JPS6144144B2 - - Google Patents
Info
- Publication number
- JPS6144144B2 JPS6144144B2 JP58232831A JP23283183A JPS6144144B2 JP S6144144 B2 JPS6144144 B2 JP S6144144B2 JP 58232831 A JP58232831 A JP 58232831A JP 23283183 A JP23283183 A JP 23283183A JP S6144144 B2 JPS6144144 B2 JP S6144144B2
- Authority
- JP
- Japan
- Prior art keywords
- neutron
- absorbing material
- neutron absorbing
- atomic
- amorphous
- 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
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
- Analysing Materials By The Use Of Radiation (AREA)
- Manufacture Of Metal Powder And Suspensions Thereof (AREA)
Description
[発明の技術分野]
本発明は中性子吸収材の改良に関する。
[発明の技術的背景とその問題点]
水冷却型原子炉における従来の中性子吸収材料
としてはボロンカーバイド(B4C)が特に用いら
れていることがよく知られている。このボロンカ
ーバイトは粉末であることから密閉容器内に約70
%の密度を保つて充填されていることが普通であ
る。この密閉容器は通常ポイズンチユーブと称さ
れるステンレス製の細長いチユーブより成りこの
中にボロンカーバイトが充填される。すなわち第
1図に示すように断面がほぼ円筒形にステンレス
鋼で形成されると共に、その内部には平均粒径約
100μのボロンカーバイトより成る中性子吸収材
粉体13が充填密封されている。この中性子吸収
材13は上記したように密度約70%で充填されて
いるのでその円筒内での粉体の移動は少ないが、
この移動を押えるために上記ポイズンチユーブ1
4内の中間部の各所にボール状の中性子吸収材移
動防止体10をポイズンチユーブ壁の一部を変形
させて固定してある。
さて上記ボロンカーバイトは粉体であることか
らその飛散を防止するためにも上記ポイズンチユ
ーブ14はその端部を封着体11によつて完全に
封着する必要がある。
ところが封有された中性子吸収材13は制御棒
に取り付けられて駆動した場合には上記ポイズン
チユーブ14内で移動が始まり上記移動防止体1
0の上方近辺にのみ集中してしまい、同図に示す
ように空間12が形成され易く極端な場合には中
性子吸収体13の下方には吸収体の存在がなくな
り、この部分での中性子吸収能力が失なわれてし
まい第2図曲線Aに示すように中性子吸収特性が
不均一となる場合があり中性子制御特性を劣化さ
せる一つの原因を作つている。
また、上記中性子吸収体13であるボロンカー
バイトは中性子吸収断面積が大きいので吸収材と
しては有利であるが、中性子と反応する(n,
α)反応即ち5B10+0n1=3Li7+2He4は発熱反応
でありボロンカーバイトはその発熱による温度上
昇とヘリウムガス発生により膨潤したポイズンチ
ユーブ内で上記の通り粉体の不所望の移動を起し
たり、チユーブ内の内圧を高くしたりして場合に
よつてはチユーブの破壊も発生する場合がある。
従つて上記中性子吸収材13を有するポイズンチ
ユーブではその寿命が短かいという難点がある。
またポイズンチユーブはチユーブ本体と中性子吸
収材と移動防止体とで形成されているので構成が
複雑であると共に粉体をチユーブ本体内に充填し
なければならないということ及び移動防止体をカ
シメ等の手段を用いて嵌挿固定する必要があるこ
と等から作業性が悪くなり易いという欠点もあ
る。
本発明は上記種々の難点を除去するように改良
したものである。
[発明の目的]
本発明の目的は中性子吸収元素が使用中に移動
しなく、かつ均一に分散するようにした中性子吸
収材を提供することである。
本発明の他の目的は構造が簡単である中性子吸
収材を提供することである。
本発明の更に他の目的は軽量化された中性子吸
収材を提供することである。
本発明の更に他の目的は製造が容易で作業性の
よい中性子吸収材を提供することである。
本発明の更に他の目的は寿命の長い中性子吸収
材を提供することである。
[発明の概要]
TM100-a-bADbREa
TMはFe,Niの少なくとも1種
REはSm,Gd,Er,Eu,Dyの少なくとも1種
ADはイ B 0〜10原子%
ロ Cr 0〜20原子%
ハ Rh,Re,In,Ag,Auの少なく
とも1種 0〜10原子%の前記イ),
ロ),ハ)の群から選ばれた少なくと
も1種
aは40〜70原子%
bは0〜40原子%
で示される非晶質合金からなる事を特徴とする中
性子吸収材である。
つまり本発明は中性子吸収断面積の大きい金属
を含む非晶質合金で中性子吸収材を形成したもの
である。すなわち結晶質では存在できない中性子
吸収断面積の大きい金属の成分比を非晶質にする
ことによつて数倍から数十倍に添加することが可
能となり、しかもリボン状の箔片が得られること
から軽量化が達成出来た。
また都合のよいことに箔状を呈し、かつ機械的
性質にも優れた中性子吸収材に形成出来ることも
判明した。上記を確認するために中性子吸収断面
積の大きい元素であるSm,Gd,Er,Eu,Dy等
の希土類元素を第2成分として40〜70%(原子
比)に第1成分である鉄(Fe)、ニツケル(Ni)
または鉄ニツケル元素を混合して非晶質合金を作
つた。この非晶質合金は巾約100mm厚さ約20〜80
μmの均一なリボン状に形成され、かつ中性子吸
収元素である上記希土類元素も均一に分散されて
いる中性子吸収材が得られる。
なお上記希土類元素の添加量は原子比で40%未
満では中性子吸収能力が期待出来ないので中性子
吸収材を多数重ね合わせて用いなければならなな
いので不経済である。また70%を越えると機械的
性質にも優れ且つ均一に上記希土類元素の分散し
た非晶質薄板を得ることは現在の技術力では困難
である。
上記希土類元素のSm,Gd,Er,Eu,Dyはい
ずれも中性子吸収能の高い元素であり、添加量の
上限は非晶質として存在できる最高値であり、下
限は最低値である。
また添加成分(AD)としてBを約10%以下、
Crを20%以下、Rh,Re,In,Ag,Auの少なく
とも1種を10%以下を加えて非晶質合金性中性子
吸収材を形成することが出来る。この場合これら
の添加成分の合計が約40%を越えないように監視
する必要がある。
Crは耐蝕性向上の為に添加するものであり、
Rh,Re,In,Ag,Auは中性子吸収能の高い元
素である為に添加するものである。それぞれの上
限は非晶質として安定性良く存在し得る最高添加
量である。
上記はいずれも中性子吸収能力が全体的に均一
であると共に箔状リボンとなつて軽量化が計られ
中性子吸収元素の不所望な移動もないこと、ある
いは非晶質合金化するのみで中性子吸収元素を分
散配置することが出来るので製造が容易であるこ
とが確認された。また中性子吸収元素は非晶質に
すると上記のように結晶質の場合と比較して数十
倍も多量に入れられるがこれにも限度があるが、
更に能力を増大するために他の元素を入れること
によつて従来と比較にならないほど多量に分散出
来るという特徴を有する。
[発明の実施例]
次に実施例について説明する。
実施例 1
中性子吸収断面積の大きい元素としてサマリウ
ム(Sm)を原子比で40%、ニツケル(Ni)を同
40%及び鉄(Fe)を同じく20%を混合してこれ
を第3図の如く石英製容器1で1250℃に加熱装置
2によつて加熱容融する。この溶融合金を直径
0.4mmのノズル5から0.2気圧の圧力を押し出すと
共に直径200mmの回転圧延ローラ3,3の間に挿
入して2000rmpの高速回転で急冷し巾3mm、厚さ
40μmのリボン状非晶質合金製中性子吸収材5を
形成した。
これはサマリウムの中性子吸収断面積が大きい
のでこれが中性子吸収材に均一に分散しているの
で、原子炉の制御棒に用いられて中性子の吸収能
力を能率よく発揮すると共に中性子による反応に
おいても不所望な移動がないので寿命も長いとい
う特徴がある。又第1図のポイズンチユーブと同
様の長さのリボンを形成し中性子吸収能を測定し
た結果、第2図曲線Bに示す如く極めて均一な吸
収能力を有する事が確認された。
実施例 2
原子比でボロン(B)10%、クロム(Cr)15
%、ジスプロシウム(Dy)55%、残りが鉄
(Fe)として第1実施例と同様な方法で非晶質合
金化して非晶質合金製中性子吸収材を形成した。
この場合はクロムの作用により耐蝕安定性もよく
中性子の吸収が出来るという特徴を有する。
実施例 3
原子比でボロン(B)5%、クロム(Cr)10
%、ユウロピユウム(Eu)50%、レニウム
(Re)5%、ニツケル(Ni)10%、残りが鉄
(Fe)から成る合金を上記のようにに非晶質合金
化して非晶質合金製中性子吸収材を作つた。この
場合も上記同様の効果を得た。
次に上記実施例を含め、各種組成の非晶質合金
の中性子吸収断面積を従来のB4C及び近年使用の
検討されているHfとの比で第1表に示す。
[Technical Field of the Invention] The present invention relates to improvements in neutron absorbers. [Technical background of the invention and its problems] It is well known that boron carbide (B 4 C) is particularly used as a conventional neutron absorbing material in water-cooled nuclear reactors. Since this boron carbide is a powder, it is stored in a sealed container for approximately 70 minutes.
% density is usually maintained. This airtight container consists of an elongated tube made of stainless steel, usually called a poison tube, into which boron carbide is filled. In other words, as shown in Figure 1, it is made of stainless steel and has an almost cylindrical cross section, and inside it is made of stainless steel with an average grain size of approximately
A neutron absorbing material powder 13 made of 100μ boron carbide is filled and sealed. As described above, this neutron absorbing material 13 is filled with a density of about 70%, so there is little movement of powder within the cylinder.
In order to suppress this movement, the above poison tube 1
Ball-shaped neutron absorbing material movement preventers 10 are fixed at various locations in the intermediate portion of the poison tube 4 by deforming a portion of the poison tube wall. Since the boron carbide is a powder, it is necessary to completely seal the ends of the poison tube 14 with the sealing body 11 in order to prevent it from scattering. However, when the sealed neutron absorber 13 is attached to a control rod and driven, it begins to move within the poison tube 14 and the movement preventer 1
As shown in the figure, a space 12 is likely to be formed, and in an extreme case, there is no absorber below the neutron absorber 13, and the neutron absorption capacity in this area decreases. As a result, the neutron absorption characteristics may become non-uniform as shown in curve A in Figure 2, which is one of the causes of deterioration of the neutron control characteristics. In addition, boron carbide, which is the neutron absorber 13, has a large neutron absorption cross section and is therefore advantageous as an absorber, but it reacts with neutrons (n,
α) Reaction, 5B10 + 0n 1 = 3Li 7 + 2He 4 , is an exothermic reaction, and boron carbide may cause undesired movement of the powder in the swollen poison tube due to the temperature rise due to the heat generation and the generation of helium gas, as described above. In some cases, the tube may be destroyed by increasing the internal pressure inside the tube.
Therefore, the poison tube having the above-mentioned neutron absorbing material 13 has the disadvantage that its lifespan is short.
Furthermore, since the poison tube is made up of a tube body, a neutron absorbing material, and a movement prevention body, the structure is complicated, and the powder must be filled into the tube body, and the movement prevention body must be crimped or other means. There is also the drawback that workability tends to deteriorate because it is necessary to insert and fix the device using a screw. The present invention has been improved to eliminate the various drawbacks mentioned above. [Object of the Invention] An object of the present invention is to provide a neutron absorbing material in which a neutron absorbing element does not move during use and is uniformly dispersed. Another object of the present invention is to provide a neutron absorber having a simple structure. Still another object of the present invention is to provide a neutron absorbing material that is lightweight. Still another object of the present invention is to provide a neutron absorbing material that is easy to manufacture and has good workability. Yet another object of the present invention is to provide a neutron absorber with a long lifetime. [Summary of the invention] TM 100-ab AD b RE a TM is at least one of Fe and Ni RE is at least one of Sm, Gd, Er, Eu, and Dy AD is A B 0-10 atomic% b Cr 0- 20 atomic% C At least one of Rh, Re, In, Ag, Au 0 to 10 atomic% of the above a),
The neutron absorbing material is characterized by being made of at least one amorphous alloy selected from the groups b) and c), in which a represents 40 to 70 atomic % and b represents 0 to 40 atomic %. That is, in the present invention, a neutron absorbing material is formed of an amorphous alloy containing a metal having a large neutron absorption cross section. In other words, by making the component ratio of a metal with a large neutron absorption cross section, which cannot exist in a crystalline state, into an amorphous state, it becomes possible to add several times to several tens of times more, and ribbon-shaped foil pieces can be obtained. We were able to achieve weight reduction. It has also been found that it can conveniently be formed into a neutron absorbing material that is foil-like and has excellent mechanical properties. To confirm the above, rare earth elements such as Sm, Gd, Er, Eu, and Dy, which are elements with large neutron absorption cross sections, are used as the second component, and 40 to 70% (atomic ratio) of the first component is iron (Fe). ), Nickel (Ni)
Alternatively, an amorphous alloy was made by mixing iron-nickel elements. This amorphous alloy is about 100mm wide and about 20~80mm thick.
A neutron absorbing material is obtained which is formed into a uniform ribbon shape with a diameter of μm and in which the above-mentioned rare earth element, which is a neutron absorbing element, is also uniformly dispersed. Note that if the amount of the rare earth element added is less than 40% in terms of atomic ratio, neutron absorption ability cannot be expected, and therefore a large number of neutron absorbing materials must be stacked and used, which is uneconomical. Furthermore, if it exceeds 70%, it is difficult with current technology to obtain an amorphous thin plate with excellent mechanical properties and in which the rare earth element is uniformly dispersed. The above-mentioned rare earth elements Sm, Gd, Er, Eu, and Dy are all elements with high neutron absorption ability, and the upper limit of the amount added is the maximum value that can exist as an amorphous state, and the lower limit is the minimum value. In addition, approximately 10% or less of B as an additive component (AD),
An amorphous alloy neutron absorbing material can be formed by adding 20% or less of Cr and 10% or less of at least one of Rh, Re, In, Ag, and Au. In this case, it is necessary to monitor so that the total of these added components does not exceed about 40%. Cr is added to improve corrosion resistance.
Rh, Re, In, Ag, and Au are added because they are elements with high neutron absorption ability. Each upper limit is the maximum amount that can be added in an amorphous state with good stability. All of the above have a uniform neutron absorption capacity as a whole, and are made into a foil-like ribbon to reduce weight, and there is no undesired movement of the neutron-absorbing element, or the neutron-absorbing element is only made into an amorphous alloy. It was confirmed that manufacturing is easy because the components can be distributed and arranged. Furthermore, when the neutron-absorbing element is made amorphous, it can be contained in an amount several tens of times more than when it is crystalline, as mentioned above, but there is a limit to this.
Furthermore, by adding other elements to increase the ability, it has the characteristic that it can be dispersed in an incomparably large amount compared to conventional methods. [Embodiments of the Invention] Next, embodiments will be described. Example 1 As an element with a large neutron absorption cross section, samarium (Sm) was used at an atomic ratio of 40%, and nickel (Ni) was used at the same rate.
40% and iron (Fe), also 20%, were mixed and heated and melted in a quartz container 1 to 1250° C. using a heating device 2, as shown in FIG. This molten alloy has a diameter
A pressure of 0.2 atm is extruded from a 0.4 mm nozzle 5, and it is inserted between rotating rolling rollers 3 and 3 with a diameter of 200 mm, and is rapidly cooled at a high speed of 2000 rpm to a width of 3 mm and a thickness.
A 40 μm ribbon-shaped neutron absorbing material 5 made of an amorphous alloy was formed. Since samarium has a large neutron absorption cross section, it is uniformly dispersed in the neutron absorbing material, so it is used in the control rods of nuclear reactors to efficiently exert its neutron absorption ability, and it also prevents undesirable reactions in neutron reactions. Since there is no physical movement, it has a long lifespan. Further, as a result of forming a ribbon having the same length as the poison tube shown in FIG. 1 and measuring its neutron absorption ability, it was confirmed that the ribbon had an extremely uniform absorption ability as shown by curve B in FIG. Example 2 Boron (B) 10%, chromium (Cr) 15% in atomic ratio
%, dysprosium (Dy) 55% and the remainder iron (Fe) to form an amorphous alloy in the same manner as in the first example to form an amorphous alloy neutron absorbing material.
In this case, due to the action of chromium, it has good corrosion resistance and stability and is able to absorb neutrons. Example 3 Boron (B) 5%, chromium (Cr) 10 in atomic ratio
%, 50% europium (Eu), 5% rhenium (Re), 10% nickel (Ni), and the balance is made into an amorphous alloy as described above to produce an amorphous alloy neutron. I made an absorbent material. In this case as well, the same effect as above was obtained. Next, Table 1 shows the neutron absorption cross sections of amorphous alloys of various compositions, including the above examples, in comparison with conventional B 4 C and Hf, which has been considered for use in recent years.
【表】【table】
【表】
この結果から明らかな如くB4C自体の中性子吸
収能よりは劣る場合もあるが、前記第2図に示し
た如く済めて均一な吸収能が得られ実用上は有効
なものと言える。
[発明の効果]
本発明中性子吸収材は上記で明らかなように中
性子吸収断面積の大きい元素を十分に合金化し得
る非晶質合金で形成することによつて非晶質の特
徴を生かして中性子吸収能力の高い中性子吸収材
を得ることが出来た。すなわち従来合金になりに
くい中性子吸収断面積の大きい金属の成分混合比
を結晶質では成形不可能とされていた混合比まで
添加することが非晶質にすることによつて始めて
得られた。そしてさらに上記中性子吸収材は20〜
80μmの厚であつて箔状でしかも機械的強度が強
く、加工性がよく任意形状に成形出来る。更に上
記中性子吸収元素は非晶質合金中に均一に分散し
ているので中性子吸収能力が均一化されていてし
かも中性子との反応等によつて移動することがな
く長期にわたつて所期の特性を維持出来るので長
寿命化が可能となつた。
また20〜80μmという極めて薄い箔状となつて
いるので中性子吸収材としても重量がポイズンチ
ユーブ等に対し格段に相違して軽量化されるとい
う特徴がある。
上記本発明中性子吸収材は次のように用いて好
適な結果が得られる。
先ず制御棒の中性子吸収材として用いることが
出来る。この場合種々の点で極めて有利である。
従来のボロンカーバイド入りポイズンチユーブ
に代えて本発明中性子吸収材を用いると、その構
造が一変して極めて簡略化され、ポイズンチユー
ブ、ブレード等を不用とし、一つの支持枠だけで
たりる。また必要に応じて上記中性子吸収材を積
層して、その能力を調整することが出来る。これ
は中性子吸収材の厚さが極めて薄い箔状である点
を巧みに利用することが出来る。更にその能力を
部分的に変化したい場合には中性子吸収材の積層
を部分的に変化させることによつて容易に得られ
るという特徴もある。このように積層しても軽量
であるから制御棒が大型化するおそれは全くな
い。また軽量化された制御棒は駆動が容易となり
駆動機構が簡略されると共にスピードリミツタを
省くことが可能となる。この場合の使用温度は約
280℃であり、上記中性子吸収材の結晶化温度は
約400℃以上もあるので、中性子吸収元素の不所
望な作用低下はほとんどない。
また臨床の中性子遮蔽材としても使用すること
が出来る。すなわち、上記中性子吸収材は箔状で
あるということ機械的強度がすぐれていること、
及び加工性に極めて優れていることの利を生かし
て例えば中性子吸収材を300〜400mmの巾の広いも
ので作り、この一部にプレス等で透孔を設け、こ
の透孔を介して中性子を疾患部に照射する場合に
他の部分を中性子から保護する場合に利用出来
る。
すなわち、例えばガン治療に中性子を患部に照
射して使用する場合である。この場合に患部のみ
に照射してガン細胞を絶滅させる等を行つている
がこのガン細胞以外の正常組織が中性子照射を受
けない様に遮蔽体として用いることが出来る。こ
の場合、上記中性子吸収材は薄いので照射部に密
接保持出来るから患部以外の部分を能率よく保護
し得るという特徴を有する。
なお鉛を含むγ線遮蔽材と本発明上記中性子吸
収材とを併用した中性子及びγ線遮蔽体を作るこ
とが出来る。この場合も非晶質の柔軟性を生かし
て組み込みして極めて効果がある。
現用の原子炉使用済燃料は、放射能が高く廃棄
物として処理あるいは再使用の為に回収するまで
に数年間使用済燃料ラツクの水槽の中に保管し放
射能低減を待つ。その際、燃料集合体の型で水槽
の中に保管し、集合体と集合体の間にはボロン入
アルミニウムが間仕切りとして挿入されており、
飛び出して来た中性子を吸収し該反応が起こらな
い様にしている。集合体と集合体の間仕切りに本
発明の非晶質中性子吸収材のうち中性子吸収断面
積の大きい元素を添加した吸収材を使用すると集
合体と集合体の距離を短縮することが出来る。こ
れは益々需要の高まる原子力発電に伴なう使用済
燃料の保管に使用済燃料ラツク容積拡大に対して
経済的に貢献する。[Table] As is clear from this result, the neutron absorption capacity is sometimes inferior to the neutron absorption capacity of B 4 C itself, but it can be said that it is practically effective as it can obtain a uniform absorption capacity as shown in Figure 2 above. . [Effects of the Invention] As is clear from the above, the neutron absorbing material of the present invention is made of an amorphous alloy that can sufficiently alloy elements with a large neutron absorption cross section, thereby making use of its amorphous characteristics to absorb neutrons. We were able to obtain a neutron absorbing material with high absorption capacity. That is, it was only possible to add a metal with a large neutron absorption cross section, which is difficult to form into an alloy, to a mixing ratio that was considered impossible to form in a crystalline material by making it amorphous. Furthermore, the above neutron absorbing material is 20~
It is 80 μm thick, foil-like, has strong mechanical strength, and has good workability and can be molded into any shape. Furthermore, since the above-mentioned neutron-absorbing elements are uniformly dispersed in the amorphous alloy, the neutron-absorbing ability is uniform, and they do not migrate due to reactions with neutrons, so the desired characteristics can be maintained over a long period of time. This makes it possible to extend the service life. Furthermore, since it is in the form of an extremely thin foil of 20 to 80 μm, it has the advantage of being much lighter in weight as a neutron absorbing material, compared to poison tubes and the like. The above-mentioned neutron absorbing material of the present invention can be used in the following manner to obtain suitable results. First, it can be used as a neutron absorber in control rods. This case is extremely advantageous in various respects. When the neutron absorbing material of the present invention is used in place of the conventional boron carbide-containing poison tube, the structure is completely changed and extremely simplified, eliminating the need for poison tubes, blades, etc., and requiring only one support frame. Further, the ability of the neutron absorbing material can be adjusted by laminating the neutron absorbing materials as necessary. This can be done by taking advantage of the fact that the neutron absorbing material is extremely thin in the form of a foil. Furthermore, if it is desired to partially change the ability, this can be easily achieved by partially changing the lamination of the neutron absorbing material. Even if they are stacked in this way, there is no risk of the control rod becoming larger because it is lightweight. Furthermore, the lighter control rod is easier to drive, the drive mechanism is simplified, and a speed limiter can be omitted. The operating temperature in this case is approx.
280° C., and the crystallization temperature of the neutron absorbing material is about 400° C. or higher, so there is almost no undesirable decrease in the effect of the neutron absorbing element. It can also be used as a clinical neutron shielding material. In other words, the neutron absorbing material is foil-shaped and has excellent mechanical strength.
Taking advantage of its excellent workability, for example, a neutron absorbing material is made of a wide material with a width of 300 to 400 mm, a hole is formed in a part of the material using a press, etc., and neutrons are absorbed through this hole. It can be used to protect other areas from neutrons when irradiating diseased areas. That is, for example, when neutrons are used to irradiate an affected area in cancer treatment. In this case, neutrons are irradiated only to the affected area to exterminate cancer cells, but neutrons can be used as a shield to prevent normal tissues other than cancer cells from receiving neutron irradiation. In this case, since the neutron absorbing material is thin, it can be held closely to the irradiated area, so that it can efficiently protect areas other than the affected area. Note that it is possible to make a neutron and gamma ray shielding body using a gamma ray shielding material containing lead and the neutron absorbing material of the present invention in combination. In this case as well, it is extremely effective to incorporate the material by taking advantage of the flexibility of the amorphous material. Spent fuel from current nuclear reactors is highly radioactive and is stored in a tank in a spent fuel rack for several years to reduce its radioactivity before it can be treated as waste or recovered for reuse. At that time, the fuel assemblies are stored in a water tank, and boron-containing aluminum is inserted between the assemblies as a partition.
It absorbs the neutrons that fly out and prevents the reaction from occurring. If an absorbing material containing an element having a large neutron absorption cross section among the amorphous neutron absorbing materials of the present invention is used as a partition between the aggregates, the distance between the aggregates can be shortened. This will economically contribute to expanding the capacity of spent fuel racks for storing spent fuel due to the ever-increasing demand for nuclear power generation.
第1図は従来の中性子吸収材であるポイズンチ
ユーブの一部を断面して内部を示す側面図、第2
図はその中性子吸収能力特性図、第3図は本発明
に係る中性子吸収材の製造装置の一部を示す側面
図である。
Figure 1 is a side view showing the inside of a poison tube, which is a conventional neutron absorbing material, partially cut away.
The figure is a characteristic diagram of its neutron absorption capacity, and FIG. 3 is a side view showing a part of the neutron absorbing material manufacturing apparatus according to the present invention.
Claims (1)
性子吸収材。 2 TM100-a-bADbREa TMはFe,Niの少なくとも1種 REはSm,Gd,Er,Eu,Dyの少なくとも1種 ADはイ B0を超え10原子%以下 ロ Cr0を超え20原子%以下 ハ Rh,Re,In,Ag,Auの少なく
とも1種0を超え10原子%以下の前記
イ),ロ),ハ)の群から選ばれた少な
くとも1種 aは40〜70原子% bは40原子%以下 で示される非晶質合金からなる事を特徴とする中
性子吸収材。[Claims] 1 TM 100-a RE a TM is at least one of Fe and Ni RE is at least one of Sm, Gd, Er, Eu, and Dy A is an amorphous alloy represented by 40 to 70 atomic % A neutron absorbing material characterized by comprising: 2 TM 100-ab AD b RE a TM is at least one of Fe and Ni RE is at least one of Sm, Gd, Er, Eu, and Dy AD is A Exceeds B0 and 10 atomic% or less B Exceeds Cr0 and 20 atomic% (c) At least one of Rh, Re, In, Ag, and Au selected from the group of (a), (b), and (c) above, exceeding 0 and up to 10 atomic %; a is 40 to 70 atomic %; b is A neutron absorbing material characterized by being made of an amorphous alloy with a content of 40 atomic % or less.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58232831A JPS59133345A (en) | 1983-12-12 | 1983-12-12 | Neutron absorber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58232831A JPS59133345A (en) | 1983-12-12 | 1983-12-12 | Neutron absorber |
Related Parent Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55185100A Division JPS5952225B2 (en) | 1980-12-27 | 1980-12-27 | Neutron absorber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59133345A JPS59133345A (en) | 1984-07-31 |
| JPS6144144B2 true JPS6144144B2 (en) | 1986-10-01 |
Family
ID=16945468
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58232831A Granted JPS59133345A (en) | 1983-12-12 | 1983-12-12 | Neutron absorber |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59133345A (en) |
-
1983
- 1983-12-12 JP JP58232831A patent/JPS59133345A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59133345A (en) | 1984-07-31 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| EP0055371A1 (en) | Neutron absorber, neutron absorber assembly utilizing the same, and other uses thereof | |
| JP2543973B2 (en) | Fuel element with oxidation resistant coating | |
| JP3094778B2 (en) | Fuel assembly for light water reactor, parts and alloys used therefor, and manufacturing method | |
| CN113851233B (en) | Radial shielding structure of molten salt reactor and molten salt reactor comprising radial shielding structure | |
| JPH0371078B2 (en) | ||
| US4663110A (en) | Fusion blanket and method for producing directly fabricable fissile fuel | |
| JPS603584A (en) | Control rod for nuclear reactor | |
| RU2663222C2 (en) | Device and method of obtaining sources of gamma-radiation from enriched iridium | |
| KR101754754B1 (en) | Storage container for spent nuclear fuel | |
| US5642390A (en) | Uranium-containing nuclear-fuel sintered pellet | |
| Foster et al. | 316 stainless steel cavity swelling in a PWR | |
| JPH07191176A (en) | Fast neutron atomic reactor wherein at least one kind of coolant is integrated into atomic reactor aggregate | |
| JPS5952225B2 (en) | Neutron absorber | |
| JPS6144144B2 (en) | ||
| JPH0827388B2 (en) | Heat resistant radiation shielding material | |
| JPS6256946B2 (en) | ||
| US3663366A (en) | Shroud for a fuel assembly in a nuclear reactor | |
| JP2017537321A (en) | Flexible irradiation equipment | |
| CN113674875A (en) | Fast spectrum reactor core design method and reactor core structure | |
| US3725663A (en) | Internally moderated heat sources and method of production | |
| KR102918596B1 (en) | neutron absorbing materials with improved neutron absorption capability and thermal conductivity | |
| RU2035076C1 (en) | Source of gamma radiation provided with active core and method for manufacturing same | |
| JPS5960286A (en) | Neutron absorber | |
| JPH0134358B2 (en) | ||
| US3567581A (en) | Uranium-silicon fuel elements for a nuclear reactor |