JPS5913146B2 - Neutron detection device for radiation emitters - Google Patents
Neutron detection device for radiation emittersInfo
- Publication number
- JPS5913146B2 JPS5913146B2 JP11468676A JP11468676A JPS5913146B2 JP S5913146 B2 JPS5913146 B2 JP S5913146B2 JP 11468676 A JP11468676 A JP 11468676A JP 11468676 A JP11468676 A JP 11468676A JP S5913146 B2 JPS5913146 B2 JP S5913146B2
- Authority
- JP
- Japan
- Prior art keywords
- neutron
- derivative
- radiation emitter
- moderator
- neutrons
- 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
- 230000005855 radiation Effects 0.000 title claims description 19
- 238000001514 detection method Methods 0.000 title claims description 13
- 238000009792 diffusion process Methods 0.000 claims description 13
- 239000006096 absorbing agent Substances 0.000 claims description 5
- 239000000463 material Substances 0.000 claims description 5
- 230000003449 preventive effect Effects 0.000 claims 2
- 239000003758 nuclear fuel Substances 0.000 claims 1
- 239000000126 substance Substances 0.000 claims 1
- 230000004907 flux Effects 0.000 description 19
- 238000005259 measurement Methods 0.000 description 8
- 238000010586 diagram Methods 0.000 description 6
- 230000005251 gamma ray Effects 0.000 description 4
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 4
- XLYOFNOQVPJJNP-ZSJDYOACSA-N Heavy water Chemical compound [2H]O[2H] XLYOFNOQVPJJNP-ZSJDYOACSA-N 0.000 description 2
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 description 2
- 238000010521 absorption reaction Methods 0.000 description 2
- 239000000470 constituent Substances 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 229910052739 hydrogen Inorganic materials 0.000 description 2
- 239000001257 hydrogen Substances 0.000 description 2
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 1
- 239000004698 Polyethylene Substances 0.000 description 1
- QCWXUUIWCKQGHC-UHFFFAOYSA-N Zirconium Chemical compound [Zr] QCWXUUIWCKQGHC-UHFFFAOYSA-N 0.000 description 1
- 229910052790 beryllium Inorganic materials 0.000 description 1
- ATBAMAFKBVZNFJ-UHFFFAOYSA-N beryllium atom Chemical compound [Be] ATBAMAFKBVZNFJ-UHFFFAOYSA-N 0.000 description 1
- 229910052799 carbon Inorganic materials 0.000 description 1
- 239000003989 dielectric material Substances 0.000 description 1
- 230000006698 induction Effects 0.000 description 1
- 230000007935 neutral effect Effects 0.000 description 1
- -1 polyethylene Polymers 0.000 description 1
- 229920000573 polyethylene Polymers 0.000 description 1
- 239000002915 spent fuel radioactive waste Substances 0.000 description 1
- 229910052726 zirconium Inorganic materials 0.000 description 1
Landscapes
- Measurement Of Radiation (AREA)
Description
【発明の詳細な説明】
本発明は非常に強いガンマ線と少量の中性子を放出する
放射線放出体たとえば原子炉の中で中性子に照射されて
使用済となった使用済燃料または使用の中途で一時的に
原子炉の中から取出された核熱料からの中性子を効率よ
くしかも高精度で測定する中性子測定装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to radiation emitters that emit very strong gamma rays and small amounts of neutrons, such as spent fuel that has been irradiated with neutrons in a nuclear reactor, or temporarily used during use. The present invention relates to a neutron measurement device that efficiently and accurately measures neutrons from nuclear heat materials extracted from a nuclear reactor.
従来この種の測定装置としては、放射線放出体のまわり
を鉛遮蔽体でおおってガンマ線を減衰させ、鉛遮蔽体の
外側に中性子減速材を設けて、この減速材中に熱中性子
検出器を挿入したものが使用されていた。Conventionally, this type of measurement device covers the radiation emitter with a lead shield to attenuate gamma rays, provides a neutron moderator on the outside of the lead shield, and inserts a thermal neutron detector into the moderator. was used.
特公昭51−17480号では鉛遮蔽体を適邑に配置す
ることによってガンマ線逗蔽能力を保持したまま、中性
子検出効率を向上させた中性子検出装置が開示さねてい
る。Japanese Patent Publication No. 51-17480 discloses a neutron detection device that improves neutron detection efficiency while maintaining gamma ray shielding ability by arranging lead shields in appropriate locations.
しかしこの装置ではガンマ線の遮蔽に重点が置かれてい
るため、中性子検出器周辺の中性子の挙動に対する工夫
が足りず、従って中性子検出器の位置が予定位置から少
しずれた場合これに起因する測定誤差が生じ、この誤差
は従来の装置の誤差と同程度の誤差を示すものである。However, since this device focuses on shielding gamma rays, there is a lack of consideration for the behavior of neutrons around the neutron detector, and therefore, if the position of the neutron detector deviates slightly from the planned position, measurement errors may occur due to this. This error is comparable to that of conventional devices.
第1図はこの装置の構成を示す図である。FIG. 1 is a diagram showing the configuration of this device.
放射線放出体1、中性子検出器2、およびガンマ線を遮
蔽する鉛遮蔽体3Sのまわりは中性子減速材である軽水
4で囲まれている。The radiation emitter 1, the neutron detector 2, and the lead shield 3S that shields gamma rays are surrounded by light water 4, which is a neutron moderator.
矢印5の方向にプロットした熱中性子束分布6は図示す
る通りである。Thermal neutron flux distribution 6 plotted in the direction of arrow 5 is as shown.
放射線放出体1の内部では熱中性子束分布はほぼ平担と
なっているが、放射線放出体1と鉛遮蔽体3Sの間隙7
aでは中性子吸収効果がなくなるため僅かに熱中性子束
は上昇する。The thermal neutron flux distribution is almost flat inside the radiation emitter 1, but the gap 7 between the radiation emitter 1 and the lead shield 3S
At a, the neutron absorption effect disappears, so the thermal neutron flux increases slightly.
鉛3Sの中では曲線1bに示すように熱中性子束はゆる
やかな勾配を示し下っている。In lead 3S, the thermal neutron flux shows a gentle slope and decreases as shown by curve 1b.
中性子検出器2のある位置Ic付近では鉛3Sを透過し
た高速中性子が減速されて熱中性子となるので、熱中性
子束分布は幾分盛り上る傾向を示すものである。Near the position Ic of the neutron detector 2, the fast neutrons that have passed through the lead 3S are decelerated and become thermal neutrons, so the thermal neutron flux distribution tends to increase somewhat.
しかし鉛3Sの厚さtlと、鉛と中性子検出器2の距離
t2との関係を最適となるよう決定できない場合、たと
えばガンマ線強度が大きく厚さtlを大きくする必要の
ある場合や中性子検出器の形状が大きい場合、熱中性子
束の盛上りは位置7cで起りにくく、従って盛上りの位
置に中性子検出器2を設置できない。However, if the relationship between the thickness tl of the lead 3S and the distance t2 between the lead and the neutron detector 2 cannot be determined optimally, for example, if the gamma ray intensity is large and the thickness tl needs to be increased, or if the neutron detector If the shape is large, a rise in thermal neutron flux is unlikely to occur at the position 7c, and therefore the neutron detector 2 cannot be installed at the position of the rise.
このような場合には中性子検出器を設置する位置の近傍
の熱中性子束分布は大きな勾配をもつことになるので、
中性子検出器の位置が少しでも予定位置からずれると中
性子検出器の検出効率はかなり大きく変化して測定誤差
が生ずるのである。In such a case, the thermal neutron flux distribution near the location where the neutron detector is installed will have a large gradient, so
If the position of the neutron detector deviates even slightly from the planned position, the detection efficiency of the neutron detector changes considerably, resulting in measurement errors.
本発明の目的は前記の欠点を除去した放射線放出体の中
性子測定装置を提供するにある。SUMMARY OF THE INVENTION An object of the present invention is to provide a neutron measuring device for a radiation emitter that eliminates the above-mentioned drawbacks.
本発明の他の目的は計数される熱中性子の量を積極的に
増大させる中性子測定装置を提供するにある。Another object of the present invention is to provide a neutron measurement device that actively increases the amount of thermal neutrons counted.
本発明の他の目的は増大させた熱中性子を有効に中性子
検出器に導く中性子測定装置を提供するにある。Another object of the present invention is to provide a neutron measuring device that effectively guides increased thermal neutrons to a neutron detector.
本発明のさらに他の目的は熱中性子束分布をできるだけ
平担化させることによって中性子検出器の位置ずれに起
因する測定誤差の少ない中性子測定装置を提供するにあ
る。Still another object of the present invention is to provide a neutron measurement device with fewer measurement errors caused by positional deviation of a neutron detector by flattening the thermal neutron flux distribution as much as possible.
本発明のさらに他の目的はバックグランドとなる中性子
を有効に遮蔽する中性子測定装置を提供するにある。Still another object of the present invention is to provide a neutron measurement device that effectively blocks background neutrons.
次に本発明の実施例について第2図以下参照して詳細に
説明する。Next, embodiments of the present invention will be described in detail with reference to FIG. 2 and subsequent figures.
第2図は本発明の第1実施例を示した図である。FIG. 2 is a diagram showing a first embodiment of the present invention.
図において放射線放出体1は適箔な厚さの高速中性子減
速材たとえば厚さ2〜3crrlの水4を隔てて中性子
誘導体3と相対しており、この誘導体3に囲まれる中性
子検出器2を設けである。In the figure, a radiation emitter 1 faces a neutron derivative 3 across a fast neutron moderator material 4 of suitable thickness, for example, water 4 with a thickness of 2 to 3 crrl, and a neutron detector 2 surrounded by this dielectric material 3 is provided. It is.
中性子誘導体3は炭素、鉛、空気、重水ベリリウムなど
のように熱中性子拡散係数の非常に大きい媒質を使用す
も
放出体1から放出された高速中性子は減速材である水4
により積極的に熱中性子化されて、この熱中性子が中性
子誘導体3を通して中性子検出器2に達している。The neutron derivative 3 uses a medium with a very large thermal neutron diffusion coefficient, such as carbon, lead, air, heavy water beryllium, etc., but the fast neutrons emitted from the emitter 1 are absorbed by water 4, which is a moderator.
The thermal neutrons are actively converted into thermal neutrons, and these thermal neutrons reach the neutron detector 2 through the neutron derivative 3.
矢印5の方向にプロットした中性子束分布は曲線8のよ
うになり大幅に増加する。The neutron flux distribution plotted in the direction of arrow 5 becomes curve 8 and increases significantly.
中性子束分布は中性子検出効率と比例関係にあるから中
性子検出効率は大幅に向上し、中性子検出器2を熱中性
拡散係数の非常に大きい中性子誘導体3中に設置してい
るため、中性子検出器の位置ずれに起因する検出器効率
は小さくなっている。Since the neutron flux distribution is proportional to the neutron detection efficiency, the neutron detection efficiency is greatly improved.Since the neutron detector 2 is installed in the neutron derivative 3 with a very large thermal neutral diffusion coefficient, the neutron detector Detector efficiency due to misalignment is reduced.
中性子誘導体内の熱中性子束分布は拡散係数が非常に大
きいためゆるやかな形を示している。Thermal neutron flux distribution within the neutron derivative exhibits a gradual shape due to the extremely large diffusion coefficient.
第3図は本発明の第2実施例を示した図である。FIG. 3 is a diagram showing a second embodiment of the present invention.
図において、第1実施例に示す中性子誘導体3のまわり
に中性子拡散防止体9を設けさらにそのまわりを中性子
吸収体10で囲んでいる。In the figure, a neutron diffusion preventer 9 is provided around the neutron derivative 3 shown in the first embodiment, and is further surrounded by a neutron absorber 10.
中性子拡散防止体9がなく直接中性子吸収体10で中性
子誘導体3を囲むと、中性子誘導体3内では熱中性子が
非常に動き易いため中性子吸収体10に吸収されて中性
子束分布が急勾配で低下する。If there is no neutron diffusion preventer 9 and the neutron derivative 3 is directly surrounded by a neutron absorber 10, thermal neutrons move very easily within the neutron derivative 3 and are absorbed by the neutron absorber 10, resulting in a steep decline in the neutron flux distribution. .
これを防止するために設ける中性子拡散防止体9は熱中
性子拡散係数が小さくかつ中性子吸収断面積の小さな材
料が好ましい。The neutron diffusion preventer 9 provided to prevent this is preferably made of a material with a small thermal neutron diffusion coefficient and a small neutron absorption cross section.
具体的には水素を多く含む軽水ポリエチレン、ジルコニ
ウム水素イ自がよい。Specifically, light water polyethylene and zirconium hydrogen containing a large amount of hydrogen are preferable.
中性子拡散防止体9の配設によって中性子束分布は急勾
配の低下から曲線11のように改良されて第1実施例に
示した中性子束分布曲線8とほぼ同様の形状になる。By disposing the neutron diffusion preventer 9, the neutron flux distribution is improved from a steep drop to a curve 11, resulting in a shape almost similar to the neutron flux distribution curve 8 shown in the first embodiment.
第4図は本発明の第3実施例を示す図である。FIG. 4 is a diagram showing a third embodiment of the present invention.
図において、放射線放出体1のまわりは高速中性子減速
材4,12,13および14で囲み、さらに外側に中性
子誘導体3がこれらの減速材を囲むように配置しである
。In the figure, a radiation emitter 1 is surrounded by fast neutron moderators 4, 12, 13, and 14, and a neutron derivative 3 is further placed outside to surround these moderators.
高速中性子減速材は熱中性子拡散距離が中性子誘導体3
よりかなり小さいため、高速中性子減速材4の部分は他
の減速材部分12.13,14より幾分厚くしである。The thermal neutron diffusion distance of fast neutron moderator is neutron derivative 3
Since it is much smaller, the fast neutron moderator section 4 is somewhat thicker than the other moderator sections 12, 13, 14.
減速材部分12,13および14に面した部分の中性子
誘導体3は高速中性子減速材4よりさらに有効な減速材
としての機能も有している。The portion of the neutron derivative 3 facing the moderator portions 12, 13, and 14 also functions as a moderator more effective than the fast neutron moderator 4.
この減速材兼誘導体により放射線放出体から一旦洩れ出
した中性子を有効に放出体に反射させて、反射体を中心
とした中性子増倍体系の中性子増倍率を増大させ。This moderator and derivative effectively reflects the neutrons that once leaked from the radiation emitter back to the emitter, increasing the neutron multiplication factor of the neutron multiplication system centered on the reflector.
中性子放出率を増大させている。Increased neutron emission rate.
この中性子増倍効果により熱中性子束分布15は第2実
施例に示す分布11よりもさらに上昇させられる。Due to this neutron multiplication effect, the thermal neutron flux distribution 15 is further raised than the distribution 11 shown in the second embodiment.
第5図は本発明の第4実施例を示す図である。FIG. 5 is a diagram showing a fourth embodiment of the present invention.
図において中性子検出器2は中性子誘導体3内に設けら
れたガンマ線遮蔽体16内に挿入される。In the figure, the neutron detector 2 is inserted into a gamma ray shield 16 provided within the neutron guide 3.
検出器をはさんで設けられる遮蔽体16は放出体1に対
する側が厚くその反輝則はうすくなっている。The shielding body 16 provided across the detector is thicker on the side facing the emitter 1, and its anti-glare law is weaker.
遮蔽体に鉛を使用するとき、鉛の中性子拡散係数がよい
ために、中性子誘導体3に準じた性質を鉛にもたせるこ
とができる。When lead is used for the shielding material, lead can have properties similar to those of the neutron derivative 3 because lead has a good neutron diffusion coefficient.
17で示す領域は中性子誘導体3の内部に設けた空洞で
ある。The region indicated by 17 is a cavity provided inside the neutron derivative 3.
この空洞も配置の仕方によって中性子の誘導特性を改良
することができる。The neutron induction characteristics of this cavity can also be improved depending on how it is arranged.
図の空洞1γは減速材12および13に面した中性子減
速材兼誘導体からの中性子を効果的に中性子検出器2の
方向に誘導する役をするものである。The illustrated cavity 1γ serves to effectively guide neutrons from the neutron moderator/inductor facing the moderators 12 and 13 toward the neutron detector 2.
これらの構成によって中性子束分布18はさらに図示す
るように上昇する。These configurations further increase the neutron flux distribution 18 as shown.
以上詳細に述べたように本発明によれば計数される熱中
性子の量を積極的に増大させ、この増大させられた熱中
性子を有効に誘導し、中性子検出器の位置ずれに起因す
る誤差を少なくして中性子検出効率を改善し、バックグ
ランドとなる中性子を有効に遮蔽する中性子検出装置が
得られる。As described in detail above, according to the present invention, the amount of thermal neutrons counted is actively increased, the increased thermal neutrons are effectively guided, and the error caused by the positional shift of the neutron detector is reduced. A neutron detection device that improves neutron detection efficiency and effectively blocks background neutrons by reducing the number of neutrons can be obtained.
第1図は本発明の基礎となる検出装置の構成部分の配置
と中性子束分布を示す図、第2図ないし第5図は第1図
の検出装置を改良した本発明の構成部分と中性子束分布
を示す図である。
1・・・・・・放射線放出体、2・・・・・・中性子検
出器、3・・・・・・中性子誘導体、4,12,13,
14・・・・・・高速中性子減速材、5・・・・・・矢
印、6,8,11 。
15.17,18・・・・・・中性子束分布曲線、9・
・−・・中性子拡散防止体、10・・−・・中性子吸収
体、16・・−・・ガンマ線遮蔽体、17・・・・・・
空洞。Fig. 1 is a diagram showing the arrangement of the constituent parts and neutron flux distribution of the detection device which is the basis of the present invention, and Figs. 2 to 5 show the constituent parts and neutron flux of the present invention, which is an improved version of the detection device shown in Fig. 1. It is a figure showing distribution. 1... Radiation emitter, 2... Neutron detector, 3... Neutron derivative, 4, 12, 13,
14... Fast neutron moderator, 5... Arrow, 6, 8, 11. 15.17,18...neutron flux distribution curve, 9.
...neutron diffusion preventer, 10...neutron absorber, 16...gamma ray shield, 17...
cavity.
Claims (1)
において、前記放射線放出体から放出された高速中性子
を減速させる減速材と、前記減速材によって熱化された
中性子を誘導する中性子誘導体と、前記中性子誘導体の
内部に配置した中性子検出器とからなることを特徴とす
る放射線放出体の中性子検出装置。 2、特許請求の範囲第1項記載の中性子検出装置におい
て、前記放射線放出体から放出されて熱化された中性子
が前記中性子誘導体を通して前記中性子検出器に達する
のを妨げられないように、放射体に関する前記中性子誘
導体のまわりに中性子拡散防止体を設け、さらに前記中
性子拡散防止体のまわりに中性子吸収体を設けたことを
特徴とする放射線放出体の中性子検体装置。 3 特許請求の範囲第2項記載の中性子検出装置におい
て核燃料物質からなる放射線放出体の中性子増倍率を増
大させる物質を前記放射線放出体の外部に配置したこと
を特徴とする放射線放出体の中性子検出装置。[Claims] 1. A device for detecting neutrons emitted from a radiation emitter, comprising: a moderator that decelerates fast neutrons emitted from the radiation emitter; and a moderator that guides neutrons thermalized by the moderator. A neutron detection device for a radiation emitter, comprising a neutron derivative and a neutron detector disposed inside the neutron derivative. 2. In the neutron detection device according to claim 1, the radiator is configured such that neutrons emitted from the radiation emitter and heated are not prevented from reaching the neutron detector through the neutron derivative. A neutron sample device for a radiation emitting body, characterized in that a neutron diffusion preventive body is provided around the neutron derivative, and a neutron absorber is further provided around the neutron diffusion preventive body. 3. Neutron detection of a radiation emitter according to claim 2, characterized in that a substance that increases the neutron multiplication factor of the radiation emitter made of nuclear fuel material is disposed outside the radiation emitter. Device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11468676A JPS5913146B2 (en) | 1976-09-27 | 1976-09-27 | Neutron detection device for radiation emitters |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11468676A JPS5913146B2 (en) | 1976-09-27 | 1976-09-27 | Neutron detection device for radiation emitters |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5340575A JPS5340575A (en) | 1978-04-13 |
| JPS5913146B2 true JPS5913146B2 (en) | 1984-03-28 |
Family
ID=14644093
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11468676A Expired JPS5913146B2 (en) | 1976-09-27 | 1976-09-27 | Neutron detection device for radiation emitters |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5913146B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB0722430D0 (en) * | 2007-11-15 | 2007-12-27 | Health Prot Agency | Radiation detection |
-
1976
- 1976-09-27 JP JP11468676A patent/JPS5913146B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5340575A (en) | 1978-04-13 |
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