JPH0222355B2 - - Google Patents
Info
- Publication number
- JPH0222355B2 JPH0222355B2 JP56145891A JP14589181A JPH0222355B2 JP H0222355 B2 JPH0222355 B2 JP H0222355B2 JP 56145891 A JP56145891 A JP 56145891A JP 14589181 A JP14589181 A JP 14589181A JP H0222355 B2 JPH0222355 B2 JP H0222355B2
- Authority
- JP
- Japan
- Prior art keywords
- test piece
- mev
- pressure vessel
- reactor pressure
- energy
- 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
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)
- Measurement Of Radiation (AREA)
Description
【発明の詳細な説明】
本発明は、原子炉圧力容器の供用期間中の健全
性を監視するために原子炉圧力容器の中性子照射
量を精度よく測定するための原子炉圧力容器監視
試験片に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a reactor pressure vessel monitoring test piece for accurately measuring the amount of neutron irradiation in the reactor pressure vessel in order to monitor the health of the reactor pressure vessel during its service life. .
従来、原子炉圧力容器内には原子炉圧力容器の
鋼材が速中性子の照射により機械的性質の変化を
受けるので、その影響を調べるために原子炉圧力
容器監視試験片が設置されている。 Conventionally, reactor pressure vessel monitoring test pieces have been installed inside the reactor pressure vessel in order to investigate the effects of fast neutron irradiation on the steel materials of the reactor pressure vessel, which undergo changes in their mechanical properties.
機械的性質の変化を調べるためのこの試験片
は、原子炉圧力容器製造時にそれと同一の鋼材か
ら採取され、ある一定期間原子炉圧力容器内で中
性子照射を受けたのち原子炉圧力容器から取り出
され機械的試験に供される。 This test piece, which is used to examine changes in mechanical properties, is taken from the same steel material used during the manufacture of the reactor pressure vessel, exposed to neutron irradiation within the reactor pressure vessel for a certain period of time, and then removed from the reactor pressure vessel. Subjected to mechanical testing.
試験片の機械的影響と中性子照射量の相関関係
を知るために試験片が受けた中性子照射量を測定
するが、その中性子照射量測定用の試験片は、所
謂モニタワイヤと呼ばれるもので、通常高純度の
Ni,Fe,Cu金属を線状にしたものである。 The amount of neutron irradiation received by the test piece is measured in order to find out the correlation between the mechanical influence of the test piece and the amount of neutron irradiation.The test piece used to measure the amount of neutron irradiation is what is called a monitor wire, High purity
It is a wire made of Ni, Fe, and Cu metals.
これらのモニタワイヤは原子炉圧力容器内で中
性子照射を受けると、金属中の一部の同位元素と
中性子との核反応により放射性同位元素を生成す
る。原子炉停止後にモニタワイヤを原子炉圧力容
器から取り出し、これらの放射性同位元素のうち
各元素毎に特有のエネルギを持つガンマ線の強度
をGe(Li)半導体検出器等の測定装置を用いて測
定し、その放射能強度を求めれば、監視試験片が
原子炉圧力容器内で実際に受けた中性子照射量を
求めることができ、これにより原子炉圧力容器が
受けた中性子照射量を推定することができる。 When these monitor wires are irradiated with neutrons in a nuclear reactor pressure vessel, radioactive isotopes are produced by a nuclear reaction between some isotopes in the metal and neutrons. After the reactor is shut down, the monitor wire is removed from the reactor pressure vessel and the intensity of gamma rays, which have energy specific to each element among these radioactive isotopes, is measured using a measuring device such as a Ge(Li) semiconductor detector. By determining the radioactivity intensity, it is possible to determine the amount of neutron irradiation that the monitoring test piece actually received inside the reactor pressure vessel, and from this it is possible to estimate the amount of neutron irradiation that the reactor pressure vessel received. .
一般に、中性子の照射による鋼材に対する機械
的性質への影響は中性子のエネルギが0.1〜
1MeVの範囲の速中性子によるものであると云わ
れているため、中性子照射量測定用の監視試験片
については速中性子との核反応のみで生成される
放射性物質のみを考慮すればよく、しかも試験片
の材質はGe(Li)半導体検出器等での放射能測定
が容易なものでなければならない。 In general, the influence of neutron irradiation on the mechanical properties of steel materials is that the neutron energy is 0.1~
It is said that fast neutrons in the 1 MeV range are responsible for the radiation, so when it comes to monitoring test pieces for measuring neutron irradiation, it is only necessary to consider radioactive substances produced only by nuclear reactions with fast neutrons, and the test The material of the piece must be one that makes it easy to measure radioactivity with a Ge(Li) semiconductor detector, etc.
そこで、従来から中性子照射量測定用として前
述のNi,Fe,Cuワイヤが用いられてきた。すな
わち、第1図の試験片の核反応断面積グラフに示
すようにNiワイヤでは主に2MeV以上の速中性
子による58Ni(n,p)反応、Feワイヤでは主に
2MeV以上の速中性子による54Fe(n,p)反応
及びCuワイヤでは主に6MeV以上の速中性子に
よる63Cu(n,α)反応で生成される放射性同位
元素である58Co,54Mn及び60Coα放射能が利用さ
れている。 Therefore, the aforementioned Ni, Fe, and Cu wires have traditionally been used for measuring neutron irradiation. In other words, as shown in the graph of the nuclear reaction cross section of the test piece in Figure 1, Ni wires mainly undergo 58 Ni(n,p) reactions due to fast neutrons of 2 MeV or higher, while Fe wires mainly undergo 58 Ni(n,p) reactions.
58 Co, 54 Mn and 60 are radioactive isotopes produced mainly by the 54 Fe (n, p) reaction caused by fast neutrons of 2 MeV or more and the 63 Cu (n, α) reaction caused by fast neutrons of 6 MeV or more in Cu wire. Coα radioactivity is used.
しかし、これらの反応は中性子のエネルギが
2MeV及び6MeV以上のものに限られ2MeV以下
には測定不可能範囲l0が存在し、測定される中性
子照射量についてもこのエネルギ以上のものに限
られ、本来必要とする0.1〜1MeVの範囲の速中
性子照射量の推定には、計算等による方法でエネ
ルギ範囲の補正をする必要があつた。 However, these reactions require the energy of the neutron to
It is limited to 2 MeV and 6 MeV or above, and there is an unmeasurable range l 0 below 2 MeV, and the measured neutron irradiation amount is also limited to those above this energy, and it cannot be measured within the originally required range of 0.1 to 1 MeV. In order to estimate the fast neutron irradiation dose, it was necessary to correct the energy range using methods such as calculations.
本発明は、かかる点に鑑み、0.1〜1MeVの範
囲の速中性子照射量をエネルギ範囲の補正を必要
とせずに直接推定できる原子炉圧力容器監視試験
片を提供することを目的とする。 In view of this, an object of the present invention is to provide a reactor pressure vessel monitoring test piece that can directly estimate the fast neutron irradiation dose in the range of 0.1 to 1 MeV without requiring correction of the energy range.
この目的は、核分裂物質を容器内に密封するこ
とによつて達成される。 This objective is achieved by sealing the fissile material within a container.
本発明による監視試験片は従来の機械的性質の
変化を監視する試験片及び中性子照射量測定用の
モニタワイヤに加えて、速中性子による核分裂を
起す核分裂物質を密封した容器に収納したもので
ある。 The monitoring test piece according to the present invention includes, in addition to the conventional test piece for monitoring changes in mechanical properties and a monitor wire for measuring neutron irradiation, a fissile material that causes nuclear fission due to fast neutrons is housed in a sealed container. .
このような監視試験片による速中性子照射量の
測定においては、数MeV以上のエネルギの中性
子による照射量は従来のモニタワイヤの放射能測
定から得られ、小さなエネルギすなわち0.1〜
1MeVのエネルギの中性子による照射量は核分裂
物質中の核分裂生成物の放射能測定から得ること
が可能となる。 In measuring the fast neutron irradiation dose using such a monitoring test piece, the irradiation dose due to neutrons with an energy of several MeV or more can be obtained from the conventional radioactivity measurement of a monitor wire, and the irradiation dose due to neutrons with an energy of several MeV or more can be obtained from the radioactivity measurement of a conventional monitor wire, and the irradiation dose with a small energy, that is, 0.1~
The irradiation dose by neutrons with an energy of 1 MeV can be obtained from radioactivity measurements of fission products in fissile materials.
たとえば、核分裂物質として238U,237Np及び
232Thを選定すれば、第2図に示すように238U及
び237Npは約2MeV以上、232Thは約0.1MeV以上の
中性子による反応で核分裂を起すので、この結果
生成される核分裂生成物は各種の放射性同位元素
を含み、その生成量は核分裂数によつて一義的に
決定される。原子炉停止後、監視試験片を原子炉
圧力容器から取り出し、放射能強度の測定が容易
な137Csが放出するガンマ線の強度をGe(Li)半
導体検出器等で測定し、放射能強度を求めれば試
験片の核分裂物質が受けた0.1MeV〜2MeVの範
囲のエネルギの中性子照射量を容易に推定するこ
とが可能である。 For example, fissile materials such as 238 U, 237 Np and
If 232 Th is selected, as shown in Figure 2, 238 U and 237 Np will undergo nuclear fission due to a reaction with neutrons of approximately 2 MeV or higher, and 232 Th will undergo nuclear fission through a reaction with neutrons of approximately 0.1 MeV or higher, so the resulting fission products will be Contains various radioactive isotopes, the amount of which is produced is uniquely determined by the number of nuclear fission. After the reactor is shut down, the monitoring test piece is removed from the reactor pressure vessel, and the intensity of gamma rays emitted by 137 Cs, which is easy to measure, is measured using a Ge(Li) semiconductor detector, etc. to determine the radioactivity intensity. For example, it is possible to easily estimate the amount of neutron irradiation in the energy range of 0.1 MeV to 2 MeV received by the fissile material of the test piece.
以上のように、監視試験片として速中性子によ
る核分裂物質を加えると0.1〜2MeVの範囲のエ
ネルギの中性子照射量を測定することができ、こ
の核分裂物質試験片と従来のモニタワイヤ試験片
とを組合せれば、機械的性質を調べるための監視
試験片が受けた中性子の必要な範囲のエネルギ分
布を推定することができるという効果を奏する。 As described above, when a fissile material using fast neutrons is added as a monitoring test piece, it is possible to measure the neutron irradiation amount with energy in the range of 0.1 to 2 MeV, and by combining this fissile material test piece with a conventional monitor wire test piece. This has the effect that it is possible to estimate the necessary range of energy distribution of neutrons received by a monitoring test piece for investigating mechanical properties.
第1図は従来の試験片の中性子エネルギと核反
応断面積との関係を示すグラフ、第2図は本発明
の試験片の中性子エネルギと核反応断面積との関
係を示すグラフである。
l0……測定不可能範囲。
FIG. 1 is a graph showing the relationship between neutron energy and nuclear reaction cross section of a conventional test piece, and FIG. 2 is a graph showing the relationship between neutron energy and nuclear reaction cross section of a test piece of the present invention. l 0 ...Unmeasurable range.
Claims (1)
の核分裂物質と、異なる中性子エネルギで核反応
が生じる複数の放射性核種生成物質を収納容器内
に密封し、前記核分裂物質として238U,232Th,お
よび237Npを使用し、前記放射性核種生成物質と
して58Ni,54Fe,および63Cuを使用したことを特
徴とする原子炉圧力容器監視試験片。1 A plurality of fissile materials that undergo nuclear fission at different neutron energies and a plurality of radionuclide generating materials that undergo nuclear reactions at different neutron energies are sealed in a storage container, and 238 U, 232 Th, and 237 Np are used as the fissionable materials. A nuclear reactor pressure vessel monitoring test piece, characterized in that 58 Ni, 54 Fe, and 63 Cu are used as the radionuclide generating substances.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56145891A JPS5847296A (en) | 1981-09-16 | 1981-09-16 | Sample piece for monitoring reactor pressure vessel |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56145891A JPS5847296A (en) | 1981-09-16 | 1981-09-16 | Sample piece for monitoring reactor pressure vessel |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5847296A JPS5847296A (en) | 1983-03-18 |
| JPH0222355B2 true JPH0222355B2 (en) | 1990-05-18 |
Family
ID=15395434
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56145891A Granted JPS5847296A (en) | 1981-09-16 | 1981-09-16 | Sample piece for monitoring reactor pressure vessel |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5847296A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS60113176A (en) * | 1983-11-01 | 1985-06-19 | アメリカ合衆国 | Portable nondestructive method for determining spatial distribution of neutron dose |
-
1981
- 1981-09-16 JP JP56145891A patent/JPS5847296A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5847296A (en) | 1983-03-18 |
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