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Print version ISSN 0100-3984On-line version ISSN 1678-7099
Radiol Bras vol.39 no.6 São Paulo Nov./Dec. 2006
Energy and angular dependence of thermoluminescent materials to beta monitoring*
Sonia Garcia Pereira CecattiI; Linda V.E. CaldasII
do Trabalho e Emprego, Instituto de Pesquisas Energéticas e Nucleares/Comissão
Nacional de Energia Nuclear
IIInstituto de Pesquisas Energéticas e Nucleares/ Comissão Nacional de Energia Nuclear
Energy and angular dependences of different thermoluminescent materials were studied with the objective to verify which type of detector would be the most appropriate for beta monitoring of workers. Three types of CaSO4:Dy + teflon pellets were studied. The energy dependence was evaluated using standard beta radiation sources (147Pm, 204Tl and 90Sr+90Y). For the angular dependence study, the pellets were exposed to beta radiation of the 90Sr+90Y source, varying the incidence angle between 0° and 90°. In relation to the studied characteristics, the CaSO4:Dy + 10% C dosimeters were the most adequate for use in beta monitoring of workers.
Key words: Thermoluminescent dosimetry; Beta radiation; Angular dependence; Energy dependence.
The increasing use of (sealed and non-sealed) beta radiation sources in medicine, industry and research implies the necessity of a metrologically reliable dose measurement in workers exposed to this type of radiation.
The value of dose limits to be determined for occupational exposure in beta radiation fields is the equivalent dose on 1 cm² of the evaluated skin, independently from the radiation-exposed area. However, a new denomination is being internationally suggested for this value which would be denominated radiation weighted dose(1).
Beta particles with energies of approximately 60 keV may reach a 0.07 mm-depth in the tissue. A detector for radiation beta monitoring must be able to evaluate beta radiation dose with energies higher than 60 keV(2).
The determination of extremity doses usually is made by means of thermoluminescent detectors because of their small dimensions. For measuring the equivalent dose in the skin, the detector must be thin, in order to avoid a significant radiation attenuation(3). However, the response in the majority of thermoluminescent dosimeters depends on the radiation energy and the irradiation geometry.
The present study objective was to analyze the energy and angular dependence of different thermoluminescent materials for an appropriate choice of the material to be employed in workers occupationally exposed to beta radiation.
MATERIALS AND METHODS
Three types of CaSO4:Dy + teflon thermoluminescent dosimeters(46), produced by the Laboratory of Thermoluminescent Materials at Instituto de Pesquisas Energéticas e Nucleares (IPEN) were utilized for radiation detection. Table 1 presents the physical characteristics of the studied CaSO4:Dy + teflon samples. These samples were submitted to a one-hour thermal treatment process at 300°C for reutilization purposes.
The beta radiation secondary standard system of IPEN Laboratory of Instruments Calibration, with Buchler GmbH & Co (Germany) 90Sr+90Y, 204Tl and 147Pm sources, was employed for irradiations (Table 2). These sources calibration is certified by the German primary-standard laboratory Physikalisch-Technische Bundesanstalt (PTB).
The detectors were irradiated in a 15 mm-thick polymethylmethacrylate phantom covered with a 1.20 mg.cm2 superficial density plastic film.
The thermoluminescent reader system employed was the Harshaw Nuclear System 2000A/B model, at a linear heating rate of 10°C.s1 and a 26 s reading cycle with a 4.0 l.min1 N2 constant flow. The three studied materials presented a dosimetric peak at 220°C. The area under the thermoluminescent curve was integrated into the interval between 140°C and 240°C.
The energy dependence of all the CaSO4:Dy + teflon samples was analyzed by means of standard 90Sr+90Y (3.5 mGy), 240Tl (1.8 mGy) and 147Pm (8.5 mGy) beta radiation sources. Thermoluminescent responses were normalized for the 90Sr+90Y radiation response. Additionally, the measures were normalized for a same absorbed dose (3.5 mGy).
Figure 1 shows the three CaSO4:Dy detectors energy dependence. The results are presented in terms of thermoluminescent response/unit of beta dose in the tissue related to the 90Sr+90Y beta radiation.
The CaSO4:Dy + teflon (50 mg) and CaSO4:Dy + teflon (20 mg) samples presented practically the same high energy dependence, while the CaSO4:Dy + teflon + 10% C samples presented a 60% energy dependence in the studied energy interval. The results compare to those obtained for CaSO4:Tm (60 µm) and CaSO4:Tm (70 µm) by Caldas(7), and for LiF (0.9 mm), LiF (0.4 mm), MgB4O7:Dy and LiF (Vinten), by Christensen and Prokié(8).
The angular dependence of the three types of CaSO4:Dy + teflon dosimeters was analyzed for three different incidence angles between 0° and 90°, in 90Sr + 90Y (3.5 mGy) beta radiation fields. The Figure 2 presents the three detectors thermoluminescent response as a function of the radiation incidence angle.
The thermoluminescent response presented an accentuated angular dependence from 45° for all the types of materials included in the present study. This is the expected behavior for the majority of thermoluminescent dosimeters. The CaSO4:Dy + 10% C pellets have shown more sensitivity than the other two materials.
Energy and angular dependence results obtained for different thermoluminescent dosimeters exposed to beta radiation emphasize the importance of utilizing thin detectors for determination of the beta radiation dose in the skin.
CaSO4:Dy + 10% C pellets have presented better energy and angular dependence results for beta radiation monitoring.
The authors express their gratitude to Dr. L.L. Campos for providing thermoluminescent samples; to Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq) and to Fundação de Amparo à Pesquisa do Estado de São Paulo (Fapesp) for the partial financial support.
1. ICRP International Commission on Radiological Protection. 2005 Recommendations of the International Commission on Radiological Protection. (In press). [ Links ]
2. Francis TM, O'Hagan JB, Richards DJ, Driscoll CMH. Responses of thermoluminescent materials to beta radiation and low energy photons. Radiat Prot Dosim 1986;17:8992. [ Links ]
3. Berus D, Cobens P, Buls N, Van den Broeck M, Van Holsbeeck G, Vanhavere F. Extremity doses of workers in nuclear medicine: mapping hand doses in function of manipulation. Proceedings of 11th International Congress of the International Radiation Protection Association. Madrid, Spain, 2328 May, 2004. [ Links ]
4. Campos LL, Lima MF. Dosimetric properties of CaSO4:Dy teflon pellets produced at IPEN. Radiat Prot Dosim 1986;14:333335. [ Links ]
5. Campos LL, Lima MF. Thermoluminescent CaSO4:Dy tefon pellets for beta radiation detection. Radiat Prot Dosim 1987;18:9597. [ Links ]
6. Campos LL. Graphite mixed CaSO4:Dy TL dosemeters for beta radiation dosimetry. Radiat Prot Dosim 1993;48:205207. [ Links ]
7. Caldas LVE. Alguns métodos de calibração e de dosimetria da radiação beta. (Tese de Doutorado). São Paulo: Universidade de São Paulo, 1980. [ Links ]
8. Christensen P, Prokié M. Energy and angular response of TL dosemeters for beta ray dosimetry. Radiat Prot Dosim 1986;17:8387. [ Links ]
Dra. Sonia Garcia Pereira Cecatti
Rua Capote Valente, 710, Pinheiros
São Paulo, SP, Brazil 05409-002
Accepted after revision October 18, 2005.
* Study developed at Instituto de Pesquisas Energéticas e Nucleares/Comissão Nacional de Energia Nuclear, São Paulo, SP, Brazil.