Fact Sheet: Radiological hazards associated with hot rock geothermal systems. David L Battye and Peter J Ashman School of Chemical Engineering, University of Adelaide SA 5005 Hot rock geothermal systems extract energy by circulating water within granites that are heated by natural radioactivity. There is potential for radioactive elements to dissolve in the circulating water and be carried to surface equipment. It is therefore natural to ask: … Will hot rock geothermal power plants present any significant radiation hazards? Radioactivity and radiation A radioactive element, or radionuclide, is an element with an unstable nucleus. Radioactive decay describes a transformation of the unstable nucleus whereby the following may happen: Alpha decay: An alpha particle, consisting of two protons and two neutrons, is ejected from the nucleus. Alpha particles may be stopped by a piece of paper. Beta decay: A neutron in the nucleus is converted into a proton and an electron is ejected. The electron is known as a beta particle and may penetrate 1-2 cm into body tissue. m en t C om Gamma radiation may accompany alpha or beta decay. Gamma radiation is a type of electromagnetic radiation like light or radio waves, except that it has a far higher frequency and energy. It is highly penetrative. Dense materials such as lead are used for shielding against gamma radiation, although any material can be used provided the thickness is great enough. D ra ft fo r Alpha particles, beta particles and gamma radiation are all types of ionizing radiation, a class of radiation that is hazardous to our health. Ionizing radiation has enough energy to knock electrons out of their orbits, ie. to “ionize” molecules. When this happens to molecules in the cells of our body, those cells can become damaged. If the genetic material (DNA) in cells is damaged, ionizing radiation can cause cancer. Damage to the DNA in reproductive cells can cause genetic mutations that can be passed on to future generations. Gamma radiation doses are the easiest to receive since gamma rays can travel further from their source than alpha and beta particles. However, radionuclides emitting alpha and beta particles can be quite harmful if inhaled or ingested. Ionizing radiation doses are measured in a unit called the Sievert (Sv), where 1 Sv represents the biological effect of 1 Joule of energy deposited in 1 kilogram of tissue by ionizing radiation. The background ionizing radiation dose in Australia is about 1.5 millisieverts (mSv) per year and can be broken down as shown below. Source Annual dose (mSv) Cosmic rays 0.3 External, terrestrial sources (eg. rock, soil) 0.6 Internal sources (eg. potassium-40 in the body) 0.4 Radon 0.2 Total 1.5 Cosmic rays are highly energetic particles (protons, alpha particles and electrons) that bombard the earth from outer space. External, terrestrial radiation comes from radionuclides present in our external environment, mostly in rocks and soil. Internal radiation is caused by radionuclides occurring naturally in our body such as the radioactive isotope of potassium, 40K. Radon is a radioactive gas produced by decay of radium isotopes present in soils, rock and building materials such as bricks, concrete, mortar and tiles. The decay products of radon can lodge in the lungs if inhaled, exposing them to ionizing radiation and increasing the risk of lung cancer. Australia’s recommended dose limits for ionizing radiation arising from activities that increase overall exposure are 20 mSv per year for occupational exposure (averaged over 5 years), and 1 mSv in a year for members of the public. These limits are based on the recommendations of the International Commission on Radiological Protection (ICRP), and do not include natural background radiation or doses received from medical procedures. However, the National Standard for limiting occupational doses requires that all doses should be kept “as low as reasonably achievable” (ALARA). en t Decay chains Abundance (grams per tonne) 16 52 5 C om Radionuclide m The most abundant radionuclides in granites are uranium-238 (238U), thorium-232 (232Th) and potassium-40 (40K). These elements have existed in the granite since it was first formed and decay very slowly. Granites in the Cooper Basin have an approximate radionuclide composition as shown below. 238U 232Th 40K ft fo r and 232Th are each at the head of a decay chain of radionuclides, shown below. Another decay chain has the uranium isotope 235U at its head, but this isotope represents only 0.72% of all naturally occurring uranium. The 238U and 232Th in granites has been there long enough that an equilibrium has been reached in both decay chains. In this radioactive equilibrium, the activity (number of atoms decaying per second) of each radionuclide is equal. D ra 238U uranium-238 decay chain Half-life Principal radiation uranium-238 thorium-234 proactinium-234m uranium-234 thorium-230 radium-226 radon-222 polonium-218 lead-214 bismuth-214 polonium-214 lead-210 bismuth-210 polonium-210 lead-206 4.5 billion years 24 days 1 minute 246 thousand years 75 thousand years 1600 years 3.8 days 3 minutes 27 minutes 20 minutes 2 microseconds 22 years 5 days 138 days stable alpha beta beta alpha alpha, gamma alpha, gamma alpha, gamma alpha, gamma beta, gamma beta, gamma alpha, gamma beta, gamma beta, gamma alpha, gamma C om m en t Radionuclide thorium-232 decay chain Half-life fo r Radionuclide 14 billion years 5.8 years 6.2 hours 1.9 years 3.7 days 56 seconds 0.15 seconds 11 hours bismuth-212 61 minutes polonium-212 (64%) lead-208 thallium-208 (36%) lead-208 0.3 microseconds stable 3.1 minutes stable D ra ft thorium-232 radium-228 actinium-228 thorium-228 radium-224 radon-220 polonium-216 lead-212 Principal radiation alpha, beta, gamma beta beta, gamma alpha alpha, gamma alpha alpha beta, gamma alpha, beta, gamma alpha, beta, gamma beta, gamma Radionuclides in solution The water circulating in a hot rock reservoir is a mixture of fresh water injected at the surface and water already present in the natural fractures of the granite, which may be quite saline. In hot rock projects overseas, the circulating water has typically had a total dissolved solids (TDS) content of less than 4 g/L and near-neutral pH. Under these conditions the solubility of uranium, thorium, radium, radon and lead isotopes is expected to be similar to that for dilute, granite groundwaters. C om m en t Geothermal power plants often produce solid residues in the form of scales and sludges precipitated from the geofluid. It is therefore reasonable to suspect that dissolved radionuclides may be included in these residues, presenting a gamma radiation hazard. Experience in the oil and gas industry offers some insight on what can be expected in this regard. Oil and gas reservoirs often also produce highly mineralized water together with the hydrocarbons. When the produced waters are cooled and depressurized in surface production equipment, radioactive scales and sludges are formed. The main source of radioactivity in these residues is radium. It has been determined that the high dissolved solids content of typical produced waters stabilizes radium in solution, preventing it from being scavenged by mineral surfaces in the reservoir. Furthermore, the produced waters are usually saturated with barium, strontium and sulfate ions at the temperature of the reservoir, such that any cooling of the water will cause the precipitation of barium and strontium sulfates. Being chemically similar to barium and strontium, radium is readily incorporated into the precipitates. The low dissolved solids content of typical hot rock geofluids means that we expect low radium levels in solution, and the geofluids are likely to be under-saturated with respect to barium and strontium sulfates. Therefore, radium in solid residues is unlikely to constitute a significant source of gamma radiation in hot rock power plants. D ra ft fo r The solubility of thorium and lead in groundwaters is low and so negligible levels are expected in hot rock geofluids. The concentration of uranium isotopes in granite groundwaters can exceed 800 μg/L, and the possibility of uranium deposition in surface residues cannot be discounted. However, the uranium isotopes only emit alpha radiation and their decay products, which emit gamma radiation, do not become significantly active for thousands of years. Hence, it appears unlikely that solid residues in hot-rock power plants will present a significant gamma radiation hazard. However, given that all radionuclides can be hazardous if inhaled, and without knowledge of the exact residue composition, workers involved with cleaning equipment will need to avoid inhaling solid residue dusts. Radon emissions Radon enters solution in groundwaters predominantly by a mechanism called ‘alpha-recoil’, whereby a radon atom is propelled into the geofluid by the alpha decay of a radium atom near the rock-fluid interface. Since radon is an inert gas, it remains in solution until it decays or is emitted to the atmosphere. In their most probable configuration, hot rock geothermal power plants will circulate the geofluid in a closed loop in which it is never exposed to the atmosphere. In this context, dissolved radon gas will reach an equilibrium concentration where the overall rate of emanation from the granite is equal to the rate of radioactive decay, as is the case in many natural groundwaters. However, there are situations where essentially all radon in the geofluid reaching the surface would be vented to the atmosphere. In open-loop circulation testing of newly created reservoirs, all produced steam is vented. If a ‘flash’ power plant is operated, where steam for power generation is produced by depressurizing the geofluid, then non-condensable gases including radon will be vented from the steam condenser. Based on experience gained in overseas hot rock projects, it is possible to estimate the radon emission rate from reservoirs of the type being developed in the Cooper Basin. For a typical reservoir of approximately 5 km2, an estimated 4 billion radon atoms per second may be emitted (8400 Bq s-1). If the radon was emitted from a point 20 metres above ground and in light wind, atmospheric dispersion modeling suggests that downwind concentrations of radon at ground-level would be almost identical to background levels. Higher concentrations will be experienced during periods of calm or during the break-up of stable air layers near the ground. However, the preliminary modelling suggests that concentrations are likely to be far below levels of concern even during these periods. Summary: Will hot rock geothermal power create any radiation hazards? Considering the above arguments, the answer is no. Concentrations of radionuclides in hot rock geofluids are likely to be similar to dilute granite groundwaters. Any scales or sludges precipitating from the geofluids are very unlikely to contain radium, the main emitter of gamma radiation in oil and gas industry residues. Should uranium be present in residues, it will not represent a radiation hazard provided proper precautions are taken against inhalation of dusts during equipment cleaning. D ra ft fo r C om m en t Preliminary modelling suggests that venting radon from a typical hot rock reservoir will increase downwind ground-level radon concentrations negligibly in light to strong winds. In periods of calm or during break-up of stable air, concentrations are still estimated to be low relative to levels of concern.
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