JPS60183584A - Nuclear fuel element - Google Patents
Nuclear fuel elementInfo
- Publication number
- JPS60183584A JPS60183584A JP59038605A JP3860584A JPS60183584A JP S60183584 A JPS60183584 A JP S60183584A JP 59038605 A JP59038605 A JP 59038605A JP 3860584 A JP3860584 A JP 3860584A JP S60183584 A JPS60183584 A JP S60183584A
- Authority
- JP
- Japan
- Prior art keywords
- cladding tube
- nuclear fuel
- liner
- stress
- layer
- 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.)
- Pending
Links
- 239000003758 nuclear fuel Substances 0.000 title claims description 32
- 238000005253 cladding Methods 0.000 claims description 56
- 239000008188 pellet Substances 0.000 claims description 20
- 239000000463 material Substances 0.000 claims description 9
- 229910052726 zirconium Inorganic materials 0.000 claims description 9
- QCWXUUIWCKQGHC-UHFFFAOYSA-N Zirconium Chemical compound [Zr] QCWXUUIWCKQGHC-UHFFFAOYSA-N 0.000 claims description 8
- 230000035882 stress Effects 0.000 description 23
- 239000010410 layer Substances 0.000 description 14
- 239000002356 single layer Substances 0.000 description 12
- 239000000446 fuel Substances 0.000 description 9
- 239000007789 gas Substances 0.000 description 9
- 230000007797 corrosion Effects 0.000 description 6
- 238000005260 corrosion Methods 0.000 description 6
- 238000005336 cracking Methods 0.000 description 6
- 239000000956 alloy Substances 0.000 description 5
- 230000003993 interaction Effects 0.000 description 5
- 229910045601 alloy Inorganic materials 0.000 description 4
- 230000004888 barrier function Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 238000006243 chemical reaction Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 230000004992 fission Effects 0.000 description 3
- 238000010521 absorption reaction Methods 0.000 description 2
- TVFDJXOCXUVLDH-UHFFFAOYSA-N caesium atom Chemical compound [Cs] TVFDJXOCXUVLDH-UHFFFAOYSA-N 0.000 description 2
- 238000000576 coating method Methods 0.000 description 2
- 239000002826 coolant Substances 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 239000012528 membrane Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 229910052750 molybdenum Inorganic materials 0.000 description 2
- 229910052758 niobium Inorganic materials 0.000 description 2
- ZCYVEMRRCGMTRW-UHFFFAOYSA-N 7553-56-2 Chemical compound [I] ZCYVEMRRCGMTRW-UHFFFAOYSA-N 0.000 description 1
- 229910000599 Cr alloy Inorganic materials 0.000 description 1
- 241000196324 Embryophyta Species 0.000 description 1
- 240000007594 Oryza sativa Species 0.000 description 1
- 235000007164 Oryza sativa Nutrition 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- 229910001093 Zr alloy Inorganic materials 0.000 description 1
- 238000009825 accumulation Methods 0.000 description 1
- 238000000137 annealing Methods 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 229910052792 caesium Inorganic materials 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000005097 cold rolling Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 230000006378 damage Effects 0.000 description 1
- 238000011156 evaluation Methods 0.000 description 1
- 230000036541 health Effects 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 238000007689 inspection Methods 0.000 description 1
- 229910052740 iodine Inorganic materials 0.000 description 1
- 239000011630 iodine Substances 0.000 description 1
- 150000002497 iodine compounds Chemical class 0.000 description 1
- 239000000314 lubricant Substances 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 238000001953 recrystallisation Methods 0.000 description 1
- 235000009566 rice Nutrition 0.000 description 1
- 238000005096 rolling process Methods 0.000 description 1
- 239000010935 stainless steel Substances 0.000 description 1
- 229910001220 stainless steel Inorganic materials 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 229910052715 tantalum Inorganic materials 0.000 description 1
- 238000012360 testing method Methods 0.000 description 1
- 230000008646 thermal stress Effects 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- 238000012546 transfer Methods 0.000 description 1
- 229910052721 tungsten Inorganic materials 0.000 description 1
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E30/00—Energy generation of nuclear origin
- Y02E30/30—Nuclear fission reactors
Landscapes
- Glass Compositions (AREA)
- Catalysts (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】 〔発明の利用分野〕 本発明は、核燃料豊素の改良に関するものである。[Detailed description of the invention] [Field of application of the invention] The present invention relates to the improvement of nuclear fuel enrichment.
第1図は通常の核燃料要素の縦断面図である。 FIG. 1 is a longitudinal cross-sectional view of a conventional nuclear fuel element.
−叡に核燃料要素は、第1図に示すように被覆管1内に
仮数個の核燃料ペレット2が積層収納され、被覆管10
両端開口が端栓3a、3bにより密閉されている。燃料
ペレット2は核分裂性の酸化物Im専↓名へ十ム 伍1
141イ見シ シiH7尽μの田植;ネ61 の用柱状
ペレットに成形焼結されたものである。伺、4は、被覆
管1内にガス溜め用プレナム5を形成する機能と核燃料
ペレット2を安定して受持する機能とをもたせたスプリ
ングである。- As shown in FIG.
Both end openings are sealed by end plugs 3a and 3b. Fuel pellet 2 is a fissile oxide Im only ↓ name to name 51
141 pieces of rice were sintered into columnar pellets of 61 pieces. Reference numeral 4 denotes a spring that has the function of forming a gas reservoir plenum 5 within the cladding tube 1 and the function of stably supporting the nuclear fuel pellets 2.
ところで、上記のように構成された核燃料要素において
、被覆管1には核燃料ベレット2との間こ
で冷却材がkp&すると及び化学反応が生じること全阻
止する機能と、燃料から放出された放射性核分裂生成物
が冷却材中に混入するのを阻止する機能とが要求される
。従って、このような機能を満足しない被覆管1、即ち
、被覆管1が破損したような場合には、冷却系プラント
の放射能レベルが上昇し、安全を確保するために原子炉
の運転を停止させなければならない事態となる。By the way, in the nuclear fuel element configured as described above, the cladding tube 1 has the function of completely preventing the occurrence of chemical reactions when the coolant is inserted between the nuclear fuel pellet 2 and the nuclear fuel pellet 2, and the function of completely preventing the occurrence of chemical reactions between the cladding tube 1 and the nuclear fuel pellet 2. The ability to prevent products from entering the coolant is required. Therefore, in the event that the cladding tube 1 that does not satisfy these functions, that is, the cladding tube 1 is damaged, the radioactivity level in the cooling system plant will increase, and the reactor operation will have to be stopped to ensure safety. This is a situation where it is necessary to do so.
一方、水冷型原子炉に用いられる核燃料長素の被覆管1
は、一般にジルコニウム及びその合金系材料で形成され
ている。ジルコニウム及びその合金は、中性子吸収断面
積が小さく、かつ、約400C以下の温度で強靭で延性
がよく、シかも、冷却せシ1 イ1i31八戯り入−ヤ
某僅μ家ゴ[欧1 h1八厩硅塾有している。On the other hand, cladding tube 1 of nuclear fuel element used in water-cooled nuclear reactor
are generally made of zirconium and its alloys. Zirconium and its alloys have a small neutron absorption cross section, are strong and ductile at temperatures below about 400C, and can be cooled. It has H1 Hachimaya Seijuku.
しかしながら、現在までの運転経験によると、ジルコニ
ウム及びその合金で形成された被覆管1にあっても、中
性子照射を受けることによる材料強度の低下及び核分裂
生成物との化学反応による腐食などの相互作用に基づく
脆性割れが発生している。このような望ましくない現象
は次のようにして発生するものとして考えられる。即ち
、核燃料ペレット2で発生した熱を被覆管1の外表面に
効率よく伝えるには、被覆管1の内側面と核燃料ペレッ
ト2との間に形成されるギャップを数十ミクロン以下に
設定する必要がある。一方、運転時には、核燃料ペレッ
ト2が発熱するのでペレット自身が熱応力で割れ、その
破面の喰い違いや、さらには燃焼とともに核燃料ペレッ
ト内に核分裂生成物が蓄積して起こる体積膨張などが原
因して核燃料要素に起シ易い問題点の説明図の第2図に
示すように被覆管1が核燃料ペレット2によって押し拡
げられ応力を受ける。However, according to operational experience to date, even if the cladding tube 1 is made of zirconium and its alloys, interactions such as a decrease in material strength due to neutron irradiation and corrosion due to chemical reactions with fission products may occur. Brittle cracking has occurred due to Such an undesirable phenomenon is thought to occur as follows. That is, in order to efficiently transfer the heat generated by the nuclear fuel pellet 2 to the outer surface of the cladding tube 1, it is necessary to set the gap formed between the inner surface of the cladding tube 1 and the nuclear fuel pellet 2 to several tens of microns or less. There is. On the other hand, during operation, the nuclear fuel pellet 2 generates heat, which causes the pellet itself to crack due to thermal stress, resulting in discrepancies in the fracture surfaces, and furthermore, volumetric expansion caused by the accumulation of fission products within the nuclear fuel pellet as it burns. As shown in FIG. 2, which is an explanatory diagram of problems that tend to occur in nuclear fuel elements, the cladding tube 1 is expanded by the nuclear fuel pellets 2 and is subjected to stress.
被覆管1が受ける歪の周方向の平均値はさほど犬さくな
いが、核燃料ペレット2に生じたクラック6近傍の壁に
は局部的に歪が果申し、この歪は降伏応力以上に達する
。さらに、核分裂に牛なって核燃料ペレット2か、ら、
よう素及びよう素化合吻、セシウム及びセシウム化合物
などの腐食性ガスが発生し、この腐食性ガスは被覆管1
内の自由空間、即ち、クラック6などに集まる。即ち、
被覆管1の特に歪が集中している部分近傍に腐食性ガス
が集まシ易い。Although the average value of the strain to which the cladding tube 1 is subjected in the circumferential direction is not so large, strain is exerted locally on the wall near the crack 6 that has occurred in the nuclear fuel pellet 2, and this strain reaches more than the yield stress. In addition, nuclear fission becomes a cow and nuclear fuel pellets 2, etc.
Corrosive gases such as iodine and iodine compounds, cesium and cesium compounds are generated, and this corrosive gas is
It gathers in the free space inside, ie, in the crack 6, etc. That is,
Corrosive gas tends to collect particularly in the vicinity of parts of the cladding tube 1 where strain is concentrated.
一般に、腐食性ガスの雰囲気中で応力(%に降伏応力以
上)が作用すると、燃料の延性が低下し、応力腐食割れ
と呼称される脆性破壊現象が発生する。応力腐食割れは
、温度、応カ、腐食性ガスの濃度、溶存酸素2合金の組
成、熱処理、加工度などによっても左右され、その発生
メカニズムは単一ではない。Generally, when stress (% yield stress or higher) is applied in a corrosive gas atmosphere, the ductility of the fuel decreases and a brittle fracture phenomenon called stress corrosion cracking occurs. Stress corrosion cracking is influenced by temperature, stress, concentration of corrosive gas, composition of dissolved oxygen 2 alloy, heat treatment, degree of processing, etc., and the mechanism by which it occurs is not unique.
これらの好ましくない破壊を防止する目的で、従来例と
して、例えば、燃料ペレット2と被覆管1との間に潤滑
剤を挿入する方法が米国特許の第3018238号明細
書に示されており、また、被覆管1と燃料ペレット2と
の間に障壁を設けた例としてDA81238115号で
はチタン層を述べている。さらに、Nb、Ta、Mo、
Zrの金網状膜で燃料を包囲した核燃料棒も知られてい
る。その他の障壁材として、ステンレス鋼、ガラス質物
質、At、Mg、Cu等が米国特許第3080893号
、同じ<3085059号、同じ< 3212788号
、同じ< 3291700号、同じ< 3230150
号明細書及び特開昭50−109397号公報で知られ
ている。For the purpose of preventing these undesirable destructions, for example, as a conventional example, a method of inserting a lubricant between the fuel pellets 2 and the cladding tube 1 is shown in US Pat. No. 3,018,238, and , DA81238115 describes a titanium layer as an example of providing a barrier between the cladding tube 1 and the fuel pellets 2. Furthermore, Nb, Ta, Mo,
Nuclear fuel rods in which the fuel is surrounded by a Zr wire mesh membrane are also known. Other barrier materials include stainless steel, glassy substances, At, Mg, Cu, etc.
It is known from the specification of No. 1 and Japanese Patent Application Laid-Open No. 109397/1983.
同様に被覆管を内張シする概念は周知であり、米国特許
第3502549号、同じ(3625821号明細書、
特開昭51−69792号、同じく51−69795号
、同じ<51−69796号及び同じく51−7149
7号公報において、内張り材としてMo、W、Nb、C
r、Ni、F’e、Mg、Cut純Zr、At、Ni−
Cr合金、アルミ化コーテング、珪素化コーテング等が
示されている。Similarly, the concept of lining a cladding tube is well known, as in U.S. Pat.
JP-A No. 51-69792, same No. 51-69795, same <51-69796 and same No. 51-7149
In Publication No. 7, Mo, W, Nb, and C are used as lining materials.
r, Ni, F'e, Mg, Cut pure Zr, At, Ni-
Cr alloys, aluminized coatings, silicided coatings, etc. are shown.
しかしながら、以上の従来技術に述べられている障壁材
及び内張り材の成るものは中性子吸収断171す噛)1
へz+2(メla/7’)ネ561g姓?−イIT−T
(,5J−2、−AG77’l/FAがある。また、上
記引用した提案の幾つかは障壁とし使用する物質が、核
燃料ペレットと両立し難い物質であるが、被覆管と両立
し難い物質である場合があり、上記引用した提案はいず
れも最近問題となっている核燃料と被覆管との間の局部
的な化学的−機械的相互作用に対する根本的な解決法ま
で達しているとは云えない。However, the barrier material and lining material described in the above prior art have a neutron absorption capacity of 171).
Hez+2 (Mela/7')ne561g Surname? -IT-T
(, 5J-2, -AG77'l/FA.Also, in some of the proposals cited above, the materials used as barriers are materials that are incompatible with nuclear fuel pellets, but there are also materials that are incompatible with cladding tubes. However, it cannot be said that the above-cited proposals reach a fundamental solution to the local chemical-mechanical interaction between the nuclear fuel and the cladding, which has recently become a problem. do not have.
〔発明の目的〕
本発明は上記の状況に鑑みなされたものであシ、腐食性
ガス中において燃料と被覆管との相互作用によシ被覆管
に応力が作用した場合に、応力腐食割れが起とシ難く、
信頼性を向上できる核燃料要素を提供することを目的と
したものである。[Object of the Invention] The present invention has been made in view of the above-mentioned situation, and is aimed at reducing stress corrosion cracking when stress is applied to the cladding tube due to the interaction between the fuel and the cladding tube in corrosive gas. It's hard to get up,
The aim is to provide nuclear fuel elements that can improve reliability.
本発明の核燃料要素は、ジルコニウム合金系の材料から
形成された被覆管内に核燃料ペレットが充填され、該被
覆管の両端開口が端栓を介し密閉されてなり、上記被覆
管の内表面にライナ一層が嵌入され、該ライナ一層が被
覆管の内表面の全面にわたシ接触しない非接触部を残し
た粗の状膜で結合されてなるものである。即ち、ライナ
一層が上記被覆管に粗に結合されることにより、上記被
覆管に発生する応力集中の大きさが、ライナ一層が被覆
管に全面にわたり緊密に結合した場合に比べて低下する
ことによシ健全性を向上できるものである。In the nuclear fuel element of the present invention, a cladding tube made of a zirconium alloy material is filled with nuclear fuel pellets, and both openings of the cladding tube are sealed through end plugs, and a liner is layered on the inner surface of the cladding tube. The liner layer is bonded to the inner surface of the cladding tube with a rough membrane that leaves a non-contact area over the entire inner surface of the cladding tube. That is, because the liner layer is loosely bonded to the cladding tube, the magnitude of stress concentration occurring in the cladding tube is reduced compared to when the liner layer is tightly bonded to the cladding tube over the entire surface. This can improve health.
以下本発明の核燃料要素を実施例を用い従来と同部品は
同符号で示し同部分の構造の説明は省略し 7.3図、
第4図により説明する。第3図は核燃料要素の横断面図
、第4図は第3図のA部の拡大図である。図において、
8はジルコニウムから形成されたライナ一層であり被覆
管1の内周に嵌合されている。ライナ一層8付被覆管1
は次の工程により得られる。ASTM規格に満足したジ
ルカロイ−2素管の被覆管1の内表面の長手方向に溝状
切欠きを設け、上記ジルカロイ−2素管の被復管1内に
円筒状ジルコニウムを嵌め込み、ピルガ一式圧延法によ
り冷間圧延を行なう。各段の圧延毎に真空焼鈍を実施し
、最終外径12V52a+内径10.80mmに仕上げ
る。その後再結晶熱処理を加え、寸法検査を行なう。Hereinafter, the nuclear fuel element of the present invention will be described as an example, and parts that are the same as those of the conventional one will be denoted by the same reference numerals, and explanations of the structures of the same parts will be omitted.
This will be explained with reference to FIG. FIG. 3 is a cross-sectional view of the nuclear fuel element, and FIG. 4 is an enlarged view of section A in FIG. 3. In the figure,
Reference numeral 8 denotes a single layer liner made of zirconium, which is fitted onto the inner periphery of the cladding tube 1. Cladding tube 1 with liner single layer 8
is obtained by the following steps. A groove-like notch is provided in the longitudinal direction of the inner surface of the cladding tube 1 of the Zircaloy-2 raw tube that satisfies ASTM standards, and a cylindrical zirconium is fitted into the reinstated tube 1 of the Zircaloy-2 raw tube, and the cylindrical zirconium is rolled as a complete pilger. Cold rolling is performed by the method. Vacuum annealing is performed for each stage of rolling to give a final outer diameter of 12V52a + inner diameter of 10.80 mm. After that, a recrystallization heat treatment is applied, and a dimensional inspection is performed.
上記のように作成されたライナ一層8付被覆管1は、第
4図に示すようにライナ一層8が被覆管1の内周面に全
面にわたり接触しないで、長手方向に形成された溝状切
欠きにより形成された非接触部9を有し接触部10によ
り嵌合されている。As shown in FIG. 4, the cladding tube 1 with a single layer of liner 8 produced as described above has a groove-like cut formed in the longitudinal direction so that the single layer of liner 8 does not contact the entire inner circumferential surface of the cladding tube 1. It has a non-contact part 9 formed by a notch and is fitted with a contact part 10.
そして、特性評価試験の結果から、接触部10より非接
触部9の面積が大きいこと、即ち、接触面積が1/2以
内であることが好ましいことが判った。From the results of the characteristic evaluation test, it was found that it is preferable that the area of the non-contact portion 9 is larger than that of the contact portion 10, that is, the contact area is preferably within 1/2.
また、本実施例の効果は、以下に述べる理由により明ら
かである。第5図(イ)に示すように、厚さaのライナ
一層8に亀裂7が生じた場合の被覆管部の応力集中の大
きさを表わすパラメータとして破壊力学における応力拡
大係数(K)を用いる。Further, the effect of this embodiment is obvious for the reasons described below. As shown in Fig. 5(a), the stress intensity factor (K) in fracture mechanics is used as a parameter representing the magnitude of stress concentration in the cladding tube when a crack 7 occurs in one liner layer 8 having a thickness of a. .
この場合、亀裂7の先端のKは(1)式で表わすことが
できる。In this case, K at the tip of the crack 7 can be expressed by equation (1).
K = AσV1− ・・・・・・・・・(1)但し、
A:形状から定まる定数、
σ:被覆管1に作用している円周方向応力、
即ち、ライナ一層8に亀裂7が入ったときには、被覆管
1の内表面上の亀裂7先端での応力集中の大きさは、ラ
イナ一層8の厚さaの平方根に比例して増加することが
わかる。K = AσV1− ・・・・・・・・・(1) However,
A: constant determined from the shape, σ: stress in the circumferential direction acting on the cladding tube 1, that is, when a crack 7 occurs in the liner layer 8, stress concentration at the tip of the crack 7 on the inner surface of the cladding tube 1 It can be seen that the magnitude increases in proportion to the square root of the thickness a of the liner layer 8.
一方、本実施例のライナ一層性被覆管1においては、ラ
イナ一層8に亀裂が入っても、ライナ一層8と被覆管1
とは連続体でないために亀裂7先・浦のKはライナ一層
8の厚さaに無関係に第5図(ロ)に示す被覆管1の四
部寸法(b)の大きさによって(2)式のように定まる
。On the other hand, in the liner single layer cladding tube 1 of this embodiment, even if the liner layer 8 is cracked, the liner layer 8 and the cladding tube 1
Since it is not a continuum, K at the tip of the crack 7 and the ura is determined by equation (2), regardless of the thickness a of the liner layer 8, depending on the size of the four dimensions (b) of the cladding tube 1 shown in Figure 5 (b). It is determined as follows.
K=Aσf丁 ・・・・・・・・・(2)従って、本実
施例のライナ一層性被覆管1では、ライナ一層8に亀裂
7が生じても被覆管1の応力集中の程度はライナ一層8
の厚さaに従って増加することなく一定である。この関
係を第6図においてさらに明確に説明する。本実施例の
ライナ一層性被覆管1の凹部寸法すは約10μmであり
、この値に対応してまる応力拡大係数を基準値(i、
o )とすると、横軸にライナー厚さをとり縦軸に正規
化した応力拡大係数をとって示した第6図の曲線Bに示
すようにライナ一層8の厚さに無関係に1.0となる。K=Aσf t (2) Therefore, in the liner single-layer cladding tube 1 of this embodiment, even if a crack 7 occurs in the liner single layer 8, the degree of stress concentration in the cladding tube 1 will be lower than the liner layer cladding tube 1. One layer 8
is constant without increasing according to the thickness a. This relationship will be explained more clearly in FIG. The dimension of the concave portion of the liner single-layer cladding tube 1 of this example is approximately 10 μm, and the stress intensity factor corresponding to this value is set to the reference value (i,
o), the liner thickness is plotted on the horizontal axis and the normalized stress intensity factor is plotted on the vertical axis, as shown in curve B of FIG. 6, which is 1.0 regardless of the thickness of the liner layer 8. Become.
一方、従来構造のライラ一層8付被覆管1においては、
亀裂先端の応力拡大係数は曲線Cに示すように増加し、
基準値りを越える可能性が考えられる。On the other hand, in the conventional structure of the cladding tube 1 with single layer 8 of Lyra,
The stress intensity factor at the crack tip increases as shown in curve C;
There is a possibility that the standard value will be exceeded.
このように本実施例の核燃料要素は、被康管の内表面に
嵌入されたライナ一層が、該被覆管の内表面の全面にわ
たり接触しないで非接触部を残した粗の状態で結合され
ていることにより、上記解析例に示したように、腐食性
ガス中において燃料との相互作用により、ライナー溜部
に亀裂が生じた場合に応力腐食割れが起り難く信頼性を
向上できる。In this way, in the nuclear fuel element of this embodiment, the liner layer fitted into the inner surface of the cladding tube is bonded in a rough state with no contact over the entire inner surface of the cladding tube, leaving a non-contact area. As shown in the above analysis example, even if cracks occur in the liner reservoir due to interaction with fuel in corrosive gas, stress corrosion cracking is less likely to occur and reliability can be improved.
以上記述した如く本発明の核燃料要素は、腐食性ガス中
において燃料と被覆管との相互作用により被覆管に応力
が作用した場合に、応力腐食割れが起り難く信頼性を向
上できる効果を有するものである。As described above, the nuclear fuel element of the present invention has the effect that stress corrosion cracking is unlikely to occur when stress is applied to the cladding tube due to the interaction between the fuel and the cladding tube in corrosive gas, thereby improving reliability. It is.
第1図は通常の核燃料要素の縦断面図、第2図は第1図
の核燃料要素に起り易い問題点の説明図、第3図は本発
明の核燃料要素の実施例の横断面図、第4図は第3図の
A部拡大図、第5図(イ)はライナ一層を被覆管内表面
に非接触部を設けないで成人した場合のライナ一層の亀
裂先端の被覆管内表面における応力集中説明図、(ロ)
は第4図のライナ一層の亀裂先端の被覆管内表面におけ
る応力集中説明図、第6図は第3図の被覆管及び第5図
の被覆管の特性比較説明図である。
1・・・被覆管、2・・・燃料ペレット、3a、3b・
・・端栓、8・・・ライナ一層、9・・・非接触部、1
0・・・接触部。
代理人 弁理士 高橋明夫
算う口
第5図
(イ)(O)
Y4図
ライナ−4ニア C〃梶)FIG. 1 is a vertical cross-sectional view of a normal nuclear fuel element, FIG. 2 is an explanatory diagram of problems that tend to occur in the nuclear fuel element of FIG. 1, and FIG. 3 is a cross-sectional view of an embodiment of the nuclear fuel element of the present invention. Figure 4 is an enlarged view of part A in Figure 3, and Figure 5 (a) is an explanation of stress concentration on the inner surface of the cladding tube at the tip of a crack in the single layer of liner when the liner has matured without providing a non-contact part on the inner surface of the cladding tube. Figure, (b)
4 is an explanatory diagram of stress concentration on the inner surface of the cladding tube at the tip of a crack in a single layer of liner, and FIG. 6 is a diagram illustrating a comparison of characteristics of the cladding tube of FIG. 3 and the cladding tube of FIG. 5. 1... Cladding tube, 2... Fuel pellets, 3a, 3b.
... End plug, 8 ... Liner single layer, 9 ... Non-contact part, 1
0...Contact part. Agent: Patent Attorney Akio Takahashi Figure 5 (A) (O) Y4 liner - 4 near C〃Kaji)
Claims (1)
省内に核燃料ペレットが充填され、該被覆管の両端開口
が端栓を介し密閉されてなるものにおいて、上記被覆・
αの内表面にライナ一層が嵌入され、6亥ライナ一層が
、上記被覆管の内民面の全面にわたり接触しない非接触
部をつ、(シた粗の状態で結合されてなることを特似と
する核燃料要素。1. Nuclear fuel pellets are filled in the cladding made of zirconium-coated zirconium-based material, and the openings at both ends of the cladding tube are sealed via end plugs.
One layer of liner is inserted into the inner surface of α, and one layer of liner 6 has a non-contact part that does not touch the entire inner surface of the cladding tube. and nuclear fuel elements.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59038605A JPS60183584A (en) | 1984-03-02 | 1984-03-02 | Nuclear fuel element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59038605A JPS60183584A (en) | 1984-03-02 | 1984-03-02 | Nuclear fuel element |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS60183584A true JPS60183584A (en) | 1985-09-19 |
Family
ID=12529900
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59038605A Pending JPS60183584A (en) | 1984-03-02 | 1984-03-02 | Nuclear fuel element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60183584A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2002305857A (en) * | 2001-04-17 | 2002-10-18 | Zexel Valeo Climate Control Corp | Hybrid compressor |
-
1984
- 1984-03-02 JP JP59038605A patent/JPS60183584A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2002305857A (en) * | 2001-04-17 | 2002-10-18 | Zexel Valeo Climate Control Corp | Hybrid compressor |
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