PORTABLE SYSTEM FOR MONITORING AIRBORNE RADIONUCLIDES

Abstract

A portable system for measuring airborne radionuclides from a target environment can include a primary gas flowpath including a cartridge dock. At least a first filter cartridge may be connectable to the cartridge dock and may include a cartridge gas inlet sealingly connectable to the sample supply port, a cartridge gas outlet sealingly connectable to the exhaust port; and a cartridge flowpath extending therebetween. The cartridge can include first and second filter chambers housing first and second filters. A gamma detector apparatus may be positionable adjacent the first filter cartridge when the first filter cartridge is connected to the cartridge dock and is configured to detect radiation emitted from the first filter and to detect radiation emitted from the second filter, and to generate a sensor output signal in based on the detected radiation.

Claims

1. A portable system for measuring airborne radionuclides from a target environment, the system being positionable in the target environment and comprising: a) a primary gas flowpath extending between a system gas inlet configured to draw in a gas sample and a system gas outlet downstream from the system gas inlet; b) a cartridge dock disposed in the primary gas flowpath and comprising a sample supply port in fluid communication downstream from the system gas inlet and an exhaust port in fluid communication upstream from the system gas outlet; c) at least a first filter cartridge connectable to the cartridge dock, the first filter cartridge comprising: i. a cartridge gas inlet sealingly connectable to the sample supply port; ii. a cartridge gas outlet sealingly connectable to the exhaust port; and iii. a cartridge flowpath extending between the cartridge gas inlet and the cartridge gas outlet, whereby connecting the first filter cartridge to the cartridge dock provides the fluid communication between the sample supply port and the exhaust port and completes the primary gas flowpath; iv. a first filter chamber disposed in the cartridge flowpath downstream from the cartridge gas inlet and housing a first filter; v. a second filter chamber disposed in the cartridge flowpath between first filter chamber and the cartridge gas outlet, and housing a second filter; d) a gamma detector apparatus that is positionable adjacent the first filter cartridge when the first filter cartridge is connected to the cartridge dock and is configured to detect radiation emitted from the first filter and to detect radiation emitted from the second filter, and to generate a sensor output signal in based on the detected radiation; and e) a system controller configured to receive the sensor output signal and generate a corresponding user output.

2. The system of claim 1, wherein the first filter cartridge is removable from the cartridge dock, and wherein removing the first filter cartridge from the cartridge dock interrupts the primary gas flowpath.

3. The system of claim 1 or 2, wherein the first filter is of a first filter type and the second filter is of a different, second filter type.

4. The system of any one of claims 1 to 3 wherein the first filter comprises an aerosol filter configured to capture particulates in the gas sample and wherein the second filter comprises an iodine filter.

5. The system of any one of claims 1 to 4, wherein the filter cartridge is connectable to the cartridge dock by translating the first filter cartridge in an insertion direction.

6. The system of any one of claims 1 to 5, wherein when the first filter cartridge is connected to the cartridge the cartridge gas inlet is registered with the outlet port and a fluid seal is created between the first cartridge and the cartridge dock.

7. The system of any one of claims 1 to 6, the first filter chamber is sealed when the first cartridge is connected to the cartridge dock and is opened by removing the first filter cartridge from the cartridge dock.

8. The system of claim 7, wherein the first filter is exposed when the first filter cartridge is removed from the cartridge dock.

9. The system of claim 8, wherein the first filter is removable from the first filter chamber in the insertion direction when the first filter cartridge is removed from the cartridge dock.

10. The system of any one of claims 1 to 9, the second filter chamber is sealed when the first cartridge is connected to the cartridge dock and is opened by removing the second filter cartridge from the cartridge dock.

11. The system of claim 10, wherein the second filter is exposed when the first filter cartridge is removed from the cartridge dock.

12. The system of claim 11, wherein the second filter is removable from the second filter chamber in the insertion direction when the first filter cartridge is removed from the cartridge dock.

13. The system of any one of claims 1 to 6, further comprising a cartridge handling apparatus that is controllable by the system controller and is configured to remove the first filter cartridge from the cartridge dock at the end of a first cartridge use period.

14. The system of claim 13, further comprising a second filter cartridge connectable to the cartridge dock, the second filter cartridge comprising: i. a cartridge gas inlet sealingly connectable to the sample supply port; ii. a cartridge gas outlet sealingly connectable to the exhaust port; and iii. a cartridge flowpath extending between the cartridge gas inlet and the cartridge gas outlet, whereby connecting the first filter cartridge to the cartridge dock provides the fluid communication between the sample supply port and the exhaust port and completes the primary gas flowpath; iv. a first filter chamber disposed in the cartridge flowpath downstream from the cartridge gas inlet and housing a first filter; v. a second filter chamber disposed in the cartridge flowpath between first filter chamber and the cartridge gas outlet, and housing a second filter; wherein the cartridge handling apparatus is controllable by the system controller to connect the second filter cartridge to the cartridge dock after the first filter cartridge is removed from the cartridge dock.

15. The system of claim 14, further comprising at least one fresh cartridge bank configured to store unused filter cartridges and containing at least the second filter cartridge, and wherein the cartridge handling apparatus is configured to retrieve the second filter cartridge and move it into registration with the cartridge dock after the first filter cartridge is removed from the cartridge dock.

16. The system of claim 15, further comprising at least one used cartridge bank that is configured to receive and store used filter cartridges, and wherein the cartridge handling apparatus is configured to remove the first filter cartridge from the cartridge dock and deposit it in the used cartridge bank.

17. The system of any one of claims 13 to 16, wherein the cartridge handling apparatus comprises an end effector that is configured to selectably grip the first filter cartridge and that is movable in at least two degrees of freedom.

18. The system of claim 17, wherein the cartridge handling apparatus comprises a carriage that is movable along a carriage rail, and an extension unit that is mounted to the carriage and is configured to support and move the end effector along an extension axis.

19. The system of claim 12 wherein the carriage rail is substantially linear.

20. The system of claim 19, wherein the extension axis is substantially linear and is substantially orthogonal to the carriage rail.

21. The system of any one of claims 1 to 20, wherein the gamma detector apparatus comprises a sensor portion that is movable between: a) a measurement position in which it is adjacent the first filter cartridge whereby removal of the first filter cartridge from the cartridge dock is inhibited by the sensor portion; and b) an exchange position, in which the sensor portion is spaced apart from the first filter cartridge whereby the first filter cartridge can be removed from the cartridge dock.

22. The system of claim 21, wherein the gamma detector apparatus further comprises a detector actuator that is communicably linked to the controller and supports the sensor portion, the detector actuator being configured to selectably move the sensor portion between the measurement position and the exchange position.

23. The system of claim 22, wherein the detector actuator comprises a linear actuator that is configured to linearly translate the sensor portion between the measurement position and the exchange position along a detector axis.

24. The system of claim 22 or 23, wherein the detector actuator is operable independently of the cartridge handling apparatus.

25. The system of any one of claims 1 to 24, wherein the gamma detector apparatus includes at least a first detector that is aligned with the first filter, and a second detector that is spaced apart from the first detector and aligned with the second filter, and wherein the first detector is configured to generate a first detection signal that is based on the gamma radiation in the first filter, and the second detector is configured to generate a second detection signal that is based on the gamma radiation in the second filter.

26. The system of claim 25, wherein at least one of the first and second detectors comprises a gamma spectrometer, and preferably a CZT gamma spectrometer, that is at least partially laterally surrounded by a radiation shield to limit exposure to background radiation not emitted from the filter cartridge.

27. The system of any one of claims 1 to 26, wherein the sample supply port comprises a sample dock coupler comprising a curved supply sealing surface and wherein the cartridge gas inlet comprises a complimentary curved inlet sealing surface configured to seal against the supply sealing surface.

28. The system of claim 27, wherein the supply sealing surface is convex and the curved inlet sealing surface is concave.

29. The system of claim 27 or 28, wherein the supply sealing surface is pressed against the inlet sealing surface to seal the first filter chamber when the first cartridge is connected to the cartridge dock, and wherein the first cartridge is translatable away from the cartridge dock thereby separating the supply sealing surface and the inlet sealing surface without releasing a fastener.

30. The system of any one of claims 1 to 29, wherein the exhaust port comprises an exhaust dock coupler comprising a curved exhaust sealing surface and wherein the cartridge gas outlet comprises a complimentary curved outlet sealing surface configured to seal against the exhaust sealing surface.

31. The system of claim 30, wherein the exhaust sealing surface is convex and the curved outlet sealing surface is concave.

32. The system of claim 30 or 31, wherein the exhaust sealing surface is pressed against the outlet sealing surface to seal the second filter chamber when the first cartridge is connected to the cartridge dock, and wherein the first cartridge is translatable away from the cartridge dock thereby separating the exhaust sealing surface and the outlet sealing surface without releasing a fastener.

Description

DRAWINGS

[0054] The drawings included herewith are for illustrating various examples of articles, methods, and apparatuses of the teaching of the present specification and are not intended to limit the scope of what is taught in any way.

[0055] In the drawings:

[0056] FIG. 1 is a graph illustrating operating envelope options relating the predicted count rate on a filter for a given airborne radionuclide concentration, for different sampling durations (line style) and energy-dependent detector efficiencies (line color);

[0057] FIG. 2 is schematic representation of one example of a system for measuring airborne radionuclides;

[0058] FIG. 3 is top view of one example of a filter cartridge;

[0059] FIG. 4 is a side view of the filter cartridge of FIG. 3;

[0060] FIG. 5 is a cross-sectional view of the filter cartridge of FIG. 3, taken along line 5-5;

[0061] FIG. 6 is a partial cross-sectional illustration of portions of a system for measuring airborne radionuclides;

[0062] FIG. 7 is an enlarged view of a portion of FIG. 6;

[0063] FIGS. 8-11 are representations of the system for measuring airborne radionuclides of FIG. 2 in different configurations;

[0064] FIG. 12 is a photograph of portions of a prototype example of a system for measuring airborne radionuclides from a target environment;

[0065] FIG. 13a is a graph showing in-situ gamma counting efficiency of the aerosol-filter detector and iodine-filter detector evaluated with the .sup.152Eu and .sup.137Cs/.sup.241Am;

[0066] FIG. 13b is a graph showing simulated detector count rates of .sup.131I, .sup.137Cs, and .sup.103Ru during a hypothetical nuclear emergency, when the air sampler was following the sampling time-based algorithm for changing filters given in Equation 7;

[0067] FIG. 14 is a graph showing reconstructions of airborne concentrations of .sup.131I, .sup.137Cs, and .sup.103Ru during the hypothetical nuclear emergency;

[0068] FIG. 15 is a schematic representation of a test apparatus for evaluating the particle retention efficiency;

[0069] FIG. 16 is a CAD representation of the test apparatus of FIG. 15;

[0070] FIGS. 17a and 17b are photos of filters used in testing;

[0071] FIG. 18 is a graph showing pressure drop vs. flowrate with paper filter only;

[0072] FIG. 19 is a graph showing Pressure drop vs. flowrate with activated carbon filter only;

[0073] FIG. 20 is a graph showing Pressure drop vs. flowrate with paper and activated carbon filter combined; and

[0074] FIG. 21 is a histogram of aerosol particle size of transmitted through the filters vs the control (with no filters in place) during testing.

DETAILED DESCRIPTION

[0075] Various apparatuses or processes will be described below to provide an example of an embodiment of each claimed invention. No embodiment described below limits any claimed invention and any claimed invention may cover processes or apparatuses that differ from those described below. The claimed inventions are not limited to apparatuses or processes having all of the features of any one apparatus or process described below or to features common to multiple or all of the apparatuses described below. It is possible that an apparatus or process described below is not an embodiment of any claimed invention. Any invention disclosed in an apparatus or process described below that is not claimed in this document may be the subject matter of another protective instrument, for example, a continuing patent application, and the applicants, inventors or owners do not intend to abandon, disclaim or dedicate to the public any such invention by its disclosure in this document.

[0076] Emergency response situations involving unplanned releases of radiological material may require monitoring or analysis. Such situations include road accidents involving radiological cargo and unplanned discharges to liquid or air. Environmental remediation and decommissioning are another example of a situation where environmental monitoring systems may be employed. Analysis of environmental materials may involve a relatively long turnaround time (sometimes up to weeks of turnaround time) to account for the collection and shipping of the physical filters and samples to an off-site laboratory, the conducting of the testing itself and then time to transmit and receive the results. On-site analysis and monitoring of contaminants in air, dose and contaminant dispersion may all be helpful in the aftermath of an unplanned release of radiological material.

[0077] As described herein, portable systems for conducting real-time or near real-time have been developed that utilize in-situ gamma spectrometers. Gamma spectrometers that are suitable for use with the systems described herein are preferably configured so that they can measure large releases from early in the accident, as well as the persistent background from smaller leakages, and as such preferably are able to measure a wide range of potential activity concentrations, c.sub.a,i likely on the order of 10.sup.2 Bq/m.sup.3 to 10.sup.8 Bq/m.sup.3. Gamma spectrometers may have a fairly wide dynamic measurement range before becoming saturated, but the measurement range may be further increased, for example by sampling the air for shorter or longer durations of time.

[0078] The gamma spectrometers can be configured to measure a physical count rate of a species, ?.sub.i, which is related to the activity of that species on the filter, A.sub.f,i, by the gamma energy-dependent detection efficiency, ?.sub.i:

[00001] $\begin{matrix} {\dot{C}}_{i} = ?_{i} A_{f, i} & 1 \end{matrix}$

[0079] The activity on the filter then relates to how much is being captured by the volumetric flow rate of air, F, the filter efficiency, ?.sub.f, and the amount of time that the filter has been used, t.sub.f. In addition, the activity of the filter is also subject to radioactive decay, based on the decay constantly. As such, the count rate relates to the air concentration, c.sub.a,i, by:

[00002] $\begin{matrix} {\dot{C}}_{i} = ?_{i} F ?_{f} c_{a, i} \frac{1 - \exp (- ?_{i} t_{f})}{?_{i}} & 2 \end{matrix}$

[0080] Equation 2 assumes that the airborne activity concentration and air sample flow rate are both constant. In order to measure the count rate, the gamma spectrometer can acquire data over a specified period of time (a detection periods), ?t.sub.aq, in order to acquire an integrated count above background level, ?C.sub.i. This detection period is preferably sufficiently long so as to provide a relatively useful/acceptable signal to noise ratio in order to identify the peaks but is preferably sufficiently short in comparison with the increase in activity capture on the filter to approximate the transient count rate.

[00003] $\begin{matrix} {\dot{C}}_{i} ? \frac{? C_{i}}{? t_{aq}} & 3 \end{matrix}$

[0081] An algorithm, such as an algorithm presented in W. C. Evans, Quantitative methods for continuous particulate air monitoring, IEEE Transactions on Nuclear Science, Vol. 48 (5), pp. 1639-1657 (2001), can be used to calculate the air concentration, including the effects of radioactive decay, and is given by:

[00004] $\begin{matrix} c_{a, i} = \frac{1}{?_{i} F ?_{f} ? t} [{\dot{C}}_{i} (? t) - {\dot{C}}_{i} (0) + ? ?_{0}^{? t} {\dot{C}}_{i} (?) d ?] & 4 \end{matrix}$

[0082] Some assumptions can be made about the system for design and review purposes, for example, the filter efficiencies, ?.sub.f, can be assumed to be near one. The activity of short-lived radioisotopes on the filters will eventually plateau and possibly decrease over time, but at least some of the radioisotopes of interest herein (.sup.131I, .sup.137Cs, .sup.132Te, .sup.103Ru) either have half-lives that are greater than about 6 hours or are in equilibrium with longer-lived isotopes. This allowed Equation 2 to be reduced as follows for the purposes of the teachings herein, implying that the count rate will go up generally linearly the longer the filter is in place:

[00005] $\begin{matrix} {\dot{C}}_{i} = ?_{i} {Fc}_{a, i} t_{f} & 5 \end{matrix}$

[0083] A number of curves were calculated using Equation 5 and are shown in FIG. 1, given a sampling flow rate of 5 L/min. The relationship between the airborne radioactivity concentration and expected count rate on the filter are shown for a number of combinations of filter collection time and detector efficiency (e.g., for different gamma energies). This plot also shows some of the constraints associated with detecting radioactivity on a filter. If the count rate for a particular radioisotope is less than ?10 counts per minute (cpm), it is relatively unlikely that it could be observed unless very long acquisition times are used, especially if there is relatively a high background due to other radioisotopes captured on the filter. If the overall count rate is above ?10.sup.6 cpm, then it appears likely that the detectors described herein would start to saturate and may not be able to work in the desired manner.

[0084] As shown in exemplary FIG. 1, air concentrations between 10.sup.2 Bq/m.sup.3 and 10.sup.8 Bq/m.sup.3 can be measured, but not necessarily with a set sampling time period. With a conventional, fixed filter arrangement, one may only expect the filter to be changed once every ?24 hours at most during an emergency, and up to every 5-7 days during routine monitoring. If one of the fixed durations in FIG. 1 is used, the measurable concentration range is decreased by nearly three orders of magnitude in this example. However, the inventors have determined that if the filter cartridge can be changed dynamically in the field, preferably without the need for human intervention, they can be changed much more frequently, and therefore the system as a whole may be capable of obtaining useful measurements for a wider range of airborne concentrations.

[0085] Another system design consideration is the reduction in the sensitivity of the detector over time due to accumulated radioactivity within a given filter. For, example, the releases from a nuclear power plant during an accident, or other similar event, may tend to come in bursts, meaning that a cloud containing a relatively high concentration of radioactivity could pass by over a relatively short period of time, after which the amount of airborne radioactivity could drop substantially. For measurements taken using a conventional fixed filter, all of the accumulated radioactivity remains within a common filter media until it is manually changed/retrieved by a user. In spectroscopy, the error of a signal (inherent in the signal, in addition to other uncertainties from Compton background or peak interferences) is for the purposes of this description considered to be equal to the square root of the signal, in this case the count rate on the filter, such that:

[00006] $\begin{matrix} ? {\dot{C}}_{i} = \sqrt{{\dot{C}}_{i}} & 6 \end{matrix}$

[0086] Under these conditions, e.g., without changing the filter or waiting for radioactive decay, the count rate measured by a conventional system would remain high, and this error would tend to increase the scatter in the data taken after the airborne radioactivity concentrations drop back down at the end of the high concentration episode.

[0087] In contrast, the systems described herein can be configured to automatically use two or more filters over a given detection period which may help improve the temporal resolution of the measurements and address some of these known challenges. The system also preferably includes at least two different types of filters, such as at least one aerosol filter and at least one iodine filter, that can be configured to capture different radionuclides from an incoming air sample. Preferably, the system can separately detect the radionuclides capture on each filter, and more preferably is configured so as to be able to differentiate between aerosol and vapor iodine species. Such systems may use a second set of iodine-specific charcoal filters as well, as described herein. The in-situ measurements can then be accomplished with a pair of CZT gamma spectrometers (or other suitable detectors, one associated with each filter), and these can collect data while the system is sampling from the air.

[0088] Referring to FIG. 2, a schematic representation of one example of a portable system 100 for measuring airborne radionuclides from a target environment is illustrated. The system 100, and its components, are intended to be sufficiently portable, and optionally generally self-contained, such that the system 100 can be transported to an area or environment where a measurement of airborne radionuclides is desired, such as the area surrounding a nuclear power station or other potential source of airborne radionuclides. For the purposes of the present teachings, such areas can be considered to be the target environment and positioning the system within such environments is considered to be positioning the system 100 in situ or on site and is generally understood to be generally different from a laboratory or other building/environment that is remote from the area where airborne radionuclides are expected/suspected.

[0089] In this schematic example, the system 100 includes a system housing 102 that can support and/or contain the other system components. The housing 102 may be a generally solid housing, for example to help protect the interior components from rain, dust and other atmospheric contaminants, and may have solid or substantially solid walls, preferably with one or more openable doors or panels to provide access to the interior of the housing 102. Alternatively, the housing 102 may be a generally open, frame-like structure with some support points for attaching and mounting other system components but need not have a protective shell or the like. While schematically shown as a single, generally continuous structure, in some examples the housing 102 may include two or more separate housings, modules, containers or other such structures that collectively can be considered to be the housing of the overall system 100. Regardless of its overall configuration, the housing 102 can include a variety of suitable openings to accommodate the air sampling described herein, and to provide connections to any external modules that can interface with the system 100, such as power sources, controllers, communication and data connections and the like.

[0090] The housing 102 and the components it supports are preferably sized so as to be generally portable, and transportable from a storage location to an active, target location when use of the system 100 is desired. Accordingly, the housing 102 is preferably sized so that it can be carried by a user, or alternatively so that it can be handled using a suitable apparatus (such as a lift truck or crane) and can be transported on a conventional vehicle (such as a passenger car or van, a pick-up truck, airplane, ship, transport truck or the like) in order to be deployed in the target environment.

[0091] In this example, the system 100 includes a system gas inlet 104 through which samples of the air, and other gases from the surrounding, target environment can be drawn into the system 100 for measurement. In this illustrated example, the system gas inlet 104 is provided in the form of the open end of a conduit that extends within the housing 102. The system 100 also includes a system gas outlet 106 through which air can exit the housing 102 when the measurements described herein are complete. The gas outlet 106 may be connected to any suitable downstream processing apparatus if desired, or alternatively, as illustrated in this example, can be a generally open end of an airflow conduit that allows the exhausted air to simply vent back into the surrounding atmosphere.

[0092] A primary system gas air flow path 108 extends between the system gas inlet 104 and the system gas outlet 106 and provides the path thorough which air can flow through the system 100. In the examples described herein, the system gas air flow path 108 includes a plurality of different sections of piping/conduits that can be connected to each other when the system 100 is in use to provide a generally continuous, one-directional air flow path through the system 100. Preferably, at least some portions of the gas air flow path 108, including one or more of the conduits and other such structures, can be formed from a generally non-reactive material, such as glass, to help reduce chemical interactions between the incoming air sample and parts of the system 100 that are upstream from the filter cartridge(s). To help the system 100 operate as described herein, a variety of different air flow devices such as pumps and compressors, valves, pressure sensors, flow sensors, temperature sensors and other suitable apparatuses and sensors can be provided along the air flow path 108. In this schematic example, an air circulating pump 110 and a flow and pressure meter 112 are included as exemplary illustrations of such features.

[0093] In addition to the air flow devices, the system 100 includes a cartridge dock 114 that is provided in and helps form part of the primary air flow path 108. The cartridge dock 114 is a part of the system 100 that is configured to detachably connect to the filter cartridges that are used to help capture the airborne radionuclides and hold them for measurement and detection using the system 100 as described herein. The cartridge dock 114 can therefore have any configuration that is suitable for connecting with a given filter cartridge design and will preferably have complimentary coupling and sealing portions to help provide a substantially gas-tight connection between the cartridge dock 114 and the interchangeable filter cartridges. Preferably, the system 100 is configured so that when a filter cartridge is coupled to the cartridge dock 114 it helps complete the primary air flow path 108 such that air can travel from the system gas inlet 104 to the system gas outlet 106 by passing through both the cartridge dock 114 and the connected filter cartridge. In this arrangement, when a filter cartridge is removed from the cartridge dock 114 it can interrupt the primary air flow path 108.

[0094] To capture the airborne radionuclides, the system 100 includes at least one filter cartridge, and preferably as described herein, can include a plurality of interchangeable filter cartridges that can be connected to the cartridge dock 114 over the course of a detection period while the system 100 is in use. In the illustrated example, multiple suitable filter cartridges 120 are shown as being part of the system, including a plurality of fresh or unused cartridges 120 and a plurality of used cartridges that have captured at least some quantity of airborne radionuclides and/or other contaminants as schematically illustrated by the presence of one or more small circles on the cartridge 120.

[0095] Referring also to FIGS. 3-6, one example of a filter cartridge 120 that is suitable for use with the systems 100 described herein includes a cartridge housing 122 that, in this example, includes and upper wall 124, an opposing lower wall 126 that is spaced from the upper wall 124 by a cartridge thickness 128 and a sidewall 130 that extends between the upper and lower walls 124 and 126. Together, the walls 124, 126 and 130 cooperate to surround an interior air flow passage or cartridge flow path 133 within the filter cartridge 120.

[0096] This filter cartridge 120 is configured to hold two filters and to allow air to pass through the body of the filter cartridge 120 such that it can form part of the overall, primary air flow path 108 when the filter cartridge 120 is in use. In this example, the filter cartridge 120 includes an air inlet 132 that can be connected to the air flow conduits (such as to the sample supply port and exhaust port, respectively, as described herein) that form part of the primary air flow path 108 in a generally air-tight manner so that air can flow into the filter cartridge 120. In this example the air inlet 132 is a hole/aperture formed in the upper wall 124 of the filter cartridge 120 but may have different configurations in different examples.

[0097] The filter cartridge 120 also includes an air outlet 134 that can be connected to another conduit forming part of the primary air flow path 108 when the cartridge 120 is in use. An internal cartridge flow path 136 (see FIG. 5) extends between the air inlet 132 and air outlet 134 and provides air flow communication through the cartridge 120.

[0098] The filter cartridge 120 in this example is configured to hold two filters that are to be positioned within the primary air flow path 108 so that material that is traveling through the air flow path 108 with the air sample will get caught on the filter(s) and can be retained for measurement and analysis. For example, the air pump 110 can be configured to turn on once the cartridge 120 is in place may start drawing air in (for example at about 5 L/min as illustrated), and the flow meter and pressure sensor 112 can be used to monitor the air sampling rate. The gamma spectrometers may start counting when the air pump 110 turns on and may, along with the controller 186, tracks the radionuclide activity as it accumulates on the filters within the cartridge 120 as described herein. Other apparatus, valves and the like can be provided in other examples.

[0099] The filters may be positioned anywhere within the cartridge airflow path 136 that is suitable, and may be positioned in parallel, or preferably in series with each other. In this example the cartridge 120 includes a first filter chamber 138 that is defined by portions of the housing/body of the cartridge 120 and is configured to house a first filter 140 (FIG. 5). The first filter chamber 138 in this example is positioned at the air inlet 132 (but could be in another location in other examples).

[0100] Preferably, the first filter 140 is sized to generally match the dimensions and shape of the first filter chamber 138 and is exposed to the incoming air flow. The first filter 140 can be any suitable type of filter media that is appropriate for capturing the target airborne contaminants, preferably can be an aerosol filter that is formed from a suitable material, such as cellulose and is operable to capture particulates from the passing air. One example of a suitable aerosol filter is a Whatman? qualitative filter paper, Grade 1 (WHA1001047). Optionally, the first filter chamber 138 can be openable to allow the first filter 140 to be inserted and removed as desired. In some examples, a used filter may be removed from the filter cartridge 120 and may be replaced with a fresh filter media. This can allow a given filter cartridge 120 to be used multiple times.

[0101] This cartridge 120 also includes a second filter chamber 142 that is downstream from the first filter chamber 138 and is, in this example, located at the air outlet 134 (but could be in another location in other examples). The second filter chamber 142 is configured to hold a second filter 144. The second filter 144 could be the same type of filter as the first filter 140, but preferably is a different type of filter-such as an iodine-specific charcoal filterthat is configured to capture a different type of airborne contaminant than the first filter 140. In this arrangement the filter cartridge 120 can be considered a two-stage filter, and different types of contaminants will be caught on the different filters 140 and 144 that are positioned in different locations. This may help facilitate the independent measuring the contaminants on the filters 140 and 144, which may allow the system 100 to separately monitor

[0102] Because each filter cartridge 120 is intended to be used for a predetermined use period, it may be advantageous the cartridges 120 can be connected and disconnected to the air flow path 108 in a relatively easy manner, and preferably in a generally one-step processes that does not require the separate activation or manipulation of a fastener, connector or the like in order to establish the desired, air-tight seal. For example, in may be preferable in some examples of the system 100 that the cartridges 120 can be coupled to the corresponding portions of the system (such as the cartridge dock 114 as described herein) via movement in single coupling direction, such as a translation of the cartridge in an insertion/removal direction. Optionally, the insertion/removal direction can be a generally linear movement path, and the cartridge 120 can be moved via a suitable linear actuator or the like. This may help facilitate automated attachment and removal of cartridges 120 and may reduce or possibly eliminate the need for a user to manually attach or remove the cartridges. Enabling this type of relatively simple attachment and removal can include having appropriate coupling and sealing features on the filter cartridge 120, and complimentary coupling and sealing features on the other portions of the system 100. Any suitable, complimentary set of features may be used.

[0103] Referring to also to FIGS. 6 and 7, an enlarged view of a portion of the system 100, illustrating some of the features of the cartridge dock 114 is illustrated. In this example, the cartridge dock 114 includes at least a portion of a filter supply conduit 150, terminating in an air sample supply port, and a filter exhaust conduit 152, terminating in an exhaust port, that form part of the primary air flow path 108. Each conduit 150 and 152 terminates in an open, free end that is provided with a dock coupler 154. In this example, the dock couplers include generally round, ball joint features that are provided at the sample supply port and exhaust port at the ends of the conduits 150 and 152. The ball joints at the ports can have generally smooth and convex outer surfaces, such as lower convex sealing surface 156 as illustrated in FIG. 7. These surfaces can form a least part of the seal with the cartridge 120. To provide a complimentary, concave sealing surface that can engage and seal with the sealing surface 156 the filter cartridge 120 illustrated in this example includes a cartridge coupling member 158 that is provided in the form of a generally annular sealing member that has a concave sealing surface 160 that is configured to seal against the convex sealing surface 156 when the cartridge 120 is docked as shown in FIG. 7. To disconnect the cartridge 120, it can be moved linearly away from the cartridge dock 114, downwardly as illustrated in FIG. 7, to disengage the concave sealing surface 160 that is configured to seal against the convex sealing surface 156. In this example, the cartridge coupling members 158 laterally surround the gas inlets and outlets 132 and 134, and the first and second filter chambers 138 and 142.

[0104] In the illustrated example, moving the cartridge 120 linearly away from the cartridge dock 114 will automatically interrupt the air flow connection between the cartridge 120 and the primary air flow path 108 and can also expose the filters 140 and 144 that are housed in their respective filter chambers 138 and 142. This may eliminate the need to touch or open a chamber door or other such structure in order to inspect or access the filters 140 and 144.

[0105] When the cartridges 120 are connected to the cartridge dock 114 and the system 100 is in use, airborne contaminants that are entrained in the air drawn into the primary air flow path 108 can be caught in the filters 140 and 144. As the contaminants accumulate on the filters 140 and 144 the amount and/or type of contaminants can be measured by the system using a suitable sensor, such as gamma detector as described herein. Because different types of contaminants may be retained in the different filter types 140 and 144, measuring the gamma radiation emitted from each filter 140 and 144 separately may allow the system 100 to simultaneously detect and/or measure the concentration of two or more different types of airborne contaminants.

[0106] Referring again to FIGS. 2 and 6, in the illustrated example the system 100 includes a gamma detector apparatus 170 with a sensor portion 172 that can be positioned adjacent the filter cartridges 120 and aligned or registered with respective filters 140 and 144 when the system 100 is in use, as shown schematically in FIG. 6. The sensor portion 172, and optionally other parts of the gamma detector apparatus 170, is preferably movable so that it can be moved between a measurement position as shown in FIG. 6 in which it is adjacent the first filter cartridge, and an exchange position (see FIG. 8), in which the sensor portion 172 is spaced apart from the filter cartridge 120 by a distance that is sufficient to allow the filter cartridge 120 to be vertically detached from the cartridge dock 114. While the sensor portion 172 is in the exchange position a used cartridge 120 can be removed from the cartridge dock and replaced with a fresh cartridge 120. With a fresh cartridge 120 in place, the sensor portion 172 can be returned to the measurement position (see also FIG. 10).

[0107] In this example, the sensor portion 172 includes two separate gamma spectrometers 174, each contained in a respective shielded housing 176 that can be a tungsten shield or the like, which may help reduce the detection of false radioactivity readings from the surrounding environment. Such shielding may be important in some situations, such as when the system 100 is deployed near nuclear power plants during an emergency, where the environment around the system 100 may be contaminated. Optionally, a tungsten collimator (e.g., a 20 mm high, 35 mm internal diameter in some examples) may be placed between the spectrometers 174 and the cartridge 120 to help further narrow the field of view. This type of directionality and limiting of exposure for each spectrometer 174, for example by using the collimators described or other such hardware, may help to prevent radioactivity from, for example, the aerosol filter 140 from being viewed by the spectrometer 174 that is focusing on the iodine filter 144, and vice versa.

[0108] To help reduce the chances of such mixed readings between the spectrometers 174, the filter chambers 138 and 142, and filters 140 and 144 therein, are preferably laterally spaced apart from each other by an offset distance 180 (FIG. 5) that is between about 2 cm and about 50 cm and may be between about 5 cm and about 20 cm (e.g., in a horizontal direction as illustrated in FIG. 5).

[0109] When the sensor portion 172 is in the measurement position, each spectrometer 174 is aligned with a respective one of the filters 140 and 144. In this arrangement, one of the spectrometer detectors 174 can generate a first detection signal that is based on the gamma radiation in the first filter 140, and the second of the one of the spectrometer detectors 174 may generate a second detection signal that is based on the gamma radiation in the second filter 144. These signals may be sent to the system controller 186 for processing. The controller 186 can then generate suitable user outputs and/or output signals. The first and second detection signals may be different if different amounts of radiation are detected in the filters 140 and 144.

[0110] Similarly, positioning the spectrometers 174 relatively close to the filters 140 and 144 in the axial direction (e.g., vertically as illustrated in FIG. 6) may help improve the quality and/or accuracy of the measurements. One factor that can affect the vertical/axial spacing between the spectrometers 174 and the filters 140 and 144 is the thickness 128 of the cartridge 120. Preferably, the cartridge thickness 128 is relatively small, so that the gamma spectrometers that are positioned adjacent the lower wall 126 can still be sufficiently close to the filters within the cartridge to obtain a useful measurement. Optionally, the thickness 128 may be less than about 20 cm, and preferably can be less that about 10 cm, and between about 3 and 6 cm. Preferably, the spectrometers 174 are positioned as close to the filters 140, 144 as practical as this can help increase signal quality.

[0111] To help move the sensor portion 172 in this manner, the gamma detector apparatus 170 can also include any suitable type of actuator, such as the detector actuator 178 schematically illustrated FIGS. 2 and 8-9 and 11, that can support the sensor portion 172, and move it between the measurement position (FIGS. 2 and 11) and the exchange position (FIG. 9). This the detector actuator 178 can include a linear actuator and may be pneumatically, hydraulically or electrically powered, or may be any other suitable apparatus. The detector actuator 178 is preferably communicably linked to the controller 186, such as by a wired or wireless connection, and supports the sensor portion 172.

[0112] Preferably, the detector actuator 178 can be controlled independently of the cartridge handling apparatus described herein, but optionally the movements of the different actuators can be coordinated, such as by the controller 186 to help facilitate the cartridge exchanges described herein.

[0113] To help facilitate the exchange of the cartridges 120, and operation of the system 100 in a generally autonomous manner, the system can include a suitable cartridge handling apparatus 190 that can be controlled by the controller 186. The cartridge handling apparatus 190 is preferably configured to be able to remove the one, used filter cartridge 120 from the cartridge dock 144 at the end of its cartridge use period and to then connect a replacement, fresh filter cartridge 120 to the cartridge dock 114 without the need for intervention by a human user/operator.

[0114] Preferably, to help manage the supply of cartridges 120 the system 100 can include at least one fresh cartridge bank that is able to hold one or more unused cartridges, illustrated schematically in FIG. 8 as fresh bank 192. Similarly, the system 100 preferably includes at least one used cartridge bank that is able to hold one or more used cartridges, illustrated schematically in FIG. 8 as used bank 194.

[0115] In this example, the cartridge handling apparatus 190 is therefore preferably configured to retrieve used cartridge 120 from the cartridge dock 114 (see FIGS. 2, 8 where the sensor portion 172 is moved to the exchange position and 9) and convey it toward the used bank 194. An unused cartridge can then be obtained from the fresh bank 192 and the cartridge handling apparatus 190, can connect it to the cartridge dock 114 (FIG. 10). The sensor portion 172 can then be returned to the measurement position (FIG. 11) for the suitable cartridge use period. A variety of apparatuses may be used for this purpose.

[0116] In the illustrated example, the cartridge handling apparatus 190 is schematically illustrated as including an end effector portion, such as a pneumatic gripper 196 that can grasp the cartridges 120. The pneumatic gripper 196 is preferably movable in at least two degrees of freedom to help achieved the desired cartridge handling operations. For example, in this case cartridge handling apparatus 190 includes a carriage 198 that is mounted to and can slide along a rail 200 in a first, lateral translation direction 202. In this example the rail 200 is illustrated as being linear/straight, but may have other shapes (e.g., curved, inclined, etc.) in other examples.

[0117] An extension unit 204 is mounted and is translatable with the carriage 198 and supports the pneumatic gripper 196 (FIG. 9) and can extend in a second direction to move the cartridge 120 toward and away from the cartridge dock 114. This may include a pneumatic piston/cylinder, ball screw, scissor lift, linear rail or other such hardware. In this example, the extension of the extension unit 204 is generally orthogonal to the movement of the carriage 198, but in other examples may be of a different arrangement.

[0118] The system controller 186 is illustrated schematically in the examples herein, but may be any suitable computer, processor, programmable logic controller and the like that can be connected to the components of the system 100, such as the cartridge handling apparatus, the gamma spectrometers, gas handling equipment and the like. The system controller can be communicably linked to these various components using any suitable communication hardware/protocol, including wires, wireless connections (such as BlueTooth or WiFi), infrared communication devices, radio transmitters/receivers and the like.

[0119] The system controller can include any suitable input and output devices to allow a user to interface with the system, including a keyboard, mouse, track pad or other input device, a monitor/screen, speakers or other sound producing transducers, lights, voice/speech capabilities, an interface with an app or other similar software running on a parallel device (such as a smart phone, tablet or the like) and other suitable devices.

[0120] While schematically shown as a single unit, the system controller may, in some examples, include multiple different, physical devices that are separate from each other but that a in communication with each other and can function together to perform the functions of the system controller described herein.

[0121] When the system 100 is in use, the gamma spectrometers 174 can each generate respective sensor output signals that are proportional to the number of radionuclides that are captured/present in the filter 140 or 144 they are aligned with. These signals may be any suitable format and can be provided to the controller 186. The controller 186 can then generate a suitable output based on the received sensor data. This output can include recording data associated with the sensors, such as radiation levels, identification or classification data that can help identify the particular airborne contaminant that is present in the sample and the like. The controller 186 can also utilize other incoming data/information, such as weather data, temperature, time, location data and other suitable data. These different sources of data can be utilized by the controller 186 to generate one or more desired user outputs, such as a time-based record of the measured radiation levels, graphs, reports, on-screen displays, warnings or alerts (for example if a recoded value exceeds a pre-determined alarm threshold) and other such outputs. The user outputs may be locally generated by the controller, such as by sounding an alarm or triggering a light, and/or the information may be communicated to an outside or remote device that is physically separate from the housing 102, such as a computer, tablet, smart phone or the like.

[0122] To confirm the operation of the system 100 described herein, a prototype system was constructed for testing purposes. Referring to FIG. 12, a photograph of a portion of the prototype apparatus is shown. Portions of the prototype are similar to portions of the system 100, and like features are identified using like reference characters. FIG. 12 shows an example test cartridge 120 that is connected to a cartridge dock 114, with the sensor portion 172 positioned in the measurement position.

[0123] The two gamma spectrometers in this example are Kromek GR1 CZT detectors, and the Kromek MultiSpect Analysis software is employed on the system controller 186 to capture and record the gamma spectrometry measurements. The tungsten shields 176 were from the Canberra CSM-GR1 system. Early prototypes of the filter cartridges 120 were 3D printed out of polylactic acid (PLA), and other versions were manufactured out of PTFE. Festo components were employed for the linear axis slide, pneumatic pistons, and pneumatic grippers, along with the control software and other accessories to provide portions of the detector actuator 178 and the cartridge handling apparatus 190.

[0124] The in-situ detector efficiency of this prototype was evaluated using a set of fixed sources, which were placed on the aerosol or iodine filters for counting to simulate the collected radioactivity. Two different sources were employed: a 6.47?10.sup.3 Bq .sup.152Eu source with gamma energies of 40.1 keV, 121.8 keV, and 344.3 keV, and a mixed source with 5.86?10.sup.3 Bq of .sup.241Am and 1.31?10.sup.4 Bq of .sup.137Cs with gamma energies of 59.5 keV and 661.7 keV. Both sources were 40 mm diameter discs that fit within the filter chambers. Four measurements were done with each source being placed over either the aerosol or iodine filters, and these were done for 5 minutes each. The in-situ efficiency could be evaluated by comparing the net count rate over the time period to the known activity of each radionuclide and the relative intensity of the gamma rays. This is shown as a function of gamma energy for the aerosol-filter detector and iodine-filter detector in FIG. 13a. In this test the filters were 56 mm above the top of the CZT spectrometers.

[0125] Using the measured detector efficiency as described herein, an expected performance of the proposed air sampling system was modelled, against a hypothetical mix of radionuclides in air samples. The detector count rates over time and the cartridge changing frequency (e.g., the length of a given cartridges use period) were particular targets of this assessment.

[0126] A sampling time-based algorithm is used to decide when to change the cartridges. A maximum acceptable count rate, ?.sub.i,max, is established, and compared to the actual count rate in the energy range of a radioisotope of interest, ?.sub.i, and the time that the filter cartridge has been in place so far, t.sub.f, and this t.sub.f,max value is evaluated up to a maximum of 24 h, as given in Equation 7. The ?.sub.i,max, value is energy-dependent, as the higher energy gamma emissions have a lower detection efficiency. This metric is evaluated continuously as data is being recorded, but its minimum value throughout that time period is used as the basis of comparison. When the actual time that the cartridge has been in place exceeds t.sub.f,max, the filter is changed. When air concentrations are increasing, t.sub.f,max will shrink rapidly as ?.sub.i approaches ?.sub.i,max, and the filter change will occur when it does so. When air concentrations are decreasing, C; would plateau and stop increasing as fast, and so a t.sub.f,max value from earlier in the sampling period to establish the maximum sampling period.

[00007] $\begin{matrix} t_{f, \max} = \min (24 h, \frac{{\dot{C}}_{i, \max}}{{\overset{?}{C}}_{i}} t_{f}) & 7 \end{matrix}$

[0127] A hypothetical case involving a time-varying mixture of .sup.131I, .sup.137Cs, and .sup.103Ru in the air, released from a nuclear power plant accident, was simulated. The simulated count rate on the aerosol filter-facing detector is given in FIG. 13b, and the real and reconstructed air concentrations of each radioisotope is shown in FIG. 14. To be more realistic, noisy count rates were generated by sampling from a normal distribution with an expected value, ?=?.sub.i, and standard deviation, ?=?{square root over (?.sub.i)}, of the count rate from Equation 5. In the scenario, there was an initial period about 12 hours after the start of the accident with major releases and very high outdoor radionuclide concentrations, followed by an intermediate period with lower releases, and a second stage of large late releases after about 40 hours. The airborne concentrations decreased significantly after the second period of large releases. The major .sup.131I and .sup.137Cs release occurred during the same time windows, but the large .sup.103Ru releases during the initial major spike had a longer duration.

[0128] Based on the inventors' analysis of the model, including FIG. 13b, it was determined that it may be desirable for the filter cartridges 120 to be changed quite frequently during the major spikes. In both spikes, the sampling duration was only around 30-40 minutes. The reconstructions of the airborne concentrations generally closely matched the actual concentrations that were simulated, as shown in FIG. 14. These were given in the figure in 10-minute increments, which allows for a relatively higher time resolution for data reporting than would normally be possible for fixed filters that are manually collected and analyzed in an external laboratory. The data for .sup.137Cs was noisier than that of .sup.131I and .sup.103Ru in this testing, possibly because of the smaller count rates and lower outdoor concentrations. There were also some periods when the airborne concentrations were over-predicted after a large decrease, which may be a result of the noise in the count rate signal masking the plateau when the amount of new activity accumulating on the filter was decreasing. This may have been caused by the high activity on the filters from earlier when airborne concentrations were higher, and the over-predictions often lasted until the filter 120 was changed. These differences were relatively small and did not appear to materially change the performance of the system 100, but it does underline the need to have a good set of metrics for changing the filters.

[0129] Some additional testing of the system 100 was conducted to determine the aerosol retention efficiency and pressure drop across the chosen filter cartridge 120 design. This testing involved testing the pressure drop across the paper (aerosol) and activated carbon (iodine) filters at multiple flow rates, testing the aerosol density measurements before and after each filter at multiple flow rates, conducting a seal test, to determine if the cartridge or associated connections can function as intended, and testing to failure to determine the pressure and flow rate limits of the filters that were used in this first example. This testing was conducted in a suitable test room at the Chalk River Laboratories, operated by Canadian Nuclear Laboratories, in Ontario, Canada.

[0130] In one part of the testing, a Whatman? aerosol filter was installed as the first filter 140 at the inlet 132 and an activated carbon iodine filter is installed as the second filter 144 at the outlet 134 of the cartridge. In order to monitor the radioactivity being captured on each filter unit, gamma spectrometers 174 are positioned immediately beneath the filter chambers 138 and 142 in the cartridge 120 as shown schematically in FIG. 6.

[0131] FIGS. 15 and 16 are representations of a test apparatus used to conduct the testing described herein. The test apparatus includes an aluminum extrusion frame supporting an assembly of tubing and various instruments and air inputs. The compressed air line 150 is split, one side going to the aerosol generator 220 and the other going to the main air inlet of the tubing assembly. The aerosol generator 220 outputs into the tubing assembly, where a pressure transducer 222 is connected. The flow from the tubing assembly is then directed through a glass tube, with sealing member 154 and into the test cartridge 120, where the aerosols are captured by the filters. Air is then vented out of a second glass tube 152, where the sampling for the optical particle sizer 224 takes place. To capture the baseline concentrations, the aerosol sampling for the optical particle sizer 224 took place at the output of the first glass tube. Different aspects of the test apparatus are listed below.

[0132] In this arrangement, the aerosol generator 220 receives compressed air at ?200 kPa and uses that to generate water aerosols at a rate of about 3 mL/min. The liquid in the aerosol generator 220 is a 5 wt % solution of NaCl in water. The water in the aerosols that are produced evaporates after mixing with the main air stream, leaving residual NaCl aerosols. The pressures and flowrates of the air that goes to the main input can be varied to allow for testing of the filter efficiency under different conditions. The tubing assembly, seen in FIGS. 15 and 16, is a series of straight sections and Ts that allow for the various inputs and sensors to connect.

[0133] A list of equipment and instrumentation installed in the test apparatus is given in Table 1.

TABLE-US-00001 TABLE 1 List of equipment/instrumentation and required calibration for each type Aerosol Purpose: NaCl aerosol generation Generator Model: TSI-3076 Calibration requirements: none Air Supply Purpose: Air supply Model: n/a (part of LSCF) Calibration requirements: none Pressure Purpose: Air supply Regulator Model: Festo MS4N-LFR Calibration requirements: none Optical Purpose: Record the density and size of airborne particles Particle Model: TSI 3330 Sizer Calibration requirements: yearly factory calibration Pressure Purpose: Measure differential pressure across the filter. Transducer 10 Volt maximum corresponds to 2 PSI linearly to 0. Model: Omega PX309-002G10V Calibration requirements: factory certification or CNL calibration shop, before start of test and yearly thereafter

[0134] Data that is recorded during the testing includes: particle size distribution of aerosols in positions up and downstream of the cartridge without filters, and downstream of the cartridge 120 with various filters; air supply volumetric flow rate, and differential pressure across the cartridge 120.

[0135] Testing was conducted using two different aerosol filters, Whatman? activated carbon loaded paper, Grade 72 and Whatman? glass microfiber filters, Grade GF/A, as shown in FIG. 17. The conditions for the experimental design are given in Table 2. These tests involved keeping the input to the aerosol generator 220 substantially constant (193 kPa and 5 SLPM). Here, SLPM refers to standard liters per minute. The flow rate into the tubing fixture was varied from 5 SLPM to 55 SLPM when possible.

TABLE-US-00002 TABLE 2 Experimental design, including filter configuration and flow rates Filter Configuration Flow Rate Range* Trial 1 control (no filter) 5 to 55 SLPM Trial 2 control (no filter) 5 to 55 SLPM Trial 3 paper only 5 to 55 SLPM Trial 4 paper only 5 to 55 SLPM Trial 5 activated carbon only 5 to 55 SLPM Trial 6 activated carbon only 5 to 55 SLPM Trial 7 paper & activated carbon 5 to 55 SLPM Trial 8 paper & activated carbon 5 to 55 SLPM *or until filter breaks

[0136] The procedure for these experiments was to assembly the cartridge 120 with the filter configuration for the given test. Insert the cartridge 120 into the test apparatus and ensure that the test preparation steps were completed with the PVC air input at the desired rate and the system at a sufficiently stable, steady state. The flowrate through the PVC air-line was then set to the first value in Table 2. After giving time for the pressure to come to steady state, the OPS was run for a standard 1-minute collection time and pressure seen by the transducer is recorded. The air flow rate was then increased by 5 SLPM and the test steps were repeated until either the maximum flow listed in Table 2 is achieved or until the filters ruptured.

[0137] No significant leakage was detected throughout any of the tests. This was confirmed with the application of a soap solution at the interface of the glass ball joint and cartridge, in addition to the cartridge-cartridge joints. No bubbles were observed throughout the duration of each test run. These observations, combined with the pressure readings, qualitatively indicate that leakage through the seals is kept sufficiently low and that the design for the cartridge 120 and cartridge dock 114 performs as intended.

[0138] The raw data from the pressure drop testing measurements are given in Table 3 to Table 6. Plots of the pressure drop across the filters vs. flowrate with the paper filter only, the activated carbon filter only, and both filters in place, are given in FIG. 18 to FIG. 20, along with a second order polynomial fit to the data. The paper filters tested began to rupture when the pressure differential was about 10 kPa, giving an upper pressure bound for the automation system to use. An example of ruptured paper filters is shown in FIG. 17 (b), which tended to tear apart. The activated carbon filters tended to slip out of their frame, rather than tearing. As such, it is recommended that the final radionuclide monitoring system 100 may be operated with overall differential pressures that are preferably less than about 10 kPa with the paper and activated carbon filters both in place, which can correspond to flow rates of about 25 SLPM (see Table 6).

TABLE-US-00003 TABLE 3 Raw data, control tests without filters installed Flow Rate, Aerosol Concentration, ?g/m.sup.3 SLPM Trial 1 Trial 5 90000 96000 10 21100 57500 15 2720 11700 20 3720 7130 25 3870 5740 30 4900 7200

TABLE-US-00004 TABLE 4 Raw data, paper filter tests Flow Rate, Pressure Drop, kPa Aerosol Concentration, ?g/m.sup.3 SLPM Trial 3 Trial 4 Trial 3 Trial 4 5 1.03 1.03 0.608 0.417 10 1.79 1.72 0.448 0.00133 15 2.76 2.76 0.483 0.00175 20 4.14 3.79 1.88 1.35 25 5.52 5.52 2.93 2.54 30 7.24 6.89 4.91 2.58 35 9.65 8.96 3.62 3.16 40 11.72 11.03 3.40 2.97 45 13.79 13.44 3.93 1.99 50 2.60

TABLE-US-00005 TABLE 5 Raw data, activated carbon filter tests Flow Rate, Pressure Drop, kPa Aerosol Concentration, ?g/m.sup.3 SLPM Trial 5 Trial 6 Trial 5 Trial 6 5 1.17 1.38 0.49 0.74 10 2.07 2.21 3.04 0.98 15 2.76 3.03 7.32 2.46 20 4.00 4.14 4.53 1.71 25 4.83 5.52 4.64 0.99 30 6.21 6.89 2.22 0.62

TABLE-US-00006 TABLE 6 Raw data, combined paper and activated carbon filter tests Flow Rate, Pressure Drop, kPa Aerosol Concentration, ?g/m.sup.3 SLPM Trial 7 Trial 8 Trial 7 Trial 8 5 2.62 2.07 5.74 1.45 10 4.14 3.45 0.651 0.0645 15 6.21 4.83 0.128 0.0614 20 7.86 6.55 0.111 0.0104 25 8.96 8.62 0.187 0.419 30 11.72 0.0845 0.0550 35 13.79 0.409

TABLE-US-00007 TABLE 7 Net filtration efficiency with confidence intervals Activated Paper & Carbon Activated Paper Only Only Carbon Average Net Filter 99.9964% 99.9849% 99.9985% Efficiency* Confidence Intervalst (99.8798% ? (99.8899% ? (99.9937% ? 99.9999%) 99.9979%) 99.9996%) *the average filter efficiency is [00008] $?_{avg} = 1 - \exp (avg (\ln (\frac{c_{filtered}}{c_{unfiltered}}))),$ based on the geometric mean of the aerosol-penetration the confidence intervals are [00009] $C . I . = 1 - \exp (avg (\ln (\frac{c_{filtered}}{c_{unfiltered}})) ? stdev (\ln (\frac{c_{filtered}}{c_{unfiltered}})))$

[0139] The raw data from the filter efficiency testing measurements are given in Table 3 to Table 6. Filter efficiency could be determined from the ratio of the aerosol concentration at the exit of the cartridge with filters in place and not in place, according to Equation 8.

[00010] $\begin{matrix} ? = 1 - \frac{c_{filtered}}{c_{unfiltered}} & 8 \end{matrix}$

[0140] The aerosol generator 220 created NaCl aerosols with a mass median diameter of about 3.3 ?m and geometric standard deviation of 1.3. Measured particle size distribution histograms are shown in FIG. 21, which compares the results with no filter to results with either the paper filter or activated carbon filter in place, in their prescribed location in the cartridge, but without the other type of filter present. There is a large downward shift in the particle size distribution, meaning the filters are more efficient for particles >0.7 ?m. The paper filter had an overall efficiency of about 99.996%, while the activated carbon filter had an overall efficiency of 99.98%, as given in Table 7. When combined, the overall filtration efficiency when both filters were in place was about 99.999%. When implemented in the final radionuclide monitoring system, this means that nearly all of the aerosols should be effectively captured on the paper filter, and there should be limited by-pass of aerosols onto the activated carbon filter.

[0141] What has been described above has been intended to be illustrative of the invention and non-limiting and it will be understood by persons skilled in the art that other variants and modifications may be made without departing from the scope of the invention as defined in the claims appended hereto.

PORTABLE SYSTEM FOR MONITORING AIRBORNE RADIONUCLIDES

Inventors

Cpc classification

Classification Explorer

G01N1/2273

PHYSICS

Classification Explorer

G01T1/366

PHYSICS

Classification Explorer

G01N1/2205

PHYSICS

Classification Explorer

G01T1/178

PHYSICS

Classification Explorer

G01T7/04

PHYSICS

Classification Explorer

G01N2001/2288

PHYSICS

Classification Explorer

G01N2001/021

PHYSICS

International classification

Classification Explorer

G01T7/04

PHYSICS

Classification Explorer

G01T1/36

PHYSICS

Abstract

Claims

Description