CONSTANT SENSITIVITY SUPERHEATED DROPLETS RADIATION DETECTOR/DOSIMETER

Abstract: Radiation detectors and dosimeters (1) of the type comprising superheated droplets or detector liquid dispersed in a transparent or translucent elastic matrix are provided with temperature compensation means in order to provide a more constant sensitivity. This comprises a self-regulating pressure control system, e.g. a pressure-multiplying piston (9,10) or bellows assembly pressurised by a volatile liquid contained in a chamber (15) and sensitive to the operating temperature, and by means of which varying pressure is applied to the matrix (1) via a diaphragm (3) in order to maintain a substantial constant differential between the vapour pressure of the liquid and the overpressure on the matrix.

Description: This invention relates to the detection and measurement of radiation, such as neutron, gamma and microwave radiation, by the observation of vapourised droplets of superheated detector liquid in a suitable matrix. Radiation detectors and dosimeters of this type are described for instance, in U.S. Patents Nos. 4,143,275; 4,350,607; 4,613,758 and 4,779,000. Similar detectors and dosimeters are also described in Soviet Atomic Energy (USA), Vol.63, No. 1, pp. 565-8, July 1987, V.I. Ivanov et al. Of particular relevance to the background of the present invention are the disclosures of EP-A-0144120 and EP-A-0260844. EP-A-0144120, which corresponds to US Patent 4779000 listed above, discloses a direct reading dosimeter for neutrons and other high linear energy transfer (LET) radiation comprising a dispersion of super-heated liquid droplets in a transparent or translucent solid, elastic medium. Impinging LET radiation causes those superheated droplets to vapourise leaving the vapourised droplets trapped and visible in the elastic medium. EP-A-0260844 describes a particular set of conditions affecting the degree of superheat of the superheated droplets and which render the detector sensitive to less energetic LET reduction such as gamma radiation and microwaves. As more experience is gained with this latter type of detector, it has become apparent that the sensitivity to radiation is affected significantly by variations in the operating temperature. Accordingly in applications where the operating temperature cannot be controlled for one reason or another, it would be highly desirable to eliminate, or compensate for this temperature dependence and thereby to provide radiation detectors and dosimeters of constant sensitivity. By constant sensitivity is meant a constant number of superheated droplets vapourised on exposure to a standard dose of radiation to be detected. The range of radiation to be detected ranges from microwave and low Linear Energy Transfer (LET) up to high (LET). In accordance with the invention as claimed this is achieved by continuously altering the overpressure on the matrix in concert with changes in the operating temperature so that the difference between the vapour pressure of the detector liquid PvL and the overpressure on the matrix Po, is substantially constant. Desirably the difference PvL-Po is typically 400 kPa for neutron detectors and greater than 400 kPa, e.g. 800-900 kPa, for gamma and microwave detectors. In accordance with one aspect of the invention, therefore, there is provided a method for the detection and measurement of neutron, gamma, microwave or similar radiation which comprises impinging said radiation on a radiation detector/dosimeter of the type comprising superheated droplets of a detector liquid dispersed throughout an elastic, translucent or transparent matrix and observing the vapourisation of those droplets consequent upon the impingement thereon of said radiation, wherein, in order to reduce sensitivity of the measuring system to operating temperature, the operating temperature is monitored substantially continuously and the overpressure Po on the matrix containing the superheated liquid droplets is adjusted automatically in consequence of any detected variation in the operating temperature in a direction to maintain a constant pressure differential between the vapour pressure PvL of the detector liquid and said overpressure Po. In a second aspect there is provided a radiation detector of the type comprising superheated droplets of a detector liquid dispersed throughout an elastic, transparent or translucent matrix and which droplets are visibly vapourised upon impingement thereon of said radiation, wherein means are provided to vary the overpressure Po on said matrix responsive to fluctuations in operating temperature and so as to maintain the pressure differential between the vapour pressure PvL of the superheated liquid droplets and said overpressure substantially constant. A self-regulating mechanical pressure control system is preferably used, for example a pressure-multiplying piston or bellows assembly pressurised by a volatile liquid, or a spring-loaded elastic diaphragm assembly. The piston or bellows assembly may be pressurised at the low pressure end by a volatile liquid. The ratio of the working area of the larger piston or bellows to the smaller is selected, in conjunction with the choice of volatile liquid, to obtain the desired constant sensitivity. The invention will be further described with reference to the accompanying drawings, in which: Figure 1 is a graph showing variation in neutron sensitivity of a superheated droplet detector (relative to that for a standard neutron dose at 20°C) with vapour pressure for two detector liquids Freon F-12 and C-318. Figure 2 is a graph depicting the change in sensitivity (droplets vapourized per millirem of radiation) with change in operating temperature for uncompensated (solid dots - prior art) and compensated (open circles - present invention) detectors. Figure 3 is a graph illustrating the various pressures for a compensated detector (Ex. 1) as operating temperature changes, and showing that Pvl-Po remained constant. Figure 4 is an exploded view of a compensated detector having pressure-multiplying pistons activated by a volatile overpressure liquid (Ex. 1). Figure 5 is an exploded view of an alternative partial assembly in which pressure-multiplying bellows are substituted for the pistons in Figure 4. Figure 6 is an exploded view of an alternative partial assembly in which a confined spring is used. Detailed Description The basic detectors are fully described in the references given above. Our studies have shown that superheated droplet detector sensitivity to radiation is related to the pressure difference between the effective vapour pressure of the detector liquid droplets (Pvl) and the pressure over the detector matrix or medium (Po). In a typical detector where no attempt is made to apply temperature compensation, the external pressure on the detector matrix is normally atmospheric pressure. We have found that (within a limited temperature range) the detector sensitivity changes in direct proportion to the term Pvl-Po (see Figure 1 where Po is constant at atmospheric). The term Pvl is fixed by the physical properties of the detector liquid, however Po (the external pressure or "overpressure") can be set arbitrarily. In Figure 1, the relative sensitivity is the ratio of the response to neutrons at various temperatures to the same response at 20°C. Given such a degree of freedom, the change in detector sensitivity with temperature can be nullified by making the external pressure applied to the detector matrix Po some appropriate function of temperature. This overpressure-temperature function must be such as to give a constant pressure difference between the overpressure and the vapour pressure (i.e. Pvl-Po is constant) over the detector working temperature range. Preferred constraints placed on a real temperature compensation system (a) For a typical neutron detector, a pressure difference (Pvl-Po) of about 400 kPa is suitable: for other forms of radiation of lower LET, higher pressure differences will be required, e.g. 750 kPa for gamma, and 900 kPa for microwave. (b) The operative compensation range is at least 15-35°C. (c) Compensation should be accurate within ± 25%. (d) The compensation system should be small and reliable, and not require external power (preferably non-powered). While typical values for Pvl-Po have been indicated, these are not critical: ranges of values for Pvl-Po could be used, e.g. for neutron radiation 100-700 kPa for gamma radiation 700-1000 kPa and for microwave radiation 800-1000 kPa. Use of vapour phase/condensed phase systems for direct overpressure generation Typical detector liquids now in use have normal boiling points in the -40 to +4°C range; however, for a typical neutron detector to operate under the constraints listed above, the normal boiling point must be below -25°C (in order to get at least 400 kPa vapour pressure at the lower temperature of 15°C). Taking Freon G-115 (trademark for chloropentafluoroethane) as a typical detector liquid, it can be shown that the set of properties for a vapour phase/condensed phase system that would act as an over-pressuring system for Freon G-115 within the above constraints is defined by a vapour pressure of about 101 kPa at about -10°C and an enthalpy of vapourization (ΔH v ) of about 40 kJ/mol. An extensive search of vapour phase/condensed phase systems has shown that such conditions do not exist in any vapour/liquid systems and could barely be approached in vapour/solid systems. A number of possible alternative methods of passive temperature compensation can be proposed. In general terms, what is required is a physical system that alters its properties or state as some reversible function of temperature and the variation is sufficiently powerful and adaptable that it can be used to apply the appropriate overpressure to the detector matrix. This involves selecting the temperature sensitive system, then determining how it can be set up to apply the desired overpressure-temperature function. The preceding observations have indicated one temperature sensitive system which could be used (two phase vapour/liquid mixture) and have shown that some adaptation is required to provide the correct pressure-temperature function. A second system that might be used is the thermal expansion of solids or liquids (amplified as necessary). For instance, a mechanical spring having an appropriate spring constant associated with or responding to a material with an appropriate thermal expansion coefficient may be used. This latter material may comprise the filling liquid above the detector matrix. These types of systems are the basis of the present invention. Temperature compensation is used to mean application of the appropriate overpressure to the detector matrix so that the detector will show the same sensitivity to radiation over the compensation temperature range. Three examples of suitable devices to accomplish the desired continuous pressure regulation are shown in Figures 4-6. Figure 4 is an exploded view of a detector with a pressure-multiplying piston assembly as in Example 1. The detector 1 (containing droplets dispersed in a suitable medium) has an open extension 2 (remote from the droplet-containing medium) adapted to seat against flexible elastic diaphragm 3 in chamber 5 in intermediate body 4. Body 4 contains passage 6 to accomodate travel of small piston 9 to contact diaphragm 3. Body 4 also contains chamber 7 adapted to receive large piston 10 and allow for piston movement therein. Opening 8 is sized to receive flexible diaphragm 11 and to mate with portion 14 of overpressure liquid container 12. Portion 14 has a chamber 13 sized to mate with part of large piston 10 via diaphragm 11. A suitable volatile liquid is introduced into chamber 15 (to a selected level) in container 12 via open extension 16: the latter is adapted to be sealed by cap 17. The detector and pressure multiplying mechanism are assembled such that the volume above the detector medium (including extension 2 in Fig. 4) is filled up to diaphragm 3 with a suitable inert filling liquid such as water or various aqueous salt solutions, in order that the pressure variations be transmitted to the droplets of detector liquid. In operation the vapour pressure of the volatile liquid in chamber 15 exerts pressure, through diaphragm 11, on large piston 10. The resultant force is transferred to diaphragm 3 through small piston 9. This force will produce a correspondingly greater pressure on the inert filling liquid portion of the detector and thus change the degree of superheat of the droplets. Figure 5 is an exploded view of an alternative to the piston assembly of Figure 4, in which the large and small pistons are replaced by large and small pressure-transmitting bellows 21 and 18 respectively. These bellows have sealing flanges at 20 and 3a. Small bellows 18 is contained in body 4a within passage 6a and projects inside large bellows 21 (chamber 5 mates with extension 2 as in Figure 4). Large bellows 21 is contained within chamber 22 of container 12a, the latter having portion 14a which mates with chamber 19 of body 4a. Chamber 15a of container 12a is adapted to contain a suitable volatile liquid and to be capped by cap 17 as in Figure 4. In operation, the vapour pressure of the volatile liquid in 15a exerts varying pressure on the bellows 21 which transmits this force directly to small bellows 18. Small bellows 18 transmits the varying pressure directly to the detector via extension 2 and the inert filling liquid as before. Figure 6 is an exploded view of a spring-driven pressure-control assembly. Extension 2 seats against diaphragm 3b in chamber 5 in body 23. Passage 6b permits travel of member 9a which is attached to rigid plate 25. Chamber 19a contains the spring 26 and allows movement of plate 25 against the spring. Portion 24 of body 23 is adapted to mate with chamber 27 in body 28 to confine the spring. In operation, the spring exerts pressure on plate 25 and thus on member 9a. Thermal expansion of the contents of detector 1 will deflect spring 26 and thus change the pressure exerted by the spring on diaphragm 3b. This pressure is arranged to vary with temperature as required for compensation of detector sensitivity by selecting an appropriate inert filling liquid above the detector medium and appropriate spring constant. Volatile overpressure liquids (e.g. for chamber 15 in Fig. 4) may be selected from octafluorocyclobutane (Freon C-318 - trademark), 1,2-dichlorotetrafluoroethane (Freon 114 - trademark), dichlorofluoromethane (Freon 21 - trademark), dichlorodifluoromethane (Freon 12 - trademark), chloropentafluoroethane (Freon G-115 - trademark), ethyl chloride and pentane; others may also be used. In the embodiments shown in Figures 4 and 5, suitable ratios of the working area of the large piston or bellows to that of the small may range from about 2 to about 8, but this range is not critical. A preferred range is about 2.5 to 3.5 with liquids of similar vapour pressure to ethyl chloride. Other possible combinations will be apparent to those skilled in the art, and the choice will take into account the vapour pressure of the detector liquid Pvl. In the embodiment shown in Figure 6, given a lower diaphragm 3b diameter of about 6 mm, the spring 26 may have a spring constant selected within the range, e.g. about 2000 to about 20000 N/m. Suitable materials for the spring include stainless steels. Suitable materials for the filling liquid include, for example, water, salt solutions, hexane, glycol, or ethyl ether. When the filling liquids are in direct contact with the detector medium, they should be inert and non-solvents with respect to this medium. Those skilled in the art will appreciate from the above disclosure other alternatives and combinations which will function to provide the desired compensation. The following Example is illustrative and should not be construed as limiting. Example 1 - Temperature Compensation of Neutron Detectors Sensitivity vs temperature for a typical neutron detector is given in Figure 2. Using a compensation assembly as shown in Figure 4 with a piston area ratio of about 2.8 and the working liquid in chamber 15 being ethyl chloride (chloroethane) we obtained a sensitivity vs temperature that was essentially constant between 10°C and 40°C (see Figure 2 - open circles-dash line). When this is compared with the vapour pressure curves for the same system (Figure 3) it can be seen that the results are exactly as desired, i.e. the resultant variable overpressure on the detector was sufficient to cancel the vapour pressure variation within the temperature range. Thus the piston assembly increased the overpressure Po above the Pv2 of the overpressuring liquid ethyl chloride, sufficiently to maintain Pvl (detector liquid)-Po (overpressure) constant (at about 400 kPa) over the desired range of temperature, in a self-regulating reliable manner. In the embodiment of Figure 4 used in this example, the actual dimensions and construction of the piston assembly was as follows. The diameter of chamber 15 was 0.79 cm and length 2.05 cm, and extension 16 and cap 17 had mating screw threads. The diameter of chamber 13 (and chamber 7) and of piston 10 was 1.27 cm with the length of 13 being 0.48 cm. The diameter of piston 9 (and passage 6) was 0.64 cm and the combined length of 9 and 10 was 1.75 cm. The depth of opening 8 was 0.64 cm and of passage 6 0.64 cm. Body 4 (diameter 2.22 cm) was split into two parts which joined by mating threads. Portion 14 and opening 8 had mating screw threads as did extension 2 and chamber 5. The length of chamber 5 was 0.95 cm. Body 4 had four side openings which were used for recompression/reactivation of the detector without dismantling.

Claims: A method for the detection and measurement of neutron, gamma, microwave or similar radiation which comprises impinging said radiation on a radiation detector/dosimeter (1) of the type comprising superheated droplets of a detector liquid dispersed throughout an elastic, translucent or transparent matrix and observing the vapourisation of those droplets consequent upon the impingement thereon of said radiation, characterised in that in order to reduce sensitivity of the measuring system to operating temperature, the operating temperature is monitored substantially continuously and the overpressure Po on the matrix containing the superheated liquid droplets is adjusted automatically in consequence of any detected variation in the operating temperature in a direction to maintain a constant pressure differential between the vapour pressure Pvl of the detector liquid and said overpressure Po. A method according to claim 1 as applied to neutron detection and wherein the pressure. differential PvL-Po is maintained at a substantially constant value in the range 100 to 700 kPa. A method according to claim 1 as applied to gamma radiation detection and wherein the pressure differential PvL-Po is maintained at a a substantially constant value in the range 700 to 1000 kPa. A method according to claim 1, as applied to microwave radiation detection, wherein the pressure differential PvL-Po is maintained at a substantially constant value in the range 800 to 1000 kPa. A radiation detector (1) of the type comprising superheated droplets of a detector liquid dispersed throughout an elastic, transparent or translucent matrix and which droplets are visibly vapourised upon impingement thereon of said radiation, characterised in the means (3 - 17) are provided to vary the overpressure Po on said matrix responsive to fluctuations in operating temperature and so as to maintain the pressure differential between the vapour pressure PvL of the superheated liquid droplets and said overpressure substantially constant. A detector according to claim 5, wherein said means comprises a self-regulating mechanical pressure control system operating on said matrix. A detector according to claim 6, wherein said mechanical pressure-control system comprises a pressure-multiplying piston (9,10) or bellows assembly (18,21) pressurised by a volatile liquid contained in a reservoir (15,15a), changes in vapour pressure of said volatile liquid consequent upon changes in ambient temperature being amplified by said pressure-multiplying piston (9,10) or bellows (18,21) assembly and transmitted thereby to said matrix. A detector according to claim 7, wherein said volatile liquid is octafluorocyclobutane, 1,2-dichlorotetrafluoroethane, dichlorofluoromethane, dichlorodifluoromethane, ethyl chloride or pentane. A detector according to claim 7 or 8, wherein the pressure is applied to said matrix from said pressure-multiplying piston (9,10) or bellows (18,21) assembly via an inert pressure-transmitting liquid in contact with the droplet-containing matrix of the radiation detector (1) and contained in a sealed chamber (2) enclosed by a pressure-transmitting diaphragm (3,3a), acted upon by said pressure multiplying piston (9,20) or bellows (18,21). A detector according to claim 7, 8 or 9, wherein the pressure-multiplying assembly comprises two different sized pistons (9,10) or two differently sized bellows (18,21) the ratio of the working areas of which, in conjunction with the volatile liquid, provide the necessary adjustments in the pressure Po consequent upon changes in operating temperature sensed by the volatile. liquid to maintain the differential PvL-Po substantially constant. A detector according to claim 10, wherein said ratio is in the range 2:1 to 8:1. A detector according to claim 11, wherein the pressure-multiplying assembly comprises two pistons (9,10) having an area ratio of about 3:1 and the volatile liquid which pressurises the larger piston is ethyl chloride. A detector according to claim 6, wherein the self-regulating mechanical pressure-control system comprises a spring-loaded elastic diaphragm assembly (3b-2b) responding to the thermal expansion of an inert filling liquid in direct contact with the droplet-containing matrix of the radiation detector (1) and acting upon a flexible diaphragm (3b) against the resilience of a compression spring (26).

Inventors: BONIFACE, HUGH, ING, HARRY, JEVCAK, JOHN, NOULTY, ROBERT
Applicants: ATOMIC ENERGY OF CANADA LIMITED L'ENERGIE ATOMIQUE DU CANADA LIMITEE
Application year: 1990
Main classification: G01T1
IPC codes: G01T5, G01T1