US2908839A - Radiation detector cathode - Google Patents
Radiation detector cathode Download PDFInfo
- Publication number
- US2908839A US2908839A US361612A US36161253A US2908839A US 2908839 A US2908839 A US 2908839A US 361612 A US361612 A US 361612A US 36161253 A US36161253 A US 36161253A US 2908839 A US2908839 A US 2908839A
- Authority
- US
- United States
- Prior art keywords
- holes
- cathode
- plates
- mesh
- detector
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
Images
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
- H01J47/00—Tubes for determining the presence, intensity, density or energy of radiation or particles
- H01J47/08—Geiger-Müller counter tubes
Definitions
- This invention relates to the detection of penetrative radiation and, more particularly, to the cathode of a gamma ray detector of the electrical pulse-producing, gas amplification type and a method of making the same.
- the principal object of the invention is the provision of a cathode for such a detector which is more eflicient than those used heretofore.
- a radiation detector of the electrical pulse-producing or counter type is disclosed, which detector has proven to be many times more eflicient in the detection of gamma rays than other counter-type or ionization chamber detectors of the same volume.
- the detector described in the Hare patent comprises essentially a cathode and an anode disposed within a chamber containing an ionizable gas filling, the cathode being formed of a plurality of spaced, parallel metallic discs or plates arranged in a bank and the bank of platesjbeing provided with one or more series of aligned holes.
- An anode wire is disposed along the axis of the holes in each series.
- the plates or discs are connected together electrically to form the cathode, and the anode wires are connected together electrically to form the anode of the detector.
- the cathode plates or discs described in the patent are formed of a suitable metal such as brass, and each plate is a few mils in thickness.
- a gamma ray, in penetrating one of the cathode plates, may cause an electron to be ejected from an atom of the cathode material, and this electron may then produce ionization of the gas filling to provide an electrical pulse, as is well understood by those familiar with this art.
- the efiiciency of a gamma ray detector of this type will depend upon the amount of effective cathode area exposed to the ionizable gas, and it has been found that the efiiciency of a detector can be increased by forming the cathode plates of wire mesh rather than of a solid material, since the total surface area of a wire mesh plate is greater than the area of the two sides of a flat, solid plate of the same diameter.
- wire mesh cathode plates formed of 35 brass wires to the inch, each wire being .006 inch in diameter, when used in a gamma ray detector of the type disclosed in the above-mentioned Hare patent, provide a detector efiiciency at least percent greater than where the same number of solid brass plates are used in a counter of the same volume.
- each of the cathode plates is pro vided with one or more round holes, and the plates are assembled in such a way that the corresponding holes in the plates are in alignment with an anode wire stretched along the axis of each series of holes. Since a high potential is impressed across the cathode and the anode of the detector, the potential being almost, but not quite high enough to cause sparking between the two electrodes, it is obviously essential that the holes in the cathode plates be accurately aligned and that they be perfectly round with smooth edges or peripheries so that every portion of the periphery of a cathode hole will be equidistant from the axially disposed anode wire.
- a mesh plate is tinned with solder at the place or places where the holes are to be formed, the tinned area being slightly larger than the diameter of the hole.
- the holes are then formed in any suitable manner, as by stamping through the tinned area, and since the solder holds in rigid position the ends of the mesh wires projecting toward the hole the edge or periphery of the hole will be smooth and every portion thereof equidistant from the center of the hole.
- the holes can be formed in the mesh plate, as by stamping and the edges of the holes then tinned. If desired, the
- edges of the holes can subsequently be reamed to insure roundness.
- Fig. 1 is an elevation partly in section of a radiation detector of the form shown generally in the aforementioned Hare patent;
- Fig. 2 is a sectional view on the line 22 of Fig. 1.
- a cylindrical shell or case 10 of brass or the like is shown as closed near its ends by means of closeure plates 12 and 13.
- a third plate 14 is shown as screwed into the right-hand end of the case 16.
- Disposed within the case 10 and arranged in parallel separate relationv is a plurality of wire mesh discs or plates 16 separated by spacer rings 17 and each of the plates being shown in this instance as provided with four holes 18.
- the periphery of each of the discs 16 is provided with a small indentation 20, and this indentation and the holes 18 are positioned in the discs so that when they are assembled, the holes in each disc will line up with the holes in the other discs to provide four separate series of holes.
- the case 10 is provided on its inner surface with a rib 22 extending longitudinally of the case, and this rib cooperates with the disc indentations 20 to align the discs, as has been described.
- An anode wire 24 of substantially 3 mils in thickness is stretched between insulators 26 in the plates 12 and 13, and these wires are connected together electrically to a lead 28 and form the anode of the detector.
- the plates 16 are connected together electrically through the rings 17 and case 10, and the bank of plates 16 forms the cathode, a connecting lead from which is shown at 29.
- the cathode material wire mesh of diiferent sizes it has been found that mesh formed of 35 brass wires to the inch, each wire being .006 inch in diameter, is satisfactory.
- the holes can be cut in the mesh plates prior to the tinning operation, and in this case that portion of the mesh immediately surrounding each hole will be tinned in any suitable manner. After the tinning metal has hardened, the holes may be reamed to size, and the finished plate will then be substantially the same as a plate in which the mesh has been tinned prior to the cutting of the holes.
- each plate of any one detector may have one or several holes.
- the cathode plates are frequently provided with seven holes, whereas in many of the smaller counters each plate has but one hole at its center.
- solder has been referred to herein, it is to be understood that other metals can be used, which are not of themselves radioactive and which can be melted to form a good bond with the wire mesh.
- the term tinning is intended to cover the use of any such metal.
- a device as described in claim 1 in which the mesh sheet is discshaped and the periphery of the disc is provided with a similar coating of soft metal to stiifen the disc and to maintain in place the outer ends of the mesh wires.
- a radiation detecting device comprising a pluraliity of cathode plates disposed in separated relation and connected together electrically to form a cathode member, each plate being provided with at least one hole and the holes in the plates being disposed in alignment, and an anode member comprising a wire extending through said aligned holes and insulated from said cathode plates
- at least one of said cathode plates comprises a flat sheet of wire mesh provided with at least one round hole through the axis of which said anode wire is disposed and wherein that portion of the wire mesh immediately surrounding the hole is provided with a solid ring-shaped coating of a soft metal, whereby the soft metal serves to hold rigidily in place the ends of the mesh wires projecting toward the hole.
Landscapes
- Measurement Of Radiation (AREA)
Description
Ot. 1-3, 1959 G. HERZOG RADIATION DETECTOR CATHODE Fil ed June 15'. 1953 United States Patent Ofiice 2,968,839 Patented Oct. 13, 1959 RADIATION DETECTOR CATHODE Gerhard Herzog, Houston, Tex., assignor to Texaco Inc., a corporation of Delaware Application June 15, 1953, Serial No. 361,612
3 Claims. (Cl. 313-93) This invention relates to the detection of penetrative radiation and, more particularly, to the cathode of a gamma ray detector of the electrical pulse-producing, gas amplification type and a method of making the same. The principal object of the invention is the provision of a cathode for such a detector which is more eflicient than those used heretofore.
In US. Letters Patent No. 2,397,071, granted March 19, 1946, to D. G. C. Hare, a radiation detector of the electrical pulse-producing or counter type is disclosed, which detector has proven to be many times more eflicient in the detection of gamma rays than other counter-type or ionization chamber detectors of the same volume. The detector described in the Hare patent comprises essentially a cathode and an anode disposed within a chamber containing an ionizable gas filling, the cathode being formed of a plurality of spaced, parallel metallic discs or plates arranged in a bank and the bank of platesjbeing provided with one or more series of aligned holes. An anode wire is disposed along the axis of the holes in each series. The plates or discs are connected together electrically to form the cathode, and the anode wires are connected together electrically to form the anode of the detector. The cathode plates or discs described in the patent are formed of a suitable metal such as brass, and each plate is a few mils in thickness. A gamma ray, in penetrating one of the cathode plates, may cause an electron to be ejected from an atom of the cathode material, and this electron may then produce ionization of the gas filling to provide an electrical pulse, as is well understood by those familiar with this art. The probability of an electron being ejected from an atom of the cathode material when the atom is struck by a gamma ray increases, of course, with increasing thickness of the cathode wall, since there are then more atoms in the path of each gamma ray. However, due to the short range of the ejected electrons in the cathode material, a cathode plate should be but a few mils in thickness.
The efiiciency of a gamma ray detector of this type will depend upon the amount of effective cathode area exposed to the ionizable gas, and it has been found that the efiiciency of a detector can be increased by forming the cathode plates of wire mesh rather than of a solid material, since the total surface area of a wire mesh plate is greater than the area of the two sides of a flat, solid plate of the same diameter. Experiments have shown that wire mesh cathode plates formed of 35 brass wires to the inch, each wire being .006 inch in diameter, when used in a gamma ray detector of the type disclosed in the above-mentioned Hare patent, provide a detector efiiciency at least percent greater than where the same number of solid brass plates are used in a counter of the same volume.
As described above, each of the cathode plates is pro vided with one or more round holes, and the plates are assembled in such a way that the corresponding holes in the plates are in alignment with an anode wire stretched along the axis of each series of holes. Since a high potential is impressed across the cathode and the anode of the detector, the potential being almost, but not quite high enough to cause sparking between the two electrodes, it is obviously essential that the holes in the cathode plates be accurately aligned and that they be perfectly round with smooth edges or peripheries so that every portion of the periphery of a cathode hole will be equidistant from the axially disposed anode wire.
In accordance with the invention in one embodiment thereof, a mesh plate is tinned with solder at the place or places where the holes are to be formed, the tinned area being slightly larger than the diameter of the hole. The holes are then formed in any suitable manner, as by stamping through the tinned area, and since the solder holds in rigid position the ends of the mesh wires projecting toward the hole the edge or periphery of the hole will be smooth and every portion thereof equidistant from the center of the hole. In a slightly different method the holes can be formed in the mesh plate, as by stamping and the edges of the holes then tinned. If desired, the
edges of the holes can subsequently be reamed to insure roundness.
For a better understanding of the invention, reference may [be had to the accompanying drawing in which-f Fig. 1 is an elevation partly in section of a radiation detector of the form shown generally in the aforementioned Hare patent; and
Fig. 2 is a sectional view on the line 22 of Fig. 1.
Referring to the drawing, a cylindrical shell or case 10 of brass or the like is shown as closed near its ends by means of closeure plates 12 and 13. A third plate 14 is shown as screwed into the right-hand end of the case 16. Disposed within the case 10 and arranged in parallel separate relationv is a plurality of wire mesh discs or plates 16 separated by spacer rings 17 and each of the plates being shown in this instance as provided with four holes 18. The periphery of each of the discs 16 is provided with a small indentation 20, and this indentation and the holes 18 are positioned in the discs so that when they are assembled, the holes in each disc will line up with the holes in the other discs to provide four separate series of holes. To this end the case 10 is provided on its inner surface with a rib 22 extending longitudinally of the case, and this rib cooperates with the disc indentations 20 to align the discs, as has been described. An anode wire 24 of substantially 3 mils in thickness is stretched between insulators 26 in the plates 12 and 13, and these wires are connected together electrically to a lead 28 and form the anode of the detector. The plates 16 are connected together electrically through the rings 17 and case 10, and the bank of plates 16 forms the cathode, a connecting lead from which is shown at 29. Although it is possible to use as the cathode material wire mesh of diiferent sizes, it has been found that mesh formed of 35 brass wires to the inch, each wire being .006 inch in diameter, is satisfactory.
It is well known that where holes are formed in wire mesh, either by punching, drilling or any other form of metal cutting, the ends of the cut wires tend to fray and a counter made in this manner with no further attention given to the edges of the holes would in all probability not function properly. If even one of the wires cut in forming the holes projected as little as a few thousandths of an inch farther toward the anode wire 24 than the other wires, the electrical field would be concentrated at this point and sparking between the projecting wires and the anode would occur.
The above-mentioned difficulty has been overcome by placing a small amount of solder 30 on each mesh disc and tinning an area slightly larger in diameter than the diameter of the hole to be cut. When the four areas have been tinned in a disc such as is illustrated in the drawing, the disc may be placed in a punch press and the four holes punched out. The solder will hold the projecting ends of the wires in fixed position, and the edge of each hole will he as smooth as though the holes had been cut in a solid sheet of metal.
If desired, the holes can be cut in the mesh plates prior to the tinning operation, and in this case that portion of the mesh immediately surrounding each hole will be tinned in any suitable manner. After the tinning metal has hardened, the holes may be reamed to size, and the finished plate will then be substantially the same as a plate in which the mesh has been tinned prior to the cutting of the holes.
While the drawing illustrates a cathode plate having four holes, it is to be understood that this is by way of illustration only and that each plate of any one detector may have one or several holes. In the large gamma ray counters used in the logging of well bores, the cathode plates are frequently provided with seven holes, whereas in many of the smaller counters each plate has but one hole at its center.
Although the invention has been described particularly with reference to the tinning of the holes in mesh plates used in gamma ray detectors, it is to be understood that the invention is also applicable to other uses and, in fact, wherever it is desired to provide a round hole having a smooth periphery in any sheet of wire mesh.
Although solder has been referred to herein, it is to be understood that other metals can be used, which are not of themselves radioactive and which can be melted to form a good bond with the wire mesh. The term tinning is intended to cover the use of any such metal.
Obviously, many modifications and variations of the invention as hereinbefore set forth may be made without departing from the spirit and scope thereof, but only such limitations should be imposed as are indicated in the appended claims.
2. A device as described in claim 1 in which the mesh sheet is discshaped and the periphery of the disc is provided with a similar coating of soft metal to stiifen the disc and to maintain in place the outer ends of the mesh wires.
3. In a radiation detecting device comprising a pluraliity of cathode plates disposed in separated relation and connected together electrically to form a cathode member, each plate being provided with at least one hole and the holes in the plates being disposed in alignment, and an anode member comprising a wire extending through said aligned holes and insulated from said cathode plates, the improvement wherein at least one of said cathode plates comprises a flat sheet of wire mesh provided with at least one round hole through the axis of which said anode wire is disposed and wherein that portion of the wire mesh immediately surrounding the hole is provided with a solid ring-shaped coating of a soft metal, whereby the soft metal serves to hold rigidily in place the ends of the mesh wires projecting toward the hole.
References Cited in the file of this patent UNITED STATES PATENTS 2,113,674 Briclcman et a1 Apr. 12, 1938 2,457,781 Metten et a1. Dec. 28, 1948 2,485,516 Thompson Oct. 18, 1949 2,543,637 McArthur Feb. 27, 1951 2,617,959 Fay Nov. 11, 1952 2,631,246 Christian Mar. 10, 1953 2,690,802 Russell Oct. 5, 1954
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US361612A US2908839A (en) | 1953-06-15 | 1953-06-15 | Radiation detector cathode |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US361612A US2908839A (en) | 1953-06-15 | 1953-06-15 | Radiation detector cathode |
Publications (1)
Publication Number | Publication Date |
---|---|
US2908839A true US2908839A (en) | 1959-10-13 |
Family
ID=23422738
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US361612A Expired - Lifetime US2908839A (en) | 1953-06-15 | 1953-06-15 | Radiation detector cathode |
Country Status (1)
Country | Link |
---|---|
US (1) | US2908839A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3047761A (en) * | 1959-03-24 | 1962-07-31 | Mc Graw Edison Co | Radiation detector tubes |
Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2113674A (en) * | 1935-01-29 | 1938-04-12 | American Steel & Wire Co | Manufacture of stranded elements |
US2457781A (en) * | 1948-01-02 | 1948-12-28 | Sylvania Electric Prod | Ray counter |
US2485516A (en) * | 1945-07-10 | 1949-10-18 | Atomic Energy Commission | Shallow plane proportional counter |
US2543637A (en) * | 1946-06-04 | 1951-02-27 | Gen Electric | Interelectrode coupling in high-frequency electric discharge devices |
US2617959A (en) * | 1950-09-30 | 1952-11-11 | Bell Telephone Labor Inc | Electron discharge device |
US2631246A (en) * | 1950-02-28 | 1953-03-10 | Rca Corp | Radiation detection |
US2690802A (en) * | 1952-08-07 | 1954-10-05 | Luber Finer Inc | Method of and apparatus for stamping and stacking filter elements |
-
1953
- 1953-06-15 US US361612A patent/US2908839A/en not_active Expired - Lifetime
Patent Citations (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US2113674A (en) * | 1935-01-29 | 1938-04-12 | American Steel & Wire Co | Manufacture of stranded elements |
US2485516A (en) * | 1945-07-10 | 1949-10-18 | Atomic Energy Commission | Shallow plane proportional counter |
US2543637A (en) * | 1946-06-04 | 1951-02-27 | Gen Electric | Interelectrode coupling in high-frequency electric discharge devices |
US2457781A (en) * | 1948-01-02 | 1948-12-28 | Sylvania Electric Prod | Ray counter |
US2631246A (en) * | 1950-02-28 | 1953-03-10 | Rca Corp | Radiation detection |
US2617959A (en) * | 1950-09-30 | 1952-11-11 | Bell Telephone Labor Inc | Electron discharge device |
US2690802A (en) * | 1952-08-07 | 1954-10-05 | Luber Finer Inc | Method of and apparatus for stamping and stacking filter elements |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3047761A (en) * | 1959-03-24 | 1962-07-31 | Mc Graw Edison Co | Radiation detector tubes |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US2397071A (en) | Radiation detector | |
US2211668A (en) | Electronic device | |
US2618760A (en) | Glow tube anode construction | |
US2513743A (en) | Electron storage device with grid control action | |
US2908839A (en) | Radiation detector cathode | |
US2493935A (en) | High-energy neutron counter | |
US2631246A (en) | Radiation detection | |
US2845560A (en) | Neutron counter | |
US2398934A (en) | Radiation detector | |
US1929067A (en) | Frequency multiplier | |
US2397073A (en) | Radiation detector | |
DE2239802A1 (en) | GAS DISCHARGE ARRANGEMENT | |
US2724779A (en) | Counters for discriminating between gamma rays of different energies | |
US3328618A (en) | High-voltage acceleration tube with inserts for the electrodes | |
US3359443A (en) | Sensitive radiation detector having alternate cathode and anode members in chamber containg ionizing gas | |
US2873399A (en) | Radiation detector | |
US4361763A (en) | Smoke detectors | |
GB976781A (en) | Ultra high vacuum ion gauge | |
US3387175A (en) | Vacuum gauge having separate electron collecting and electron accelerating electrodes | |
US3112401A (en) | Shielding to confine magnetic field to ion source area of a neutron generator | |
US2512247A (en) | Antimagnetically shielded photocell | |
US3272984A (en) | Electron multiplier for measuring the flow of positively charged particles | |
US2745970A (en) | Radioactivity detector | |
US2489133A (en) | Radiation detecting device | |
US2485516A (en) | Shallow plane proportional counter |