{"id":83,"date":"2017-12-01T19:29:06","date_gmt":"2017-12-02T00:29:06","guid":{"rendered":"https:\/\/www.crpa-acrp-bulletin.ca\/?p=83"},"modified":"2020-02-18T20:50:12","modified_gmt":"2020-02-19T02:50:12","slug":"comparison-cs-137-x-ray-sources-calibration-references-thermoluminescent-dosimeter-chips-student-paper-contest-winner","status":"publish","type":"post","link":"https:\/\/www.crpa-acrp-bulletin.ca\/fr\/2017\/12\/01\/comparison-cs-137-x-ray-sources-calibration-references-thermoluminescent-dosimeter-chips-student-paper-contest-winner\/","title":{"rendered":"A Comparison of Cs-137 and X-ray Sources as Calibration References for Thermoluminescent Dosimeter Chips"},"content":{"rendered":"
\n

R\u00e9sum\u00e9<\/h4>\n

Ce travail porte sur l\u2019\u00e9talonnage de dosim\u00e8tres thermoluminescents utilisant le c\u00e9sium-137 au lieu des rayons X. Les cristaux de dosim\u00e8tre utilis\u00e9s dans le programme d\u2019assurance de la qualit\u00e9 postale du minist\u00e8re du Travail de la Saskatchewan ont \u00e9t\u00e9 irradi\u00e9s en utilisant une appareil \u00e0 rayons X et un \u00e9talonneur d\u2019appareil AEA mod\u00e8le\u00a0773 utilisant du Cs 137 \u00e0 des niveaux d\u2019exposition connus. Les expositions aux rayons X ont \u00e9t\u00e9 r\u00e9alis\u00e9es \u00e0 plusieurs r\u00e9glages kVp et avec diff\u00e9rentes filtrations de faisceau pour identifier tout facteur de confusion dans la r\u00e9ponse mesur\u00e9e des cristaux de dosim\u00e8tre. On a laiss\u00e9 les cristaux irradi\u00e9s s\u2019att\u00e9nuer pendant au moins 48\u00a0heures, puis on a mesur\u00e9 en nanocoulombs l\u2019\u00e9mission lumineuse des cristaux de dosim\u00e8tre en utilisant un lecteur de dosim\u00e8tre Harshaw mod\u00e8le 5500. La r\u00e9ponse donne un r\u00e9sultat de 0,1275 \u00b1 0.0049 nC \/ mR pour les expositions aux rayons X et de 0,0772 \u00b1 0,0028 nC \/ mR pour les expositions au c\u00e9sium 137. Il semble que le kVp ou la filtration de faisceau n\u2019ont eu aucun effet sur la r\u00e9ponse du cristal. Ces r\u00e9sultats d\u00e9montrent que l\u2019application d\u2019un facteur de correction appropri\u00e9 k = 0,6056 \u00b1 0,0057 permettra l\u2019\u00e9talonnage des cristaux en utilisant une source c\u00e9sium 137.<\/p>\n<\/div><\/div><\/div>\n

Introduction<\/h2>\n

The Radiation Emitting Devices (RED) Act (Radiation Emitting Devices, 1985) regulates the manufacture, import, or sale of radiation devices within Canada; however, it is up to each province to regulate the installation, maintenance, and use of the equipment. Health Canada\u2019s Safety Code 35 (Safety Code 35, 2008) provides information on safety procedures for the installation, safe use, and control of diagnostic X-ray machines. However, with the exception of federally operated facilities, SC 35 is a guide only, and it is up to provincial regulations to provide the necessary enforcement for protection of individuals who may be exposed to radiation emitted by X-ray equipment.<\/p>\n

In Saskatchewan, the postal quality assurance (PQA) program is included in Section 16 of the Radiation Health and Safety Regulations, 2005 (Radiation Health and Safety, 2005) and specifies that operators using ionizing radiation equipment participate in the PQA program. The test package (medical pack) used in the PQA program is mailed to a hospital or dental clinic and contains a test plate containing eight thermoluminescent dosimeters (TLDs), an aluminum step wedge, and a test phantom. The medical pack is placed on top of the test phantom with the aluminum step wedge placed on top of the test phantom to simulate human body scattering. When the pack is radiographed and the TLD chips analyzed, the entrance exposure, and the half-value layer of the X-ray beam can be determined.<\/p>\n

Historically calibration of the chips has used an X-ray combined with a calibrated reference instrument. This process, however, is tedious and expensive because it is not always easy to get access to an X-ray machine for extended periods of time. A solution to this problem is to calibrate these chips using a commercial 137<\/sup>Cs (Browne & Tuli, 2007), a naturally occurring radioactive gamma ray source.<\/p>\n

X-ray and gamma ray radiations are both ionizing radiations (Cember & Johnson, 2008). However, in order to calibrate TLD chips using 137<\/sup>Cs, we need to find a factor that when multiplied gives the correct X-ray exposure for a 137<\/sup>Cs-calibrated chip. In addition, how filtration of the X-ray beam might affect this factor must be determined. The focus of this work is to measure the appropriate calibration factor to allow for in-house calibrations of the TLD chips using a 137<\/sup>Cs source.<\/p>\n

\n

\"\"<\/p>\n

Figure 1:<\/strong> Model 773 Instrument Calibrator beam profile<\/p>\n

\n

Background<\/h2>\n

To find the appropriate calibration factor, first TLD chips will be exposed using a calibrated X-ray machine for different amounts of X-ray exposures with different beam filtration settings. Then TLD chips will be analyzed using a TLD reader, the charge contained in those chips will be saved, and those TLD chips will be annealed for fresh exposures. In the second part of the experiment, the same TLD chips will be exposed using a 137<\/sup>Cs calibrator for different exposure levels. Exposed chips will be analyzed and the charge contained in them will be noted. Details of calculating exposure from the charge contained in a TLD chip is described in a later section.<\/p>\n

137<\/sup>Cs Calibrator<\/h2>\n

An AEA Technology, QSA Inc. Model 773 Instrument Calibrator (Operating Manual Model 773, n.d.) was used in this experiment. It contained a 137<\/sup>Cs source with a nominal activity of 6.142 GBq. The source was well-shielded and equipped with a collimated beam port. It has 3 attenuators with transmission factors of 0.25, 0.10, and 0.10 located at the collimator port to produce a radiation field whose intensity is uniform in any plane perpendicular to the beam axis. Figure 1 shows the beam profile.<\/p>\n

Measuring Exposure with TLD Reader<\/h2>\n

A Harshaw Model 5500 TLD reader was used for measuring the TLD chips. As TLD chips are heated, the light output is analyzed using a photomultiplier tube (PMT). The PMT provides an output current that is directly proportional to the chips radiation exposure. Exposure measured from TLD charge is calculated using Equation 1<\/p>\n

\"\"<\/p>\n

where ECC is the Element Correction Coefficient (Savva, 2010) for an individual chip, and the RCF is the Reader Calibration Factor, which converts the measured light output to a desired exposure unit, and the charge is the integrated current measured by the PMT.<\/p>\n

Not all TLDs have the same response. To correct for variation in chip response and to correlate it to the population response, the ECC is determined using Equation 2<\/p>\n

\"\"<\/p>\n

where is the average charge of a set of TLD chips, is the integrated current measured for a TLD.<\/q><\/p>\n

The RCF is calculated using Equation\u00a03<\/p>\n

\"\"<\/p>\n

where is the average integrated current measured for a set, E is the radiation exposure delivered to that set.<\/q><\/p>\n

Method<\/h2>\n

Medical and dental packs are holders of TLD chips (Figure 2). A medical pack can hold up to 8 TLD chips and a dental pack can hold up to 2 TLD chips. In this experiment, 18 medical packs and 12 dental packs were grouped into 8 sets for X-ray exposure and 3 sets for 137<\/sup>Cs exposure. While exposing medical packs, phantom slabs were used to simulate human body scattering. Phantom slabs were not used for dental packs since this is not the practice observed in the field. X-ray exposures were conducted at several levels with varying filtration parameters for each set. 137<\/sup>Cs exposures were conducted at 21.2 cm from the calibrator, and packs were exposed to 3 different exposure levels. Figure 3 shows a medical pack attached to phantom slab during 137<\/sup>Cs exposure.<\/p>\n

After exposure, TLD chips from medical and dental packs were set aside for at least 2 days in a dark environment to allow the chips to relax. During analysis, TLD chips were first preheated in an oven for 30 minutes at 100 \u00b0C to remove low-level noise from the chips. They were then cooled for 10 minutes before they were analyzed using the Harshaw 5500 TLD Reader. After analysis, chips were annealed by heating in an annealing oven for at least 1 hour at 450\u00b0C. After annealing, they were transferred to a fridge and cooled for at least 1 hour at 5\u00b0C.<\/p>\n

\n\n\n\n
<\/td>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

Figure 2:<\/strong> Medical pack (left) and dental pack (right)<\/p>\n

\n\n\n\n
<\/td>\n<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n

Figure 3:<\/strong> Set up of 137<\/sup>Cs exposure<\/p>\n

\n

Results<\/h2>\n

The PMT in the TLD reader measures the light output from the TLD chip in units of integrated current (charge). The charge contained in the TLD chips were measured for different levels of X-ray and 137<\/sup>Cs exposure. Using the measured charge, exposure levels, and average charge for each set, element correction coefficients (ECC) for each chip and a reader calibration factor (RCF) could be determined. For each set of 137<\/sup>Cs and X-ray exposures, ECC and RCFs were computed using equations 2 and 3 respectively and are shown in Table 1 and Table 2. Figure 4 shows the distribution of ECC computed from both X-ray and 137<\/sup>Cs exposures.<\/p>\n

\n

Table 1:<\/strong> 137<\/sup>Cs Measurement results<\/p>\n

\"\"<\/p>\n

\n

Table 2:<\/strong> X-ray measurement results<\/p>\n

\"\"<\/p>\n

\n

\"\"<\/p>\n

Figure 4:<\/strong> ECC distribution, x-axis shows the range of ECC; the distribution is centred around ECC value of 1<\/p>\n

\n

It can be noted that the ECC distribution is approximately a Gaussian distribution and has a similar shape for both X-ray and 137<\/sup>Cs exposures.<\/p>\n

Figure 5 illustrates the average charge measured from the chip as a function of radiation exposure for X-ray and 137<\/sup>Cs treatments. From Equation 3, the slope of these lines is the RCF. Figure 6 shows the effect of filtration and kVp.<\/p>\n

\n

\"\"<\/p>\n

Figure 5:<\/strong> Exposure versus average charge<\/p>\n

\n

\"Figure<\/p>\n

Figure 6a:<\/strong> Effect on RCF with kVp and X-ray<\/p>\n

\n

\"\"<\/p>\n

Figure 6b:<\/strong> Effect of filtration on RCF<\/p>\n

\n

The TLD chip response was measured as 0.1275 \u00b1 0.0049 nC\/mR for X-ray exposures and 0.0772 \u00b1 0.0028 nC\/mR for 137<\/sup>Cs exposures.<\/p>\n

\"\"<\/p>\n

is the correction factor relating TLD response for an X-ray exposed chip, given it is calibrated for 137<\/sup>Cs source. Neither kVp nor beam filtration appeared to have any effect on the chip response.<\/p>\n

Conclusion<\/h2>\n

\"\"A comparison of TLD chip response for X-ray and 137<\/sup>Cs exposures was conducted. A calibration factor relating 137<\/sup>Cs exposure to X-ray exposure was calculated as K = 0.6056 \u00b1 0.0057. It was found that X-ray machine settings like kVp, or beam filtration does not affect the calibration factor K. Given a TLD chip calibrated using 137<\/sup>Cs and exposed to an X-ray source, we can now multiply the obtained result from a TLD reader by K to get its equivalent X-ray exposure. Chips calibrated using 137<\/sup>Cs source can now be used in the Saskatchewan PQA program to monitor X-ray machines within the province.<\/p>\n

References<\/h2>\n

Browne E, Tuli J K. Adopted Levels Gamma for 137Cs. Nuclear Data Sheets 108,2173. 2007. Available from https:\/\/www.nndc.bnl.gov\/chart\/getdataset.jsp?nucleus=137CS&unc=nds<\/a><\/p>\n

Cember H, Johnson T. Introduction to health physics. 4th ed. New York (NY): McGraw Hill Medical 2008. p. 195.<\/p>\n

Operating Manual Model 773 Instrument Calibrator. QSA Global. n.d. Available from https:\/\/qsa-global.com\/wp-content\/uploads\/2014\/11\/773-Operating-Manual0001.pdf<\/a><\/p>\n

Safety Code 35: Safety procedures for the installation, use and control of x-ray equipment in large medical radiological facilities. Health Canada. 2008. Available from https:\/\/www.canada.ca\/en\/health-canada\/services\/environmental-workplace-health\/reports-publications\/radiation\/safety-code-35-safety-procedures-installation-use-control-equipment-large-medical-radiological-facilities-safety-code.html<\/a><\/p>\n

Savva A. Personal TLD monitors, their calibration and response [dissertation]. [Guilford (UK)]: Department of Physics, University of Surrey, 2010, p. 60. Available from http:\/\/personal.ph.surrey.ac.uk\/~phs1pr\/msc_dissertations\/msc-diss-2010\/Antonia%20Savva-%20Summer%20project%20corrected.pdf<\/p>\n

Radiation emitting devices act\u00a0(R.S.C., 1985, c. R-1). Available from http:\/\/laws-lois.justice.gc.ca\/eng\/acts\/R-1\/<\/a><\/p>\n

Radiation health and safety regulations, The. (Chapter. R-1.1 Reg 2 2005). Regina, Saskatchewan. Available from http:\/\/www.publications.gov.sk.ca\/freelaw\/documents\/English\/Regulations\/Regulations\/R1-1r2.pdf<\/a><\/p>\n

\n

\"\"Aravind Ravichandran<\/h2>\n

Originally from Coimbatore, a city in the south Indian state of Tamil Nadu, Aravind Ravichandran is a 4th year, physics major at the University of Saskatchewan.<\/p>\n

Originaire de Coimbatore, une ville dans l\u2019\u00c9tat de Tamil\u00a0Nadu, dans le sud de l\u2019Inde, Aravind Ravichandran est un \u00e9tudiant de quatri\u00e8me\u00a0ann\u00e9e \u00e0 la majeure en physique \u00e0 l\u2019Universit\u00e9 de la Saskatchewan.<\/p>\n<\/div><\/div><\/div>

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Historically, calibration of thermoluminescent dosimeter chips has used an X-ray combined with a calibrated reference instrument. This process, however, is tedious and expensive. 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