The ARN Critical Dosimetry System. Gregori, B.N.; Papadópulos, S.; Cruzate, J.A.; Equillor, H.E. and Kunst, J.J.

Transcription

1 The ARN Critical Dosimetry System Gregori, B.N.; Papadópulos, S.; Cruzate, J.A.; Equillor, H.E. and Kunst, J.J. Presentado en: 11 th International Congress on the International Radiation Protection Association. Madrid, España, mayo 2004

2 THE ARN CRITICAL DOSIMETRY SYSTEM Gregori, B.N.; Papadópulos, S.; Cruzate, J.A.; Equillor, H.E. and Kunst, J.J. Autoridad Regulatoria Nuclear Argentina Abstract The ARN critical dosimetry system is shown in this work. It includes personal and area dosemeters, and the information of typical spectra. The spectra of the critical facilities in our country are characterised by measurements with our Bonner Sphere System (BSS) or by computational methods in order to evaluate the dose in each case with the actual spectrum. The personal and area dosemeters are able to evaluate the gamma and neutron contributions. The detectors used are thermoluminiscents, (TLD) 7 Li:Mg,Ti for gamma and threshold detectors (Indium and sulphur pellets) and activation detectors Au (bare and Cd cover) for neutron. The Gamma-ray spectrometry is made with GeHp and MCA (Canberra) calibrated with 133 Ba and 137 Cs sources. The Beta-ray counting is made with a Geiger Muller (LND)(8%) with an electronic counter prototype developed in Argentina. The system is calibrated with the tioacetamida-technique carried out in our chemistry laboratory. The TLD are calibrated in Argentine SSDL with 60 Co source, free in air. The calibration curve has been extended up to 10Gy. The neutron fluence distribution is obtained considering the thermal region as a Maxwellian distribution with a modal energy of ev and the intermediate region with a 1/E spectrum from 0.5 ev to E200 kev. The basic data are the measured activities in the gold foils. The fast neutron fluence is calculated considering the mean cross section for the selected spectrum over the energy range. The basic data are the measured activities in indium foil and sulphur pellets with threshold energy of 1.7MeV y 2.5MeV respectively. The neutron kerma dose, the recoil charged particle dose and the contribution of the 1 H(n, γ) 2 H dose component, are calculated applying the dose conversion factors published in TRS211. The area dosemeter gives the gamma incident radiation kerma, and the personal dosemeter, the gamma total dose. This system has participated at the International Intercomparison of Criticality Accident Dosimetry Systems at Silene Reactor in 2002, showing a good performance. 1. Introduction Critical accident dosimetry is required to screen and provide a rapid personnel dose assessment following a criticality accident. For this requirement specific techniques are used to determine both neutron and gamma contributions of the acute radiation dose to the body. In order to evaluate the dose in a critical accident the Physical Dosimetric Group (PDG) of Nuclear Regulatory Authority has elaborated a procedure to attend the situation based on international recommendations and its own experience. PDG has developed a critical dosimetric system, (SDC), personal and area dosemeters, and is still working in the neutron spectrum facility characterisation using the Multisphere Spectrometric System (MSS). In this framework the performance of the system was evaluated in the International Intercomparison of Criticality Accident Dosimetry Systems at Silene in Valduc (France). The objectives were to test and evaluate the SDC under realistic conditions in order to establish the dose-assessment performance for different quality radiation fields (different neutron spectra and neutron to gamma dose ratios). 2. Dosimetry System The SDC ( personal and area dosemeters ) has gamma and neutron detectors. The gamma-ray dosemeter is based on TLD, 7 Li:Mg, Ti (TLD-700, Bicron).

3 The neutron dosemeter is based on activation detectors: gold foil (bare and Cd covered), and threshold indium foil and sulphur pellet. The reactions considered are: 197 Au(n,γ) 198 Au 115 In (n,n ) 115m In 32 S (n, p) 32 P The main characteristics of the activation detectors used are showed in the Table 1: Table 1: Components of Activation Detectors COMPONENTS OF ACTIVATION DETECTORS Material detector Mass (g) Gold (bare) 0.05 Gold (Cd) 0.05 Indium 0.2 Sulphur 1.08 Isotopes to be measure Energy (MeV) 198 Au (γ) m In (γ) P (β) 1.7 The foils have a thickness of 0.02 mm and a diameter of 12 mm, meanwhile the pellets dimension is 0,04 mm and 16mm respectively. 3. Measurements procedures The gamma-ray spectrometry is made with a GeHp and a MCA (Canberra). The system is calibrated with 133 Ba and 137 Cs sources. The beta ray counting is performed with a Geiger Muller (LND) with an 8% efficiency. It works with an electronic counter and associated software (NuclearLab) [1]. The system is calibrated with the tioacetamida technique, improved in Argentine [2]. The gamma-ray dosemeters are processed in a TLD reader, Bicron-Harshaw 3500QS. The detectors are calibrated in the Argentine Secondary Standard Dosimetry Laboratory with a 60 Co source, free in air. The calibration curve has been extended up to 10Gy. 4. Evaluation procedure In order to obtain the neutron fluence distribution, the following assumptions were made: For thermal and intermediate-energy fluences assessment, a Maxwellian distribution has been chosen: with a modal energy of ev for thermal, with a 1/E spectrum for the intermediate-energy region from 0.5 ev (E Cd ) to E 2 (200 kev),. The measured activities in the gold foils, bare (A Au ) and under cadmium (A AuCd ), are converted into incident fluence as shown below [3]:

4 Thermal fluence: Intermediate fluence: th 1.13 λnσ o [ A A ] (1) Au AuCd int Φ epi ln( E2 / E Cd ) (2) Φ epi A AuCd λnri (3) Where, λ is the decay constant for 198 Au; N is the number of Au atoms; σ 0 is the cross-section of gold at 2200 m/s; RI is the resonance integral from E Cd to E 2. For fast neutron fluence distribution it is necessary to make several assumptions or to measure previously the critical facility characteristic spectrum. The spectra of several Argentine critical facilities have been measured with the MSS [4]. The basic data is obtained from indium foil and sulphur pellets with threshold energy of 1.7 and 2.5MeV respectively. The following expression is used to calculate the fast neutron fluence E > E act ( i ) λn A < σ > ( i ) i ( E > Eact ( i ) (4) Where i means indium or sulphur reactions; A(i) is the activity, E act(i) is a i- threshold energy and <σ> i (E>Eact(i) is the mean cross section of i for the selected spectrum till E act(i). The theoretical calculation of the apparent cross section, <σ> i (E>Eact(i) for a given neutron reaction, is obtained solving the following expression: Emax Emin < σ > i( E> Eact( i) Emax ( E) σ ( E) Emin ( E) (5) Where (E) is the differential fluence of the particular spectrum selected and the neutron energy E ranges between energy points of interest. The total neutron fluence is calculated considering the apparent cross section of the reaction i for the selected spectrum over all the energy range. 4. Dose assessment The gamma dose is calculated as: Dγ L(nC ). S (nc/gy). S k (6) Where L (nc) is the net TLD reading; S (nc/gy) is the 60 Co calibration factor in free air and

5 S k is the individual sensitivity factor. The net TLD readings have been also corrected for fast neutron influence [3]. The personal dosemeter gives the gamma total dose (Kγ, backscatter component and 1 H(n, γ) 2 H), corrected by the tissue energymass absorption coefficient ratio. The area dosemeter gives the gamma incident radiation kerma, Kγ. The thermal and intermediate neutron dose is calculated as follow [3]: Thermal neutron dose, D th 5, th (7) Intermediate neutron dose, D int 1, int 1, Φ epi Where th is the total neutron fluence, int is the total intermediate fluence and Φ epi is the fluence per unit lethargy, assumed to be constant over this energy region. In order to calculate the neutron kerma dose, the recoil charged particle dose and the 1 H(n, γ) 2 H dose components in all the energy range, the dose conversion factors are obtained from the selected spectrum. The dosimetric quantities are calculated by: D d k ( E) ( E) ( E) (8) Where d k is a fluence to dose conversion factor [3] and (E) the total fluence. 5. Intercomparison The performance of the system was evaluated in the International Intercomparison of Criticality Accident Dosimetry Systems in the Silene Reactor (Valduc, France) in During the exercise, the participants determined with their dosemeters, for each pulse, both gamma and neutron components of the dose, giving a first data. These evaluation results were informed to the organisers to compare with those given by the other participants. The Silene staff was in charged of positioning the participants dosemeters. The area dosemeters were located in free air, and the personal dosemeters were on an anthropomorphic phantom. Both were located on 4m arc from the reactor at 1.2m height The experience consist of three independent irradiations, two were free evolutions with bare and lead shield reactor configurations respectively and another one was a steady evolution with a lead shield reactor configuration. After the irradiation, the dosemeters were stored until the rate exposition was low enough to manipulate them according with the international radiology protection recommendations The SDC results were obtained in 24 hours. The data request were not only dose quantities but also reaction rates per atoms. The gamma- ray spectrometry and beta measurements were made in Valduc with our equipment, but the TLD were processed with a Harshaw Bicron 3500QS that belongs to Canada group. The TLD used for gamma calibration were carried from Argentina. In order to evaluate the total neutron dose, the Silene spectrum reactor was selected from published data [5]. The assessment was made considering the mean spectrum resulting from experimental spectra determined by National Physical Laboratory (NPL), Fontenay-aux-Roses (ISPN) and Harwell (AEA Technology). The specific neutron reactions analysed were those related to the criticality detectors used at measurements. The reference measurements were made under free air condition. However, the neutron

6 measurements are expressed, not only in terms of neutron kerma (K n ) appropriate to free air conditions, but also in terms of the dose recoil charged particle and the 1 H(n,γ) 2 H component of the dose appropriate to dosemeters exposed on the front of the phantom. Because of that, the calculation of the apparent values of these quantities was made applying formula (8). The components thermal and intermediate of the dose were evaluated applying equation [7]. The table 2 shows the dosimetric results to the reference data ratio [6] for each pulse and reactor configuration. Table 2: Performance of the ARN Critical Dosimetric System in the International Intercomparison of Criticality Accident Dosimetry Systems in Silene Reactor Area Dosemeter Personal Dosemeter Bare - Free evolution Lead - Steady state Lead - Free evolution Quantities ARN / reference ARN / reference ARN / reference neutron kerma 1,16 1,01 1,02 neutron recoil dose 1,17 1,01 1,03 neutron 1 H(n,γ) 2 H 0,85 0,78 0,82 incident γ dose 0,80 1,66 1,57 neutron kerma 1,30 1,03 1,08 neutron recoil dose 1,30 1,01 1,08 neutron 1 H(n, γ) 2 H 0,94 0,81 0,86 total γ dose 0,84 1,06 1,00 Same methods have been used in measurement, calculations and conversion factor to evaluate area and personal dosemeters. For the lead shielded configurations, there is good agreement between the neutron kerma and neutron recoil dose values to the reference values, better than 10%, for both area and personal dosemeter. For the bare configuration, the neutron kerma and neutron recoil dose measured by the area dosemeter agrees with the reference better than 20%., meanwhile the personal dosemeter over measured the neutron kerma and the neutron recoil dose, with no further explanation yet. In the case of lead reactor configurations, the incident gamma dose is over evaluated. The published results [7] show that the ratio of the mean value of the laboratories to the reference are 1,73±0.4(1σ)in steady state and 1,57 ±0.46(1σ)in free evolution, and the Argentine data are included in those ranges. These results show the difficulties of measuring the gamma-ray dose in mixed fields with lead shield configurations. There is a good agreement in the measurement of total gamma-ray dose (better than 20%). The thermal and intermediate contributions to the total neutron dose were less than 12%. 6. Conclusions The DCS showed a good performance in the intercomparison not only about the evaluation results but also in the capability of giving them in a short time. The dose given at the Valduc meeting was about 5% higher than the final reported results.

7 The DCS response is strongly dependent of the spectrum selected, variation between the facility spectra obtained by different method influenced both the cross section and the dose calculation. As the Silene spectrum is fission one, the best detector to evaluate the neutron dose is based on the Indium reaction. The DCS assessment method can be applied even though one of the activation measurements (indium or sulphur reactions) failed because it is a redundant methodology. In this exercise, as the thermal and intermediate dose components do not contribute significantly, the performance in terms of the dose has not been analysed. Performance criteria for criticality accident dosimetry systems recommended for doses greater than 250mGy [5] that the neutron and gamma components of dose uncertainties should be less than ±25% each. If it assume that the true dose is given by the reference dose (±10%) then the data evaluated satisfy the criteria except in the case of lead configuration - incident gamma kerma and of bare configurationpersonal neutron dose. 7. Acknowledgments We want to thanks the help giving by the Silene Staff to solve the equipment problems and to Dr, Louise Prud Homme-Lalonde (Canada) that lets us used their TLD reader. 8. Bibliography 1- NuclearLab. Counter NLA-003. Technical Report.. Argentina (2002). 2- Equillor, H; Papadópulos, S; Gregori, B., Activity determination of 32 P in sulphur critical dosemeters by liquid centelleo. IRPA, Lima- Perú (2002). 3- International Atomic Energy Agency. Dosimetry for Critical Accident. Technical Reports Series No. 211, Vienna, Gregori, B., Papadópulos, S., Cruzate J.A., Kunst, J.J., Multisphere Neutron Spectrometric System With Thermoluminescent Detectors: Sensitive Improvement.Rad. Prot. Dos. Vol 101, Nos 1-4, pp (2002). 5- Medioni, R., Delafield H.J., An International Intercomparison of Criticality Accident Dosimetry Systems at the Silene Reactor, Report HPS/TR/H/3(95), Valduc, Dijon, France, 7-18 June Assilineu, B., Trompier, F., Texier, C., Itié, C., Medioni, R., Tikunov, D., Muller, H., Pelcot, G., Reference Dosimetry Measurements For The International Intercomparison Of Criticality Accident Dosimetry, Ninth Neutron Dosimetry Symposium. The Netherlands Medioni, R., Asselineau, B., Verrey, B., Trompier F., Itie, C., Texier, C., Muller H., Pelcot, G., Clairand, I., Jacquet X., and. Pochat, J.L., Criticality Accident Dosimetry Systems. An International Intercomparison At The Silene Reactor, Ninth Neutron Dosimetry Symposium. The Netherlands