 0 Page 29 IC-06

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