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Radon is a dangerous radioactive gas that is odorless, tasteless, and colorless. It is the second leading cause of lung cancer in America, only behind cigarette smoking. Excess levels of radon entry into a property is not very expensive to correct. It is not prudent to waive your rights to a radon test as part of an agreement of sale. EPA has reported elevated radon levels in every zip code across the country.

Commonly Used Radon Measurement Devices

Charcoal Canisters - Charcoal Canisters (CC) are passive devices requiring no power to function.  The passive nature of the activated charcoal allows continual adsorption and desorption of radon.  During the measurement period, the adsorbed radon undergoes radioactive decay.  Therefore, the technique does not uniformly integrate radon concentrations during the exposure period.  As with all devices that store radon, the average concentration calculated using the midexposure time is subject to error if the ambient radon concentration adsorbed during the first half of the sampling period is substantially higher or lower than the average over the period.  For a 2- to 7-day exposure period, the lower level of detection (LLD) should be 0.5 pCi/L or less  (U.S. EPA Measurement Protocols 1989).  This level of sensitivity can normally be achieved with a counting time of up to 30 minutes.  This LLD should be calculated using the results of charcoal background determinations.  The coefficient of variation should not exceed 10 percent (1 sigma) at radon concentrations of 4 pCi/L or greater  (U.S. EPA Measurement Protocols 1989).  This precision should be monitored using the results of duplicate canister analyses.  CCs can achieve an average coefficient of variation of less than 5 percent at concentrations of 4 pCi/L or greater.

Alpha Track Detectors - An alpha track detector (ATD) consists of a small piece of plastic or film enclosed in a container with a filter-covered opening.  Radon diffuses through the filter into the container and alpha particles emitted by the radon and its decay products strike the detector and produce submicrocopic damage tracks.  At the end of the measurement period, the detectors are returned to a laboratory.  Plastic detectors are placed in a caustic solution that accentuates the damage tracks so they can be counted using a microscope or an automated counting system.  The number of tracks per unit area is correlated to the radon concentration in air, using a conversion factor derived from data generated at a calibration facility.  The number of tracks produced per unit of time is proportional to the radon concentration, so an ATD functions as a true integrating detector and measures the average concentration over the measurement period.  The LLD (sensitivity) and the precision of an ATD system is dependent upon the tracks counted, and therefore the counting achieves and LLD of 180 pCi/L-days.  The coefficient of variation (precision) should be monitored using the results of duplicate detectors.  The coefficient of variation should not exceed 20 percent (1 sigma) at radon concentrations of 4 pCi/L or greater (U.S. EPA Measurement Protocols 1989).

Electret-Passive Environmental Radon Monitors

Electret-passive environmental radon monitors (E-PERMs) required no power and function as true integrating detectors, measuring the average concentration during the measurement.  E-PERMs contain a permanently charged electret (an electrostatically-charged disk of Teflon), which collects ions formed in the chamber by radiation emitted from radon decay products.  When the device is exposed, radon diffused into the chamber through filtered openings.  Ions which are generated continuously by the decay or radon and radon decay products are drawn to the surface of the electret and reduce its surface voltage.  The amount of voltage reduction is directly related to the average radon concentration present during the exposure period.  There are both short-term (2- to 7-day) and long-term (1- to 12-month) E-PERMs that are currently marketed.  The thickness of the electret affects the usable measurement period.  For a 7-day exposure period using a short-term E-PERM, as well as for a long-term E-PERM, the LLD (sensitivity) is about 0.3 pCi/L  (U.S. EPA Measurement Protocols 1989).  The coefficient of variation should not exceed 10 percent (1 sigma) at radon concentrations of 4 pCi/L or greater (U.S. EPA Measurement Protocols 1989).  This precision should be monitored by using results of duplicate detector analyses.  

Continuous Radon Monitors

There are three types of continuous radon monitors (CRMs).  In the first type of CRM, ambient air is sampled for radon in a scintillation cell after passing through a filter that removes radon decay products and dust.  Alpha particles (produced by radon decays) strike the zinc sulphide coating of the cell, yielding scintillations which are detected by a photo-multiplier tube in the detector.  A second type of CRM operates as an ionization chamber.  Radon in the ambient air diffuses into the chamber through a filtered area so that the radon concentration in the chamber follows the radon concentration in the ambient air with some small time lag.  The third type of CRM functions by allowing ambient air to diffuse through a filter into a detection chamber.  As the radon decays, the alpha particles are counted using a solid state silicon detector.  Most CRMs are capable of an LLD (sensitivity) of 0.5 pCi/L or less  (U.S. EPA Measurement Protocols 1989).  Special cells are available for some CRMs which have LLDs of 0.1 pCi/L.  The precision of most CRMs can achieve a coefficient of variation of less than 10 percent (1 sigma) at 4 pCi/L or greater  (U.S. EPA Measurement Protocols 1989).

 

 

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