Study on the influence of density in the dose uniformity of the CDTN gamma irradiator --------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------ABSTRACT This paper describes an experimental study carried out to determine the dependence of the dose uniformity with the irradiated product bulk density. The knowledge of this dependence helps to ensure that the irradiation process is carried out with acceptable doses uniformity. The measurements were made in the Gamma Irradiation Facility at Nuclear Technology Development Center (CDTN) an R&D Institute connected to the Nacional Nuclear Energy Commission (CNEN), Brazil. Four different bulk densities were investigated. The results showed that the dose uniformity decreases with the product bulk density increasing. It is interesting to note that the DUR obtained values are consistent with a high dose uniformity that is requiring, e.g. in R&D studies. It is important to note that these results apply to the specific geometry conditions studied. Keywords: dose uniformity, gamma processing, gamma ray, irradiator 1. INTRODUCTION In cases where it is indicated, the irradiation process promotes improvements of products and materials functional properties. Irradiation can be used, for example, to improve mechanical properties of polymers and plastics or to reduce the pathogen burden in foods, making them safer. The main parameter involved in the process is the energy transferred by radiation to the material. This amount of energy per material mass unit characterizes the absorbed dose. Specific improvements are associated with characteristics dose ranges. The doses necessary to achieve the desired effect are within these ranges that in the most cases are determined through experimental dose-effect studies. The minimum scale values are those from which the desired effects are obtained, whereas the maximum values correspond to those from which there is a risk that the functional properties of the product are adversely affected (e.g., deteriorating mechanical properties of plastic parts for medical / pharmaceutical or organoleptic changes in foodstuffs). Each process/product set has its typical limits that, in the case of products regulated as foodstuffs and products for healthcare, are prescribe by government authorities [1]. During the irradiation process, several types of interactions occur between the radiation and the material. These interactions attenuate the radiation by depositing a portion of its energy in the material. This attenuation produces a decrease in absorbed dose with depth whose rate depends on the product composition and density and on the energy carried by the radiation. Besides this depth variation there is also a lateral variation that depends on the irradiation geometry. Such variations affect the product absorbed dose uniformity and its knowledge is essential for the quality assurance of the irradiation process. To study these variations is adopted the concept of Dose Uniformity Ratio (DUR), defined as the ratio between maximum and minimum values of absorbed dose in all the extension of the irradiated product [2]. This paper presents experimental results of a study conducted within the framework of Quality Assurance Program of the CDTN Gamma Irradiation Facility [3]. The purpose of this study was to determine the dependence of the DUR with the irradiated material bulk density. The adopted methodology has used five cardboard boxes irradiated at 41 cm from the source. The first one empty and the other four filled with different bulk densities products. DUR were calculated using the maximum and minimum values of the absorbed dose measurements. 2. EXPERIMENTAL SETUP 2.1. The Irradiation Facility The CDTN irrradiator is a GammaBeam-127 type, manufactured by MDS Nordion [4]. The GB127 is a dry storage, panoramic irradiator that uses Nordion’s F-127 shipping container for source storage and operation. Products to be irradiated are placed inside the biological shield, either on turntables or directly on the floor. After safety interlocks have been engaged, the source is raised by a pneumatic hoist for the prescribed amount of time and then returned to the safe position inside the container. Source to product distance can be varied easily, resulting in good dose uniformity across a wide variety of densities. This batch processing approach lends itself well to research and testing, food irradiation, sterile insect technique and many other applications. The Table 1 shows the irradiator specifications. The irradiator is a box chamber with high-density concrete walls. Figure 1 presents a close up of the irradiation facility. Table 1: Irradiator Specifications Maximum Source Activity 60 kCi (2.220 TBq) Dose Rate @ 1 m 600 Gy/h Product Configurations 12 turntables (50 cm diameter, 2 rpm) Maximum Product Weight (on turntables) 700 lbs. (320 kg) Source to Product Distance Variable up to 300 cm Floor Area 33 ft. x 39 ft. (10.1 m x 11.9 m) Mode of Operation Manual batch Figure 1: Irradiator close up 2.2. Dosimeters Dose measurements were carried out using 15 Red Perspex 4034 Batch LS dosimeters [5]. These routine dosimeters are made of polymethyl methacrylate (PMMA) with an overall uncertainty of ± 8.2% at a 95% confidence level, in the range of 5-50 kGy, calibrated against Fricke reference dosimeters at the facility [6]. Therefore, all the values of absorbed dose measurements are affected by this uncertainty and the DUR calculated values are affected by ± 11.6%. 2.3. Product Irradiation The products were irradiated within carton boxes (30x30x20 cm) over turntables. The boxes centers were shifted by 41 cm from the source and its middle levels at 55 cm from the floor. They were divided into five vertical planes and three horizontal levels. The 15 dosimeters locations are shown in Figure 2. In order to optimize the dose homogeneity in the product, the turntable has turned at 2 rpm during the irradiation cycle. Figure 2: Carton with dosimeter positions (dots) Dosimeter Vertical planes 3 Source center 2 41cm 1 2 3 4 1 55cm Horizontal levels 5 Carton packing Turntable 3. RESULTS AND DISCUSSION Five carton boxes were irradiated in order to study the bulck density effect in the dose uniformity. The first one empty and the other four filled with sawdust, pharmaceutical gauze, dry vermiculite and wet vermiculite). At the irradiation position, the dose rate at the center point of the box was 1.4 kGy/h. It is considered the “global dose uniformity” as the ratio between their maximum and minimum dose in the boxes [7]. 3.1. Dose Measurements 3.1.1. Empty carton box Experimental dose measurements with empty carton box (bulk density 0.02 g/cm3) are shown in Figure 3-A and 3-B. For all levels, the results show a symmetrical distribution relatively to the vertical axis passing through the middle of the box (Fig. 3-A). The maximum dose value found was (24.7 ± 2.0) kGy, located on level 2 (middle level) while the lowest was (22.0 ± 1.8) kGy, on level 3 (DUR=1.12 ± 0.13). Figure 3-A: Horizontal dose profile (empty) For all vertical planes, the results show an asymmetrical distribution relatively to the horizontal axis passing through the middle of the carton box (plane 2 in Fig. 3-B). The observed asymmetry is due to displacement of the geometric center of the source of their design position. This displacement resulted from a mistake in the mounting phase of the source and was observed through measurements of dose rates performed in a previous study [8]. Figure 3-B: Vertical dose profile (empty) 3.1.2. Pharmaceutical gauze filled box The experimental dose measurements carried out with pharmaceutical gauze filled box (bulk density 0.08 g/cm3) at 41 cm from source, are shown in Figure 4-A and 4-B. The results have the same behavior as the empty box case in both horizonal and vertical axis, but with more pronounced dose profiles resulting from higher density. The maximum dose value found was (24.5 ± 2.0) kGy, located on level 2 while the lowest was (21.5 ± 1.8) kGy, on level 3 (DUR=1.14 ± 0.13). Figure 4-A: Horizontal dose profile (gauze) Figure 4-B: Vertical dose profile (gauze) 3.1.3. Sawdust filled box The experimental dose measurements carried out with sawdust-filled box (bulk density 0.2 g/cm3) at 41 cm from the source, are shown in Figure 5-A and 5-B. Figure 5-A: Horizontal dose profile (sawdust) The results have the same behavior as the previous case, in both horizonal and vertical axis, but with a more pronounced profiles resulting from higher density. The maximum dose value found was (26.8 ± 2.2) kGy, located on level 2 while the lowest was (23.2 ± 1.9) kGy, on level 3 (DUR=1.16 ± 0.14). Figure 5-B: Vertical dose profile (sawdust) 3.1.4. Dry vermiculite filled box The experimental dose measurements carried out with dry vermiculite-filled box (bulk density 0.3 g/cm3) at 41 cm from the source, are shown in Figure 6-A and 6-B. Figure 6-A: Horizontal profile (dry vermiculite) The results have the same behavior as the previous case, in both horizonal and vertical axis. The maximum dose value found was (25.0 ± 2.1) kGy, located on level 2 while the lowest was (21.0 ± 1.7) kGy, on level 3 (DUR=1.19 ± 0.14). Figure 6-B: Vertical profile (dry vermiculite) 26,0 Dose [kGy] 25,0 24,0 Plane 1 Plane 2 23,0 Plane 3 22,0 Plane 4 Plane 5 21,0 20,0 1 2 3 Horizontal levels 3.1.5.Wet vermiculite filled box The experimental dose measurements carried out with wet vermiculite-filled box (bulk density 0.6 g/cm3) at 41 cm from the source, are shown in Figure 7-A and 7-B. Figure 7-A: Horizontal profile (wet vermiculite) The results have the same behavior as the previous case, in both horizonal and vertical axis. Here the profile is the most pronounced of all, since it is the case of higher density. The maximum dose value found was (21.6 ± 1.8) kGy, located on level 2 while the lowest was (17.2 ± 1.4) kGy, located on level 3 (DUR = 1.25 ± 0.15). Figure 7-B: Vertical profile (wet vermiculite) 3.2. Global Dose Uniformity The DUR calculated values are shown in Table 2 for all cases. The effect of bulk density on global DUR is shown in Figure 7. Table 2: Global DUR calculated values Filling Vermiculite dry wet Empty Gauze Sawdust Density [g/cm3] 0.02 0.08 0.2 0.3 0.6 DUR 1.12 ± 0.13 1.14 ± 0.13 1.16 ± 0.14 1.19 ± 0.14 1.25 ± 0.15 Figure 8: Effects of bulk density on DUR 4. CONCLUSIONS The results showed that the dose uniformity decreases with the product bulk density increasing. It is interesting to note that the DUR obtained values are consistent with a high dose uniformity that is requiring, e.g. in R&D studies. It is important to note that these results apply to the specific geometry conditions studied. These facts are important because a priori knowledge of dose distribuition guarantees an appropriate irradiation protocol and ensures total quality results. 5. ACKNOWLEDGEMENTS ----------------------------------------------------------------------------------------------------------------------------- ------------------------------------------------------------------------------------------------------------------------------ ------------------------------------------------------------------------------------------------------------------------------- ------------------------. 6. REFERENCES 1. ISO - INTERNATIONAL ORGANIZATION FOR STANDARDISATION. Sterilization of health care products - Radiation - Part 2: Establishing the sterilization dose. Geneve. 2013. (ISO - 11137-2: 2013). 2. IAEA - INTERNATIONAL ATOMIC ENERGY AGENCY. Gamma irradiators for radiation processing. Vienna. 2004. (IAEA-TECDOC-1386). 3. LADEIRA, L. C. D.; PINTO, F. C. Safety analysis report of the Gamma Irradiation Laboratory - Chapter 4 - Irradiator detailed description. CDTN - Centro de Desenvolvimento da Tecnologia Nuclear. Belo Horizonte. 2002. (RASIR/LIG/CDTN). 4. MDS NORDION. Licensing information package for Gamma Irradiator GB-127 serial number IR-214. Québec. 2001. (IN/LP 1725 IR214(1)). 5. HARWELL. Dosimetry systems for radiation processing. Harwell Dosimeters Ltd. Oxfordshire. 1999. 6. CONCEIÇÃO, C. C. S. Implementação de dosimetria química para altas taxas de dose em instalações industriais. Rio de Janeiro. 2006. 7. KADRI, O.; GHARBI, F.; FARAH, K. Monte Carlo Improvement of dose uniformity in gamma irradiation processing using the GEANT4 Code, 2005. Disponivel em: <www.sciencedirect.com/science/journal/0168583X.>. Acesso em: 03 mar. 2014. 8. SOARES, G. A.; GROSSI, P. A. Survey of dose rates in an industrial irradiator, calibration dosimeter TLD-800 dosimeters using Fricke dosimetry, and irradiation of blood. CDTN Centro de Desenvolvimento da Tecnologia Nuclear. Belo Horizonte. 2009.
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