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Reference transfer equipment which CNSC uses for periodic verification of a and b emission rates and gamma activity measurements of traceable calibration sources includes a large area planar NaI(Tl) planar detector, small diameter dual phosphor ZnS(Ag), a large area ZnS(Ag) scintillator detector for alpha and beta counting and a large area sealed gas proportional counter.  Appendix on measurement traceability and secondary measurement standards provides details of the program for maintaining traceability of reference equipment.
 
Reference transfer equipment which CNSC uses for periodic verification of a and b emission rates and gamma activity measurements of traceable calibration sources includes a large area planar NaI(Tl) planar detector, small diameter dual phosphor ZnS(Ag), a large area ZnS(Ag) scintillator detector for alpha and beta counting and a large area sealed gas proportional counter.  Appendix on measurement traceability and secondary measurement standards provides details of the program for maintaining traceability of reference equipment.
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{| class="wikitable"
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|The  corrected meter reading ''M''  is given by:
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                                  (3)
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where ''M<sub>raw</sub>'' is the uncorrected meter  reading as read  directly from  the instrument.
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''P<sub>TP</sub>'' is the correction factor for air  density, required when the temperature and pressure of the air in the cavity of the ionization chamber differ  from the reference values of 22°C and  760.0 mm of Hg (101.325 kPa). At a temperature ''T'' (in  degrees Celsius) and pressure ''P'' (in mm of Hg) the correct ion factor can be calculated from:
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                                 (4)
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The air in the ionization chamber is assumed to be moist with the relative humidity in the range of 20% to 75%.
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''P<sub>leak</sub>'' is  the correction factor to take into account any leakage or drift  of the instrument readings in the absence of the radiation to be  measured. If the instrument reading is represented by ''M<sub>raw</sub>'' (Coulomb/s) and the leakage rate by ''B'' (Coulomb/s), ''P<sub>leak</sub>'' has the effect of replacing ''M<sub>raw</sub>'' by ''M<sub>raw</sub>'' - ''B''. The factor ''P<sub>leak</sub>'' may  be calculated from:
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                                      (5)
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The only correction factors applied at the time of  calibration are ''P<sub>TP</sub>'' and ''P<sub>1eak</sub>''. The remaining factors, as discussed below, are not generally applied because these  factors are not applicable under the circumstances of the calibration and the  quantity of interest.
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''P<sub>ion</sub>'' is  the correction factor to take into account the incomplete collection of  charge from an ionization chamber. ''P<sub>ion</sub>'' is taken to be unity because measurements with  the reference standard are conducted under the same configuration (including  the bias voltage) as those applied at NRC.
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''P<sub>pol</sub>'' is  the correction factor used to  take into account that, in general, changing the polarity of the charge being  collected results in a change in its absolute value. Calibrations are  performed at the same polarity as that used in the calibration of the  reference standard at NRC.
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''P<sub>elec</sub>'' is the  electrometer calibration coefficient.  Calibration  of the reference standard is performed at NRC for the ionization chamber and electrometer as a complete system so  there is no separate electrometer factor and therefore no associated  uncertainty.
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''P<sub>rp</sub>'' is  the correction factor to account for radial  variation in the intensity profile of the radiation field over the sensitive  volume of the ionization chamber. ''P<sub>rp</sub>'' is  taken to be unity under the circumstances of the calibration.
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|}
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