Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 MEASUREMENT OF RADON EXHALATION RATE FROM INDIAN GRANITE TILES Sundar, S. Bala; Ajoy, K.C; Dhanasekaran, A., Gajendiran, V & Santhanam, R. S. Bala Sundar. K.C. Aiov, A. Dhanasekaran. V. Gaiendiran, and R. Santhanam Radiation Safety Section, Radiological Safety Division, Indira Gandhi Centre for Atomic Research, Kalpakkam-603 102, Tamil Nadu, India. ABSTRACT Measurement of radon exhalation rate from different varieties of granite tiles quarried from various parts of India has been carried out. Seventeen varieties of widely exported granite tiles of dimensions 5 x 5 x 2.5 cm have been tested. Five samples were received for each variety. The samples were exposed for 24 hours in a leak tight mild steel chamber. Gas samples were then collected using Lucas cell and counted for alpha activity to evaluate, using standard procedure, the concentration of radon from which, radon exhalation rate was estimated. Powder samples of the tiles were subjected to gamma spectral analysis. The results obtained are presented and discussed. Key words : radon, granite, Lucas cell Corresponding author: S.Bala Sundar email : sbs^?.iecar.ernet.in INTRODUCTION Human beings have always been exposed to ionizing radiation from various natural sources of radiation and one of the major routes of internal exposures is through inhalation of radioactivity present in the atmosphere. The three primordial radionuclides, viz, ^K, ^U and 2 3 2 ~ hthat are present in the building materials in varying concentrations cause both internal and external exposures to the residents. External 238" exposure is caused by the gamma radiation from '*OK and the daughter products of and ^ ~ h . It is known that as a result of inhalation of ^ ~ n ,a daughter product of decay chain of ^u, and its daughter products, the equivalent dose to the entire lung is 20 % and 45 % higher than the equivalent dose in other tissues. Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 Soil, natural gas, water, construction materials are some of the sources of radon. From the epidemiological study made on the mortality rate among uranium and nonuranium miners, the correlation between cumulative exposure to the short-lived radon daughters and the excess incidence of lung cancer has vividly demonstrated the existence of a positive relation (Ahemed,J.U.,1992). For this reason, an assessment of radon, exhaling from building materials assumes significance. Several studies have been undertaken to evaluate the radon exhalation rate from building materials (Maged and Borhem, 1997; Abu-Jarad et al 1980). The Austrian Standard ONORM S 5200 has proposed that a type of building material is considered acceptable if in a room the annual effective dose does not exceed 2.5 mSv (Steger.F et al. 1999). Granite is a form of igneous rock, which is composed primarily of Quartz, Alkalie, and Felspar. India stands third in export of granite stone and first in granite stone production. In this paper, the results of radon exhalation measurements of different varieties of granites mined in southern parts of India are presented. These results are of general interest since granites are globally used as building, ornamental and monumental materials especially due to its elegant look, durability and scratch resistant properties. MATERIALS AND METHODS Seventeen varieties of granite tile samples of dimensions 5 x 5 x 2.5 cm each weighing about 120 - 150 g were collected. Five samples were received for each variety. Of these, two samples were crushed and sieved through one mm sieve and preserved for gamma spectral analysis and remaining three tiles were used for exhalation rate measurements. (I) Radon exhalation measurements: Lucas cells (Scintillation cells) were used for the estimation of radon exhalation rate (RER) from these materials (Somalai J. et al, IRPA, Poffijin A. et al, 1983). A cylindrical shaped of mild-steel container was fabricated for carrying out the measurement. The container was 10 cm in diameter with an internal volume 750 cc. Nozzles fitted with valves were provided for collecting samples with the Lucas cells. The back diffusion process and leak rate , which hamper the exhalation measurement results, are significant for the sampling time more than 30 hours (Stranden, 1983). Hence, the residence time of the sample in the container was restricted to about 24 Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 hours, to minimize back diffusion. The ratio of volumes of the container and sample was more than 10, which further reduced the probability of back diffusion (Hafez.A.F, 2001). In order to establish the leak rate of the container, a separate study was carried out. The chambers were pressurized upto 1.2 kg/cm2 and sealed. The reduction in pressure was continuously monitored for about a month. A graph was plotted with the pressure against time (Fig 1). It was observed that the leak rate was 0.5% by volume per day. The samples were kept in the containers and sealed. After allowing a growth time of 24 hours, gas samples were collected from the container in Lucas cell of volume 150 ml. After a delay of three hours to allow radon gas to attain equilibrium with its daughters, the Lucas cells were counted using a PM tube assembly. The efficiency of the counting system used in the study was 70%. From the counts, the concentration of radon gas collected in the Lucas cell was estimated using the following equation (Jha, et al, 200 1 ): cy. Q = ...................... 3EV e'" ( 1- e'?lT) Where, Q is the radon concentration (Bq m"3) C is the net counts in T seconds A is the decay constant of radon (s") (1) Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 E is the efficiency of the counting system (fraction) V is the volume of the Lucas cell (m3) t is the counting delay (s) As stated above, it may be noted that radon is in equilibrium with its daughters; for the decay of each radon atom there will be simultaneous disintegration of its two daughters and hence the factor 3 is used in the equation. From the sample surface area and residence time in the container, radon exhalation rate was calculated using the equation given below. Q Vem \ E - ---------------- (2) A (1- e^) Where, E is the radon exhalation rate (Bq m'2h-') Q is the concentration of radon (Bq m'3) Vcm is the effective volume of the container (m3) 1 is the decay constant of radon (h-') A is the surface area of the sample (m2) T is the growth time (h) The MDA for the exhalation rate for the above experimental conditions was estimated to be 0.10 Bq mV2h-'. Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 (II) Gamma spectral analysis - The crushed samples were homogenized and dried in an oven at 100 1 lo0 C for about 24 hours. The samples were then filled in standard 250 ml air tight PVC containers. The containers were sealed hermetically and externally using a adhesive tape and kept aside for about 30 days. This will ensure the equilibrium between * Ra and its daughters. The containers were subjected to gamma ray spectral analysis using 3" x 3" NaI (TI) detector. The detector is shielded on all the four sides as well as at the top portion by 15-cm thick lead. Aluminum, cadmium and copper sheets in that order (graded lining) are also provided in between the lead shield and the detector so as to decrease the intensity of characteristic X-rays emitted by the high atomic number shield materials. 95% of background reduction is achieved by this arrangement. This system is situated in a nuclear counting facility, which is constructed using soil with low natural radioactivity. The system was calibrated using IAEA reference standards similar in geometry as that of the sample containers. Each sample was counted for 20000 sec and the natural primordial radionuclides present in the tiles were identified. For the quantification, the peaks corresponding to Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 1.46 MeV (Â¥"'K)1.76 MeV ('"~i) and 2.61 MeV (""~1)were considered in arriving at the activity levels of OK, 238", 226 Ra and ^ ~ hrespectively. The activity of each radionuclide in the sample was determined using the total net counts under the selected photo peaks after subtracting appropriate background counts and applying appropriate factors for photo peak efficiency and weight of the sample. The MDA (30) for each radionuclide was established from the background radiation spectrum for a counting time of 20000 sec and the values were 8.5, 1 and 13.25 ~~k~~ for ^U ( ^ ~ a ) , ^ ~ hand ^K respectively. RESULTS AND DISCUSSION To estimate the leak rate of the chamber, plot between pressure and number of days is given Fig. 1. The average volumetric leak rate was calculated using the formula (V.Barashko et.al, 2002). Where Q is average volumetric flow rate in cm3m" * H is initial and final pressure difference in bar * B is initial and final atmospheric pressure change during observation in bar V is the volume of the chamber in cm3 ~t is the time of observation in min The volumetric leak rate was calculated to be 4.2k0.33 cm3d'l The radon concentration inside the container varied from 60 to 485 ~ ~ m The ' ~ . exhalation rate of the tiles varied from 0.24  0.01 to 2.07  0.07 Bq m^h" which are tabulated in Table I . Out of seventeen samples 11 were havin ^ ~ hcontent above 1 ~ ~ k ~10" ' , samples were having 2 3 8 content ~ above 8.5 Bqkg' ? and all the samples were having '"K. Proceedings of the 2003 International Radon Symposium - Volume 11 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 The activity concentration of the primordial radionuclides in the tiles are given table.2 The ^ ~ hconcentration varied from 17± to 212± Bqkg"', 2 3 8 ~ ( 2 2 6 concentration ~a) ~ the ' ' 4 0 concentration ~ varied from 132  5 to varied from 17 ± to 195±~ ~ k and 2 1 16Â9 ~ ~ k ~ - ' , In order to compare the specific activities of the radionuclides, a common index is required to obtain the sum of activities. The index, which is called the radium equivalent activity ,for the samples, was calculated using the formula (Beretka and Mathew, 1985). where, AK,Apa and A n are the activities of Potassium, Radium and Thorium respectively, in Bq kg"'. This formula is based on the estimation that 370 Bq kg"' of "'~a, 259 Bq kg" of * " ~ hor 48 10 Bq kg" of "K produce the same gamma dose rate. The radium equivalent for the tested samples varied from 10 to 563 Bqkgm'. Fig 2 gives the correlation between radon exhalation rate and uranium content of the tile. An exponential fitting was done which yielded equation with a correlation coefficient 0.9469 given below. E (Bq m'2h" ) = 0.107 * Exp (-0.0 147 * X) (5) ' 'calculated . where X is uranium activity concentration of the sample in ~ ~ k ~The values using the above equation and the measured values are given in table 3. The variation between calculated and experimental values of radon exhalation rate may be attributed to the inadequacy of the number of samples with detectable uranium content and also to the fact that the porosity and the density of the samples, which influence the radon exhalation rate, were not normalized for the plot. CONCLUSION Out of seventeen samples nine samples were found to have higher thorium content upto a maximum of 10 times the uranium content. Due to this, estimation of thoron exhalation rate also assumes importance. Attempts are being made to study the thoron exhalation too. Six samples showed radon exhalation rate above detectable level and these values are in good agreement with the reported values for Indian granite tiles (Mentazul I. Choudhury, JRNC,1998, Al Jarallah, 2001). There exists a good correlation between the uranium content of the sample and radon exhalation rate. This implies that there exists a possibility to use the concentration of 238 u ( ^ R ~ ) as an indicator for the extent of radon exhalation. Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 REFERENCE Abu-Jarad F., Frem1in.J.H. and Bull.R.,1980. A study of radon emitted from building materials using plastic alpha track detectors. Physics of Medical Biology 25, pp. 683-694. Ahemed.J.U. (1992) Regulatory Approach Toward Controlling Exposure to Radon in Dwellings, Radiation protection and Dosimetry vol.45, pp 745-750. Al Jarallah, 2001. Radon exhalation from granites used in Saudi Arabia Journal of Environmental Research 53, pp 9 1-98. Barashko.V, Dolinsky.S, Ignatenko.M, K0rytov.A and Procofiev.0, 2002. EMU CSC systems chamber leak rate measurements, internal report, university of Florida. Beretka J. and Mathew P.J, 1985. Natural radioactivity of Australian building materials, industrial wastes and by products. Health Physics 48, pp.87-95, Erling Stranden, (1.983). Assessment Of The Radiological Impact Of Using Fly Ash In Cement, Health Physics vol. 44 no.2, pp 145 - 153. Hafez.A.F, Hussein.A.S. and Rasheed.N.M., 2001. A study of radon and thoron release from Egyptian building materials using polymeric nuclear track detectors. Applied Radiation and Isotopes.54, pp 291-298. Jha.S, Khan A.H, Mishra U.C. (2001), A Study Of The Technologically Modified Sources Of Radon And Its Environmental Impacts In An Indian U Mineralized Belt. Journal of Environmental Radioactivity Vol53, pp no. 183 - 197. Maged.A.F. and Borham.E., 1997. A study of the radon emitted from various building materials using alpha track detectors. Radiation Measurements 28, pp 61 3-6 17. Mentazul I. Choudhury,(1998) Concentration Of Radio Nuclides In Building And Ceramic Materials Of Bungladesh And Evaluation Of Radiation Hazard. Jrnl. Radioanalytical and Nuclear Chemistry, vol23 1, Poffijin A., Bourgoignie.R, Marijns.R, Uyttenhove.J, JanssensA and. Jac0bs.R (1984); Laboratory measurements of radon exhalation and diffusion, Radiation Protection Dosimetry, vol7, p 77-79. Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 Somalai.J, . Nemeth Cs, Kanyar.B, K0vacs.J; Variations of Radon Emanation of CoalSlags with the Burning Temperature, Proceedings of IRPA 10. Steger F. And Grun K.(1999),Proceedings of Radon in the Living Environment, Athens, Greece. Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 0 0 5 10 15 20 25 30 MIMBKR OF DAYS FIG1 GRAPH SHOWING PRESSURE DECREASE WITH TIME 35 Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 ow 50.00 150.00 100.w 200.00 U-238 (Bafkg) FIG.2. CORRELEATION BETWEEN URANIUM CONTENT AND EXHALTION RATE OF THE SAMPLES 250.00 Proceedings of the 2003 International Radon Symposium - Volume I1 American Association of Radon Scientists and Technologists, Inc. October 5 - 8,2003 TABLE 1 RADON EXHALATION RATE (RER) OF GRANITE TILES SAMPLE CODE RER (Bq m^h") S7 €0 0 S8 €0. S9 20 mSv1a percentage > 6 mSv/a and < 20 mSv/a 201 region Fig. 4: Effective annual dose distribution amongst the Bavarian water supply facility personnel. This effective dose is from radon exposure during working time in the supply facilities. ventilation 9 <^ <^ 2 2^ -Ct- ^