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1.
Health Phys ; 107(5): 395-402, 2014 Nov.
Article in English | MEDLINE | ID: mdl-25271929

ABSTRACT

A method is presented that provides a way to calculate the unknown activity of a source by using experimental exposure rate measurements from an ion chamber and exposure rates calculated using the MCNP radiation transport code. The method consists of fitting experimental data to MCNP results with both data sets in the form of (Equation is included in full-text article.)where r is the distance from the source at which the measurement was taken, X˙ is the exposure rate, and An is an assumed nominal activity of the source. The fit is done by calculating a correction factor for the nominal activity that shifts the experimental data to match the MCNP results. The actual activity of the source in question is found by multiplying the assumed nominal activity by the activity correction factor. The method was used to calculate the activities of the three Cs sources used in the Ohio Emergency Management Agency's instrument calibration range. It was found that the activities were less than the decay-corrected nominal activities by factors ranging from 3% to 10%.


Subject(s)
Radiation Monitoring/standards , Radiometry/methods , Calibration , Cesium Radioisotopes/analysis , Computer Simulation , Humans , Models, Theoretical , Ohio , Radiation Dosage , Radiation Monitoring/methods , Radiometry/instrumentation , Reproducibility of Results
2.
Health Phys ; 105(3): 261-270, 2013 Sep.
Article in English | MEDLINE | ID: mdl-30522250

ABSTRACT

The method presented provides an alternative to the shadow shield method for experimentally measuring the contribution due to scattering radiation in a calibration range. Scattering of 0.6616 MeV photons from a Cs irradiator in a calibration range does not only occur due to the walls and floor of the range. It also occurs due to the source material itself, its encapsulation, the brass cup that holds the source, the two stainless tubes that surround the source capsule and the brass cup, and the irradiator structure that surrounds the aforementioned objects. The shadow shield method underestimates this scattering radiation that originates in the irradiator. By measuring the uncollided effective activity using a CZT detector and a total effective activity using a survey meter, the contribution of scattered radiation (including all of the abovementioned sources of scatter) to the effective source activity is able to be measured. In this paper, the measured mean effective source activities for a Cs irradiator in a calibration range are reported for a CZT detector and a survey meter. The measured activities are compared among themselves and with the results of MCNP calculations. From these comparisons, the new alternative method for measuring the scatter contribution was validated by agreement in both the MCNP calculations and experimental measurements that scattering contributed about 28% to the overall effective activity of the range.

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