US3147225A - Radioactive sources and method for making - Google Patents
Radioactive sources and method for making Download PDFInfo
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- US3147225A US3147225A US712254A US71225458A US3147225A US 3147225 A US3147225 A US 3147225A US 712254 A US712254 A US 712254A US 71225458 A US71225458 A US 71225458A US 3147225 A US3147225 A US 3147225A
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- G—PHYSICS
- G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
- G21G—CONVERSION OF CHEMICAL ELEMENTS; RADIOACTIVE SOURCES
- G21G4/00—Radioactive sources
- G21G4/04—Radioactive sources other than neutron sources
- G21G4/06—Radioactive sources other than neutron sources characterised by constructional features
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- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03C—CHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
- C03C10/00—Devitrified glass ceramics, i.e. glass ceramics having a crystalline phase dispersed in a glassy phase and constituting at least 50% by weight of the total composition
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- C—CHEMISTRY; METALLURGY
- C03—GLASS; MINERAL OR SLAG WOOL
- C03C—CHEMICAL COMPOSITION OF GLASSES, GLAZES OR VITREOUS ENAMELS; SURFACE TREATMENT OF GLASS; SURFACE TREATMENT OF FIBRES OR FILAMENTS MADE FROM GLASS, MINERALS OR SLAGS; JOINING GLASS TO GLASS OR OTHER MATERIALS
- C03C3/00—Glass compositions
- C03C3/12—Silica-free oxide glass compositions
- C03C3/16—Silica-free oxide glass compositions containing phosphorus
- C03C3/21—Silica-free oxide glass compositions containing phosphorus containing titanium, zirconium, vanadium, tungsten or molybdenum
Definitions
- This invention relates to small discrete weatherresistant refractory particles in which radioactive ions are widely dispersed and firmly xed so as to resist removal.
- the particles hereof constitute discrete sources of radioactivity which may conveniently be handled with a minimum of hazard.
- My particles have an inorganic refractory matrix which not only resists discoloration and degradation by radiation, but also permits substantial transmission of radioactive emanations therethrough.
- This matrix serves as a barrier against actual contact between radioactive ions entrapped therein and an individual who may accidentally or intentionally touch the articles. It is highly resistant to damage by weathering, and by acid and alkaline chemicals. While the matrix is translucent or transparent to light, and is formed using a glassy material, it is actually composed of inorganic refractory materials which are present in such amount that one cannot, in face, form a glass from a raw material batch of such composition by merely using ordinaly glassforming temperatures up to about 1000 C. (or in most cases even 1500 C. or higher). Yet, in aiiixing radioactivity in such a matrix to form my articles, it is unnecessary to exceed about 1000 C., or so; and desired results may be gained using much lower temperatures.
- Radioactive isotopes are dispersed in essentially ionic form within the refractory inorganic matrix aforenoted, and are mechanically entrapped so as to resist dislodgment. It is also likely, as will be explained, that the radioactivity in my articles is held in position by forces of ionic attraction, or is chemically bound in place so as to resist migration from the matrix. The strongest chemical bonding (and mechanical bonding) is achieved particularly in cases where higher temperatures of alhxation are employed, as illustrated hereinafter.
- Ions or particles of non-radioactive material may be affixed in or about the matrix of my radioactive source particles; and such additional constituents may or may not function in combination with the entrapped radioactivity to producen useful result.
- my articles may be subjected to varied temperature conditions, from freezing temperatures well below C. up to temperatures as high as approximately 1000 C., or even higher, without danger of radioactive material loss. They may be employed as sources of radioactivity in high temperature environments where all other small sources of radioactivity known to me deteriorate and allow escape of radioactive material, thus creating unwanted hazards.
- particles of this invention may be used in applications around molten metals (eg, in a liquid level indicator apparatus where the radioactive source would be inside the furnace and a detector outside its walls), in combination with phosphors as a heat resistant self-luminous marker on the exterior of rockets and missiles, in spark-gap equipment to introduce pre-ionization; and in a multitude of other applications, particularly where the hazards associated with radioactivity migrating from a source are to be avoided.
- molten metals eg, in a liquid level indicator apparatus where the radioactive source would be inside the furnace and a detector outside its walls
- phosphors as a heat resistant self-luminous marker on the exterior of rockets and missiles
- spark-gap equipment to introduce pre-ionization
- FIGURE l A drawing7 made a part hereof schematically illustrates in FIGURE l an enlarged cross-sectional View of a radioactive source article of this invention.
- the article is preferably a small sphere or spheroid in shape and comprises a matrix 10 in which radioactive isotopes l1 are dispersed and entrapped.
- Dotted lines l2 are representations of the shrunken, and even obliterated, pores of the matrix in which the radioactive isotopes are bound.
- These radioactive isotopes are held within the chemically-resistant matrix by physical forces, i.c., by the pinching action of the walls of the shrunken pores around the radioactive atoms.
- chemical forces also play a very important part in retaining the radioactive ions or isotopes in fixed position within the matrix.
- FIGURE 2 of the drawing is a schematic representation in side elevation of a sheet layer of Vself-luminous material, wherein radioactive source articles 20 of this invention are held in a plastic matrix or layer 21 in intimate association with a phosphor compound 22 (represented by dots in the plastic layer of this figure).
- the resulting leached refractory glassy particles having very high ion exchange properties, are then placed in solutions containing radioactive ions.
- the radioactive ions are rapidly picked up and absorbed by ion exchange within the leached pores of the glassy particles. From the solution which contained radioactive ions, the particles are dried and then raised to a temperature of at least about 350 C.
- the articles After this heat treatment, the articles, still in a translucent or transparent condition, and still as discrete articles (i.e., not fused together), are subjected to a brief treatment with acid solution so as to remove exposed radioactive ions which may have clung to the outer surfaces of the particles. They are then dried and are ready for use.
- the particles so formed are preferably in the range of about to 150 microns average diameter. While larger sized particles may be formed where desired for specialized uses (e.g., thicknesses of about 2 mm. or even greater for the particles or layers), it has been found most practical to keep the size of particles usually within a range capable of passing through a screen of about 50 mesh (i.e., about 200 microns).
- a solution of strontium-90 in the form of strontium chloride was shaken for tive hours with leached beads of about 125 to 175 microns average diameter and of the type hereinafter described in Example 1.
- the beads Were then Washed with water, dried overnight at about 54 C., and placed in an oven and heated to 250 C. over a period of 4 hours. They were then raised rapidly to 500 C. and maintained at that temperature overnight. Then, they were raised rapidly to 1000 C. and held for 6 hours, after which they were cooled gradually over a period of about 18 hours to room temperature.
- the shrunken beads were then immersed in an acid wash consisting of 0.1 normal HC1 for two weeks to remove radioactive ions on the exposed outer surfaces of the beads. The amount removed was noted (less than 1%). Such beads Were then tested for leach resistance and found to lose less than 0.0004% (i.e., less than four parts per million) of their entrapped radioactive ions in a water exposure test at 54 C. lasting 42 days. Such resistance to leaching, insofar as I am aware, has never been approached in discrete small radioactive sources. Indeed, one could drink the water used in this leaching test without harmful effects.
- radioactive materials may be used in making the articles hereof.
- the particular radioactive isotope selected must be capable of ionization. Radioactive isotopes are commonly recognized as those which are unstable and decay to a less unstable state with the emission of penetrating radiation from the nucleus. From the illustrative examples, it is seen that a variety of wellknown radioactive materials of widely differing halflife, radioactive particle or ray emanation, valence, etc., are suitable to employ.
- EXAMPLE l A raw material batch of inorganic oxides having a compositional analysis in mol percent consisting of about ZlOg, A1915, B015, P025 and 32.0% NaO0 5 is melted to a homogeneous mass at about 1350 C., and then quenched by pouring the melt in a cool bath of water so as to form small fractured glass particles (frit) of varied shapes.
- the glass particles are then formed into spheres.
- this can be done by passing them through a radiant heating zone or high temperature flame where they soften suciently to permit surface tension forces to form them into spheres while they are freely moving through air. They are then cooled rapidly to prevent devitrication. Beads or spheres averaging about 50 to 100 microns in diameter are formed.
- leached beads have an effective surface area of about 670 square meters per gram, as may be determined by the Brunauer-Emmett-Teller (B.E.T.) method, the method being set forth in an article by P. H. Emmett appearing on page et seq. of a published volume entitled Symposium on New Methods for Particle Size Determination in the Subsieve Range, containing the minutes of the Washington spring meeting, March 4, 1941, of the American Society for Testing Materials.
- B.E.T. Brunauer-Emmett-Teller
- the beads were then rinsed with Water, dried in air a few hours, and raised to 500 C. over a period of about 4 hours. They were tired at 500 C. for about 18 hours, and then raised over a period of 3- hours to 1000 C. Where they were maintained for about 4 hours, after which they were cooled to room temperature gradually over a period of about 16 hours. No sintering together of the beads occurred even though firing was accomplished while they were piled in a mass. During firing, the leached pores throughout the beads contracted and the ionically-bonded radioactive Pm-147 ions become an integral part of the structure. They were mechanically and chemically entrapped therein.
- the beads ⁇ containing afiixed 19m-147 were shaken for one hour with a 100 ml. aliquot of one normal aqueous H2804 to remove any small amount of Pm-147 which may have clung to the outer surfaces of the beads. This acid wash was then repeated as an added precaution to remove residual surface radioactive ions, and then the product was rinsed with water and dried in air.
- the resulting articles were spherical in shape and had a substantially divitried refractory matrix Within which Pm-147 was chemically and mechanically entrapped.
- the extent to which 13m-147 was entrapped and resistant to removal by leaching was tested, as set forth in Table I below.
- Example 2 The procedure of Example 1 was followed except that different leached glassy articles were employed. These glassy articles were formed from a raw material batch having an analysis in mol percent consisting o f about 1.1% TiOZ, 5.7% Zr02, 5.7% Si02, 5.7% A101 5 25.0% B015, P0215, NaO 5, and KO0'5, using a melting temperature of 1350 C. The quenched glass particles were formed into beads of about 50 to 2,00 microns average diameter and then leached for four hours under conditons otherwise as specified in Example 1. The resulting glassy matrices exhibitedA an ion exchange capacity of about 5.9 rnilliequivalents per gram and had an effective surface area of about 450 square meters per gram.
- EXAMPLE 3 A raw material batch analyzing to contain, in mol percent, 6.0% TiOZ, 6.0% Hf02, 36.0% B015, 22.0% P025 and 30.0% CaO was melted at 1350 C. and quenched in a cool bath of water to form glass frit particles. The particles were converted to beads of about 50 to 200 microns average diameter and leached for a period of 30 hours using conditions set forth in Example 1. Analysis of the leached product showed its composition 4to be, in mol percent, about 13.9% Ti02, 19.1% Hf02, 63.5% P0215, 3.5% CaO, and a trace of B015. Its ion exchange capacity measured to 'be about 5.7 milliequivalents with an effective surface area of about 530 square meters per gram.
- montmorillonite article of the type known heretofore in the art.
- the montmorillonite article was made by exposing the montmorillonite clay for 24 hours to4 Pm147 ions in water solution containing chloride as the anion. About 94 percent of the Pm-147 ions were adsorbed from solution, after which the inontmorillonite was subgected to the same heat treatment as set forth in Example 1. Instead of remaining as powder particles, it fused into a plurality of relatively larger particles under this heat treatment. It was then washed with acid as specified in Example 1 hereof, before conducting the tests hei'e set forth.
- a particularly highly refractory matrix comprised in essential respects of at least one phosphate complex selected from the group consisting of titanium phosphate, zirconium phosphate and hafnium phosphate.
- a particularly highly refractory matrix comprised in essential respects of at least one phosphate complex selected from the group consisting of titanium phosphate, zirconium phosphate and hafnium phosphate.
- each rat was fed a capsule containing about 0.5 millicuries of Sr-90 aixed within a matrix as described in Example 1 hereof.
- Those rats which were sacrificed at the end of 4 days were found on analysis to have only a small harmless amount of radioactive substance in their systems. Based on the amount of radioactive substance initially fed to them, less than 0.001% remained in their bodies. Such a residual low amount of radioactive substance would not produce harmful effects.
- a particularly interesting use of my articles lies in the area of providing new types of self-luminous sheet materials, signs, markers, etc.
- two parts of the articles of Example 1 formed so as to range in size from about 40 to 80 microns, were mixed with 3 parts of phosphor (e.g., a zinc sulfide phosphor) excited by radioactive emanations (such as beta particles from Pm-147), and about 5 parts of a solution of 30% ethyl methacrylate polymer solids in xylene.
- the solvent mixture was then coated on a low adhesion surface at a thickness of about 60 mils, and dried at about 140 F. for one-half hour and at about 200 F. for 15 minutes.
- the resulting sheet layer may be used as a low intensity self-luminescent marker, or as a light source in applications Where electrical illumination is impractical or undesired, e.g., under battle conditions in remote areas.
- composition comprising a plurality of particles as defined in claim 1 in intimate association with a radiation-excitable phosphor.
- a self-luminous article comprising a plastic material having therein a plurality of particles as defined in claim 1 in intimate association with a radiation-excitable phosphor.
- a mass of particles capable of passing through a screen of about 50 mesh each of said particles consisting essentially of an at least partially devitrified weather-resistant inorganicoxide refractory matrix and a radioactive isotope dispersed in said matrix by ion exchange, said radioactive isotope being firmly and substantially insolubly affixed Within shrunken pores of said matrix without substantial attenuation of radioactive emanations from said isotope, said mass of particles being characterized by remaining as a mass of discrete entities not fused and not sintered to each other even when subjected to 1000 C. in contact with each other, and being further characterized by an ability to withstand water exposure for one week at 50 C. with less than 0.1% weight loss of said affixed radioactive isotope.
- a composition comprising a plurality of particles as defined in claim 5 in intimate association with a radiation-excitable phosphor.
- a self-luminous article comprising a plastic material having therein a plurality of particles as defined in claim 5 in intimate association with a radiation-excitable phosphor.
- a particle no larger than about 200 microns having a weatherresistant refractory devitrified matrix comprised essentially of at least one inorganic complex selected from the group consisting of titanium phosphate, zirconium phosphate, and hafnium phosphate, and containing a radioactive isotope dispersed in said matrix by ion exchange and firmly mechanically and substantially insolubly bound within shrunken pores of said matrix.
- a mass of small spherical sealed sources of radioactivity having an average diameter smaller than microns, and each source comprising a radioactive isotope dispersed and substantially insolubly aixed within shrunken pores of a weather-resistant refractory matrix, said matrix being characterized by remaining as a discrete entity not bonded to like particles of identical matrix even when subjected to 1000 C. in contact with said like particles, and being characterized further by serving as a barrier against actual physical contact of the radioactive isotope entrapped therein, the chemical analysis of said matrix being such as to satisfy the requirements of the following table wherein amounts are set forth in mol percent:
- particles of small sealed sources of radioactivity having an average particle size greater than microns and smaller than 2 mm. in thickness, and each comprising a radioactive isotope dispersed and chemically and mechanically affixed within shrunken pores of a weather-resistant inorganicoxide refractory matrix, said matrix being infusible at temperatures below 1000 C. and serving as a barrier against actual physical contact of the radioactive isotope entrapped therein, the chemical analysis of said matrix satisfying the requirements of the following table wherein amounts are set forth in mol percent:
- said uxes being selected from the group consisting of oxides of alkali and alkaline earth metals.
- Method of preparing small sealed sources of radioactivity comprising (1) contacting a solution of radioactive cations in ion exchange relationship with small, leached, highly-porous, refractory, cation exchanging glassy articles infusible at temperatures below 1000 C., said glassy articles being comprised essentially of at least one inorganic complex selected from the group consisting of titanium phosphate, zirconium phosphate, and hafnium phosphate, (2) allowing a period of time for said radioactive cations to be adsorbed Within the pores of said glassy articles, then (3) heat-treating said articles to a temperature above 350 C.
- a composition comprising radiation-excitable phosphor in intimate association with particulate sources of radioactivity having a Weather-resistant inorganic-oxide refractory matrix and containing radioactive isotope for excitation of said phosphor, said radioactive isotope being dispersed in said matrix by ion exchange and structurally bonded within shrunken pores of said matrix, said matrix being at least partially devitriiied and characterized by an ability to withstand 1000 C. in contact with separate particles of identical matrix without sintering and without fusing to said separate particles of identical matrix, and said particulate sources of radioactivity being characterized by an ability to withstand water exposure for one Week at 50 C. with less than ⁇ 0.1% Weight loss of said structurally bonded radioactive isotope.
- a self-luminous article comprising a plastic material within which radiation-excitable phosphor is mixed with particulate sources of radioactivity having a weatherresistant inorganic-oxide refractory matrix and containing radioactive isotope adapted to excite said phosphor, said radioactive isotope being dispersed in said matrix by ion exchange and structurally bonded within shrunken pores of said matrix, said matrix being at least partially devitried and characterized by an ability to withstand 1000 C. in contact with separate particles of identical matrix without sintering and without fusing to said separate particles of identical matrix, and said particulate sources of radioactivity being characterized by an ability to withstand Water exposure for one week at 50 C. with less than 0.1% weight loss of said structurally bonded radioactive isotope.
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Description
Sept. l, 1964 J. P. RYAN RADIoAcTIvE soURcEs AND METHOD FOR MAKING Filed Jan. 30, 1958 United States Patent O FCice 3,147,225 RADIUACTIVE SURCES AND METHGD FR MAKING .lohn P. Ryan, West St. Paul, Minn., assignor to minnesota Mining and Manufacturing Company, St. Paul, Minn.,
a corporation of Delaware Filed Jan. 3d, 1958, Ser. No. 712,254 13 Claims. (Cl. 252-3tiL1) This invention relates to small discrete weatherresistant refractory particles in which radioactive ions are widely dispersed and firmly xed so as to resist removal. The particles hereof constitute discrete sources of radioactivity which may conveniently be handled with a minimum of hazard.
My particles have an inorganic refractory matrix which not only resists discoloration and degradation by radiation, but also permits substantial transmission of radioactive emanations therethrough. This matrix serves as a barrier against actual contact between radioactive ions entrapped therein and an individual who may accidentally or intentionally touch the articles. It is highly resistant to damage by weathering, and by acid and alkaline chemicals. While the matrix is translucent or transparent to light, and is formed using a glassy material, it is actually composed of inorganic refractory materials which are present in such amount that one cannot, in face, form a glass from a raw material batch of such composition by merely using ordinaly glassforming temperatures up to about 1000 C. (or in most cases even 1500 C. or higher). Yet, in aiiixing radioactivity in such a matrix to form my articles, it is unnecessary to exceed about 1000 C., or so; and desired results may be gained using much lower temperatures.
Radioactive isotopes are dispersed in essentially ionic form within the refractory inorganic matrix aforenoted, and are mechanically entrapped so as to resist dislodgment. It is also likely, as will be explained, that the radioactivity in my articles is held in position by forces of ionic attraction, or is chemically bound in place so as to resist migration from the matrix. The strongest chemical bonding (and mechanical bonding) is achieved particularly in cases where higher temperatures of alhxation are employed, as illustrated hereinafter.
Ions or particles of non-radioactive material may be affixed in or about the matrix of my radioactive source particles; and such additional constituents may or may not function in combination with the entrapped radioactivity to producen useful result.
In use, my articles may be subjected to varied temperature conditions, from freezing temperatures well below C. up to temperatures as high as approximately 1000 C., or even higher, without danger of radioactive material loss. They may be employed as sources of radioactivity in high temperature environments where all other small sources of radioactivity known to me deteriorate and allow escape of radioactive material, thus creating unwanted hazards. For example, particles of this invention may be used in applications around molten metals (eg, in a liquid level indicator apparatus where the radioactive source would be inside the furnace and a detector outside its walls), in combination with phosphors as a heat resistant self-luminous marker on the exterior of rockets and missiles, in spark-gap equipment to introduce pre-ionization; and in a multitude of other applications, particularly where the hazards associated with radioactivity migrating from a source are to be avoided. At temperatures at least as high as about l000 C., sources hereof still remain as discrete entities without fusing or flowing together.
lThe size, and therefore weight, of my articles may 3,147,225 Patented Sept. 1, 17964 easily be controlled so that they will not remain suspended in air to create unwanted hazards; thus, intake of the sources with air in breathing can be obviated. The hazards ordinarily associated with accidental or intentional ingestion of radioactivity are reduced to a minimum in using my sources. Indeeed, in cases Where the radioactive emanations from a particular source hereof are on .the order of those tolerable by an individual for short periods, ingestion and egestion of particles of this invention by an individual can be accomplished without any significant harmful effect. Experiments indicate that only very little, or insignificant, residual radioactive material of the source would be left behind in the individual. However, I do not recommend wanton ingestion of my sources; rather I point out here that they show promise of being suitable for medical use in such manner, and that a minimum of hazard is encountered in the case of accidental inegstion. Other medical uses for my articles are also contemplated.
insofar as I am aware, no other source of radioactivity is as easily and safely prepared, is as conveniently handleable, and additionally possesses all of the herein-noted advantageous properties of my articles. Known glassy sources of radioactivity are not resistant to higher temperature deterioration or fusion as aforenoted, and become discolored readily due to radiation, or lose radioactive substance readily when placed in solutions of acid or alkaline chemicals. While some sources of radioactivity have been prepared where the radioactive substance is dispersed, non of these prior art sources have possessed the extraordinary high temperature resistance and resistance to leaching exhibited by my articles; and none have been capable of a concentration of radioactive substance even approaching that possible in the case of my articles. It is estimated that the possible concentration of dispersed radioactive ions per unit of volume in my articles is up to about live times greater than is possible in the case of fused montmorillonite prior art sources containing widely-dispersed radioactive material.
A drawing7 made a part hereof schematically illustrates in FIGURE l an enlarged cross-sectional View of a radioactive source article of this invention. As shown in FIGURE l, the article is preferably a small sphere or spheroid in shape and comprises a matrix 10 in which radioactive isotopes l1 are dispersed and entrapped. Dotted lines l2 are representations of the shrunken, and even obliterated, pores of the matrix in which the radioactive isotopes are bound. These radioactive isotopes are held within the chemically-resistant matrix by physical forces, i.c., by the pinching action of the walls of the shrunken pores around the radioactive atoms. However, as may be gleaned from the discussion to follow, chemical forces also play a very important part in retaining the radioactive ions or isotopes in fixed position within the matrix.
FIGURE 2 of the drawing is a schematic representation in side elevation of a sheet layer of Vself-luminous material, wherein radioactive source articles 20 of this invention are held in a plastic matrix or layer 21 in intimate association with a phosphor compound 22 (represented by dots in the plastic layer of this figure).
In making my source articles l employ the following convenient and simple procedure: First a batch of inorganic oxide ingredients selected to provide a particular glass on melting at ordinary glassforming temperatures is heated to a uid state, using temperatures generally between about 1l00 C.l500 C., and quenched ina bath of Water to form glass frit particles. These particles may then, if desired, be formed into sphere-like bodies by dropping them through a radiant heating zone wherein they will become fluid while free falling and assume a generally spherical shape due to forces of surface tension. While free falling, they are cooled so as to retain their glassy nature and spherical shape. Then I place these glassy particles in an acid solution so as to leach therefrom a substantial amount of the acid soluble, non-refractory constituents of the original glassforming batch. As illustrated in the examples to follow, the resulting leached refractory glassy particles, having very high ion exchange properties, are then placed in solutions containing radioactive ions. The radioactive ions are rapidly picked up and absorbed by ion exchange within the leached pores of the glassy particles. From the solution which contained radioactive ions, the particles are dried and then raised to a temperature of at least about 350 C. up to approximately 1000 C., or even higher, under which treatment the pores of the glassy matrix actually shrink and seal the radioactive ions Within the matrix, even though this temperature treatment is totally insufficient to effect a fusion or melting of the leached matrix. It has been noted that when temperaures on the order of around 350 F. up to approximately 700 C. are employed, the glassy nature of the matrix is largely preserved; Whereas in the case of employing temperatures in excess of approximately Y700" C., a crystalline phase develops in the refractory matrix of the article. For highest resistance to acid and alkaline attack, it is preferable to heat the refractory matrix above about 700 C., preferably about 1000-1200o C. so as to largely devitrify the matrix to a substantially crystalline phase. After this heat treatment, the articles, still in a translucent or transparent condition, and still as discrete articles (i.e., not fused together), are subjected to a brief treatment with acid solution so as to remove exposed radioactive ions which may have clung to the outer surfaces of the particles. They are then dried and are ready for use.
For convenience of handling and use in sheet material applications, the particles so formed are preferably in the range of about to 150 microns average diameter. While larger sized particles may be formed where desired for specialized uses (e.g., thicknesses of about 2 mm. or even greater for the particles or layers), it has been found most practical to keep the size of particles usually within a range capable of passing through a screen of about 50 mesh (i.e., about 200 microns).
In an early preliminary experiment to test the principles of this invention, the following was done: A solution of strontium-90 in the form of strontium chloride Was shaken for tive hours with leached beads of about 125 to 175 microns average diameter and of the type hereinafter described in Example 1. The beads Were then Washed with water, dried overnight at about 54 C., and placed in an oven and heated to 250 C. over a period of 4 hours. They were then raised rapidly to 500 C. and maintained at that temperature overnight. Then, they were raised rapidly to 1000 C. and held for 6 hours, after which they were cooled gradually over a period of about 18 hours to room temperature. The shrunken beads were then immersed in an acid wash consisting of 0.1 normal HC1 for two weeks to remove radioactive ions on the exposed outer surfaces of the beads. The amount removed was noted (less than 1%). Such beads Were then tested for leach resistance and found to lose less than 0.0004% (i.e., less than four parts per million) of their entrapped radioactive ions in a water exposure test at 54 C. lasting 42 days. Such resistance to leaching, insofar as I am aware, has never been approached in discrete small radioactive sources. Indeed, one could drink the water used in this leaching test without harmful effects.
A Wide variety of radioactive materials may be used in making the articles hereof. The particular radioactive isotope selected must be capable of ionization. Radioactive isotopes are commonly recognized as those which are unstable and decay to a less unstable state with the emission of penetrating radiation from the nucleus. From the illustrative examples, it is seen that a variety of wellknown radioactive materials of widely differing halflife, radioactive particle or ray emanation, valence, etc., are suitable to employ.
In describing the composition of the preferred matrix of the articles hereof, I set forth the individual inorganic constituents as being presumptively present in oxide form, in accordance with general practice in glass and related arts. Also, for convenience and in the interest of accuraCy, the various constituents of the matrix are set forth in terms of unit cations, combined with just sufficient oxygen to satisfy the valence of the particular cation (eg, B015 instead of B203); and the mol percent of the various inorganic constituents of the matrix is calculated on the basis of these unit cation formulas.
The following examples are offered to illustrate this invention, but are not to be construed as limitative thereof.
EXAMPLE l A raw material batch of inorganic oxides having a compositional analysis in mol percent consisting of about ZlOg, A1915, B015, P025 and 32.0% NaO0 5 is melted to a homogeneous mass at about 1350 C., and then quenched by pouring the melt in a cool bath of water so as to form small fractured glass particles (frit) of varied shapes.
The glass particles are then formed into spheres. Suitably this can be done by passing them through a radiant heating zone or high temperature flame where they soften suciently to permit surface tension forces to form them into spheres while they are freely moving through air. They are then cooled rapidly to prevent devitrication. Beads or spheres averaging about 50 to 100 microns in diameter are formed.
About 10 parts by weight of beads so formed are immersed in about 150 parts by weight of a five normal solution of nitric acid for about 6 hours with continuous agitation at room temperature, after which the beads are washed with water. The resulting leached beads, on chemical analysis, show an inorganic composition, set forth in mol percent, consisting of about 33% ZrOZ, about 2% A1015, about 64% P025 and traces of small amounts of BOM, and NaOH. The wash water is drained from the beads, but the beads are not dried. They have an ion exchange capacity of about 6.8 milliequivalents per gram, as may be determined by the following test: To a one gram sample of beads is added 100 ml. of 0.1 normal sodium hydroxide solution and the Whole shaken to equilibrium for about 24 to 72 hours. Thereafter, the solution is drained from the sample and ti'trated with 0.1 normal solution of hydrochloric acid. The milliequivalents of hydrochloric acid used in titration (32 ml. 0.1 N=3.2 meq.) subtracted from the milliequivalents of sodium hydroxide added to the sample (100 ml. 0.1 N=10 meq.) gives the ion exchange capacity (6.8 meq.) of the sample in milliequivalents per gram.
These leached beads have an effective surface area of about 670 square meters per gram, as may be determined by the Brunauer-Emmett-Teller (B.E.T.) method, the method being set forth in an article by P. H. Emmett appearing on page et seq. of a published volume entitled Symposium on New Methods for Particle Size Determination in the Subsieve Range, containing the minutes of the Washington spring meeting, March 4, 1941, of the American Society for Testing Materials.
About three grams of the leached beads of this example, from which excess Water had been drained, were then shaken for 24 hours with ve millicuries of prometheum- 147 in the form of PmClg, dissolved in 100 ml. of a very dilute acid solution. The prometheum-147 was supplied by Oak Ridge National Laboratories and contained less than about 0.1% europium and less than about 15 mg. of neodymium per curie of Pm-147. It was in about 0.1 to 1.0 normal HCl water solution. At the end of 24 hours, the supernatant was decanted and counted to determine the percent of lm-147 adsorbed by the beads. About L, d 99% of the Pnl-147 was found to have been adsorbed by the beads from solution.
The beads were then rinsed with Water, dried in air a few hours, and raised to 500 C. over a period of about 4 hours. They were tired at 500 C. for about 18 hours, and then raised over a period of 3- hours to 1000 C. Where they were maintained for about 4 hours, after which they were cooled to room temperature gradually over a period of about 16 hours. No sintering together of the beads occurred even though firing was accomplished while they were piled in a mass. During firing, the leached pores throughout the beads contracted and the ionically-bonded radioactive Pm-147 ions become an integral part of the structure. They were mechanically and chemically entrapped therein. X-ray diffraction analysis of the inorganic matrix of the bead indicated that a large percentage of the matrix was converted by the heating step to a crystalline phase, and thus I characterize the resulting matrix as devitried (Analysis of beads of this example fired at various maximum temperatures indicated that at about 700 C. the tendency for the matrix to devitrify is noticeable, and that at 1000" C. devitrification is substantial.)
After shrinking the pores of the matrix, the beads` containing afiixed 19m-147 were shaken for one hour with a 100 ml. aliquot of one normal aqueous H2804 to remove any small amount of Pm-147 which may have clung to the outer surfaces of the beads. This acid wash was then repeated as an added precaution to remove residual surface radioactive ions, and then the product was rinsed with water and dried in air.
The resulting articles were spherical in shape and had a substantially divitried refractory matrix Within which Pm-147 was chemically and mechanically entrapped. The extent to which 13m-147 was entrapped and resistant to removal by leaching was tested, as set forth in Table I below.
The articles of this example have further been employed in sign and marker applications. They show every promise of being what might be termed a safe source for radioactive emanations in signs and markers.
Using the procedure and leached beads of this example, the following varied radioactive isotopes, ionized in water solution with an acid anion such as a chloride or nitrate, have been affixed, as described, to provide the new and improved sources of this invention: Sir-90, Tl-204, Co-60, Zn-65, Ag-110, 13e-59, Na-22, Ca-45, and Cs-134. In each case refractory damage-resistant radioactive sources were formed whichwere highly-resistant to loss of their radioactive ions by migration and leaching. For illustrative purposes, the results obtainedA in testing the articles formed using Sr-90 are set forth in Table I.
EXAMPLE 2 The procedure of Example 1 was followed except that different leached glassy articles were employed. These glassy articles were formed from a raw material batch having an analysis in mol percent consisting o f about 1.1% TiOZ, 5.7% Zr02, 5.7% Si02, 5.7% A101 5 25.0% B015, P0215, NaO 5, and KO0'5, using a melting temperature of 1350 C. The quenched glass particles were formed into beads of about 50 to 2,00 microns average diameter and then leached for four hours under conditons otherwise as specified in Example 1. The resulting glassy matrices exhibitedA an ion exchange capacity of about 5.9 rnilliequivalents per gram and had an effective surface area of about 450 square meters per gram. Their leached compositori analyzed to contain, in mol percent, about 5.1% Ti02, 26.8% Zr02, 7.4% Si02, 1.6% A1015, 0.5% B01 5, 56.9% POM, 1.7% KOM, and a trace of Na00 5.
About 94% of Pm-147 ions was adsorbed by the matrix d of these articles, after which the articles were processed as specied in Example 1.
EXAMPLE 3 A raw material batch analyzing to contain, in mol percent, 6.0% TiOZ, 6.0% Hf02, 36.0% B015, 22.0% P025 and 30.0% CaO was melted at 1350 C. and quenched in a cool bath of water to form glass frit particles. The particles were converted to beads of about 50 to 200 microns average diameter and leached for a period of 30 hours using conditions set forth in Example 1. Analysis of the leached product showed its composition 4to be, in mol percent, about 13.9% Ti02, 19.1% Hf02, 63.5% P0215, 3.5% CaO, and a trace of B015. Its ion exchange capacity measured to 'be about 5.7 milliequivalents with an effective surface area of about 530 square meters per gram.
About 93% of the Pmi-147 was adsorbed by these particles, after which the articles were processed as in Examle 1.
EXAMPLE 4 Table I 1 Example 2 3 4 M 2 Pm- Sr- Reagent test 1 a. 2 0.007 0.002 0.007 2. 0 b. 5% NaCl 0. 002 0. 002 0. 002 1. 4 c. .5% Versene 0. 044 0.011 0. 002 2.0 d. 5% Na 2CO3. 0. 10 0.16 0.060 0.16 0.09 e. 0.1 N HCl 0.17 0.022 0. 070 0.11 0.12 48. 8
1 About one gram of the articles of the examples was soaked in m1. of each specied reagent at 50 C. for one week. Reagents li, c, and d are set forth in percent by weight in Water solution. All reagents contain, in addition to the component listed in the table, about 0.01 percent by Weight of CeCls, which served to occupy sites on the vessel in which the test was conducted, and therefore, inhibited. the radioactive isotope from occupying such sites. In this manner, essentially accurate readings of the quantity of the isotope removed from the articles was insured. (The use of CeCla may be omitted, except in the case of testing sources in which the radioactive isotope is a rare earth, such as Pni-147.)
2 This column of test results is for a montmorillonite article of the type known heretofore in the art. The montmorillonite article was made by exposing the montmorillonite clay for 24 hours to4 Pm147 ions in water solution containing chloride as the anion. About 94 percent of the Pm-147 ions were adsorbed from solution, after which the inontmorillonite was subgected to the same heat treatment as set forth in Example 1. Instead of remaining as powder particles, it fused into a plurality of relatively larger particles under this heat treatment. It was then washed with acid as specified in Example 1 hereof, before conducting the tests hei'e set forth.
There is a vast difference between the characteristics and behavior of the refractory materials of my articles and the material of fused montmorillonite articles such as set forth in the table. The highly refractory matrixof my articles, contrary to that of montmorillonite, cannot be fused at temperatures up to about '1000 C. Test results in the table further illustrate that montmorillonite sources have poor resistance to leaching, and thus are unsuitable for use in many weathering applications,
whereas the articles of this invention satisfy the requirements for use in such weathering applications. For example, it may be noted that my articles lost less than 0.1% of their entrapped radioactivity in water exposure tests lasting for one week at 50 C., whereas montmorillonite articles lost 2% as aforenoted in the table.
While a wide variety of materials may be used in forming a refractory matrix of the infusible character and other properties specified herein, it is preferable to employ, as illustrated in the examples, a particularly highly refractory matrix comprised in essential respects of at least one phosphate complex selected from the group consisting of titanium phosphate, zirconium phosphate and hafnium phosphate. A more detailed teaching o-f such inorganic-oxide matrices may be found in U.S. patent application Serial No. 513,156, filed June 3, 1955, by Warren R. Beck and George C. Hann, now Letters Patent No. 2,943,059, having a common assignee with this application. Leached matrices which satisfy the following compositional analysis, in mol percent, are particularly suitable to employ in the practice of this invention:
Table II TiOZ -40 ZrOZ 0-35 HOZ 0-35 Si()2 0-40 A1015 0-10 B015 0-25 POM 20-70 PozmcnoL5 20-70 Fluxes 0-15 BOM-l-uxes 0-25 Total of listed ingredients 90-100 Where fluxes, if present, are selected from alkali and alkaline earth oxides.
As further evidence of the striking properties possessed by the sealed sources of this invention, several rats Were fed my articles and then sacrificed after various periods of time to determine the radioactive material retained in their bodies. Specifically, each rat was fed a capsule containing about 0.5 millicuries of Sr-90 aixed within a matrix as described in Example 1 hereof. Those rats which were sacrificed at the end of 4 days were found on analysis to have only a small harmless amount of radioactive substance in their systems. Based on the amount of radioactive substance initially fed to them, less than 0.001% remained in their bodies. Such a residual low amount of radioactive substance would not produce harmful effects.
Leach tests on my sources also indicate that they are highly resistant to weathering under acid, alkaline, and high ionic strength conditions, and thus may be used in many outdoor environments Where other sources would be unsatisfactory. For example, they may be used in applications of a nautical nature, where salty air and spray may be expected to Contact them.
A particularly interesting use of my articles lies in the area of providing new types of self-luminous sheet materials, signs, markers, etc. For example, two parts of the articles of Example 1, formed so as to range in size from about 40 to 80 microns, were mixed with 3 parts of phosphor (e.g., a zinc sulfide phosphor) excited by radioactive emanations (such as beta particles from Pm-147), and about 5 parts of a solution of 30% ethyl methacrylate polymer solids in xylene. The solvent mixture was then coated on a low adhesion surface at a thickness of about 60 mils, and dried at about 140 F. for one-half hour and at about 200 F. for 15 minutes. The resulting sheet layer may be used as a low intensity self-luminescent marker, or as a light source in applications Where electrical illumination is impractical or undesired, e.g., under battle conditions in remote areas.
The foregoing is offered to illustrate but not limit my invention, as further set forth in the appended claims.
That which is claimed is:
l. As a new article source of radioactivity: a particle having a thickness no greater than 2 mm. and consisting essentially of a weather-resistant refractory matrix at least partially devitritied and characterized by remaining as a discrete entity not bonded to a like particle of identical matrix even when subjected to 1000 C. in contact with said like particle, and a radioactive isotope dispersed in said matrix by ion exchange and structurally bonded within shrunken pores of said matrix, said particle being characterized by an ability to withstand water exposure for one Week at 50 C. with less than 0.1% weight loss of said structurally bonded radioactive isotope.
2. A composition comprising a plurality of particles as defined in claim 1 in intimate association with a radiation-excitable phosphor.
3. A self-luminous article comprising a plastic material having therein a plurality of particles as defined in claim 1 in intimate association with a radiation-excitable phosphor.
4. As new article sources of radioactivity: a mass of particles capable of passing through a screen of about 50 mesh, each of said particles consisting essentially of an at least partially devitrified weather-resistant inorganicoxide refractory matrix and a radioactive isotope dispersed in said matrix by ion exchange, said radioactive isotope being firmly and substantially insolubly affixed Within shrunken pores of said matrix without substantial attenuation of radioactive emanations from said isotope, said mass of particles being characterized by remaining as a mass of discrete entities not fused and not sintered to each other even when subjected to 1000 C. in contact with each other, and being further characterized by an ability to withstand water exposure for one week at 50 C. with less than 0.1% weight loss of said affixed radioactive isotope.
5. As a new article source of radioactivity: a particle having a thickness no greater than 2 mm. and consisting essentially of a weather-resistant refractory devitritied matrix comprised essentially of at least one inorganic complex selected from the group consisting of titanium phosphate, zirconium phosphate and hafnium phosphate, and a radioactive isotope dispersed in said matrix by ion exchange and structurally bonded within shrunken pores of said matrix.
6. A composition comprising a plurality of particles as defined in claim 5 in intimate association with a radiation-excitable phosphor.
7. A self-luminous article comprising a plastic material having therein a plurality of particles as defined in claim 5 in intimate association with a radiation-excitable phosphor.
8. As a new article source of radioactivity: a particle no larger than about 200 microns having a weatherresistant refractory devitrified matrix comprised essentially of at least one inorganic complex selected from the group consisting of titanium phosphate, zirconium phosphate, and hafnium phosphate, and containing a radioactive isotope dispersed in said matrix by ion exchange and firmly mechanically and substantially insolubly bound within shrunken pores of said matrix.
9. As new article sources of radioactivity: a mass of small spherical sealed sources of radioactivity having an average diameter smaller than microns, and each source comprising a radioactive isotope dispersed and substantially insolubly aixed within shrunken pores of a weather-resistant refractory matrix, said matrix being characterized by remaining as a discrete entity not bonded to like particles of identical matrix even when subjected to 1000 C. in contact with said like particles, and being characterized further by serving as a barrier against actual physical contact of the radioactive isotope entrapped therein, the chemical analysis of said matrix being such as to satisfy the requirements of the following table wherein amounts are set forth in mol percent:
Ti02 0-40 ZrOZ 0435 Hf02 0-35 TiOg-I-Zr02-i-Hf02 10-40 SiO?l -40 A1015 0-10 B015 0-25 P025 20-70 PO2 5-|B01,5 20-70 Fluxes 0-15 B015`[-fluxes 0-25 Total of listed ingredients 90-100 said uxes being selected from the group consisting of oxides of alkali and alkaline earth metals.
10. As new article sources of radioactivity: particles of small sealed sources of radioactivity having an average particle size greater than microns and smaller than 2 mm. in thickness, and each comprising a radioactive isotope dispersed and chemically and mechanically affixed within shrunken pores of a weather-resistant inorganicoxide refractory matrix, said matrix being infusible at temperatures below 1000 C. and serving as a barrier against actual physical contact of the radioactive isotope entrapped therein, the chemical analysis of said matrix satisfying the requirements of the following table wherein amounts are set forth in mol percent:
said uxes being selected from the group consisting of oxides of alkali and alkaline earth metals.
11. Method of preparing small sealed sources of radioactivity comprising (1) contacting a solution of radioactive cations in ion exchange relationship with small, leached, highly-porous, refractory, cation exchanging glassy articles infusible at temperatures below 1000 C., said glassy articles being comprised essentially of at least one inorganic complex selected from the group consisting of titanium phosphate, zirconium phosphate, and hafnium phosphate, (2) allowing a period of time for said radioactive cations to be adsorbed Within the pores of said glassy articles, then (3) heat-treating said articles to a temperature above 350 C. to shrink the pores of said articles and substantially insolubly aix the radioactive cations in the form of a radioactive isotope within said shrunken pores of said articles, and (4) washing said articles in acid water to remove from the outer exposed surfaces of said articles incidental radioactive cations 'l0 which may have been adsorbed on said outer surfaces during the time of conducting steps (1) and (2) aforesetforth.
l2. A composition comprising radiation-excitable phosphor in intimate association with particulate sources of radioactivity having a Weather-resistant inorganic-oxide refractory matrix and containing radioactive isotope for excitation of said phosphor, said radioactive isotope being dispersed in said matrix by ion exchange and structurally bonded within shrunken pores of said matrix, said matrix being at least partially devitriiied and characterized by an ability to withstand 1000 C. in contact with separate particles of identical matrix without sintering and without fusing to said separate particles of identical matrix, and said particulate sources of radioactivity being characterized by an ability to withstand water exposure for one Week at 50 C. with less than `0.1% Weight loss of said structurally bonded radioactive isotope.
13. A self-luminous article comprising a plastic material within which radiation-excitable phosphor is mixed with particulate sources of radioactivity having a weatherresistant inorganic-oxide refractory matrix and containing radioactive isotope adapted to excite said phosphor, said radioactive isotope being dispersed in said matrix by ion exchange and structurally bonded within shrunken pores of said matrix, said matrix being at least partially devitried and characterized by an ability to withstand 1000 C. in contact with separate particles of identical matrix without sintering and without fusing to said separate particles of identical matrix, and said particulate sources of radioactivity being characterized by an ability to withstand Water exposure for one week at 50 C. with less than 0.1% weight loss of said structurally bonded radioactive isotope.
References Cited in the le of this patent UNITED STATES PATENTS 789,812 Kunz May 16, 1905 1,202,625 Viol Oct. 24, 1916 1,210,731 Viol Jan. 2, 1917 2,106,744 Hood et al. Feb. 1, 1938 2,255,109 Fischer Sept. 9, 1941 2,303,756 Mordberg et al. Dec. 1, 1942 2,315,329 Hood et al. Mar. 30, 1943 2,361,319 Paul Oct. 24, 1944 2,378,328 Robinson et al. June 12, 1945 2,470,449 Williams May 17, 1949 2,510,795 Blau June 6, 1950 2,588,210 Crisman Mar. 4, 1952 2,616,847 Ginell Nov. 4, 1952 2,903,333 Lowe Sept. 8, 1959 2,928,780 Harteck et al Mar. 15, 1960 2,943,059 Beck et al. lune 28, 1960 OTHER REFERENCES AEC Document, TID-7550, pp. 1-14; Report on Working Meeting on Fixation of Radioactivity in Stable, Solid Media at the Johns Hopkins University, June 19-21, 1957.
Wallhausen: First Geneva Conference on Peaceful Uses of Atomic Energy, vol. 15, pp. 307-309.
Claims (1)
1. AS A NEW ARTICLE SOURCE OF RADIOACTIVITY: A PARTICLE HAVING A THICKNESS NO GREATER THAN 2 MM. AND CONSISTING ESENTIALLY OF A WEATHER-RESISTANT REFRACTORY MATRIX AT LEAST PARTIALLY DEVITRIFIED AND CHARACTERIZED BY REMAINING AS A DESCRETE ENTITY NOT BONDED TO A LIKE PARTICLE OF IDENTICAL MATRIX EVEN WHEN SUBJECTED TO 1000*C. IN CONTACT WITH SAID LIKE PARTICLE, AND A RADIOACTIVE ISOTOPE DISPERSED IN SAID MATRIX BY ION EXCHANGE AND STRUCTURALLY BONDED WITHIN SHRUNKEN PORES OF SAID MATRIX, SAID PARTICLE BEING CHARACTERIZED BY AN ABILITY TO WITHSTAND WATER EXPOSURE FOR ONE WEEK AT 50*C. WITH LESS THAN 0.1% WEIGHT LOSS OF SAID STRUCTRUALLY BONDED RADIOACTIVE ISOTOPE.
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US3230374A (en) * | 1962-12-18 | 1966-01-18 | Leroy V Jones | Radioactive radiation emitting sources |
US3264473A (en) * | 1963-06-26 | 1966-08-02 | Marquardt Corp | Radiation sterilization device with uniformly distributed beta emitters |
US3334050A (en) * | 1964-08-24 | 1967-08-01 | Minnesota Mining & Mfg | Organic carbonaceous matrix with radioisotope dispersed therein |
US3364148A (en) * | 1964-08-26 | 1968-01-16 | Atlantic Res Corp | High silica matrix radioactive source and method of preparation |
US3378498A (en) * | 1965-01-25 | 1968-04-16 | Metal Diffusions Ltd | Process for diffusing metal into a refractory or ceramic oxide using a nitrate promoter |
US3457181A (en) * | 1967-05-03 | 1969-07-22 | Susquehanna Corp | Methods of making sources of radioactive energy |
US3729690A (en) * | 1961-10-27 | 1973-04-24 | American Optical Corp | Means for producing and amplifying optical energy |
US4044315A (en) * | 1962-01-16 | 1977-08-23 | American Optical Corporation | Means for producing and amplifying optical energy |
US4214820A (en) * | 1978-09-15 | 1980-07-29 | Timex Corporation | Electrochromic display having enhanced night viewability |
US4224177A (en) * | 1978-03-09 | 1980-09-23 | Pedro B. Macedo | Fixation of radioactive materials in a glass matrix |
US4362659A (en) * | 1978-03-09 | 1982-12-07 | Pedro B. Macedo | Fixation of radioactive materials in a glass matrix |
US4505888A (en) * | 1983-05-27 | 1985-03-19 | E. I. Du Pont De Nemours & Company | Tracer for circulation determinations |
US4659512A (en) * | 1983-12-21 | 1987-04-21 | Pedro B. Macedo | Fixation of dissolved metal species with a complexing agent |
US4659477A (en) * | 1982-08-16 | 1987-04-21 | Pedro B. Macedo | Fixation of anionic materials with a complexing agent |
US4687581A (en) * | 1984-01-30 | 1987-08-18 | Pedro B. Macedo | Method of separating and purifying cations by ion exchange with regenerable porous glass |
US5011797A (en) * | 1988-01-29 | 1991-04-30 | The Curators Of The University Of Missouri | Composition and method for radiation synovectomy of arthritic joints |
US5480556A (en) * | 1991-07-01 | 1996-01-02 | Ulan; Judith G. | Trapping and sealing process |
US20070290170A1 (en) * | 2006-06-16 | 2007-12-20 | Ding Tuan-Jye | Method of increasing fluorescence intensity of oxide glass |
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US4659512A (en) * | 1983-12-21 | 1987-04-21 | Pedro B. Macedo | Fixation of dissolved metal species with a complexing agent |
US4687581A (en) * | 1984-01-30 | 1987-08-18 | Pedro B. Macedo | Method of separating and purifying cations by ion exchange with regenerable porous glass |
US5011797A (en) * | 1988-01-29 | 1991-04-30 | The Curators Of The University Of Missouri | Composition and method for radiation synovectomy of arthritic joints |
US5480556A (en) * | 1991-07-01 | 1996-01-02 | Ulan; Judith G. | Trapping and sealing process |
US20070290170A1 (en) * | 2006-06-16 | 2007-12-20 | Ding Tuan-Jye | Method of increasing fluorescence intensity of oxide glass |
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