US2465821A - Thin-walled geiger-muller counter - Google Patents
Thin-walled geiger-muller counter Download PDFInfo
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- US2465821A US2465821A US673419A US67341946A US2465821A US 2465821 A US2465821 A US 2465821A US 673419 A US673419 A US 673419A US 67341946 A US67341946 A US 67341946A US 2465821 A US2465821 A US 2465821A
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- geiger
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- muller counter
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- 230000005855 radiation Effects 0.000 description 13
- 239000000463 material Substances 0.000 description 8
- 239000002245 particle Substances 0.000 description 6
- 239000011521 glass Substances 0.000 description 5
- 239000000941 radioactive substance Substances 0.000 description 5
- 238000010521 absorption reaction Methods 0.000 description 4
- NINIDFKCEFEMDL-UHFFFAOYSA-N Sulfur Chemical compound [S] NINIDFKCEFEMDL-UHFFFAOYSA-N 0.000 description 3
- 239000005864 Sulphur Substances 0.000 description 3
- 239000011248 coating agent Substances 0.000 description 3
- 238000000576 coating method Methods 0.000 description 3
- 229910052751 metal Inorganic materials 0.000 description 3
- 239000002184 metal Substances 0.000 description 3
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 2
- 239000004568 cement Substances 0.000 description 2
- 229910052802 copper Inorganic materials 0.000 description 2
- 239000010949 copper Substances 0.000 description 2
- 239000000126 substance Substances 0.000 description 2
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 2
- WSLDOOZREJYCGB-UHFFFAOYSA-N 1,2-Dichloroethane Chemical compound ClCCCl WSLDOOZREJYCGB-UHFFFAOYSA-N 0.000 description 1
- OYPRJOBELJOOCE-UHFFFAOYSA-N Calcium Chemical compound [Ca] OYPRJOBELJOOCE-UHFFFAOYSA-N 0.000 description 1
- 229910000531 Co alloy Inorganic materials 0.000 description 1
- KGWWEXORQXHJJQ-UHFFFAOYSA-N [Fe].[Co].[Ni] Chemical compound [Fe].[Co].[Ni] KGWWEXORQXHJJQ-UHFFFAOYSA-N 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052786 argon Inorganic materials 0.000 description 1
- 239000007767 bonding agent Substances 0.000 description 1
- 229910052791 calcium Inorganic materials 0.000 description 1
- 239000011575 calcium Substances 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 229910000830 fernico Inorganic materials 0.000 description 1
- 230000001788 irregular Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- QSHDDOUJBYECFT-UHFFFAOYSA-N mercury Chemical compound [Hg] QSHDDOUJBYECFT-UHFFFAOYSA-N 0.000 description 1
- 229910052753 mercury Inorganic materials 0.000 description 1
- 150000002739 metals Chemical class 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000002285 radioactive effect Effects 0.000 description 1
- 230000003014 reinforcing effect Effects 0.000 description 1
- 238000009877 rendering Methods 0.000 description 1
- 238000005096 rolling process Methods 0.000 description 1
- 229910000679 solder Inorganic materials 0.000 description 1
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J5/00—Details relating to vessels or to leading-in conductors common to two or more basic types of discharge tubes or lamps
- H01J5/02—Vessels; Containers; Shields associated therewith; Vacuum locks
- H01J5/18—Windows permeable to X-rays, gamma-rays, or particles
Definitions
- My invention relates to an improved apparatus for measuring radioactivity and more particularly to an improved Geiger-Muller counter for use through a greatly extended range of energies.
- the alpha, beta, and gamma particles emitted by radioactive substances possess energy respectively to an extent dependent upon the radioactive characteristics of the substance from which they are emitted. This energy is usually expressed in terms of electron volts. For example, beta particles emitted from one isotope of sulphur possess an energy of 107,000 electron volts while beta particles emitted from one isotope of argon possess an energy of 4,400,000 electron volts.
- the length of travel depends upon the initial energy and the nature of the medium traversed.
- the energy which a beta particle at the surface of a material must possess in order to penetrate a given thickness of the material may be determined by considering the molecular densities of the material and of aluminum and the known absorption values in the latter. If measurement of beta particles of low energy is to be made, the total absorption along the path from the radioactive substance to the measuring device must be low.
- the enclosing walls of a Geiger-Miiller counter must be structurally sufilcient to withstand the pressure differential between atmospheric pressure and the pressure within the partially evacuated interior. To render it operative, however, the enclosing wall must include a portion thin enough to allow the radiations from radioactive substances to penetrate it.
- Geiger- Miiller counters have been provided with such windows but the windows themselves have been too thick to allow the low energy level radiations to penetrate even though thehigh energy level radiations may, Many radioactive substances such as sulphur, calcium and others emit low energy radiations and in cases such as measuring the diffusion rate of sulphur along grain boundaries and surfaces of metals, it is important that these low energy radiations may be detected and counted. Heretofore, this has been made possible only by placing the material under study directly within the enclosure of the Geiger counter after which evacuation must take place before the instrument is again operative. Disadvantages of such a method are evident. Ac-
- Fig. 1 is a partially cutaway front view of a Geiger-Muller counter provided with a plurality of windows constructed in accordance with my invention
- Fig, 2 is an enlarged cross-sectional view along the line 2-2 of Fig. 1 showing in detail the structured the windows
- Fig. 3 is a front view of a Geiger-Muller counterprovided with another embodiment of my invention
- Fig. 4 is an enlarged cross-sectional viewalong the lip 4-4 of Fig. 3.
- the objects of my invention may be carried out by providing a plurality of windows in the enclosing wall of a Geiger-Miiller counter, each window being of such small area that suilicient support is offered to allow the use of extremely thin material for rendering the windows gastight.
- Figs. 1- and 3 show a Geiger-Muller counter I with a cylindrical cathode 2, preferably of an iron nickel cobalt alloy commonly known as fernico, forming a substantial part of the enclosure casing and to which glass end bells 3 are attached as by a gastight glass to metal joint 4.
- the anode 5 is a straight wire through the axis of the cathode cylinder and supported by the glass seals 6.
- An opening at I is provided whereby the enclosure may be evacuated to the proper amount and then sealed, or it may remain connected to a vacuum pump, not shown, by which the degree of evacuation can be controlled or evacuated from time to time in case of slow leaks, Leads 8 and 9 to a registering device, not shown, are attached to the cathode 2 and anode 5 respectively.
- a plurality of rectangular openings l0 are provided in the wall of the cylindrical cathode 2 over which are placed the window structures shown in enlarged detail in Fig. 2 and described by reference thereto.
- spacing, and arrangement of these openings may obviously be varied in any desired fashion as long as suiilcient supporting cathode structure remains between adjacent openings.
- a metal net or screen ll preferably of copper, covers the opening I0 and is soft soldered to the cathode structure around the edges of opening l0.
- Screen l I ma have a large enough area to cover all of the plurality of openings provided in the cathode 2. In any case, it is desirable to attach it to the cathode external surface along the edges of each opening which it covers.
- the soft solder bond as at I! should be smooth with no sharply irregular surfaces.
- the external side of net II is covered by extremely thin gastight sheets l3 of material prepared in a manner to be described.
- a multiplicity of windows covered only by the extremely thin sheets may also be obtained by utilizing the structure shown in Figs. 3 and 4.
- a Geiger-Miiller counter is shown with its principal parts numbered as in Fig. 1.
- a multiplicity of small holes IS in the cathode wall are separated only sufliciently to retain structural rigidity of the cathode wall.
- Extremely thin sheets I 3 are placed over the area covered by the holes and-rubber cement H or other suitable bonding agent used along the edges. This structure is more clearly shown in Fig. 4 in which the various portions retain the same numbers as in Fig. 3. If a, structure of this type is utilized, I have found that sheets as thin as .5 micron may be used with holes of 40 mils diameter.
- I employ the substance'polyvinylformal in extremely thin sheets in the construction of a thin-walled Geiger-Muller counter.
- Polyvinylformal is easily formed into thin sheets and its beta radiation energy absorption is low, being only about 2,000 electron volts per micron at 30,000 to 50,000 electron volts energy radiations or one micron is essentially equivalent in absorption .to .6 millimeter of air.
- These sheets were obtained in the following manner. Polyvinylformal was dissolved in ethylene dichloride to form a solution of approximately one per cent concentration. A clean glass plate was covered struments, vol. 14, No. 206
- the solution and allowed to dry.
- the thin coating was out along a line near one edge of the plate. It the plate is slowl immersed into water with its coated side up and if the edge' near which the coating was cut is the first to be immersed, the coating will be freed from the glass plate and will float as a sheet upon the surface of the water. This was done and the sheet transferred to the proper portion of the cathode structure by allowing contact 01' one edge of the sheet with the cathode structure to which it will adhere and then essentially rolling the counter tube over the floating sheet thereby picking it up in proper position over the cathode window structure. Each sheet is similarly obtained and transferred to its proper position up on the window area of the cathode.
- a tubular cathode In a Geiger-Muller counter, a tubular cathode, an anode wire extending along the axis of said cathode, members hermetically closing the ends of said cathode and supporting said anode wire, and at least one window in said cathode, said window being covered by a sheet of polyvinylformal having a 7 thickness not exceeding 1% microns.
- a cathode In a Geiger-Muller counter, a cathode, an anode, an envelope hermetically enclosing said electrodes, and a plurality of radiation permeable windows comprising a portion of said envelope, said windows comprising a reinforcing mesh covered by a sheet of polyvinylformal having a thicknem not exceeding 1 /2 microns.
- a tubular cathode having at least one small opening in a portion of the wall thereof.
- an anode wire extending along the axis of said cathode, members hermetically closing the ends of said cathode and supporting said anode wire, and a thin sheet of polyvinylformal totaling to 1 microns in thickness aflixed to the exterior surface of said cathode and covering said opening therein and in gastlght relation thereto.
Description
R. SMOLUCHOWSKI 2,465,821
IHIN-WALLED GEIGER-MULLER COUNTER M ch 29, 1949.
Filed lay 91, 1946 Inventor: I Roman smowchowskl,
b WWW His Attorney.
hunted Mar. 29, 1949 2,465,821 THIN-WALLED GEIGER-MULLER COUNTER Roman Smoluchowskl, Schenectady, N. Y., assignor to General Electric Company, a corporation of New York Application May 31, 1946, Serial No. 673,419 3 Claims. (Cl. 250-833) My invention relates to an improved apparatus for measuring radioactivity and more particularly to an improved Geiger-Muller counter for use through a greatly extended range of energies.
The alpha, beta, and gamma particles emitted by radioactive substances possess energy respectively to an extent dependent upon the radioactive characteristics of the substance from which they are emitted. This energy is usually expressed in terms of electron volts. For example, beta particles emitted from one isotope of sulphur possess an energy of 107,000 electron volts while beta particles emitted from one isotope of argon possess an energy of 4,400,000 electron volts.
Since this energy is absorbed by the medium through which the particles travel, the length of travel depends upon the initial energy and the nature of the medium traversed. The energy which a beta particle at the surface of a material must possess in order to penetrate a given thickness of the material may be determined by considering the molecular densities of the material and of aluminum and the known absorption values in the latter. If measurement of beta particles of low energy is to be made, the total absorption along the path from the radioactive substance to the measuring device must be low.
The enclosing walls of a Geiger-Miiller counter must be structurally sufilcient to withstand the pressure differential between atmospheric pressure and the pressure within the partially evacuated interior. To render it operative, however, the enclosing wall must include a portion thin enough to allow the radiations from radioactive substances to penetrate it. In the past, Geiger- Miiller counters have been provided with such windows but the windows themselves have been too thick to allow the low energy level radiations to penetrate even though thehigh energy level radiations may, Many radioactive substances such as sulphur, calcium and others emit low energy radiations and in cases such as measuring the diffusion rate of sulphur along grain boundaries and surfaces of metals, it is important that these low energy radiations may be detected and counted. Heretofore, this has been made possible only by placing the material under study directly within the enclosure of the Geiger counter after which evacuation must take place before the instrument is again operative. Disadvantages of such a method are evident. Ac-
cordingly, it is an object of my invention to pro-- vide an improved Geiger-Muller counter possessing windows through which low level radiations may penetrate.
It is a further object of my invention to provide an improved Geiger-Muller counter which responds to radiations of a wider range of energies than heretofore provided.
It is a still further object of my invention to provide a compact and easily movable instrument for detecting low energy radiations which may easily be placed very close to the subject being studied. This advantage is particularly valuable in the study of low energy radiations since they are dissipated within very short distances through air.
The features of the invention which are be-' lieved to be novel and patentable will be pointed out in the claims appended hereto.- For a better understanding of the invention, reference is made in the following description to the accompanying drawings in which Fig. 1 is a partially cutaway front view of a Geiger-Muller counter provided with a plurality of windows constructed in accordance with my invention, Fig, 2 is an enlarged cross-sectional view along the line 2-2 of Fig. 1 showing in detail the structured the windows, Fig. 3 is a front view of a Geiger-Muller counterprovided with another embodiment of my invention, and Fig. 4 is an enlarged cross-sectional viewalong the lip 4-4 of Fig. 3.
The objects of my invention may be carried out by providing a plurality of windows in the enclosing wall of a Geiger-Miiller counter, each window being of such small area that suilicient support is offered to allow the use of extremely thin material for rendering the windows gastight.
Referring now to the drawing, Figs. 1- and 3 show a Geiger-Muller counter I with a cylindrical cathode 2, preferably of an iron nickel cobalt alloy commonly known as fernico, forming a substantial part of the enclosure casing and to which glass end bells 3 are attached as by a gastight glass to metal joint 4. The anode 5 is a straight wire through the axis of the cathode cylinder and supported by the glass seals 6. An opening at I is provided whereby the enclosure may be evacuated to the proper amount and then sealed, or it may remain connected to a vacuum pump, not shown, by which the degree of evacuation can be controlled or evacuated from time to time in case of slow leaks, Leads 8 and 9 to a registering device, not shown, are attached to the cathode 2 and anode 5 respectively.
In Fig. 1 a plurality of rectangular openings l0 are provided in the wall of the cylindrical cathode 2 over which are placed the window structures shown in enlarged detail in Fig. 2 and described by reference thereto. The number,
spacing, and arrangement of these openings may obviously be varied in any desired fashion as long as suiilcient supporting cathode structure remains between adjacent openings.
The details of the window structure may be described by reference to Fig. 2 wherein a crosssectional portion of the cathode 2 is taken through the opening l along the line 2-2 of Fig. 1. A metal net or screen ll, preferably of copper, covers the opening I0 and is soft soldered to the cathode structure around the edges of opening l0. Screen l I ma have a large enough area to cover all of the plurality of openings provided in the cathode 2. In any case, it is desirable to attach it to the cathode external surface along the edges of each opening which it covers. The soft solder bond as at I! should be smooth with no sharply irregular surfaces. The external side of net II is covered by extremely thin gastight sheets l3 of material prepared in a manner to be described. The edges of these sheets extend beyond the net I land are attached to the cathode surface by rubber cement H or other suitable bonding material. Thus an essentially gastight enclosure for the Geiger-Muller counter results which possesses a multiplicity of small areas wherein the exterior and interior are separated by an extremely thin sheet of material easily traversed by low energy radiations from radioactive substances. The number of sheets or their total thickness will be determined by the size of openings in net II and by the degree of evacuation to be used. I have employed a 500 mesh copper net and sheets totaling 1 to 1 microns in thickness with satisfactory results while using an internal pressure of 4 to 5cm. of mercury.
A multiplicity of windows covered only by the extremely thin sheets may also be obtained by utilizing the structure shown in Figs. 3 and 4. Refen'ing to Fig. 3, a Geiger-Miiller counter is shown with its principal parts numbered as in Fig. 1. A multiplicity of small holes IS in the cathode wall are separated only sufliciently to retain structural rigidity of the cathode wall. Extremely thin sheets I 3 are placed over the area covered by the holes and-rubber cement H or other suitable bonding agent used along the edges. This structure is more clearly shown in Fig. 4 in which the various portions retain the same numbers as in Fig. 3. If a, structure of this type is utilized, I have found that sheets as thin as .5 micron may be used with holes of 40 mils diameter.
Preferably, I employ the substance'polyvinylformal in extremely thin sheets in the construction of a thin-walled Geiger-Muller counter. Polyvinylformal is easily formed into thin sheets and its beta radiation energy absorption is low, being only about 2,000 electron volts per micron at 30,000 to 50,000 electron volts energy radiations or one micron is essentially equivalent in absorption .to .6 millimeter of air. These sheets were obtained in the following manner. Polyvinylformal was dissolved in ethylene dichloride to form a solution of approximately one per cent concentration. A clean glass plate was covered struments, vol. 14, No. 206
by the solution and allowed to dry. When dry, the thin coating was out along a line near one edge of the plate. It the plate is slowl immersed into water with its coated side up and if the edge' near which the coating was cut is the first to be immersed, the coating will be freed from the glass plate and will float as a sheet upon the surface of the water. This was done and the sheet transferred to the proper portion of the cathode structure by allowing contact 01' one edge of the sheet with the cathode structure to which it will adhere and then essentially rolling the counter tube over the floating sheet thereby picking it up in proper position over the cathode window structure. Each sheet is similarly obtained and transferred to its proper position up on the window area of the cathode.
As will occur to those skilled in the art, various different arrangements and combinations of the principles described above may be employed without departing from thetrue spirit and scope of the invention and I therefore do not wish to limit my invention to the particular arrangement described.
What I claim as new and desire to secure by Letters Patent of the United States is:
1. In a Geiger-Muller counter, a tubular cathode, an anode wire extending along the axis of said cathode, members hermetically closing the ends of said cathode and supporting said anode wire, and at least one window in said cathode, said window being covered by a sheet of polyvinylformal having a 7 thickness not exceeding 1% microns.
2. In a Geiger-Muller counter, a cathode, an anode, an envelope hermetically enclosing said electrodes, and a plurality of radiation permeable windows comprising a portion of said envelope, said windows comprising a reinforcing mesh covered by a sheet of polyvinylformal having a thicknem not exceeding 1 /2 microns.
3. In a Geiger-Miiller counter, a tubular cathode having at least one small opening in a portion of the wall thereof. an anode wire extending along the axis of said cathode, members hermetically closing the ends of said cathode and supporting said anode wire, and a thin sheet of polyvinylformal totaling to 1 microns in thickness aflixed to the exterior surface of said cathode and covering said opening therein and in gastlght relation thereto.
' ROMAN SMOLUCHOWSKI.
REFERENCES CITED The following references are of record in the I file of this patent:
UNITED STATES PATENTS Number OTHER REFERENCES 'Co'pp and Greenberg, Review of Scientific In- 7, July 1943, pages 205 and
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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US673419A US2465821A (en) | 1946-05-31 | 1946-05-31 | Thin-walled geiger-muller counter |
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US673419A US2465821A (en) | 1946-05-31 | 1946-05-31 | Thin-walled geiger-muller counter |
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US2465821A true US2465821A (en) | 1949-03-29 |
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US673419A Expired - Lifetime US2465821A (en) | 1946-05-31 | 1946-05-31 | Thin-walled geiger-muller counter |
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Cited By (14)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2538632A (en) * | 1948-01-21 | 1951-01-16 | Edward R Tompkins | Combination beta and gamma chamber |
US2631334A (en) * | 1947-12-27 | 1953-03-17 | Rauland Corp | Process of making thin free films |
US2654041A (en) * | 1950-06-01 | 1953-09-29 | Westinghouse Electric Corp | Radiation counter |
US2656476A (en) * | 1950-02-01 | 1953-10-20 | Ralph H Firminhac | Survey instrument |
US2666865A (en) * | 1947-05-16 | 1954-01-19 | Casimer J Borkowski | Survey instrument |
US2675483A (en) * | 1952-03-25 | 1954-04-13 | Isotope Products Ltd | Method and apparatus for measuring the mass per unit area of sheet material |
US2695364A (en) * | 1951-04-26 | 1954-11-23 | Ralph A Wolfe | Pyrometer |
US2959679A (en) * | 1956-05-15 | 1960-11-08 | Molins Machine Co Ltd | Radiation gauges having ionization chambers |
US2978602A (en) * | 1956-05-14 | 1961-04-04 | Jeno M Barnothy | Radiation measuring device |
US3004165A (en) * | 1958-04-25 | 1961-10-10 | Tung Sol Electric Inc | Ionization chamber |
US3132249A (en) * | 1961-02-16 | 1964-05-05 | Ralph C Maggio | Detection, segregation and counting of radiations of different energies |
US3207938A (en) * | 1953-07-24 | 1965-09-21 | Anton Nicholas | Superatmospheric pressure ionization chamber for detection of radiant energy |
US3262002A (en) * | 1961-07-17 | 1966-07-19 | Robert W Kreplin | Convertible x-ray detector |
US3614445A (en) * | 1969-09-15 | 1971-10-19 | Tno | Measuring width variations of a moving sheet by the use of beta-rays |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2222450A (en) * | 1937-11-20 | 1940-11-19 | Forderung Zerstorungsfreier Pr | Method for measuring short-wave radiations |
US2368486A (en) * | 1942-02-02 | 1945-01-30 | Standard Oil Dev Co | Well logging |
US2429217A (en) * | 1942-05-07 | 1947-10-21 | Electronized Chem Corp | Device for treatment of matters with high-speed electrons |
-
1946
- 1946-05-31 US US673419A patent/US2465821A/en not_active Expired - Lifetime
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2222450A (en) * | 1937-11-20 | 1940-11-19 | Forderung Zerstorungsfreier Pr | Method for measuring short-wave radiations |
US2368486A (en) * | 1942-02-02 | 1945-01-30 | Standard Oil Dev Co | Well logging |
US2429217A (en) * | 1942-05-07 | 1947-10-21 | Electronized Chem Corp | Device for treatment of matters with high-speed electrons |
Cited By (14)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2666865A (en) * | 1947-05-16 | 1954-01-19 | Casimer J Borkowski | Survey instrument |
US2631334A (en) * | 1947-12-27 | 1953-03-17 | Rauland Corp | Process of making thin free films |
US2538632A (en) * | 1948-01-21 | 1951-01-16 | Edward R Tompkins | Combination beta and gamma chamber |
US2656476A (en) * | 1950-02-01 | 1953-10-20 | Ralph H Firminhac | Survey instrument |
US2654041A (en) * | 1950-06-01 | 1953-09-29 | Westinghouse Electric Corp | Radiation counter |
US2695364A (en) * | 1951-04-26 | 1954-11-23 | Ralph A Wolfe | Pyrometer |
US2675483A (en) * | 1952-03-25 | 1954-04-13 | Isotope Products Ltd | Method and apparatus for measuring the mass per unit area of sheet material |
US3207938A (en) * | 1953-07-24 | 1965-09-21 | Anton Nicholas | Superatmospheric pressure ionization chamber for detection of radiant energy |
US2978602A (en) * | 1956-05-14 | 1961-04-04 | Jeno M Barnothy | Radiation measuring device |
US2959679A (en) * | 1956-05-15 | 1960-11-08 | Molins Machine Co Ltd | Radiation gauges having ionization chambers |
US3004165A (en) * | 1958-04-25 | 1961-10-10 | Tung Sol Electric Inc | Ionization chamber |
US3132249A (en) * | 1961-02-16 | 1964-05-05 | Ralph C Maggio | Detection, segregation and counting of radiations of different energies |
US3262002A (en) * | 1961-07-17 | 1966-07-19 | Robert W Kreplin | Convertible x-ray detector |
US3614445A (en) * | 1969-09-15 | 1971-10-19 | Tno | Measuring width variations of a moving sheet by the use of beta-rays |
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