US3188471A - Coin identification apparatus utilizing radiation bombardment - Google Patents

Coin identification apparatus utilizing radiation bombardment Download PDF

Info

Publication number
US3188471A
US3188471A US84236A US8423661A US3188471A US 3188471 A US3188471 A US 3188471A US 84236 A US84236 A US 84236A US 8423661 A US8423661 A US 8423661A US 3188471 A US3188471 A US 3188471A
Authority
US
United States
Prior art keywords
coin
beta
coins
path
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
Application number
US84236A
Inventor
Hansen Carl Woodrow
Peter J Clack
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Laboratory For Electronics Inc
Original Assignee
Laboratory For Electronics Inc
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Laboratory For Electronics Inc filed Critical Laboratory For Electronics Inc
Priority to US84236A priority Critical patent/US3188471A/en
Application granted granted Critical
Publication of US3188471A publication Critical patent/US3188471A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N23/00Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00
    • G01N23/20Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by using diffraction of the radiation by the materials, e.g. for investigating crystal structure; by using scattering of the radiation by the materials, e.g. for investigating non-crystalline materials; by using reflection of the radiation by the materials
    • G01N23/20083Investigating or analysing materials by the use of wave or particle radiation, e.g. X-rays or neutrons, not covered by groups G01N3/00 – G01N17/00, G01N21/00 or G01N22/00 by using diffraction of the radiation by the materials, e.g. for investigating crystal structure; by using scattering of the radiation by the materials, e.g. for investigating non-crystalline materials; by using reflection of the radiation by the materials by using a combination of at least two measurements at least one being a transmission measurement and one a scatter measurement

Definitions

  • This invention relates in general to a coin identication system and, more particularly, to an apparatus for identitying coins by a determination of their atomic number and their weight per unit area.
  • the apparatus of the present inven-V tion identities coins by determining the atomic number and weight per unit area of each coin entered into the machine. The measurement of these quantities is accomplished by means of measuring both the transmission and reflection of nuclear radiation bythe coin.
  • the backscattering coeiiicient of beta radiation from a material is directly dependent upon the atomic number of that material, and hence the amount of beta radiation scattered back to a beta detector in a iixed geometrical arrangement provides a clear indication of the atomic number of the backscattering material.
  • X- rays and gamma rays are transmitted through materials with the percent absorption of these rays depending upon the weight per unit area of the material.
  • the weight per unit area can be determined by measurement of the amount of such radiation transmitted.
  • FIG. l is an illustration in block diagrammatic form of a one embodiment of a Vcoin identiiication apparatus in accordance with the principles for this invention.; ⁇
  • FIG. ⁇ 2 is a graphical illustration of the dependence of beta Vbackscatter signal on atomic number of materials
  • FIG. 3 is a graphical illustration of the dependence of transmitted radiation on the weight per unit area of the absorber.
  • FlG. 4 is an illustration in block diagrammatic form of a coin identication apparatus employing multiple sensor elements.
  • a-radioactive source lei is located to one side of the path ofV opposite side of the path ofV travel lll from the sourceV 14 and has anopening 13 in it allowing radiation from the source lA- which passes through the coin l1 to pass dollar and dollar.
  • detector 2@ is provided to terminal 25 labeled backscatter output, while the output of detector 21 is provided to terminal 26 labeled transmission output.
  • This configuration of elements provides on the output 25 of detector 2@ signals resulting from radiation backscattered from either a coin 11 or the backscatter plate 12.
  • the signals represent the radiation transmitted through the opening 13 in plate 12 and when a coin 11 intercepts this radiation beam, the signals represent the radiation transmitted through the coin and through the opening.
  • the radioactive source 14 would typically consist of a beta emitting radioisotope admired with a high Z material so that the source would emit both the beta radiation and bremsstrahlung radiation.
  • the portion of beta radiation backscattered from a coin travelling along path 1d is a function of the atomic number of the elements ywithin the coin, whereas the amount of bremsstrahlung radiation transmitted through the coin is a function of the weight per unit area of the coin.
  • Backscatter detector 20 is a beta sensitive detector, typically a geiger Vmueller tube or a cadmium sulphide crystal
  • X- ray Vdetector 21 is a detector relatively insensitive to beta radiation and typically would be a scintillation crystal and photomultiplier combination.
  • the ⁇ backscatter output signal is related to the atomic number of the coin from which the beta radiation is scattered, while the transmission output is related to the weight per unit area.
  • the device may be operated as a no-go instrumer1t in which a signal should appear on terminal 25 only when the coin 11 is characterized by an atomic number different from that of the material in the acceptable coin. For example, if the machine is setto accept dimes, which are 98% silver having an,
  • the function of the backscatter plate 12 is to provide a standardizing bias signal equivalent to the signal developed by the acceptable coin so that theV test of acceptability becomes one relative to the signal derived from the backscatter plate when no coin is present. Since the backscatter signal depends upon both atomic number and spacing and since the backscatter plate 12 is spaced further from the source than the path of the coin 10, then the backscatter plate must be made of higher atomic number material than the acceptable coin material. Both lead plate and tungsten alloy have been found to be acceptable materials with convenient spacings.
  • the backscatter plate 12 may be eliminated and a second radioactive source employed to create the bias signal.
  • This second source is arranged such that the presence of the coin absorbs the radiation from it, hence the signal from the beta detector in this case also represents only the radiation from source 14 scattered from the com.
  • the output terminal 25 signal distinguishes between the copper and silver group, whereas the signal on terminal 26 provides a clear indication of which coin within either group it is.
  • slugs which are not coins at all
  • fabricated slugs would probably be equal to or greater than the value of the coin and hence a coin pass meter or the like need not be capable of distinguishing them.
  • the device illustrated in FlG. 1 employed a backscatter plate 12 in order to provide a standardizing signal and to eliminate problems of drift and the like in the detector and circuitry. It should be clear, however, that the backscatter plate standardization is not essential to the coin detection, inasmuch as a circuit can be employed at the output of terminal 25 to distinguishbetween several positive signals of different magnitude.
  • FIG. 4 a coin identification apparatus, capable of accepting-two different preselected types of coins while rejecting all others, is shown.
  • like numbers refer to like parts of FIG. l
  • the coin again travels along a path as indicated by the dotted line 10 between a backscatter plate 12 and source and detector combinationl and 20.
  • the coin travels along an extension of this path beside a second backscatterplate 32.
  • This second backscatter plate 32 is formed of a similar material to backscatter plate 12, however, it has no opening through it.
  • a beta ray source 30 and beta i ray detector 31 separated by a shielding element 29.
  • the output of the beta detector 31 is provided to a terminal 3S.
  • the backscatter plate 12 is spaced appropriately from the source 14 and detector 2t) combination, so that in the absence of a coin, a signal is presented on terminal 25 equivalent to the signal which would be received from a silver coin.
  • any change of signal in terminal 25 represents a non-silver coin passing along path 1t?.
  • the output terminal 25 is connected to a gating circuit 33, as isoutput terminal 26 from detector 21.
  • the output terminal 35 of beta detector 31 is also coupled to gating circuit 33.
  • the radioactive source 30 associated with detector 31k is a pure beta ray source, since there is no opening through plate 32 and no transmission detector associated with these components.
  • the backscatter plate 32 may be formed conveniently of the same material as backscatter plate 12, however its spacing from the path of coin travel 1d is arranged such that the output signal from Vdetector 31 when there is no coin between the plate 32 and source 30 is equivalent to that received when a coin formed of copper is within this area. Hence the outputV on terminal 35 will remain kthe same exceptA when there is a noncopper coin travelling between the source 3() and plate 32.
  • Apparatus providing an 'output signal indicative of the presence of a preselected type of coin comprising, means defining a path of travel for said coins; a radioactive source emitting a beam of beta rays and X-rays, said source being disposed on one side of said path in such a manner that said X-rays and said beta rays impinge upon said coin within said path; an X-ray detector disposed on the opposite side of said path from said source; a beta ray detector disposed on the same side of said path as said source; a scattering plate interposed between said coin path and said X-ray detector, said plate having an opening therethrough allowing X-rays transmitted from said source through said coin within said path to reach said X-ray detector; said plate being formed in such a manner as to scatter the same amount of beta rays from said source into said beta ray detector when no coin is present as is scattered from said preselected type of coin; shielding means disposed between said source and said beta detector to shield saidbeta
  • radioactive source comprises krypton 85 mixed with a high Z material.
  • Apparatus providing output signals indicative of the presence of preselected types of coins comprising, means defining a path of travel for said coins; a first radioactive source emitting a beam of beta rays and X-rays, said beam being incident upon said coins in said path; a first X-ray detector disposed on the opposite side of said path from said first radioactive source; a first backscatter plate interposed between said coin path Vand said X-ray detector, said first backscatter plate having an opening therethrough for passing X-rays transmitted through said coin to said X-ray detector; a iirst beta ray detector disposed on the Y d same side of said coin path as said beta ray first radioactive source, said rst backscatter plate being adapted to scatter the same amount of beta rays from said first radioactive source into said beta ray detector when no coin is travelling along said path as is scattered from a first preselected one of said coin types travelling along said path;
  • a second radioactive source emitting a beam of beta radiation, said second radioactive source being spaced apart from said first radioactive source and disposed in a manner such that said beta ray beam impinges upon coins travelling along said path; a second backscatter platedisposed on the opposite side of said path from said second radioactive source, said second backscatter plate being adapted to scatter the same amount of beta rays from said second source to said second beta ray detector when no coin is travelling along said path between said second source and said second plate as is scattered from a second preselected one of said coin types when passing along said path, the signals from said X-ray detector, said first beta detector and said second beta detector being provided as independent outputs indicative of the types of coins passing along i said path.
  • said beta detector is a cadmium suiide crystal and said X-ray detector is a scintillation crystal operating in conjunction with a photomultiplier tube.
  • Apparatus providing an output signal indicative of the presence of a preselected type of coin comprising, means defining a path of' travel for said coins; a first radioactive source emitting a beam of beta rays and X- rays, said source being disposed on one side of said path in such a manner that said X-rays and said beta rays impinge upon said coin Vwithin said path; an X-ray detector ⁇ disposed on the opposite side of said path from said rst radioactive source; a beta ray detector disposed on the same side of said path as said first source; a shielding member disposed in a manner to shield said beta detector from direct rays from said source; a second radioactive source disposed on the opposite side of said path from said beta detector; said second radioactive source being adapted to provide, with no coin present, an amount of radiation to said beta detect-or equivalent to the amount scattered to said beta detector from said first source by said preselected type of coin; said second source being disposed such that said preselected type
  • Apparatus for identifying coins comprised of radioactive source emitting a beam of beta rays and. X-rays, said beam being impingent upon said coins; first detector means providing an output signal indicating the quantity of beta rays backscattered from each of said coins; second detector means providing independent output signals indicating the quantity of X-rays transmitted through each of said coins; and means responsive to said output signal from said first detector and said output signal from said second detector for providing an output indication of the type of coin.

Description

June 8, 1965 c. w. HANSEN ETAL 3,188,471
COIN IDENTIFICATION APPARATUS UTILIZING RADIATION BOMBARDMENT Filed Jan. 25, 1961 United States Patent l 3,188,471 COIN IDENTHFECATHGN APPARATUS UTILIZING RADIATIUN BUMBARDMENT Carl Woodrow Hansen, Wayland, and Peter J. Claclr, Bedford, Mass., assignors, by mesne assignments, 'to Laboratory for Electronics, lne., Boston, Mass., a corporation of Delaware Filed Jan. 23, 1961, Ser. No. 84,236 8 Claims. (Cl. Z50-83.3)
This invention relates in general to a coin identication system and, more particularly, to an apparatus for identitying coins by a determination of their atomic number and their weight per unit area.
The widespread use of coin operated vending machines and unattended coin pass meters emphasizes the necessity of having accurate and reliable coin identication apparatus. Coin identification, in the sense used here, consists of negative identitication in that all coins, with the exception of a preselected choice, are rejected by the system. Thus, if a pass meter is intended to be operated by a dime, the coin identification system of the pass meter must be capable of rejecting all other coins except dimes and also rejecting slugs intended to represent dimes. While a dime-operated pass meter is a typical example, the same requirement of rejection applies to pass meters and vending machines which may operate on other types of coins or combinations of coins or specially prepared tokens. The problem, of course, becomes more complex when it involves a multi coin machine, such as a '15 cent pass meter or the like.
ln the past a variety of sensor elements had been used to reject false coins in the above type of machines. Each of these sensor elements has been directed to particular characteristics of the coins to be accepted or to particular characteristics such as magnetic permeability of likely slug material. Thus, pass meters have usually employed feeler elements to produce an accepting output signal when the coin is of the appropriate diameter and totreject all coins of greater or lesser diameters. Generaliy a weight indication would be employed in combination with the diameter sensor and this weight indicator would provide an accept signal only when the weight was within preset limits. The thickness of the coin, also, is a characteristic which can readily be determined by mechanical or electromechanical means. Systems of coin identilication and rejection based on these characteristics of physical dimension `and total weight become complex, in terms of likely slug substitutes, and are further complicated by variations inthese dimensions due to normal Wear on coins. But, perhaps the chief problem with existing coin identification systems lies in the fact that these determinations of the physical dimensions depend upon mechanical contact devices. Consequently heavily used machines tend to become unreliable and require frequent and costly maintenance. The lack of reliability frequently takes the form of the machine rejecting legitimate coins or jamming and when the machine is controlling the gate of an unattended toll highway or a relatively remote `street railway station, the resultant inoperability of the gate causes major inconvenience.
It is, therefore, a primary object of the present invention to provide an economic, reliable coin identification system utilizing electromagnetic radiation absorption and reliection characteristics to identify coins.
It is another object of the present invention to provide an efficient, economic, non-contacting coin identification system utilizing radioactive sources and detectors as the sensor elements.
It is still another object' of the present invention to provide a reliable, economic coin or token identilication BSSAYI Patented .lune 8, 1965 ICC system wherein the coin identication is based upon the atomic number and weight per unit area characteristics of the coins.
roadly speaking, the apparatus of the present inven-V tion identities coins by determining the atomic number and weight per unit area of each coin entered into the machine. The measurement of these quantities is accomplished by means of measuring both the transmission and reflection of nuclear radiation bythe coin. The backscattering coeiiicient of beta radiation from a material is directly dependent upon the atomic number of that material, and hence the amount of beta radiation scattered back to a beta detector in a iixed geometrical arrangement provides a clear indication of the atomic number of the backscattering material. In addition, X- rays and gamma rays are transmitted through materials with the percent absorption of these rays depending upon the weight per unit area of the material. Hence, by interposing the coin to be identiiied between a source of X-rays or gamma rays and a detector, the weight per unit area can be determined by measurement of the amount of such radiation transmitted.
The table below lists the United States Currency Coins together with their metallic composition, atomic number,
specific gravity, thickness and weight per unit area.
WtJunit Coin Metal At. S. G. Thickarea Numness (ms/- ber cm.2)
Penny Copper 29 8 89 055 1, 240 Nickel @8% ggg-j: 8.85 065 1,465 98% silver 47 10. 5 045 1, 20() d 47 10.5 060 1,590 47 10.5 702 1,910 47 10. 5 08s 2,340
From the above table it can be seen in every case of coins having the same atomic number the difference in weight per unit area exceeds 10%. Even with the normal Wear of coins, this difference in weight is a sutlicient basis of distinction for coins of the same atomic number, and all others may be distinguished on thebasis` of atomic number. Hence, these two characteristics are suiiicient to identify each coin as to the type and to reject the usual slug material, such as steel, lead, plastics and the like. It should be noted that in coin identification of this type there is -no mechanical contact between the sensors and the coin, hence wear is greatly reduced.
Other objects and advantages will become apparent from the following detailed description when taken in conjunction with accompanying drawing in which:
FIG. l is an illustration in block diagrammatic form of a one embodiment of a Vcoin identiiication apparatus in accordance with the principles for this invention.;`
FIG.` 2 is a graphical illustration of the dependence of beta Vbackscatter signal on atomic number of materials;
FIG. 3 is a graphical illustration of the dependence of transmitted radiation on the weight per unit area of the absorber; and
FlG. 4 is an illustration in block diagrammatic form of a coin identication apparatus employing multiple sensor elements.
l With reference now specifically to FlG. l, a-radioactive source lei is located to one side of the path ofV opposite side of the path ofV travel lll from the sourceV 14 and has anopening 13 in it allowing radiation from the source lA- which passes through the coin l1 to pass dollar and dollar.
through the opening and strike the sensitive surface 22 of a second radiation detector 21. The output of detector 2@ is provided to terminal 25 labeled backscatter output, while the output of detector 21 is provided to terminal 26 labeled transmission output. This configuration of elements provides on the output 25 of detector 2@ signals resulting from radiation backscattered from either a coin 11 or the backscatter plate 12. On the output terminal 26 of Vdetector 21 the signals represent the radiation transmitted through the opening 13 in plate 12 and when a coin 11 intercepts this radiation beam, the signals represent the radiation transmitted through the coin and through the opening.
The radioactive source 14 would typically consist of a beta emitting radioisotope admired with a high Z material so that the source would emit both the beta radiation and bremsstrahlung radiation. The portion of beta radiation backscattered from a coin travelling along path 1d is a function of the atomic number of the elements ywithin the coin, whereas the amount of bremsstrahlung radiation transmitted through the coin is a function of the weight per unit area of the coin. Backscatter detector 20 is a beta sensitive detector, typically a geiger Vmueller tube or a cadmium sulphide crystal, whereas X- ray Vdetector 21 is a detector relatively insensitive to beta radiation and typically would be a scintillation crystal and photomultiplier combination. As previously indicated, the` backscatter output signal is related to the atomic number of the coin from which the beta radiation is scattered, while the transmission output is related to the weight per unit area. The device may be operated as a no-go instrumer1t in which a signal should appear on terminal 25 only when the coin 11 is characterized by an atomic number different from that of the material in the acceptable coin. For example, if the machine is setto accept dimes, which are 98% silver having an,
' catter output 25 when a dime is present, while signals should appear as a no-go signal when any other material is traversing the coin path 10. The function of the backscatter plate 12 is to provide a standardizing bias signal equivalent to the signal developed by the acceptable coin so that theV test of acceptability becomes one relative to the signal derived from the backscatter plate when no coin is present. Since the backscatter signal depends upon both atomic number and spacing and since the backscatter plate 12 is spaced further from the source than the path of the coin 10, then the backscatter plate must be made of higher atomic number material than the acceptable coin material. Both lead plate and tungsten alloy have been found to be acceptable materials with convenient spacings.
The backscatter plate 12 may be eliminated and a second radioactive source employed to create the bias signal. This second source is arranged such that the presence of the coin absorbs the radiation from it, hence the signal from the beta detector in this case also represents only the radiation from source 14 scattered from the com.
With reference now to FIG. 2, the dependence of the beta ray backscatter signal from a krypton 85 beta ray source on the atomic number of the backscattering material is illustrated.v From this gure it can be seen that there is a significant difference between the backscatter signal from silver having an atomic number of 47 and Vcopper having an atomic number of 29. As indicated in Table I,l all U.S. coins are substantially either silver or copper. Accordinglyif the device of FIG. l were arranged such that a silver coin only was acceptable, then other materials would provide a no-go signal on terminal 25. Hence, the presence or absence of a signal on terminal 25 would indicate whether the coin lay within or without the group consisting of a dime, quarter, half- With reference now to FIG. 3, the dependence on weight per unit area of X-ray transmisv sion is shown. As indicated therein, there is a substantial difference in signal between any coins within the same atomic number group. For example, the penny and nickel, of which both are mostly copper (atomic number 29), exhibit a substantial difference in transmitted X-ray signals. The silver group, consisting of the dirne, quarter, half-dollar and dollar, exhibit even more substantial differences in transmitted X-ray signals. Hence referring again to the apparatus of FIG. 1, the output terminal 25 signal distinguishes between the copper and silver group, whereas the signal on terminal 26 provides a clear indication of which coin within either group it is. In regard to slugs, which are not coins at all, it would probably be possible to make slugs giving readings comparable to any one of the regular coins by coating relatively inexpensive material with thin coatings of lead or other heavy metal. fabricated slugs would probably be equal to or greater than the value of the coin and hence a coin pass meter or the like need not be capable of distinguishing them. The device illustrated in FlG. 1 employed a backscatter plate 12 in order to provide a standardizing signal and to eliminate problems of drift and the like in the detector and circuitry. It should be clear, however, that the backscatter plate standardization is not essential to the coin detection, inasmuch as a circuit can be employed at the output of terminal 25 to distinguishbetween several positive signals of different magnitude.
With reference now to FIG. 4 a coin identification apparatus, capable of accepting-two different preselected types of coins while rejecting all others, is shown. In this illustration like numbers refer to like parts of FIG. l, In this embodiment the coin again travels along a path as indicated by the dotted line 10 between a backscatter plate 12 and source and detector combinationl and 20. However, the coin travels along an extension of this path beside a second backscatterplate 32. This second backscatter plate 32 is formed of a similar material to backscatter plate 12, however, it has no opening through it. On the other side of the coin path from the backscatter plate 32 are placed a beta ray source 30 and beta i ray detector 31 separated by a shielding element 29. The output of the beta detector 31 is provided to a terminal 3S. In this embodiment the backscatter plate 12 is spaced appropriately from the source 14 and detector 2t) combination, so that in the absence of a coin, a signal is presented on terminal 25 equivalent to the signal which would be received from a silver coin. Hence any change of signal in terminal 25 represents a non-silver coin passing along path 1t?. The output terminal 25 is connected to a gating circuit 33, as isoutput terminal 26 from detector 21. Similarly, the output terminal 35 of beta detector 31 is also coupled to gating circuit 33.
The radioactive source 30 associated with detector 31k is a pure beta ray source, since there is no opening through plate 32 and no transmission detector associated with these components. The backscatter plate 32 may be formed conveniently of the same material as backscatter plate 12, however its spacing from the path of coin travel 1d is arranged such that the output signal from Vdetector 31 when there is no coin between the plate 32 and source 30 is equivalent to that received when a coin formed of copper is within this area. Hence the outputV on terminal 35 will remain kthe same exceptA when there is a noncopper coin travelling between the source 3() and plate 32. Three types of information, then, .are provided to gating circuit 33, namely a signal from terminal 25 indi- However, the cost of these s, rea-1.71
An absence of a no-silver signal from terminal 25, coupled with a signal from terminal 26 indicating a weight per unit area of approximately 1200 mm./cm.2, would be indicative of a dime hence provide a positive signal on a dime output. On the other hand, an absence of a no-silver signal from terminal 25, coupled with any other weight per unit area, would again provide a reject output. Similarly, absence of a no-copper signal from terminal coupled with a weight per unit area indication from terminal 2o of 1465 mg./cm.2 would provide a positive nickel output, whereas an absence of a no-copper signal coupled with any other weight would again provide a reject output. YBy an extension of these gating circuit principles, it is apparent that the device may be made to provide a positive output indication of any type of coin.
While the devices has been described above in terms of United States coins, the invention is not so limited. It is apparent that the same principles and apparatus may be applied to the identification of special tokens and the like, as well as suitable types of non U.S. coins. Having descibcd the invention herein, it is apparent that many modifications and improvements may now be made by those skilled in the art, and it is intended that the invention disclosed herein should be limited only by the spirit and scopevof means responsive to the outputs of said beta ray and said i X-ray detectors providing an output indicative of the type of said coin.
2. Apparatus providing an 'output signal indicative of the presence of a preselected type of coin comprising, means defining a path of travel for said coins; a radioactive source emitting a beam of beta rays and X-rays, said source being disposed on one side of said path in such a manner that said X-rays and said beta rays impinge upon said coin within said path; an X-ray detector disposed on the opposite side of said path from said source; a beta ray detector disposed on the same side of said path as said source; a scattering plate interposed between said coin path and said X-ray detector, said plate having an opening therethrough allowing X-rays transmitted from said source through said coin within said path to reach said X-ray detector; said plate being formed in such a manner as to scatter the same amount of beta rays from said source into said beta ray detector when no coin is present as is scattered from said preselected type of coin; shielding means disposed between said source and said beta detector to shield saidbeta detector from direct beta radiation from said source.
3. Apparatus in accordance with claim 1 wherein said radioactive source comprises krypton 85 mixed with a high Z material. v
4. Apparatus providing output signals indicative of the presence of preselected types of coins comprising, means defining a path of travel for said coins; a first radioactive source emitting a beam of beta rays and X-rays, said beam being incident upon said coins in said path; a first X-ray detector disposed on the opposite side of said path from said first radioactive source; a first backscatter plate interposed between said coin path Vand said X-ray detector, said first backscatter plate having an opening therethrough for passing X-rays transmitted through said coin to said X-ray detector; a iirst beta ray detector disposed on the Y d same side of said coin path as said beta ray first radioactive source, said rst backscatter plate being adapted to scatter the same amount of beta rays from said first radioactive source into said beta ray detector when no coin is travelling along said path as is scattered from a first preselected one of said coin types travelling along said path;
a second radioactive source emitting a beam of beta radiation, said second radioactive source being spaced apart from said first radioactive source and disposed in a manner such that said beta ray beam impinges upon coins travelling along said path; a second backscatter platedisposed on the opposite side of said path from said second radioactive source, said second backscatter plate being adapted to scatter the same amount of beta rays from said second source to said second beta ray detector when no coin is travelling along said path between said second source and said second plate as is scattered from a second preselected one of said coin types when passing along said path, the signals from said X-ray detector, said first beta detector and said second beta detector being provided as independent outputs indicative of the types of coins passing along i said path.
5. Apparatus in accordance with claim 4- wherein said first and said second backscatter plates are both formed of tungsten alloy.
6. Apparatus in accordance with claim 2 in which said beta detector is a cadmium suiide crystal and said X-ray detector is a scintillation crystal operating in conjunction with a photomultiplier tube.
7. Apparatus providing an output signal indicative of the presence of a preselected type of coin comprising, means defining a path of' travel for said coins; a first radioactive source emitting a beam of beta rays and X- rays, said source being disposed on one side of said path in such a manner that said X-rays and said beta rays impinge upon said coin Vwithin said path; an X-ray detector` disposed on the opposite side of said path from said rst radioactive source; a beta ray detector disposed on the same side of said path as said first source; a shielding member disposed in a manner to shield said beta detector from direct rays from said source; a second radioactive source disposed on the opposite side of said path from said beta detector; said second radioactive source being adapted to provide, with no coin present, an amount of radiation to said beta detect-or equivalent to the amount scattered to said beta detector from said first source by said preselected type of coin; said second source being disposed such that said preselected type of coin within said path preventsV beta rays from said second source from reaching said detector.
8.V Apparatus for identifying coins comprised of radioactive source emitting a beam of beta rays and. X-rays, said beam being impingent upon said coins; first detector means providing an output signal indicating the quantity of beta rays backscattered from each of said coins; second detector means providing independent output signals indicating the quantity of X-rays transmitted through each of said coins; and means responsive to said output signal from said first detector and said output signal from said second detector for providing an output indication of the type of coin.
References Cited by the Examiner UNITED STATES PATENTS 2,884,535 4/59 Swift Z750-83.4 X 2,903,590 9/59 Somerville Z50-83.4 X 2,951,159 8/60 Hariner Z50-83.4 X 2,964,631 12/60 Foster 250-83.4 2,977,478 3/61 Wuppermann Z50-83.4 3,092,724 6/63 Foster 250--83.4 X
RALPH G. NILSON, Primary Examiner.
ARTHUR GAUSS, ARCHIE R. BROCHELT,
Examiners.

Claims (1)

1. APPARATUS FOR IDENTIFYING COINS COMPRISING, MEANS DEFINING A PATH OF TRAVEL FOR SAID COINS; A RADIOACTIVE SOURCE DISPOSED IN FIXED RELATIONSHIP TO SAID PATH, SAID RADIOACTIVE SOURCE BEING ADAPTED TO EMIT A BEAM OF BETA RAYS AND X-RAYS IMPINGING UPON SAID COIN WITHIN SAID PATH; A BETA RAY DETECTOR DISPOSED IN A MANNER TO RECEIVE BETA RAYS BACKSCATTERED FROM SAID COIN; A SHIELDING ELEMENT ADAPTED TO SHIELD SAID DETECTOR FROM NON-SCATTERED BETA RAYS FROM SAID SOURCE; AN X-RAY DETECTOR DISPOSED TO RECEIVE X-RAYS FROM SAID SOURCE TRANSMITTED THROUGH SAID COINS, MEANS RESPONSIVE TO THE OUTPUTS OF SAID BETA RAY AND SAID X-RAY DETECTORS PROVIDING AN OUTPUT INDICATIVE OF THE TYPE OF SAID COIN.
US84236A 1961-01-23 1961-01-23 Coin identification apparatus utilizing radiation bombardment Expired - Lifetime US3188471A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US84236A US3188471A (en) 1961-01-23 1961-01-23 Coin identification apparatus utilizing radiation bombardment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US84236A US3188471A (en) 1961-01-23 1961-01-23 Coin identification apparatus utilizing radiation bombardment

Publications (1)

Publication Number Publication Date
US3188471A true US3188471A (en) 1965-06-08

Family

ID=22183679

Family Applications (1)

Application Number Title Priority Date Filing Date
US84236A Expired - Lifetime US3188471A (en) 1961-01-23 1961-01-23 Coin identification apparatus utilizing radiation bombardment

Country Status (1)

Country Link
US (1) US3188471A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3808444A (en) * 1973-01-05 1974-04-30 Westinghouse Electric Corp X-ray contrast detection system
US4182954A (en) * 1978-04-21 1980-01-08 Phillips Petroleum Company Method and apparatus for measuring material properties related to radiation attenuation
US4768214A (en) * 1985-01-16 1988-08-30 American Science And Engineering, Inc. Imaging
US5400380A (en) * 1991-03-18 1995-03-21 Data Measurement Corporation Dynamic alloy correction gauge
US7660687B1 (en) * 2006-05-25 2010-02-09 Kla-Tencor Corporation Robust measurement of parameters
US20150201721A1 (en) * 2012-07-30 2015-07-23 Crane Payment Solutions Gmbh Coin and method for testing the coin

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2093590A (en) * 1935-05-24 1937-09-21 Gen Aniline Works Inc 2-aminoquinizarin and substitution products thereof and a process of preparing them
US2884535A (en) * 1956-01-26 1959-04-28 Foxboro Co Radio-active gauging system
US2951159A (en) * 1953-05-04 1960-08-30 Armstrong Cork Co Method and apparatus for making repetitive measurements
US2964631A (en) * 1958-06-30 1960-12-13 Industrial Nucleonics Corp Measuring system
US2977478A (en) * 1953-11-11 1961-03-28 Exatest Ges Fur Messtechnik Mi Method of and apparatus for measuring the thickness of materials
US3092724A (en) * 1959-07-27 1963-06-04 Industrial Nucleonics Corp Mass distribution analyzer

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2093590A (en) * 1935-05-24 1937-09-21 Gen Aniline Works Inc 2-aminoquinizarin and substitution products thereof and a process of preparing them
US2951159A (en) * 1953-05-04 1960-08-30 Armstrong Cork Co Method and apparatus for making repetitive measurements
US2977478A (en) * 1953-11-11 1961-03-28 Exatest Ges Fur Messtechnik Mi Method of and apparatus for measuring the thickness of materials
US2884535A (en) * 1956-01-26 1959-04-28 Foxboro Co Radio-active gauging system
US2964631A (en) * 1958-06-30 1960-12-13 Industrial Nucleonics Corp Measuring system
US3092724A (en) * 1959-07-27 1963-06-04 Industrial Nucleonics Corp Mass distribution analyzer

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3808444A (en) * 1973-01-05 1974-04-30 Westinghouse Electric Corp X-ray contrast detection system
DE2365221A1 (en) * 1973-01-05 1974-07-18 Westinghouse Electric Corp METHOD FOR MONITORING AN OBJECTIVE FOR THE PRESENCE OF HANDGUN OR AMMUNITION AND DEVICE FOR PERFORMING SUCH A PROCEDURE
US4182954A (en) * 1978-04-21 1980-01-08 Phillips Petroleum Company Method and apparatus for measuring material properties related to radiation attenuation
US4768214A (en) * 1985-01-16 1988-08-30 American Science And Engineering, Inc. Imaging
US5400380A (en) * 1991-03-18 1995-03-21 Data Measurement Corporation Dynamic alloy correction gauge
US7660687B1 (en) * 2006-05-25 2010-02-09 Kla-Tencor Corporation Robust measurement of parameters
US20150201721A1 (en) * 2012-07-30 2015-07-23 Crane Payment Solutions Gmbh Coin and method for testing the coin
US9894966B2 (en) * 2012-07-30 2018-02-20 Crane Payment Innovations, Inc. Coin and method for testing the coin

Similar Documents

Publication Publication Date Title
US3018374A (en) Methods of and means for assaying material having a fissionable component
US10942292B2 (en) Non-intrusive method to identify presence of nuclear materials using energetic prompt neutrons from photon-induced fission
US3928765A (en) Determining composition of a substance by the use of both reflected and transmitted radiation
US20070290136A1 (en) Pulse shape discrimination method and apparatus for high-sensitivity radioisotope identification with an integrated neutron-gamma radiation detector
US3188471A (en) Coin identification apparatus utilizing radiation bombardment
US3840746A (en) Gamma ray density probe utilizing a pair of gamma ray sources and a gamma ray detector
US2903590A (en) Nuclear radiation measuring instrument
US3412249A (en) Backscatter thickness measuring gauge utilizing different energy levels of bremsstrahlung and two ionization chambers
US3452192A (en) Multiple energy detection for mixture analysis
CN108535770A (en) Twilight sunset detection device and twilight sunset detection method
US3032658A (en) Radiation detectors
US3409774A (en) Method of determining the thickness of a coating on a metal base and method of calibrating the thickness gauge
US3366791A (en) Geiger-muller radiation detector with means to prevent erroneous readings at high radiation intensity
EP2171723B1 (en) Non-intrusive method to identify presence of nuclear materials using energetic prompt neutrons from photon-induced fission
US3193680A (en) Thickness measurement using alpha particles
US2557868A (en) Measuring and testing methods and apparatus employing x-rays
US2967938A (en) Thickness measurement
CN208283569U (en) Twilight sunset detection device
US3012143A (en) Testing and measuring device
CA1132262A (en) Method and apparatus for evaluating notes
US3234382A (en) Gamma ray measuring system utilizing plural detectors
US3452202A (en) Method for determining the surface density and thickness of sheet materials and films
US3329815A (en) Device for measuring beam quality of ionizing radiation comprising first and second detectors of different radiation lengths
US3223839A (en) Apparatus for exploring geological strata utilizing a neutron source and detector
US4066897A (en) Chemical change measuring apparatus