WO1996013038A1 - Target for use in the production of molybdenum-99 - Google Patents

Target for use in the production of molybdenum-99 Download PDF

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Publication number
WO1996013038A1
WO1996013038A1 PCT/CA1995/000332 CA9500332W WO9613038A1 WO 1996013038 A1 WO1996013038 A1 WO 1996013038A1 CA 9500332 W CA9500332 W CA 9500332W WO 9613038 A1 WO9613038 A1 WO 9613038A1
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WIPO (PCT)
Prior art keywords
uranium
target
walls
oxide
members
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Application number
PCT/CA1995/000332
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French (fr)
Inventor
William T. Hancox
Jean-Pierre Labrie
Richard J. Harrison
Deonaraine Singh
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Atomic Energy Of Canada Limited/Energie Atomique Du Canada Limitee
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Publication date
Application filed by Atomic Energy Of Canada Limited/Energie Atomique Du Canada Limitee filed Critical Atomic Energy Of Canada Limited/Energie Atomique Du Canada Limitee
Priority to AU25591/95A priority Critical patent/AU2559195A/en
Publication of WO1996013038A1 publication Critical patent/WO1996013038A1/en

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    • GPHYSICS
    • G21NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21GCONVERSION OF CHEMICAL ELEMENTS; RADIOACTIVE SOURCES
    • G21G1/00Arrangements for converting chemical elements by electromagnetic radiation, corpuscular radiation or particle bombardment, e.g. producing radioactive isotopes
    • G21G1/02Arrangements for converting chemical elements by electromagnetic radiation, corpuscular radiation or particle bombardment, e.g. producing radioactive isotopes in nuclear reactors
    • GPHYSICS
    • G21NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21GCONVERSION OF CHEMICAL ELEMENTS; RADIOACTIVE SOURCES
    • G21G4/00Radioactive sources
    • G21G4/04Radioactive sources other than neutron sources
    • G21G4/06Radioactive sources other than neutron sources characterised by constructional features
    • G21G4/08Radioactive sources other than neutron sources characterised by constructional features specially adapted for medical application

Definitions

  • This invention is directed to the production of molybdenum-99 and, in particular a target for production of molybdenum-99.
  • Molybdenum-99 is the parent nucleus to technetium-99m (Tc- 99m).
  • Tc-99m is used in nuclear medicine for liver, kidney, lung, blood pool, thyroid and tumour scanning.
  • Tc-99m decays to a stable isotope, technetium-99, emitting a low energy gamma ray which can be detected outside the body and used to reconstruct the image of an organ.
  • Tc-99m is preferred over many other radio isotopes for nuclear medicine because of its short half-life of approximately 6 hours which results in reduced radiation exposure of organs relative to the exposure given by most other imaging radio isotopes.
  • Tc-99m Because of its short half-life Tc-99m must be produced just prior to administration. Tc-99m can be produced from its parent nucleus Mo-99 which has a half-life of approximately 66 hours. Mo-99 is produced by nuclear fission of uranium-235 (U-235). Production techniques for Mo-99 have been developed which yield a suitable product for use in nuclear medicine. However, current production techniques are complex and time consuming and result in considerable decay losses. In addition, current production techniques create large quantities of high level radioactive liquid waste, thus increasing production costs and reducing the suitability of such processes for large scale commercial production of Mo-99. A process for production of Mo-99 is required which reduces the amount of waste produced.
  • a target for use in Mo-99 production having high heat transfer will allow irradiation at high fluxes so that a high rate of fission is obtained.
  • Targets having high heat transfer have been proposed incorporating uranium embedded in an aluminum matrix typically containing 79% by weight of aluminum and 21% by weight of uranium.
  • the use of aluminum in the target presents serious disadvantages in the production of Mo-99.
  • the need to dissolve the aluminum matrix in order to obtain the uranium requires a considerable period of time, adding several hours to the production process. During this time, the radioactive materials are decaying and therefore final product is being lost.
  • the presence of dissolved aluminum in the solution complicates the separation steps and renders it difficult to obtain pure products.
  • Mercury is required as a catalyst in the process to remove aluminum. Mercury is of course toxic, and thereby adds to process hazard.
  • the relatively high volume of solution needed for dissolution of the large mass of aluminum results in corresponding large volumes of radioactive waste solution. This is difficult and expensive to store, and cannot easily be disposed of in a safe way.
  • targets consisting of closed cylinders in which uranium oxide or metal is electroplated about the inner surface.
  • the cylinder is made from stainless steel or zirconium alloy (zircaloy) and allows for a direct exposure of the irradiated uranium for processing.
  • zirconium alloy zircaloy
  • a target has been invented for production of Mo-99 having effective heat transfer without the use of aluminum and which is suitable for use in high power reactors.
  • a target for the production of Mo-99 comprising: a first outer wall member; a second outer wall member; and, a layer of substantially aluminum-free uranium or uranium oxide disposed therebetween, such that heat produced by fission of the uranium or uranium oxide is transferred directly to the first and the second outer wall members.
  • a process for producing a target for the production of Mo-99 comprising: loading substantially aluminum-free uranium or uranium oxide between a pair of walls such that the uranium or uranium oxide is in intimate contact with walls, and sealing the uranium or uranium oxide within the walls.
  • a target for the production of Mo-99 comprising: a first tubular member; a second tubular member arranged concentrically with the first member and a layer of substantially aluminum-free uranium or uranium oxide disposed therebetween, such that heat produced by fission of the uranium or uranium oxide is transferred directly to the first and second members.
  • Figure 1 shows a perspective, cutaway view of a target according to the present invention.
  • Figure 2 shows a perspective, cutaway view of another embodiment of a target according to the present invention.
  • Figure 3 shows a flow diagram of a process for using the target of the present invention.
  • the target of the present invention comprises a first wall member and a second wall member which sandwich a layer of uranium or uranium oxide therebetween.
  • the layer can be in the form of uranium oxides such as, U0 2 or U 3 O ⁇ , in powder form, uranium metal foil, uranium metal foil oxidized to U0 2 or electrodeposited U0 2 or U 3 0 8 .
  • the uranium or uranium oxide is highly enriched.
  • At least one of the outer wall members are in contact with the uranium or uranium oxide layer such that the target has effective heat transfer during fission.
  • Target 10 comprises a first wall member 12, a second wall member 14 and a layer of uranium 16 therebetween.
  • Wall members 12 and 14 are rolled to be in intimate contact with layer 16 to provide for effective heat transfer and to stabilize the uranium within the target. Edges 17 of wall members 12 and 14 are then sealed such as by welding.
  • Target 110 comprises an inner wall member 112, an outer wall member 114 and a layer of uranium oxide 116 therebetween. End caps 118 are provided to seal a gap formed between the wall members 112, 114 during loading of the uranium oxide.
  • Wall members are produced from any suitable material for use in nuclear reactor environments, such as, for example zirconium alloy. Stainless steel can be used but is not preferred because of its high neutron absorption when compared to zirconium alloy.
  • the members are preferably compressed about the layer, such as by rolling or swaging.
  • the uranium or uranium oxide is in close contact with at least one member and the target is helium filled to provide for heat transfer.
  • helium filling provides good heat transfer across small gaps, such as less than about 1 mm.
  • Heat transfer by means of helium filling is diminished substantially as the space between the wall members of the target is increased.
  • the outer wall members are adapted to facilitate exposure and dissolution of the layer after irradiation.
  • the zirconium alloy surfaces are anodized prior to application of the foil to facilitate removal of the foil after irradiation.
  • an annular target is 470 mm in length having an inner diameter of 13 mm and an outer diameter of 15 mm and has loaded therein about 20 g of uranium oxide.
  • uranium oxide in the form of a finely divided powder is vibration packed into an annular gap formed between the wail members.
  • a film of uranium oxide is electrodeposited onto the wall members.
  • uranium metal or oxidized uranium metal is disposed between the wall members.
  • the wall members are positioned such that a uniform annular gap of between about 0.10 and 0.20 mm is formed between the members.
  • the edges of the wall members are sealed to contain the powder, such as by insertion of end caps or welding, and the powder is vibration packed into the gap such as, for example, by use of a Syntron vibrator.
  • the outer walls are then rolled or swaged to compress the uranium oxide to the desired density of about 6.5 to 11 g/cm 3 and to cause the wall members to be in intimate contact with the uranium oxide.
  • a target is produced using electrodeposition by first washing one or both wail members in preparation for electrodeposition of the uranium oxide.
  • the uranium oxide is electrodeposited over the surface of the wall members such that it will be disposed between the wall members in the assembled target and such that a total amount of about 100 mg/cm 2 is disposed between the walls.
  • Such electrodeposition is affected by any known method suitable for uranium loading.
  • the uranium oxide can be electrodeposited by use of a bath containing 0.042 M uranyl nitrate and 0.125 M ammonium oxalate, the pH being adjusted to 7.2 with NH 4 OH.
  • Uranium is electrodeposited to suitable thicknesses by use of current of 0.9 amperes, 1.5 volts and a temperature of about 93 # C.
  • the wall member having the electrodeposited layer thereon is then heated to 500'C.
  • the walls are dipped in nitric acid to remove a portion of the uranium oxide such that a portion of the wall is exposed for sealing the target.
  • the walls are then positioned in close relation and preferably such that the space between the walls is less than about 0.2 mm.
  • the walls are then sealed at their edges and then pressed such as by rolling or swaging. Alternatively, the walls are sealed at their edges and the space between the walls is helium filled, to provide for good heat transfer.
  • a target having uranium metal or oxidized uranium metal foil therein is prepared by placing the foil between wall members which have, preferably, been anodized. The members are then rolled or swaged to provide intimate contact between the metal and the walls. The edges are sealed by any suitable means such as by welding.
  • the target can be of any suitable shape which will allow heat transfer through each wall member such as, for example, a plate assembly, as shown in Figure 1, an annular assembly, as shown in Figure 2, or other suitable shapes that provide for direct heat transfer from the uranium or uranium oxide through the walls to a heat sink or cooling fluid.
  • a plate assembly as shown in Figure 1
  • an annular assembly as shown in Figure 2
  • some targets generally as described in relation to Figure 2 have been successfully irradiated at target powers of 18.2 kW/g of U-235.
  • Steps 1 to 4 pertain to the irradiation of uranium oxide and recovery of Mo-99.
  • Steps 5 to 8 pertain to a process for management of a waste stream after Mo-99 recovery.
  • Mo-99 is produced by placement of a target containing uranium-235 into the irradiation zone of a nuclear reactor, particle generator or neutron particle source.
  • the target can be according to the present invention or, alternatively, any suitable target containing uranium or uranium oxide which is substantially free of aluminum. After a suitable period of irradiation, such as up to about 21 days, the target is removed and cooled for a suitable period such as, for example, for 2 to 16 hours.
  • the Mo-99 is recovered by a process comprising opening the target to expose the uranium and dissolving the uranium or uranium oxide in nitric acid solution.
  • Dissolution requires at least stoichiometric equivalents of nitric acid for each gram of uranium-235 irradiated. However, this may be increased depending on the form of uranium or uranium oxide used. For example, 5 to 40 ml of 2 to 16 N nitric acid are required to dissolve each gram of U-235, depending on the form of U-235 used. For example, powder forms of uranium oxide require the least amount of nitric acid. Where it is necessary to submerge the target, amounts greater than this may be required.
  • the volume of acid used should be as little as conveniently possible to provide dissolution. Immersion in the acid is maintained until the layer is dissolved.
  • the time for dissolution is not critical and should be optimized on a cost benefit analysis in terms of amount dissolved versus time spent. Gases released during exposure of the uranium or uranium oxide layer and dissolution thereof are collected for off-gas treatment.
  • the target is punctured to release fission products such as Xe-133 and 1-131 prior to target decladding and dissolution.
  • the target is removed from the acid solution and is managed as low level waste.
  • Mo-99 is recovered from the acid solution by contacting with an adsorbent.
  • the acid solution is passed at least once through an alumina column.
  • the alumina column useful in the preferred method is prepared by dissolving aluminum oxide in 1N nitric acid to form a slurry. A column packed with 150 ml to 250 ml of wet aluminum oxide is sufficient to absorb 100 to 2000 six day Ci of Mo- 99.
  • the alumina column containing adsorbed Mo-99 is passed to treatment for removal of Mo-99.
  • waste acid solution contains uranium nitrite.
  • waste is passed to a process wherein it is converted to solid uranium oxide.
  • the process includes de-watering, such as for example, by boiling, and heating to about 500 * C in the presence of oxygen to allow oxidation and calcination.
  • suitable time is provided prior to evaporation for decay of isotopes having a short-half life.
  • waste solution is passed to an evaporation cell, wherein it is boiled to remove the water, and then to a calciner where it is further heated to about 500 * C in the presence until solid uranium oxide and calx thereof is formed.
  • the waste solution is passed directly to a calciner where the process steps of evaporation and calcination can be combined.
  • Any suitable calciner can be used such as an in-pot calciner where temperatures are increased from 400 * C to 650'C, or a rotary calciner where calcination can be affected at temperatures of 400"C to 500 * C. Waste in the form of stable, ceramic-like uranium oxide calx is obtained by the process and is suitable for long term storage in sealed canisters.
  • U-235 target in the form of aluminum-uranium alloy (79% Al, 21% U) were irradiated for 10 days at 15.5 kW.
  • the targets were cooled and processed to recover Mo- 99.
  • the targets containing uranium oxide were opened and treated with 2 N nitric acid until completely dissolved.
  • the targets containing aluminum-uranium alloy was dissolved in 2 N nitric acid containing Hg(N0 3 ) 2 until completely dissolved.
  • the resulting solutions were passed though an alumina column to recover the Mo-99.
  • Target power (kW/g U-235) 6.46 3.28 Mo-99 yield from irradiation (Ci/g U-235) 229 140 Process time (hours) 28.5 21.0 Mo-99 yield from processing (Ci/g U-235) 153 101

Abstract

A target is taught for use in the production of Mo-99 from aluminum-free uranium. The target is formed so that the uranium is disposed between a pair of walls and thereby provides for efficient heat transfer during fission of the uranium. The target can be used in high power reactors where efficient heat transfer is essential.

Description

TARGET FOR USE IN THE PRODUCTION OF MOLYBDENUM-99
Field of the Invention
This invention is directed to the production of molybdenum-99 and, in particular a target for production of molybdenum-99.
Background of the Invention
Molybdenum-99 (Mo-99) is the parent nucleus to technetium-99m (Tc- 99m). Tc-99m is used in nuclear medicine for liver, kidney, lung, blood pool, thyroid and tumour scanning. Tc-99m decays to a stable isotope, technetium-99, emitting a low energy gamma ray which can be detected outside the body and used to reconstruct the image of an organ. Tc-99m is preferred over many other radio isotopes for nuclear medicine because of its short half-life of approximately 6 hours which results in reduced radiation exposure of organs relative to the exposure given by most other imaging radio isotopes.
Because of its short half-life Tc-99m must be produced just prior to administration. Tc-99m can be produced from its parent nucleus Mo-99 which has a half-life of approximately 66 hours. Mo-99 is produced by nuclear fission of uranium-235 (U-235). Production techniques for Mo-99 have been developed which yield a suitable product for use in nuclear medicine. However, current production techniques are complex and time consuming and result in considerable decay losses. In addition, current production techniques create large quantities of high level radioactive liquid waste, thus increasing production costs and reducing the suitability of such processes for large scale commercial production of Mo-99. A process for production of Mo-99 is required which reduces the amount of waste produced. A target for use in Mo-99 production having high heat transfer will allow irradiation at high fluxes so that a high rate of fission is obtained. Targets having high heat transfer have been proposed incorporating uranium embedded in an aluminum matrix typically containing 79% by weight of aluminum and 21% by weight of uranium. However, the use of aluminum in the target presents serious disadvantages in the production of Mo-99. The need to dissolve the aluminum matrix in order to obtain the uranium requires a considerable period of time, adding several hours to the production process. During this time, the radioactive materials are decaying and therefore final product is being lost. Moreover, the presence of dissolved aluminum in the solution complicates the separation steps and renders it difficult to obtain pure products. Mercury is required as a catalyst in the process to remove aluminum. Mercury is of course toxic, and thereby adds to process hazard. The relatively high volume of solution needed for dissolution of the large mass of aluminum results in corresponding large volumes of radioactive waste solution. This is difficult and expensive to store, and cannot easily be disposed of in a safe way.
Other targets are known consisting of closed cylinders in which uranium oxide or metal is electroplated about the inner surface. The cylinder is made from stainless steel or zirconium alloy (zircaloy) and allows for a direct exposure of the irradiated uranium for processing. However, such targets are useful only in low power reactors since heat transfer is a problem at higher powers.
Summary of the Invention
A target has been invented for production of Mo-99 having effective heat transfer without the use of aluminum and which is suitable for use in high power reactors.
In accordance with a broad aspect of the present invention there is provided a target for the production of Mo-99 comprising: a first outer wall member; a second outer wall member; and, a layer of substantially aluminum-free uranium or uranium oxide disposed therebetween, such that heat produced by fission of the uranium or uranium oxide is transferred directly to the first and the second outer wall members.
In accordance with a further broad aspect of the present invention, there is provided a process for producing a target for the production of Mo-99 comprising: loading substantially aluminum-free uranium or uranium oxide between a pair of walls such that the uranium or uranium oxide is in intimate contact with walls, and sealing the uranium or uranium oxide within the walls.
In accordance with a further broad aspect of the present invention, there is provided a target for the production of Mo-99 comprising: a first tubular member; a second tubular member arranged concentrically with the first member and a layer of substantially aluminum-free uranium or uranium oxide disposed therebetween, such that heat produced by fission of the uranium or uranium oxide is transferred directly to the first and second members.
Brief Description of the Drawings
A further, detailed, description of the invention, briefly described above, will follow by reference to the following drawings of specific embodiments of the invention, which depict only typical embodiments of the invention and are therefore not to be considered limiting of its scope. In the drawings:
Figure 1 shows a perspective, cutaway view of a target according to the present invention; and,
Figure 2 shows a perspective, cutaway view of another embodiment of a target according to the present invention; and,
Figure 3 shows a flow diagram of a process for using the target of the present invention.
Detailed Description of the Present Invention
The target of the present invention comprises a first wall member and a second wall member which sandwich a layer of uranium or uranium oxide therebetween. The layer can be in the form of uranium oxides such as, U02 or U3Oθ, in powder form, uranium metal foil, uranium metal foil oxidized to U02 or electrodeposited U02 or U308. In a preferred embodiment, the uranium or uranium oxide is highly enriched. At least one of the outer wall members are in contact with the uranium or uranium oxide layer such that the target has effective heat transfer during fission.
Referring to Figure 1 there is shown a view of a target 10 according to the present invention, cutaway to reveal its inner contents. Target 10 comprises a first wall member 12, a second wall member 14 and a layer of uranium 16 therebetween. Wall members 12 and 14 are rolled to be in intimate contact with layer 16 to provide for effective heat transfer and to stabilize the uranium within the target. Edges 17 of wall members 12 and 14 are then sealed such as by welding.
Referring to Figure 2 there is shown a view of another target 110 according to the present invention. Target 110 comprises an inner wall member 112, an outer wall member 114 and a layer of uranium oxide 116 therebetween. End caps 118 are provided to seal a gap formed between the wall members 112, 114 during loading of the uranium oxide.
Wall members are produced from any suitable material for use in nuclear reactor environments, such as, for example zirconium alloy. Stainless steel can be used but is not preferred because of its high neutron absorption when compared to zirconium alloy. To provide close contact between the uranium or uranium oxide layer and the wall members and, thereby, effective heat transfer during fission, the members are preferably compressed about the layer, such as by rolling or swaging. In an alternate embodiment, the uranium or uranium oxide is in close contact with at least one member and the target is helium filled to provide for heat transfer. However, it is to be noted that helium filling provides good heat transfer across small gaps, such as less than about 1 mm. Heat transfer by means of helium filling is diminished substantially as the space between the wall members of the target is increased. The outer wall members are adapted to facilitate exposure and dissolution of the layer after irradiation. For example, where uranium foil is used, the zirconium alloy surfaces are anodized prior to application of the foil to facilitate removal of the foil after irradiation.
The uranium or uranium oxide is loaded between the wall members in a thin layer and in an amount to give the desired power level such as for example about 100 mg/cm2 and, thereby, the desired Mo-99 production. In a preferred embodiment, an annular target, generally as shown in Figure 2, is 470 mm in length having an inner diameter of 13 mm and an outer diameter of 15 mm and has loaded therein about 20 g of uranium oxide.
In an embodiment, uranium oxide in the form of a finely divided powder is vibration packed into an annular gap formed between the wail members. In an another embodiment, a film of uranium oxide is electrodeposited onto the wall members. In still another embodiment, uranium metal or oxidized uranium metal is disposed between the wall members.
To produce a target having a packed powder layer of uranium oxide, the wall members are positioned such that a uniform annular gap of between about 0.10 and 0.20 mm is formed between the members. The edges of the wall members are sealed to contain the powder, such as by insertion of end caps or welding, and the powder is vibration packed into the gap such as, for example, by use of a Syntron vibrator. The outer walls are then rolled or swaged to compress the uranium oxide to the desired density of about 6.5 to 11 g/cm3 and to cause the wall members to be in intimate contact with the uranium oxide.
A target is produced using electrodeposition by first washing one or both wail members in preparation for electrodeposition of the uranium oxide. The uranium oxide is electrodeposited over the surface of the wall members such that it will be disposed between the wall members in the assembled target and such that a total amount of about 100 mg/cm2 is disposed between the walls. Such electrodeposition is affected by any known method suitable for uranium loading. For example, the uranium oxide can be electrodeposited by use of a bath containing 0.042 M uranyl nitrate and 0.125 M ammonium oxalate, the pH being adjusted to 7.2 with NH4OH. Uranium is electrodeposited to suitable thicknesses by use of current of 0.9 amperes, 1.5 volts and a temperature of about 93#C. The wall member having the electrodeposited layer thereon is then heated to 500'C.
After electrodeposition, the walls are dipped in nitric acid to remove a portion of the uranium oxide such that a portion of the wall is exposed for sealing the target. The walls are then positioned in close relation and preferably such that the space between the walls is less than about 0.2 mm. The walls are then sealed at their edges and then pressed such as by rolling or swaging. Alternatively, the walls are sealed at their edges and the space between the walls is helium filled, to provide for good heat transfer.
A target having uranium metal or oxidized uranium metal foil therein is prepared by placing the foil between wall members which have, preferably, been anodized. The members are then rolled or swaged to provide intimate contact between the metal and the walls. The edges are sealed by any suitable means such as by welding.
The target can be of any suitable shape which will allow heat transfer through each wall member such as, for example, a plate assembly, as shown in Figure 1, an annular assembly, as shown in Figure 2, or other suitable shapes that provide for direct heat transfer from the uranium or uranium oxide through the walls to a heat sink or cooling fluid. As an example, some targets generally as described in relation to Figure 2, have been successfully irradiated at target powers of 18.2 kW/g of U-235.
Referring to Figure 3, a flow diagram of a preferred process for production of Mo-99 and management of the waste produced therefrom is shown. Steps 1 to 4 pertain to the irradiation of uranium oxide and recovery of Mo-99. Steps 5 to 8 pertain to a process for management of a waste stream after Mo-99 recovery.
Mo-99 is produced by placement of a target containing uranium-235 into the irradiation zone of a nuclear reactor, particle generator or neutron particle source. The target can be according to the present invention or, alternatively, any suitable target containing uranium or uranium oxide which is substantially free of aluminum. After a suitable period of irradiation, such as up to about 21 days, the target is removed and cooled for a suitable period such as, for example, for 2 to 16 hours.
The Mo-99 is recovered by a process comprising opening the target to expose the uranium and dissolving the uranium or uranium oxide in nitric acid solution. Dissolution requires at least stoichiometric equivalents of nitric acid for each gram of uranium-235 irradiated. However, this may be increased depending on the form of uranium or uranium oxide used. For example, 5 to 40 ml of 2 to 16 N nitric acid are required to dissolve each gram of U-235, depending on the form of U-235 used. For example, powder forms of uranium oxide require the least amount of nitric acid. Where it is necessary to submerge the target, amounts greater than this may be required. To reduce the amount of waste produced the volume of acid used should be as little as conveniently possible to provide dissolution. Immersion in the acid is maintained until the layer is dissolved. The time for dissolution is not critical and should be optimized on a cost benefit analysis in terms of amount dissolved versus time spent. Gases released during exposure of the uranium or uranium oxide layer and dissolution thereof are collected for off-gas treatment. In an embodiment, the target is punctured to release fission products such as Xe-133 and 1-131 prior to target decladding and dissolution.
After the uranium or uranium oxide has dissolved, the target is removed from the acid solution and is managed as low level waste. Mo-99 is recovered from the acid solution by contacting with an adsorbent. In an embodiment, the acid solution is passed at least once through an alumina column. The alumina column useful in the preferred method is prepared by dissolving aluminum oxide in 1N nitric acid to form a slurry. A column packed with 150 ml to 250 ml of wet aluminum oxide is sufficient to absorb 100 to 2000 six day Ci of Mo- 99. The alumina column containing adsorbed Mo-99 is passed to treatment for removal of Mo-99.
After recovery of Mo-99, waste acid solution remains which contains uranium nitrite. Such waste is passed to a process wherein it is converted to solid uranium oxide. The process includes de-watering, such as for example, by boiling, and heating to about 500*C in the presence of oxygen to allow oxidation and calcination. In a preferred embodiment, suitable time is provided prior to evaporation for decay of isotopes having a short-half life.
In one embodiment, waste solution is passed to an evaporation cell, wherein it is boiled to remove the water, and then to a calciner where it is further heated to about 500*C in the presence until solid uranium oxide and calx thereof is formed. Alternately, the waste solution is passed directly to a calciner where the process steps of evaporation and calcination can be combined.
Any suitable calciner can be used such as an in-pot calciner where temperatures are increased from 400*C to 650'C, or a rotary calciner where calcination can be affected at temperatures of 400"C to 500*C. Waste in the form of stable, ceramic-like uranium oxide calx is obtained by the process and is suitable for long term storage in sealed canisters.
Examples
Four targets, generally as shown in Figure 2, containing 18.5 g of U- 235 target in the form of highly enriched uranium oxide powder were irradiated for
10 days at a target power of 60.7 kW. Similarly, sixteen targets containing 2.4 g of
U-235 target in the form of aluminum-uranium alloy (79% Al, 21% U) were irradiated for 10 days at 15.5 kW.
After irradiation, the targets were cooled and processed to recover Mo- 99. The targets containing uranium oxide were opened and treated with 2 N nitric acid until completely dissolved. The targets containing aluminum-uranium alloy was dissolved in 2 N nitric acid containing Hg(N03)2 until completely dissolved. The resulting solutions were passed though an alumina column to recover the Mo-99.
Liquid waste remaining after the recovery was allowed decay time followed by evaporation and calcination. Results are shown in Table I.
Table I
Process Parameters Al-U UC
Target power (kW/g U-235) 6.46 3.28 Mo-99 yield from irradiation (Ci/g U-235) 229 140 Process time (hours) 28.5 21.0 Mo-99 yield from processing (Ci/g U-235) 153 101
Volume liquid waste/g U-235 (ml) 200 18 Volume of calcined waste/g U-235 (ml) 13 1.3
The target of the offers faster process time over previous Al-containing targets. Thus, less Mo-99 is lost due to decay during processing. It will be apparent that many other changes may be made to the illustrative embodiments, while falling within the scope of the invention and it is intended that all such changes be covered by the claims appended hereto.

Claims

THE EMBODIMENTS OF THE INVENTION IN WHICH AN EXCLUSIVE PROPERTY OR PRIVILEGE IS CLAIMED ARE DEFINED AS FOLLOWS:
1. A target for the production of Mo-99 comprising: a first outer wall member; a second outer wall member; and, a layer of substantially aluminum-free uranium or uranium oxide disposed therebetween, such that heat produced by fission of the uranium or uranium oxide is transferred directly to the first and the second outer wall members.
2. The target of claim 1 wherein the uranium is uranium metal.
3. The target of claim 2 wherein the uranium metal is oxidized.
4. The target of claim 1 wherein the uranium oxide is a powder and is compressed between the tubular members by swaging.
5. The target of claim 1 wherein the uranium oxide is electrodeposited onto at least one of the members.
6. The target of claim 1 wherein the members are formed of zirconium alloy.
7. A target for the production of Mo-99 comprising: a first tubular member; a second tubular member arranged concentrically with the first member; and, a layer of substantially aluminum-free uranium or uranium oxide disposed therebetween, such that heat produced by fission of the uranium or uranium oxide is transferred directly to the first and second members.
8. The target of claim 7 wherein the uranium is uranium metal.
9. The target of claim 8 wherein the uranium metal is oxidized.
10. The target of claim 7 wherein the uranium oxide is a powder and is compressed between the tubular members by swaging.
11. The target of claim 7 wherein the uranium oxide is electrodeposited onto at least one of the members.
12. The target of claim 7 wherein the members are formed of zirconium alloy.
13. A process for producing a target for the production of Mo-99 comprising: loading substantially aluminum-free uranium or uranium oxide between a pair of walls such that the uranium or uranium oxide is in intimate contact with at least one of the walls, and sealing the uranium or uranium oxide within the walls.
14. The process of claim 13 wherein the uranium oxide is a powder and is loaded between the walls by means of vibration packing.
15. The process of claim 14 wherein the walls are compressed about the uranium oxide powder.
16. The process of claim 13 wherein the uranium oxide is electrodeposited onto at least one of the members.
17. The process of claim 16 wherein the walls are compressed about the uranium oxide.
18. The process of claim 13 further comprising helium-filling the target.
19. The process of claim 13 wherein the uranium is uranium metal.
20. The process of claim 19 wherein the uranium metal is oxidized.
21. The process of claim 13 wherein the walls are formed of zirconium alloy.
22. The process of claim 21 wherein the walls are formed as plates.
23. The process of claim 21 wherein the walls are formed as tubular members and are arranged concentrically.
24. The process of claim 13 wherein the uranium is sealed within the walls by means of end caps.
25. The process of claim 13 wherein the uranium is sealed within the walls by means of welding the walls together at their edges.
PCT/CA1995/000332 1994-10-25 1995-06-07 Target for use in the production of molybdenum-99 WO1996013038A1 (en)

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CN103038831A (en) * 2010-07-29 2013-04-10 由俄勒冈州高等教育管理委员会代表的俄勒冈州立大学 Isotope production target
AU2011282744B2 (en) * 2010-07-29 2014-11-06 The State Of Oregon Acting By And Through The State Board Of Higher Education On Behalf Of Oregon State University Isotope production target
US9396826B2 (en) 2010-07-29 2016-07-19 Oregon State University Isotope production target
AU2015200445B2 (en) * 2010-07-29 2016-11-03 The State Of Oregon Acting By And Through The State Board Of Higher Education On Behalf Of Oregon State University Isotope production target
CN114540828A (en) * 2022-03-23 2022-05-27 中国原子能科学研究院 Method for electrodepositing uranium on metal surface
CN115449764A (en) * 2022-09-14 2022-12-09 中国工程物理研究院材料研究所 Actinide alloy gradient film and preparation method thereof
CN115449764B (en) * 2022-09-14 2023-09-01 中国工程物理研究院材料研究所 Actinide alloy gradient film and preparation method thereof

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AU2559195A (en) 1996-05-15
ZA958981B (en) 1996-05-23

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