CA1079093A - Zirconium-base alloy nuclear fuel container and method - Google Patents
Zirconium-base alloy nuclear fuel container and methodInfo
- Publication number
- CA1079093A CA1079093A CA241,901A CA241901A CA1079093A CA 1079093 A CA1079093 A CA 1079093A CA 241901 A CA241901 A CA 241901A CA 1079093 A CA1079093 A CA 1079093A
- Authority
- CA
- Canada
- Prior art keywords
- per cent
- zirconium
- base alloy
- beryllium
- irradiated
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
- 229910045601 alloy Inorganic materials 0.000 title claims abstract description 24
- 239000000956 alloy Substances 0.000 title claims abstract description 24
- 239000003758 nuclear fuel Substances 0.000 title description 11
- 238000000034 method Methods 0.000 title description 8
- 229910052790 beryllium Inorganic materials 0.000 claims abstract description 14
- ATBAMAFKBVZNFJ-UHFFFAOYSA-N beryllium atom Chemical compound [Be] ATBAMAFKBVZNFJ-UHFFFAOYSA-N 0.000 claims abstract description 14
- 230000000704 physical effect Effects 0.000 claims description 4
- 230000009467 reduction Effects 0.000 claims description 2
- 230000004907 flux Effects 0.000 abstract description 6
- QCWXUUIWCKQGHC-UHFFFAOYSA-N Zirconium Chemical compound [Zr] QCWXUUIWCKQGHC-UHFFFAOYSA-N 0.000 abstract description 5
- 229910052726 zirconium Inorganic materials 0.000 abstract description 3
- 239000000446 fuel Substances 0.000 description 16
- 238000005253 cladding Methods 0.000 description 15
- 238000005260 corrosion Methods 0.000 description 11
- 230000007797 corrosion Effects 0.000 description 9
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 9
- PXHVJJICTQNCMI-UHFFFAOYSA-N Nickel Chemical compound [Ni] PXHVJJICTQNCMI-UHFFFAOYSA-N 0.000 description 8
- ZCYVEMRRCGMTRW-UHFFFAOYSA-N 7553-56-2 Chemical compound [I] ZCYVEMRRCGMTRW-UHFFFAOYSA-N 0.000 description 7
- 239000012298 atmosphere Substances 0.000 description 7
- 238000009835 boiling Methods 0.000 description 7
- 239000011630 iodine Substances 0.000 description 7
- 229910052740 iodine Inorganic materials 0.000 description 7
- 229910001093 Zr alloy Inorganic materials 0.000 description 6
- 238000010438 heat treatment Methods 0.000 description 6
- 239000000463 material Substances 0.000 description 6
- 238000007792 addition Methods 0.000 description 5
- 238000010791 quenching Methods 0.000 description 5
- 230000009466 transformation Effects 0.000 description 5
- XKRFYHLGVUSROY-UHFFFAOYSA-N Argon Chemical compound [Ar] XKRFYHLGVUSROY-UHFFFAOYSA-N 0.000 description 4
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 4
- 239000007789 gas Substances 0.000 description 4
- 239000001307 helium Substances 0.000 description 4
- 229910052734 helium Inorganic materials 0.000 description 4
- 229910052759 nickel Inorganic materials 0.000 description 4
- 239000002826 coolant Substances 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 3
- 230000008569 process Effects 0.000 description 3
- 230000000171 quenching effect Effects 0.000 description 3
- 230000005855 radiation Effects 0.000 description 3
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 2
- 229910052786 argon Inorganic materials 0.000 description 2
- 230000008901 benefit Effects 0.000 description 2
- 229910052742 iron Inorganic materials 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 230000007935 neutral effect Effects 0.000 description 2
- OYPRJOBELJOOCE-UHFFFAOYSA-N Calcium Chemical compound [Ca] OYPRJOBELJOOCE-UHFFFAOYSA-N 0.000 description 1
- 229910052684 Cerium Inorganic materials 0.000 description 1
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 1
- 229910052777 Praseodymium Inorganic materials 0.000 description 1
- 238000009825 accumulation Methods 0.000 description 1
- 238000000137 annealing Methods 0.000 description 1
- 230000000712 assembly Effects 0.000 description 1
- 238000000429 assembly Methods 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 229910052791 calcium Inorganic materials 0.000 description 1
- 239000011575 calcium Substances 0.000 description 1
- GWXLDORMOJMVQZ-UHFFFAOYSA-N cerium Chemical compound [Ce] GWXLDORMOJMVQZ-UHFFFAOYSA-N 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
- 239000011651 chromium Substances 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000005097 cold rolling Methods 0.000 description 1
- 239000000470 constituent Substances 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000005336 cracking Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 230000001627 detrimental effect Effects 0.000 description 1
- 238000010891 electric arc Methods 0.000 description 1
- 229910000765 intermetallic Inorganic materials 0.000 description 1
- 229910052746 lanthanum Inorganic materials 0.000 description 1
- FZLIPJUXYLNCLC-UHFFFAOYSA-N lanthanum atom Chemical compound [La] FZLIPJUXYLNCLC-UHFFFAOYSA-N 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 230000003071 parasitic effect Effects 0.000 description 1
- 239000008188 pellet Substances 0.000 description 1
- PUDIUYLPXJFUGB-UHFFFAOYSA-N praseodymium atom Chemical compound [Pr] PUDIUYLPXJFUGB-UHFFFAOYSA-N 0.000 description 1
- 230000002028 premature Effects 0.000 description 1
- 230000002035 prolonged effect Effects 0.000 description 1
- 238000005204 segregation Methods 0.000 description 1
- 230000008961 swelling Effects 0.000 description 1
- 238000000844 transformation Methods 0.000 description 1
- 230000001131 transforming effect Effects 0.000 description 1
- 239000011800 void material Substances 0.000 description 1
- 229910052727 yttrium Inorganic materials 0.000 description 1
- VWQVUPCCIRVNHF-UHFFFAOYSA-N yttrium atom Chemical compound [Y] VWQVUPCCIRVNHF-UHFFFAOYSA-N 0.000 description 1
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- Monitoring And Testing Of Nuclear Reactors (AREA)
Abstract
Abstract of the Disclosure A fast neutron-irradiated zirconium-base alloy body having load-carrying capacity substantially greater than similar conventional zirconium-base alloy bodies like-wise irradiated is produced by subjecting a body heat treated at 930°C and then water-quenched and containing 0.2 weight per cent beryllium and at least 95 weight per cent zirconium to integrated neutron flux approximating 1.2 x 1021 nvt while maintaining the body at about 330°C.
Description
1~79093 ZIRCONIUM-BASE ALLOY NUCLEAR FUEL CONTAINER AND METHOD
The present invention relates generally to materials of contruction of nuclear reactors and is more particularly concerned with a novel zirconium-base alloy nuclear reactor structural member or body having unique corrosion resistance, ductility and load-carrying capacity (resistance to stress corrosion) and possibly corrosion resistance in the irradiated condition.
CROSS REFERENCE
This invention is related to that disclosed and claimed in Canadian patent application Serial No. 241,879, filed December 11, 1975 in the names of Rodney E. Hanneman, Daeyong Lee and Craig S. Tedmon, Jr., which is based on the concept that a small amount of lanthanum or praseodymium will substantially improve the slow strain rate ductility of certain zirconium-base alloys and on the additional concept that these new zirconium alloys and certain others in the irradiated condition can under certain circumstances have surprising load-carrying capacity.
BACKGROUND OF THE INVENTION
_ _ Important requirements for materials used in boiling water nuclear reactor construction include low ~7~3093 absorption for thermal neutrons, corrosion and stress corrosion resistance and mechanical strength. Zirconium-base alloys sufficiently satisfy these requirements that they are widely used for such purposes, "Zircaloy-2"
(containing about 1.5 per cent tin, 0.15 per cent iron, 0.1 per cent chromium, 0.05 per cent nickel and 0.1 per cent oxygen) and "Zircaloy-4" (containing substantially no nickel but otherwise similar to Zircaloy-2) being two of the important commercial alloys commonly finding such use. These alloys, however, are not nearly all that one would desire, particularly in respect to useful service life, despite many efforts of others during the past two decades to improve them.
Mainly, these efforst have been aimed at improving corrosion resistance and usually this has involved changes in composition. Thus, in U.S. Patent 3,005,706, it is proposed that from 0.03 to 1.0 per cent of beryllium be added to zirconium alloys intended for use in conventional boilers, boiling water reactors and similar apparatus. Similarly, in U.S. Patents 3,261,682 and 3,150,972, cerium and/or yttrium additions and a calcium addition, respectively, are proposed as zirconium alloy additions in like proportions for the same purpose. Accounts and reports of the results of such compositional changes are sparse, however, and the present commercial alloys do not include and of these additional constituents.
The present invention relates generally to materials of contruction of nuclear reactors and is more particularly concerned with a novel zirconium-base alloy nuclear reactor structural member or body having unique corrosion resistance, ductility and load-carrying capacity (resistance to stress corrosion) and possibly corrosion resistance in the irradiated condition.
CROSS REFERENCE
This invention is related to that disclosed and claimed in Canadian patent application Serial No. 241,879, filed December 11, 1975 in the names of Rodney E. Hanneman, Daeyong Lee and Craig S. Tedmon, Jr., which is based on the concept that a small amount of lanthanum or praseodymium will substantially improve the slow strain rate ductility of certain zirconium-base alloys and on the additional concept that these new zirconium alloys and certain others in the irradiated condition can under certain circumstances have surprising load-carrying capacity.
BACKGROUND OF THE INVENTION
_ _ Important requirements for materials used in boiling water nuclear reactor construction include low ~7~3093 absorption for thermal neutrons, corrosion and stress corrosion resistance and mechanical strength. Zirconium-base alloys sufficiently satisfy these requirements that they are widely used for such purposes, "Zircaloy-2"
(containing about 1.5 per cent tin, 0.15 per cent iron, 0.1 per cent chromium, 0.05 per cent nickel and 0.1 per cent oxygen) and "Zircaloy-4" (containing substantially no nickel but otherwise similar to Zircaloy-2) being two of the important commercial alloys commonly finding such use. These alloys, however, are not nearly all that one would desire, particularly in respect to useful service life, despite many efforts of others during the past two decades to improve them.
Mainly, these efforst have been aimed at improving corrosion resistance and usually this has involved changes in composition. Thus, in U.S. Patent 3,005,706, it is proposed that from 0.03 to 1.0 per cent of beryllium be added to zirconium alloys intended for use in conventional boilers, boiling water reactors and similar apparatus. Similarly, in U.S. Patents 3,261,682 and 3,150,972, cerium and/or yttrium additions and a calcium addition, respectively, are proposed as zirconium alloy additions in like proportions for the same purpose. Accounts and reports of the results of such compositional changes are sparse, however, and the present commercial alloys do not include and of these additional constituents.
-2-, ~, .
The literature in this field, however, contains little concerning efforts to improve upon the mechanical strength of zirconium-base alloys and particularly the load-carrying capacity of fuel cladding and other reactor parts subjected to prolonged exposure to typical boiling water reactor conditions. This is in spite of the fact that it has long been general knowledge that slow strain rate ductility of these alloys is lost to a great extent as a result of radiation exposure over periods of a year or more. The problem of premature termination of service life because of fast neutron radiation-induced embrittlement is particularly aggravated in the case of nuclear fuel containment channels and tubes or cladding. The natural swelling of the fuel as it is burned produced high localized stresses leading to stress--corrosion cracking of the cladding at a time before corrosion of the type described in the above patents might normally necessitate cladding replacement.
; THE INVENTION
This invention, which is predicated on my discovery and new concept to be described, provides an answer to both the iodine stress-corrosion problem and the embrittlement problem in the form of a process which can result in doubl1ng the length of the service life of ~' ' : , 1~79~)93 zirconium-base alloy nuclear fuel cladding. Moreover, this result is obtained without incurring any significant offsetting cost or performance disadvantage.
My discovery is that a zirconium-base alloy of the kind presently used in nuclear reactors will have a much greater load-carrying capacity after being subiected to fast neutron radiation for a period of a year or so if it contains from 0.05 to 0.25 per cent beryllium. More specifically, such an alloy will characteristically exhibit S00 to 600 per cent greater load-carrying capacity ti.e., uniform strain to maximum load) than conventional beryllium-free cladding and can therefore be expected to serve in that use and environment much longer and possibly twice as long as the zirconium-base alloys in general use in nuclear reactors.
My new concept is to prepare a zirconium-base alloy containing o.n5 to 0.25 per cent beryllium for use as nuclear fuel cladding by heating to a temperature of the order of 900C and then water-quenching it. Although such heat treatment results in a phase transformation, the zirconium alloy transforming in part or totally from the alpha to the beta phase, and the prior art warns that detrimental effects on mechanical properties will result, I have found that there are substantial advantages to be gained by effecting such transformation. For one thing, , ~ 4_ :
1079093 RD-724~
ductility is enhanced materially, as will subsequently be described in more detail. For another, resistance to corrosion under boiling water nuclear reactor conditions resulting in heavy oxide coating formation on fuel cladding may thereby he substantially reduced or limited.
In its method aspect, this invention in brief description includes the steps of forming a zirconium-base alloy body containing 0.05 to 0.25 per cent beryllium, heating the body to a temperature above 900C and then quenching, and finally subjecting the body to boiling water reactor conditions for a long period of time such as a year or more. More specifically, the alloy body will be of at least ~5 percent zirconium, the quenching will be done with water and the nuclear reactor conditions will be a temperature of about 325C and a fast-neutron flux of l.O to 10.0 x 1021 nvt.
In its product or article aspect, this invention takes the form of a zirconium-base alloy body of substantially greater load-carrying capacity than similar conventional bodies of the alloy irradiated in the same way and to the same extent and having at 325C an unique combination of physical properties including 2.5 per cent uniform ~ 5 ~
~ ,. .
-: - ~ . ' , -. ~ ., . -~079093 elongation, 8.2 per cent total elongation and 35 per cent ~ area reduction, yield strength greater than 76,000 psi, ~ and tensile strength greather than 80,000 psi. In more specific terms, the body is a nuclear fuel container for use in a nuclear reactor, and is in the form of a tube having microstructure in which the intermetallic phase is to some extent segregated at the grain boundaries as a consequence of the heat treatment and quenching steps stated above. Additionally, the fuel container or cladding is irradiated as a result of having been subjected for a long period to fast-neutron flux and has greater load-carrying capacity than a counterpart fuel container similarly irradiated but containing no beryllium.
DESCRIPTION OF THE DRAWINGS
Figure 1 presents a partial cutaway sectional view of a nuclear fuel assembly containing nuclear fuel elements constructed according to the teaching of this invention, Figure 2 is a chart bearing curves illustrating : 20 physical property data obtained in tests of the new product of this invention and the corresponding prior art product, and Figure 3 is another chart on which stress is plotted against strain and the curves illustrate data taken in tests perforred under an iodine atmosphere.
~79093 DETAILED DESCRIPTION OF THE INVENTION
-As indicated by Figure 1, a primary application of the present invention is for the fabrication of nuclear fuel assemblies such as that illustrated at 10 consisting of a tubular flow channel 11 of generally square cross section provided at its upper end with lifting bale 12 and at its lower end with a nose piece (not shown due to the lower portion of assembly 10 being omitted). The upper end of channel 11 is open at 13 and the lower end of the nose piece is provided with coolant flow openings. An array of fuel elements or rods 14 is enclosed in channel 11 and supported therein by means of upper end plate 15 and a lower end plate (not shown due to the lower portion being omitted). The liquid coolant ordinarily enters through the openings in the lower end of the nose piece, passes upwardly around fuel elements 14, and discharges at upper outlet 13 in a partially vaporized condition for boiling water reactors or in an unvaporized condition for pressurized reactors at an elevated temperature.
The nuclear fuel elements or rods 14 are sealed at their ends by means of end plugs 18 welded to the cladding 17, which may include studs 19 to facilitate the mounting of the fuel rod in the assembly. A void space or plenum 20 is provided at one end of the element to permit longitudinal expansion of the fuel material and accumulation .... . . , ,, . . . ~ .
.
.
1~9~93 of gases released from the fuel material. A nuclear fuel material retainer means 24 in the form of a helical member is positioned within space 20 to provide restraint against the axial movement of the pellet column, especially during handling and transportation of the fuel element.
The fuel element is designed to provide an excellent thermal contact between the cladding and the fuel material, a minimum of parasitic neutron absorption, and resistance to bowing and vibration which is occasionally caused by flow of the coolant at high velocity.
Cladding 17 is produced in accordance with this invention by a process which includes in addition to the usual tube-forming operations a heat treatment in argon or other inert atmosphere above the alpha--alpha plus beta transformation temperature followed by a water quench. The rate at which the work piece is heated up to the trans-formation temperature range is a matter of choice, but the time it is maintained in that range is preferably about ' 30 seconds and the cooling rate down to 700 to 750C may ', 20 be as low as 50C per second. As so treated, the zirconium alloy body is made more easily workable and forming operations are facilitated through the warm-working stage. It also ; appears, as indicated above, that the physical properties and particularly the ductility of the ultimate cladding product may be considerably enhanced in this manner. As a ., :
' .
1(379~93 further advantage, depending upon the nature of the finishing operations involved in producing the cladding, the tendency toward corrosion may be to a large extent suppressed as a consequence of the heat treatment ~bove the alpha--alpha plus beta transformation temperature of about 810C. This latter effect would be attributable, possibly, to the segregation of the inter-metallic phase at the grain boundaries. In any event, the zirconium alloy employed in this process is one which contains beryllium in amount from 0.05 to 0.25 weight per cent, and preferably also contains about 1.;
weight per cent tin and 0.05 weight per cent nickel, and at least 95 weight per cent zirconium. In other words, it is preferably either Zircaloy-2 or Zircaloy-4.
The method and products of this invention are ~ set forth in more detail together with actual test ; results in the following illustrative example in which Zircaloy-2 was used, being melted in an electric arc furnace under vacuum to provide control specimens as well as test specimens meeting the special compositional requirements of this invention.
~ :~
_ 9 _ - ,. .. ...
1~79093 EXAMPLE
Of the total of seven test specimens, four were of commercial Zircaloy-2 composition and the others differed therefrom only in that they each contained 0.2 weight per cent beryllium. These specimens in the form of cast buttons about 2.5 inches in diameter and about one-half inch thick were machined to provide a smooth surface and then wrapped in zirconium foil, offset-forged approximately 30 per cent, heated to 930C in argon and then again offset-forged.
They were sandblasted and wrapped again in zirconium foil and reheated to 930C for 20 minutes and water-quenched.
The four specimens (Nos. 1, 3, 4 and 5 in Table I below) containing no beryllium were then rolled to ultimate thickness of one-sixteenth inch by a mutliple pass method, the final passes being cold-rolling operations. These sheets were sandblasted, pickled in aqueous 2.0 per cent HF and 6.0 per cent HN03, and then Specimens 1 and 3 were finally annealed at 650C for one hour while Specimens 4 and 5 were annealed at 580C for four hours. Beryllium-containing Specimens 2, 6 and 7 were processed in the same manner as Specimens 4 and 5 through the final annealing stage.
Specimens 1 and 2 were maintained at 327 C (620F) in a neutral atmosphere for one year, and Specimens 3, 4, 5, 6 and 7 were exposed to fast-neutron radiation at temperatures :', -10- ~, ' 15~79093 of either 250C or 327C for the same twelve-month period, being located within standard-size fuel cladding dummy fuel rods installed in fuel bundles in a working boiling water reactor core. Flux wires of nickel and iron indicated that these specimens were subjected to radiation exposure, peaking at 3.1 x 1021 nvt for corresponding peak fast flux values of 7 x 1013 n/cm2-sec. Thus, the typical specimen of this series was exposed to the fast flux over a period of one to 1-1/2 years in a neutral or an inert helium atmos-phere at the temperature indicated in Table I.
The results of all of the tests made on these irradiated and unirradiated specimens are set out in Table I:
`: :
1 ~
. I .
.. . .
.... . ..
- : . . .
, ' . . ~ - ' ' . .
- . ,.. . . .. - - .: . . : -~79093 o On On O ~ o ~ ~
o o o o o ~ :
~ ~I ~ ~ cn o o o o o o ~
H ~ ~
ooOOooI~
C
r ~ ~ O ~ ~ O
1 ~
-12.
1~379 [)93 The test temperature stated in Table I is the temperature at which the mechanical properties of the specimen were tested in each instance, all these specimens being subjected to the same 327C temperature environment over the twelve-month period under the conditions as set forth above.
The effect of the beryllium addition is demonstrated in Figure 2 where the dramatic difference in load-carrying capacity between Specimens 3 and 7 is indicated by Curves A and B, respectively. Also, it will be noted in this connection that in Table I the same inherent characteristic is reflected in the uniform strain-to-maximun-load which increased from 0.35 per cent in Specimen 3 to 2.5 per cent in Specimen 7, a net increase over 600 per cent. The tests yielding these data were conducted at a strain rate of 8.3 x 10-4 cm/cm/sec.
Metallographic examination of these two specimens revealed that deformation was noticeably more diffuse in Specimen 7 than in Specimen 3.
The effect of the beryllium addition is further illustrated in Fig. 3 where, again, there is a dramatic difference in strength betweeh Specimens 3 and 7 as indi-cated by Curves C and D, respectively. As previosly noted, the tests resulting in the data represented by these curves ~-were conducted in an aggresive environment (i.e.3 under .
.. . . . . .
.
. - ' ,' . :, - .
. - . . - . . ~ , ~ .
1~79093 an iodine atmosphere) at a strain rate of 2.83 x 10-6 cm/cm/sec.
The iodine atmosphere tests were conducted by subjecting the work piece at 325C in each case to an atmosphere of helium gas containing iodine in amount approximating the room temperature iodine partial pressure.
Thus, helium gas is flowed continuously through an iodine crystal bed from which it entered the test chamber. -Helium gas flow through the chamber was continuous as the pressure within the chamber was maintained slightly greater than atmospheric pressure.
.~ . .
; : . - - . -
The literature in this field, however, contains little concerning efforts to improve upon the mechanical strength of zirconium-base alloys and particularly the load-carrying capacity of fuel cladding and other reactor parts subjected to prolonged exposure to typical boiling water reactor conditions. This is in spite of the fact that it has long been general knowledge that slow strain rate ductility of these alloys is lost to a great extent as a result of radiation exposure over periods of a year or more. The problem of premature termination of service life because of fast neutron radiation-induced embrittlement is particularly aggravated in the case of nuclear fuel containment channels and tubes or cladding. The natural swelling of the fuel as it is burned produced high localized stresses leading to stress--corrosion cracking of the cladding at a time before corrosion of the type described in the above patents might normally necessitate cladding replacement.
; THE INVENTION
This invention, which is predicated on my discovery and new concept to be described, provides an answer to both the iodine stress-corrosion problem and the embrittlement problem in the form of a process which can result in doubl1ng the length of the service life of ~' ' : , 1~79~)93 zirconium-base alloy nuclear fuel cladding. Moreover, this result is obtained without incurring any significant offsetting cost or performance disadvantage.
My discovery is that a zirconium-base alloy of the kind presently used in nuclear reactors will have a much greater load-carrying capacity after being subiected to fast neutron radiation for a period of a year or so if it contains from 0.05 to 0.25 per cent beryllium. More specifically, such an alloy will characteristically exhibit S00 to 600 per cent greater load-carrying capacity ti.e., uniform strain to maximum load) than conventional beryllium-free cladding and can therefore be expected to serve in that use and environment much longer and possibly twice as long as the zirconium-base alloys in general use in nuclear reactors.
My new concept is to prepare a zirconium-base alloy containing o.n5 to 0.25 per cent beryllium for use as nuclear fuel cladding by heating to a temperature of the order of 900C and then water-quenching it. Although such heat treatment results in a phase transformation, the zirconium alloy transforming in part or totally from the alpha to the beta phase, and the prior art warns that detrimental effects on mechanical properties will result, I have found that there are substantial advantages to be gained by effecting such transformation. For one thing, , ~ 4_ :
1079093 RD-724~
ductility is enhanced materially, as will subsequently be described in more detail. For another, resistance to corrosion under boiling water nuclear reactor conditions resulting in heavy oxide coating formation on fuel cladding may thereby he substantially reduced or limited.
In its method aspect, this invention in brief description includes the steps of forming a zirconium-base alloy body containing 0.05 to 0.25 per cent beryllium, heating the body to a temperature above 900C and then quenching, and finally subjecting the body to boiling water reactor conditions for a long period of time such as a year or more. More specifically, the alloy body will be of at least ~5 percent zirconium, the quenching will be done with water and the nuclear reactor conditions will be a temperature of about 325C and a fast-neutron flux of l.O to 10.0 x 1021 nvt.
In its product or article aspect, this invention takes the form of a zirconium-base alloy body of substantially greater load-carrying capacity than similar conventional bodies of the alloy irradiated in the same way and to the same extent and having at 325C an unique combination of physical properties including 2.5 per cent uniform ~ 5 ~
~ ,. .
-: - ~ . ' , -. ~ ., . -~079093 elongation, 8.2 per cent total elongation and 35 per cent ~ area reduction, yield strength greater than 76,000 psi, ~ and tensile strength greather than 80,000 psi. In more specific terms, the body is a nuclear fuel container for use in a nuclear reactor, and is in the form of a tube having microstructure in which the intermetallic phase is to some extent segregated at the grain boundaries as a consequence of the heat treatment and quenching steps stated above. Additionally, the fuel container or cladding is irradiated as a result of having been subjected for a long period to fast-neutron flux and has greater load-carrying capacity than a counterpart fuel container similarly irradiated but containing no beryllium.
DESCRIPTION OF THE DRAWINGS
Figure 1 presents a partial cutaway sectional view of a nuclear fuel assembly containing nuclear fuel elements constructed according to the teaching of this invention, Figure 2 is a chart bearing curves illustrating : 20 physical property data obtained in tests of the new product of this invention and the corresponding prior art product, and Figure 3 is another chart on which stress is plotted against strain and the curves illustrate data taken in tests perforred under an iodine atmosphere.
~79093 DETAILED DESCRIPTION OF THE INVENTION
-As indicated by Figure 1, a primary application of the present invention is for the fabrication of nuclear fuel assemblies such as that illustrated at 10 consisting of a tubular flow channel 11 of generally square cross section provided at its upper end with lifting bale 12 and at its lower end with a nose piece (not shown due to the lower portion of assembly 10 being omitted). The upper end of channel 11 is open at 13 and the lower end of the nose piece is provided with coolant flow openings. An array of fuel elements or rods 14 is enclosed in channel 11 and supported therein by means of upper end plate 15 and a lower end plate (not shown due to the lower portion being omitted). The liquid coolant ordinarily enters through the openings in the lower end of the nose piece, passes upwardly around fuel elements 14, and discharges at upper outlet 13 in a partially vaporized condition for boiling water reactors or in an unvaporized condition for pressurized reactors at an elevated temperature.
The nuclear fuel elements or rods 14 are sealed at their ends by means of end plugs 18 welded to the cladding 17, which may include studs 19 to facilitate the mounting of the fuel rod in the assembly. A void space or plenum 20 is provided at one end of the element to permit longitudinal expansion of the fuel material and accumulation .... . . , ,, . . . ~ .
.
.
1~9~93 of gases released from the fuel material. A nuclear fuel material retainer means 24 in the form of a helical member is positioned within space 20 to provide restraint against the axial movement of the pellet column, especially during handling and transportation of the fuel element.
The fuel element is designed to provide an excellent thermal contact between the cladding and the fuel material, a minimum of parasitic neutron absorption, and resistance to bowing and vibration which is occasionally caused by flow of the coolant at high velocity.
Cladding 17 is produced in accordance with this invention by a process which includes in addition to the usual tube-forming operations a heat treatment in argon or other inert atmosphere above the alpha--alpha plus beta transformation temperature followed by a water quench. The rate at which the work piece is heated up to the trans-formation temperature range is a matter of choice, but the time it is maintained in that range is preferably about ' 30 seconds and the cooling rate down to 700 to 750C may ', 20 be as low as 50C per second. As so treated, the zirconium alloy body is made more easily workable and forming operations are facilitated through the warm-working stage. It also ; appears, as indicated above, that the physical properties and particularly the ductility of the ultimate cladding product may be considerably enhanced in this manner. As a ., :
' .
1(379~93 further advantage, depending upon the nature of the finishing operations involved in producing the cladding, the tendency toward corrosion may be to a large extent suppressed as a consequence of the heat treatment ~bove the alpha--alpha plus beta transformation temperature of about 810C. This latter effect would be attributable, possibly, to the segregation of the inter-metallic phase at the grain boundaries. In any event, the zirconium alloy employed in this process is one which contains beryllium in amount from 0.05 to 0.25 weight per cent, and preferably also contains about 1.;
weight per cent tin and 0.05 weight per cent nickel, and at least 95 weight per cent zirconium. In other words, it is preferably either Zircaloy-2 or Zircaloy-4.
The method and products of this invention are ~ set forth in more detail together with actual test ; results in the following illustrative example in which Zircaloy-2 was used, being melted in an electric arc furnace under vacuum to provide control specimens as well as test specimens meeting the special compositional requirements of this invention.
~ :~
_ 9 _ - ,. .. ...
1~79093 EXAMPLE
Of the total of seven test specimens, four were of commercial Zircaloy-2 composition and the others differed therefrom only in that they each contained 0.2 weight per cent beryllium. These specimens in the form of cast buttons about 2.5 inches in diameter and about one-half inch thick were machined to provide a smooth surface and then wrapped in zirconium foil, offset-forged approximately 30 per cent, heated to 930C in argon and then again offset-forged.
They were sandblasted and wrapped again in zirconium foil and reheated to 930C for 20 minutes and water-quenched.
The four specimens (Nos. 1, 3, 4 and 5 in Table I below) containing no beryllium were then rolled to ultimate thickness of one-sixteenth inch by a mutliple pass method, the final passes being cold-rolling operations. These sheets were sandblasted, pickled in aqueous 2.0 per cent HF and 6.0 per cent HN03, and then Specimens 1 and 3 were finally annealed at 650C for one hour while Specimens 4 and 5 were annealed at 580C for four hours. Beryllium-containing Specimens 2, 6 and 7 were processed in the same manner as Specimens 4 and 5 through the final annealing stage.
Specimens 1 and 2 were maintained at 327 C (620F) in a neutral atmosphere for one year, and Specimens 3, 4, 5, 6 and 7 were exposed to fast-neutron radiation at temperatures :', -10- ~, ' 15~79093 of either 250C or 327C for the same twelve-month period, being located within standard-size fuel cladding dummy fuel rods installed in fuel bundles in a working boiling water reactor core. Flux wires of nickel and iron indicated that these specimens were subjected to radiation exposure, peaking at 3.1 x 1021 nvt for corresponding peak fast flux values of 7 x 1013 n/cm2-sec. Thus, the typical specimen of this series was exposed to the fast flux over a period of one to 1-1/2 years in a neutral or an inert helium atmos-phere at the temperature indicated in Table I.
The results of all of the tests made on these irradiated and unirradiated specimens are set out in Table I:
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- . ,.. . . .. - - .: . . : -~79093 o On On O ~ o ~ ~
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1~379 [)93 The test temperature stated in Table I is the temperature at which the mechanical properties of the specimen were tested in each instance, all these specimens being subjected to the same 327C temperature environment over the twelve-month period under the conditions as set forth above.
The effect of the beryllium addition is demonstrated in Figure 2 where the dramatic difference in load-carrying capacity between Specimens 3 and 7 is indicated by Curves A and B, respectively. Also, it will be noted in this connection that in Table I the same inherent characteristic is reflected in the uniform strain-to-maximun-load which increased from 0.35 per cent in Specimen 3 to 2.5 per cent in Specimen 7, a net increase over 600 per cent. The tests yielding these data were conducted at a strain rate of 8.3 x 10-4 cm/cm/sec.
Metallographic examination of these two specimens revealed that deformation was noticeably more diffuse in Specimen 7 than in Specimen 3.
The effect of the beryllium addition is further illustrated in Fig. 3 where, again, there is a dramatic difference in strength betweeh Specimens 3 and 7 as indi-cated by Curves C and D, respectively. As previosly noted, the tests resulting in the data represented by these curves ~-were conducted in an aggresive environment (i.e.3 under .
.. . . . . .
.
. - ' ,' . :, - .
. - . . - . . ~ , ~ .
1~79093 an iodine atmosphere) at a strain rate of 2.83 x 10-6 cm/cm/sec.
The iodine atmosphere tests were conducted by subjecting the work piece at 325C in each case to an atmosphere of helium gas containing iodine in amount approximating the room temperature iodine partial pressure.
Thus, helium gas is flowed continuously through an iodine crystal bed from which it entered the test chamber. -Helium gas flow through the chamber was continuous as the pressure within the chamber was maintained slightly greater than atmospheric pressure.
.~ . .
; : . - - . -
Claims (2)
1. A fast neutron-irradiated zirconium-base alloy body selected from the group consisting of Zircaloy-2 and Zircaloy-4 containing from 0.05 to 0.25 weight per cent beryllium and having substantially greater load-carrying capacity than similar conventional zirconium-base alloy bodies irradiated in the same way and to the same degree, and having at 327°C an unique combination of physical properties including 2.5 per cent uniform elongation, 8.2 per cent total elongation and 35 per cent area reduction, yield strength greater than 76,000 psi, and tensile strength greater than 80,000 psi.
2. The alloy body of claim 1 wherein the weight per cent of beryllium is 0.2
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US53527174A | 1974-12-23 | 1974-12-23 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA1079093A true CA1079093A (en) | 1980-06-10 |
Family
ID=24133522
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA241,901A Expired CA1079093A (en) | 1974-12-23 | 1975-12-11 | Zirconium-base alloy nuclear fuel container and method |
Country Status (1)
| Country | Link |
|---|---|
| CA (1) | CA1079093A (en) |
-
1975
- 1975-12-11 CA CA241,901A patent/CA1079093A/en not_active Expired
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