JPH0254518B2 - - Google Patents
Info
- Publication number
- JPH0254518B2 JPH0254518B2 JP56126205A JP12620581A JPH0254518B2 JP H0254518 B2 JPH0254518 B2 JP H0254518B2 JP 56126205 A JP56126205 A JP 56126205A JP 12620581 A JP12620581 A JP 12620581A JP H0254518 B2 JPH0254518 B2 JP H0254518B2
- Authority
- JP
- Japan
- Prior art keywords
- reactor
- control rod
- core
- cladding tube
- rod
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 238000010521 absorption reaction Methods 0.000 claims description 17
- 238000005253 cladding Methods 0.000 claims description 17
- 239000008188 pellet Substances 0.000 claims description 9
- 239000000843 powder Substances 0.000 claims description 9
- 230000000694 effects Effects 0.000 claims description 5
- 239000011358 absorbing material Substances 0.000 claims description 4
- 239000000463 material Substances 0.000 claims description 3
- 239000000126 substance Substances 0.000 claims description 3
- 230000009257 reactivity Effects 0.000 description 15
- 239000000446 fuel Substances 0.000 description 4
- 238000009835 boiling Methods 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 239000011800 void material Substances 0.000 description 3
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- 230000037431 insertion Effects 0.000 description 2
- 238000003780 insertion Methods 0.000 description 2
- 239000000203 mixture Substances 0.000 description 2
- 229910001220 stainless steel Inorganic materials 0.000 description 2
- 239000010935 stainless steel Substances 0.000 description 2
- JFALSRSLKYAFGM-UHFFFAOYSA-N uranium(0) Chemical compound [U] JFALSRSLKYAFGM-UHFFFAOYSA-N 0.000 description 2
- 229910052778 Plutonium Inorganic materials 0.000 description 1
- 229910052770 Uranium Inorganic materials 0.000 description 1
- 239000006096 absorbing agent Substances 0.000 description 1
- 230000000712 assembly Effects 0.000 description 1
- 238000000429 assembly Methods 0.000 description 1
- 230000004323 axial length Effects 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 238000002485 combustion reaction Methods 0.000 description 1
- 239000002826 coolant Substances 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 230000004992 fission Effects 0.000 description 1
- 230000005484 gravity Effects 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000005192 partition Methods 0.000 description 1
- OYEHPCDNVJXUIW-UHFFFAOYSA-N plutonium atom Chemical compound [Pu] OYEHPCDNVJXUIW-UHFFFAOYSA-N 0.000 description 1
- 238000001228 spectrum Methods 0.000 description 1
- 230000008961 swelling Effects 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
- Monitoring And Testing Of Nuclear Reactors (AREA)
- Particle Accelerators (AREA)
Description
【発明の詳細な説明】
本発明は原子炉用制御棒に係り、特に沸騰水型
原子炉の炉停止余裕を効果的に向上せしめ原子炉
を安全確実に停止させることができる原子炉用制
御棒に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a control rod for a nuclear reactor, and in particular to a control rod for a nuclear reactor that can effectively improve the reactor shutdown margin of a boiling water reactor and can safely and reliably shut down a nuclear reactor. Regarding.
原子炉用制御棒は、中央構造材に細長いU字状
のシースを取り付けて形成した複数箇のウイング
内に、多数の中性子吸収棒を装填して構成されて
いる。前記の中性子吸収棒は一般にステンレス鋼
(SUS)から成る被覆管内に中性子吸収材として
のB4C粉末を一様な密度分布で充填し、被覆管内
に一定間隔で粉末移動防止用の仕切球を配置して
構成されている。 A nuclear reactor control rod is constructed by loading a large number of neutron absorption rods into a plurality of wings formed by attaching an elongated U-shaped sheath to a central structural member. The above-mentioned neutron absorption rod generally has a cladding tube made of stainless steel (SUS) filled with B 4 C powder as a neutron absorbing material in a uniform density distribution, and partition balls are placed at regular intervals in the cladding tube to prevent powder movement. arranged and configured.
上記原子炉用制御棒は、多数の燃料集合体を装
荷した炉心に挿抜自在に配置され、原子炉の出力
を制御するために使用される。 The above-mentioned nuclear reactor control rods are arranged so as to be freely inserted into and removed from a reactor core loaded with a large number of fuel assemblies, and are used to control the output of the nuclear reactor.
ところで、沸騰水型原子炉(以下BWRと呼
ぶ)の燃料集合体にあつては、運転中冷却材の蒸
発によりボイドを生じる。このボイドの発生率は
炉心下部、中央部において小であり、上部におい
て大である。また燃料の燃焼度はボイド率の低い
所で大きく、高い所で小さい。ところが、炉心上
下端では中性子の洩れが大きいので、燃焼度の炉
心軸方向分布は、炉心下部が炉心中央部より小と
なり、炉心上部が下部よりも小となる。 By the way, in the fuel assembly of a boiling water nuclear reactor (hereinafter referred to as BWR), voids occur due to evaporation of coolant during operation. The incidence of voids is small in the lower and central parts of the core, and larger in the upper part. Also, the burnup of the fuel is large at low void ratios and small at high void ratios. However, since neutron leakage is large at the upper and lower ends of the core, the axial distribution of burnup is smaller in the lower part of the core than in the center of the core, and smaller in the upper part of the core than in the lower part.
すなわち原子炉炉心の軸方向長さをLとした場
合、下端から3/4Lの位置から上端にかけての上
端領域においては、運転時の気泡率(ボイド率)
が高く、炉の出力密度が若干低下するため、核分
裂性物質である質量数235のウラン(U―235)
の残存量が比較的多く、また発生する気泡(ボイ
ド)によつて中性子スペクトルの硬化現象を生じ
る。その結果、プルトニウム生成反応(中性子吸
収反応)が促進されるため、原子炉の運転後にお
いて炉心上部の核分裂核種濃度が高くなり、その
領域の原子炉停止余裕(未臨界度)が低下する。 In other words, when the axial length of the nuclear reactor core is L, in the upper end region from 3/4L from the lower end to the upper end, the air bubble ratio (void ratio) during operation is
uranium (U-235) with a mass number of 235, which is a fissile material,
The remaining amount of neutron is relatively large, and the generated bubbles (voids) cause a phenomenon of hardening of the neutron spectrum. As a result, the plutonium production reaction (neutron absorption reaction) is promoted, so the concentration of fission nuclides in the upper part of the reactor core increases after the reactor is operated, and the reactor shutdown margin (subcriticality) in that region decreases.
ここで原子炉停止余裕Δkは、原子炉が臨界状
態にある制御棒位置より全挿入したときに炉心に
加えられる反応度であり、原子炉を停止したとき
の炉心の中性子の実効増倍率keffとすると、下記
(1)式で定義される。 Here, the reactor shutdown margin Δk is the reactivity added to the reactor core when the control rods are fully inserted from the position where the reactor is in a critical state, and the effective multiplication factor of neutrons in the reactor when the reactor is shut down k eff Then, the following
Defined by equation (1).
Δk=1−keff ……(1)
この原子炉停止余裕は、原子炉の停止能力をは
かるる目安として管理上極めて重視される。通常
の原子炉では、原子炉を停止するため手段の一部
または全部として制御棒を炉心内に挿入する。こ
の場合原子炉停止余裕の基準として、万一最も反
応度効果(反応度価値ともいう)が大きい1本の
制御棒が挿入不能に陥つた場合でも、十分な余裕
をもつて停止できるような適切な原子炉停止余裕
があることが求められている。 Δk=1− keff ...(1) This reactor shutdown margin is extremely important for management purposes as a measure of the reactor's shutdown ability. In a typical nuclear reactor, control rods are inserted into the reactor core as part or all of the means to shut down the reactor. In this case, as a standard for the reactor shutdown margin, even if one control rod with the largest reactivity effect (also called reactivity value) becomes unable to be inserted, the reactor can be shut down with sufficient margin. It is required that there be sufficient margin for reactor shutdown.
一方、未臨界度ρは、一般に炉心の中性子の実
効増倍率keffを用いて下記(2)式で定義される。 On the other hand, the degree of subcriticality ρ is generally defined by the following equation (2) using the effective multiplication factor k eff of neutrons in the core.
ρ=(1−keff)/keff ……(2)
この未臨界度ρは、炉心に装荷された燃料の分
布組成、位置等によつて異なり、また原子炉停止
余裕は制御棒の炉心に対する挿入位置やその位置
における炉心組成の変化によつて変わり、双方と
も場所依存性を有する値である。そしてこの未臨
界度ρと上記原子炉停止余裕Δkとは必ずしも数
値的に正確に対応するものではない。しかし制御
棒挿入により原子炉が停止しているときの未臨界
度ρは、制御棒の反応度価値が大きい程大きく、
また原子炉停止余裕が大きいというほぼ比例した
相関関係を有することから、本発明の説明では、
原子炉の停止能力を計る目安として原子炉停止余
裕と未臨界度ρとを同等に使用する。 ρ=(1−k eff )/k eff ……(2) This subcriticality ρ varies depending on the distribution composition and position of the fuel loaded in the reactor core, and the reactor shutdown margin depends on the control rod core It changes depending on the insertion position and changes in the core composition at that position, and both values have location dependence. This degree of subcriticality ρ and the reactor shutdown margin Δk do not necessarily correspond numerically accurately. However, when the reactor is stopped due to control rod insertion, the degree of subcriticality ρ increases as the reactivity value of the control rod increases.
In addition, since there is an almost proportional correlation that the reactor shutdown margin is large, in the explanation of the present invention,
Reactor shutdown margin and subcriticality ρ are equally used as a guideline for measuring the reactor shutdown ability.
沸騰水型原子炉を所定期間運転すると、U―
235の燃焼の結果生じるPuの生成量は炉心下部で
中央部より少なく、炉心上部では下部より多くな
る。したがつて炉停止余裕(未臨界度)は第1図
Aに示すように、炉心上端より炉心全長Lの約1/
4領域のほぼ中央の位置Xにおいて最小となつて
いる。 When a boiling water reactor is operated for a specified period of time, U-
The amount of Pu produced as a result of the combustion of 235 is lower in the lower part of the core than in the middle, and more in the upper part of the core than in the lower part. Therefore, as shown in Figure 1A, the reactor shutdown margin (subcriticality) is approximately 1/1/1 of the total core length L from the top of the core.
The minimum value is reached at position X, which is approximately in the center of the four areas.
ところが、従来の制御棒はその有効長全長に亘
り中性子吸収材として、通常の反応度を有する
B4C粉末を均一な密度で被覆管に充填して形成さ
れており、軸方向の中性子吸収能力分布、すなわ
ち反応度がほぼ等しく調製されているため、さら
に運転後において高強度の中性子照射を受けて、
中性子吸収材の反応度が部分的に低下する場合が
あるため、原子炉停止に際して制御棒を挿入して
も、前記未臨界度の低い炉心上部で臨界をこえる
おそれがあり、原子炉を確実かつ安全に停止し得
ないおそれがあり得る。 However, conventional control rods act as neutron absorbers over their entire effective length and have normal reactivity.
It is formed by filling a cladding tube with B 4 C powder at a uniform density, and the neutron absorption capacity distribution in the axial direction, that is, the reactivity, is adjusted to be approximately equal, so it is possible to receive high-intensity neutron irradiation after operation. receive,
Since the reactivity of the neutron absorbing material may partially decrease, even if control rods are inserted to shut down the reactor, there is a risk that the upper part of the core, which has a low degree of subcriticality, will exceed criticality. There is a possibility that it may not be able to stop safely.
本発明は上記の事情に基づきなされたもので、
BWRを安全確実に停止させることができる原子
炉用制御棒を得ることを目的とする。 The present invention was made based on the above circumstances, and
The aim is to obtain a control rod for a nuclear reactor that can safely and reliably shut down a BWR.
本発明においては、燃焼度が低く未臨界度が小
となる炉心区域に、制御棒を全挿入した時にその
炉心区域に対向する制御棒の部分を高反応度とし
て前記目的を達成している。 In the present invention, when a control rod is fully inserted into a core region where burnup is low and subcriticality is small, the reactivity of the portion of the control rod facing the core region is high to achieve the above object.
ここで高反応度とは、制御棒の中性子吸収効果
が大きいことを意味し、特に本発明においては、
従来から一般的に使用されているステンレス鋼製
被覆管にB4C粉末を充填した中性子吸収棒を各シ
ース内に配列して構成した従来の原子炉用制御棒
と比較して中性子吸収効果が大きいことを意味す
る。 High reactivity here means that the control rod has a large neutron absorption effect, and in particular in the present invention,
Compared to conventional reactor control rods, which are constructed by arranging neutron absorption rods filled with B 4 C powder in a stainless steel cladding tube, which has been commonly used in the past, each sheath has a greater neutron absorption effect. It means big.
すなわち本発明に係る原子炉用制御棒は、中央
構造材に細長いU字状のシースを取付けて複数の
ウイングを形成し、被覆管内に中性子吸収材を充
填して形成した中性子吸収棒を上記ウイング内に
装填して成る原子炉用制御棒において、先端若干
長を除き、制御棒の全有効長の約1/4に当る先端
領域に位置する被覆管内部に、B4C粉末より中性
子吸収効果が大きい高反応度物質を充填する一
方、上記先端領域以外の領域に位置する被覆管内
部にB4C粉末を充填して構成される。 That is, the control rod for a nuclear reactor according to the present invention has a plurality of wings formed by attaching an elongated U-shaped sheath to a central structural member, and a neutron absorbing rod formed by filling a neutron absorbing material in a cladding tube to form a plurality of wings. In the control rod for a nuclear reactor, the B 4 C powder has a neutron absorption effect inside the cladding tube located at the tip region, which is about 1/4 of the total effective length of the control rod, excluding the slightly longer tip. The cladding tube is filled with a highly reactive material having a large amount of reactivity, while the inside of the cladding tube located in an area other than the above-mentioned tip area is filled with B 4 C powder.
上記構成によれば、原子炉用制御棒が炉心に全
挿入された場合に、本来未臨界度が特に小さくな
る炉心の上部領域に、高反応度物質を充填した制
御棒の先端領域が対向するため、炉心上部領域の
未臨界度すなわち原子炉停止余裕が増大し、原子
炉を安全確実に停止させることが可能となり、原
子炉プラトンの運転管理の安全性をより向上させ
ることができる。 According to the above configuration, when a reactor control rod is fully inserted into the reactor core, the tip region of the control rod filled with a highly reactive substance faces the upper region of the core where the degree of subcriticality is originally particularly small. Therefore, the degree of subcriticality in the upper region of the reactor core, that is, the reactor shutdown margin increases, making it possible to safely and reliably shut down the reactor, and further improving the safety of the operation management of the nuclear reactor Plato.
次に本発明の一実施例について添付図面を参照
して説明する。第2図において本実施例に係る断
面十字型の原子炉用制御棒1は、十字状の断面を
有する中央構造材2の各突出脚に細長いU字状断
面を有するシース3を取り付けて4枚のウイング
を形成し、各ウイング内に多数の中性子吸収棒4
を装填して形成される。 Next, an embodiment of the present invention will be described with reference to the accompanying drawings. In FIG. 2, the nuclear reactor control rod 1 having a cross-shaped cross section according to the present embodiment has four sheaths 3 each having an elongated U-shaped cross section attached to each protruding leg of a central structural member 2 having a cross-shaped cross section. neutron absorbing rods 4 are formed in each wing.
It is formed by loading.
そして制御棒の先端部から若干長l離れた位置
5から制御棒の全有効長Lの約1/4、すなわち
L/4の長さの先端領域6を他の領域と比較して
相対的に高反応度としている。 Then, a tip region 6 having a length of about 1/4 of the total effective length L of the control rod, that is, L/4, is relative to the other regions from a position 5 a little distance l from the tip of the control rod. It has a high reactivity.
すなわち上記先端領域6に位置する中性子吸収
棒4の被覆管内部Eu2O3ペレツトまたはB―10を
濃縮した濃縮10B4Cペレツトを充填することによ
り先端領域6を高反応度としている。一方、上記
先端領域6以外の領域に位置する被覆管内部に
は、通常の反応度を有するB4C粉末を充填してい
る。 That is, the tip region 6 is made to have a high reactivity by filling the inside of the cladding tube of the neutron absorption rod 4 located in the tip region 6 with Eu 2 O 3 pellets or concentrated 10 B 4 C pellets obtained by concentrating B-10. On the other hand, the inside of the cladding tube located in a region other than the tip region 6 is filled with B 4 C powder having a normal reactivity.
本実施例に係る原子炉用制御棒1を原子炉炉心
に全挿入した時の、炉心の未臨界度分布は第1図
Bに実線で示すようになる。 When the reactor control rod 1 according to this embodiment is fully inserted into the reactor core, the subcriticality distribution of the reactor core is as shown by the solid line in FIG. 1B.
すなわち第2図においてEu2O3または濃縮
10B4Cペレツトなどの高反応度物質を充填して高
反応度とした原子炉用制御棒1の先端領域6は、
未臨界都度が低くなる炉心上部領域に対向するた
め、炉心上部領域における中性子吸収能力すなわ
ち反応度を増大させる。したがつて炉心上部領域
の未臨界度すなわち原子炉停止余裕は改善され、
原子炉をより安全確実に停止することが可能とな
る。 That is, in Fig. 2, Eu 2 O 3 or enriched
The tip region 6 of the reactor control rod 1 is filled with a highly reactive substance such as 10 B 4 C pellets to have a high reactivity.
Since it is opposed to the upper core region where the frequency of subcriticality is lower, the neutron absorption capacity, that is, the reactivity in the upper core region is increased. Therefore, the subcriticality of the upper core region, that is, the margin for reactor shutdown, is improved,
It becomes possible to shut down the nuclear reactor more safely and reliably.
なお、本発明は上記実施例のみに限定されな
い。例えば、先端領域6に位置する中性子吸収棒
4の被覆管内に充填すべきEu2O3、濃縮10B4Cペ
レツトを、肉厚の小さなHf管内に充填して、そ
のHf管とともに中性子吸収棒の被覆管内に配置
してもよい。 Note that the present invention is not limited to the above embodiments. For example, Eu 2 O 3 and concentrated 10 B 4 C pellets to be filled in the cladding tube of the neutron absorption rod 4 located in the tip region 6 are filled in a small-walled Hf tube, and the neutron absorption rod is attached together with the Hf tube. It may be placed inside the cladding tube.
ここでHfは、中性子を複数回にわたり吸収し
ても、なお中性子吸収断面積が大きな同位体を形
成するため、一度の中性子吸収によつて吸収能力
を喪失するB4Cと比較して中性子吸収能力が長期
間にわたつて持続する。 Here, even if Hf absorbs neutrons multiple times, it still forms an isotope with a large neutron absorption cross section. Ability lasts for a long time.
この場合、先端領域6における制御棒の核的寿
命を延長させることができるだけでなく、
Eu2O3、濃縮10B4Cペレツトの中性子吸収による
性状変化に基づくスエリングをHf管と被覆管内
周面との微小な空隙で充分吸収できるため、制御
棒の機械的寿命をも向上させることができる。な
お、本発明においては、高価で比重の大きな
Eu2O3、Hf等を制御棒の先端領域6において部
分的に使用しているのみであるから、制御棒の価
格、重量等が著しく増大することはない。 In this case, not only can the nuclear life of the control rod in the tip region 6 be extended;
Swelling due to changes in properties due to neutron absorption of Eu 2 O 3 and enriched 10 B 4 C pellets can be sufficiently absorbed by the tiny gaps between the Hf tube and the inner circumferential surface of the cladding tube, thereby improving the mechanical life of the control rods. Can be done. In addition, in the present invention, expensive and large specific gravity
Since Eu 2 O 3 , Hf, etc. are only partially used in the tip region 6 of the control rod, the cost, weight, etc. of the control rod will not increase significantly.
そのため、従来の制御棒の荷重条件で設計建造
された既設の原子炉への適用も容易であり、また
交換費用も安価である。 Therefore, it is easy to apply to existing nuclear reactors designed and built under conventional control rod loading conditions, and replacement costs are low.
第1図Aは従来の制御棒を使用した場合におけ
るBWR炉心の運転停止時の軸方向未臨界界度分
布図、第1図Bは本発明に係る原子炉用制御棒を
使用したBWRの運転停止時の軸方向未臨界度分
布図、第2図は本発明に係る原子炉用制御棒の一
実施例を示す模式図である。
1……原子炉用制御棒、2……中央構造材、3
……シース、4……中性子吸収棒、6……先端領
域。
Figure 1A is an axial subcriticality distribution diagram at the time of shutdown of the BWR core when conventional control rods are used, and Figure 1B is the operation of a BWR using the reactor control rods according to the present invention. The axial subcriticality distribution diagram at the time of shutdown, FIG. 2 is a schematic diagram showing an embodiment of the nuclear reactor control rod according to the present invention. 1...Reactor control rod, 2...Central structural member, 3
...Sheath, 4...Neutron absorption rod, 6...Tip region.
Claims (1)
て複数のウイングを形成し、被覆管内に中性子吸
収材を充填して形成した中性子吸収棒を上記ウイ
ング内に装填して成る原子炉用制御棒において、
先端若干長を除き、制御棒の全有効長の約1/4に
当る先端領域に位置する被覆管内部に、B4C粉末
より中性子吸収効果が大きい高反応度物質を充填
する一方、上記先端領域以外の領域に位置する被
覆管内部にB4C粉末を充填したことを特徴とする
原子炉用制御棒。 2 高反応度物質は、Eu2O3ペレツトまたはB―
10を濃縮した濃縮10B4Cペレツトであることを特
徴とする特許請求の範囲第1項記載の原子炉用制
御棒。 3 Eu2O3ペレツトまたは10B4Cペレツトは、肉
厚が小さなHf管内に挿入され、Hf管とともに中
性子吸収棒の被覆管内に配置されたことを特徴と
する特許請求の範囲第2項記載の原子炉用制御
棒。[Claims] 1. A plurality of wings are formed by attaching an elongated U-shaped sheath to the central structural member, and a neutron absorbing rod formed by filling a cladding tube with a neutron absorbing material is loaded into the wing. In a nuclear reactor control rod consisting of
The inside of the cladding tube located at the tip area, which is about 1/4 of the total effective length of the control rod, excluding the slightly longer tip, is filled with a highly reactive material that has a greater neutron absorption effect than B 4 C powder. A control rod for a nuclear reactor, characterized in that the inside of a cladding tube located in an area other than the area is filled with B 4 C powder. 2 Highly reactive substances are Eu 2 O 3 pellets or B-
The control rod for a nuclear reactor according to claim 1, wherein the control rod is a concentrated 10 B 4 C pellet. Claim 2, characterized in that the 3 Eu 2 O 3 pellets or the 10 B 4 C pellets are inserted into an Hf tube with a small wall thickness, and are placed together with the Hf tube in a cladding tube of a neutron absorption rod. Control rods for nuclear reactors.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56126205A JPS5827092A (en) | 1981-08-12 | 1981-08-12 | Reactor control rod |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56126205A JPS5827092A (en) | 1981-08-12 | 1981-08-12 | Reactor control rod |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5827092A JPS5827092A (en) | 1983-02-17 |
| JPH0254518B2 true JPH0254518B2 (en) | 1990-11-21 |
Family
ID=14929309
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56126205A Granted JPS5827092A (en) | 1981-08-12 | 1981-08-12 | Reactor control rod |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5827092A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63215992A (en) * | 1987-03-04 | 1988-09-08 | 株式会社東芝 | Control-rod for nuclear reactor |
| JP3121543B2 (en) * | 1996-07-18 | 2001-01-09 | 株式会社日立製作所 | Control rods for boiling water reactors and boiling water reactor cores |
-
1981
- 1981-08-12 JP JP56126205A patent/JPS5827092A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5827092A (en) | 1983-02-17 |
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