JP3559727B2 - Radionuclide absorber and method for measuring radionuclide concentration using it - Google Patents
Radionuclide absorber and method for measuring radionuclide concentration using it Download PDFInfo
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- JP3559727B2 JP3559727B2 JP19820899A JP19820899A JP3559727B2 JP 3559727 B2 JP3559727 B2 JP 3559727B2 JP 19820899 A JP19820899 A JP 19820899A JP 19820899 A JP19820899 A JP 19820899A JP 3559727 B2 JP3559727 B2 JP 3559727B2
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- 239000006096 absorbing agent Substances 0.000 title claims description 27
- 238000000034 method Methods 0.000 title claims description 10
- 239000007787 solid Substances 0.000 claims description 21
- 239000004794 expanded polystyrene Substances 0.000 claims description 20
- 239000012071 phase Substances 0.000 claims description 19
- 239000000126 substance Substances 0.000 claims description 19
- 239000007791 liquid phase Substances 0.000 claims description 17
- 229920000642 polymer Polymers 0.000 claims description 16
- 239000002904 solvent Substances 0.000 claims description 5
- 230000005855 radiation Effects 0.000 claims description 4
- 239000007788 liquid Substances 0.000 description 29
- YXFVVABEGXRONW-UHFFFAOYSA-N Toluene Chemical compound CC1=CC=CC=C1 YXFVVABEGXRONW-UHFFFAOYSA-N 0.000 description 24
- 229910052704 radon Inorganic materials 0.000 description 24
- SYUHGPGVQRZVTB-UHFFFAOYSA-N radon atom Chemical compound [Rn] SYUHGPGVQRZVTB-UHFFFAOYSA-N 0.000 description 24
- 238000005259 measurement Methods 0.000 description 18
- 239000007789 gas Substances 0.000 description 15
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 12
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 description 8
- 239000004793 Polystyrene Substances 0.000 description 8
- 229920002223 polystyrene Polymers 0.000 description 8
- 238000004090 dissolution Methods 0.000 description 4
- 238000005192 partition Methods 0.000 description 4
- 239000000843 powder Substances 0.000 description 4
- 238000010521 absorption reaction Methods 0.000 description 3
- 239000002861 polymer material Substances 0.000 description 3
- 239000011347 resin Substances 0.000 description 3
- 229920005989 resin Polymers 0.000 description 3
- 238000000638 solvent extraction Methods 0.000 description 3
- 238000001514 detection method Methods 0.000 description 2
- 238000005187 foaming Methods 0.000 description 2
- 238000000691 measurement method Methods 0.000 description 2
- 229920003229 poly(methyl methacrylate) Polymers 0.000 description 2
- -1 polyethylene Polymers 0.000 description 2
- 239000004926 polymethyl methacrylate Substances 0.000 description 2
- 230000002285 radioactive effect Effects 0.000 description 2
- 239000000243 solution Substances 0.000 description 2
- 238000001179 sorption measurement Methods 0.000 description 2
- CTQNGGLPUBDAKN-UHFFFAOYSA-N O-Xylene Chemical compound CC1=CC=CC=C1C CTQNGGLPUBDAKN-UHFFFAOYSA-N 0.000 description 1
- 239000004698 Polyethylene Substances 0.000 description 1
- 239000004743 Polypropylene Substances 0.000 description 1
- 239000002250 absorbent Substances 0.000 description 1
- 230000002745 absorbent Effects 0.000 description 1
- 239000003463 adsorbent Substances 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 229920006248 expandable polystyrene Polymers 0.000 description 1
- 239000007792 gaseous phase Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 125000002496 methyl group Chemical group [H]C([H])([H])* 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 229920000573 polyethylene Polymers 0.000 description 1
- 229920001155 polypropylene Polymers 0.000 description 1
- 230000001737 promoting effect Effects 0.000 description 1
- 230000000717 retained effect Effects 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
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- 238000009423 ventilation Methods 0.000 description 1
- 229920002554 vinyl polymer Polymers 0.000 description 1
- 239000008096 xylene Substances 0.000 description 1
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- Measurement Of Radiation (AREA)
Description
【0001】
【発明の属する技術分野】
本発明は気相又は液相中に存在する放射性核種の吸収体とこれを用いた放射性核種の濃度測定法に関する。
【0002】
【従来の技術】
従来液体中の放射性核種吸収体としてトルエンを用い、このトルエンを放射性核種が存在する液体中に添加して放射性核種を吸収させ、該放射性核種を吸収したトルエンを液体中から取り出す溶媒抽出法を用い、該放射性核種を吸収させたトルエン溶液の放射性核種の濃度を液体シンチレーション計測により測定する液体シンチレーション検出器を用いた計測法が一般的に用いられている。この放射性核種の濃度測定法は液相の測定に適している。
【0003】
他方気相中の放射性核種吸着体として活性炭が知られており、この活性炭(粉末)を放射性核種が存在する気相中に一定時間設置して該気相中の放射性核種を吸着させる活性炭吸着法を用い、該活性炭に吸着させた放射性核種をトルエンに吸収させ、上記と同様の液体シンチレーション検出器を用いた計測により放射性核種の有無及び相対濃度を測定する方法が知られている。
【0004】
上記吸収とは他物質に取り込まれることを意味し、吸着とは固体又は液体の表面に保持されることを意味し、上記固体又は液体に入り込む吸収とは異なる。
【0005】
【発明が解決しようとする課題】
然しながら溶媒抽出法に用いられるトルエンは健康に有害であり、取り扱い安全性が要求されるばかりか、測定操作を行う特殊な測定機器を要し、工数がかかる。又上記の通り、気相中測定には不向きである。
【0006】
又上記活性炭吸着法は気相中測定が可能であるが、放射性核種の有無及び相対濃度の測定が行えるだけで、絶対濃度の測定が困難で正確な濃度測定が行えない致命的な欠点を有している。
【0007】
【課題を解決するための手段】
本発明はこれらの問題点を適切に解決し、気相又は液相中に存在する放射性核種の測定を簡便に、且つ高信頼性を以て遂行することができる放射性核種吸収体とこれを用いた放射性核種の濃度測定法を提供するものである。
【0008】
本発明に係る放射性核種吸収体は、発泡ポリスチレンに代表される油溶性固体高分子物質、その他の固体高分子物質から成る。
【0009】
即ち本発明に係る放射性核種吸収体は、気相又は液相中に存在する放射性核種の吸収体であって、上記気相又は液相中に設置して使用される固体高分子物質から成る。
【0010】
固体高分子物質を気相又は液相中に一定時間設置して放射性核種を吸収させ、該放射性核種を吸収した固体高分子物質を溶媒にて溶解し、該溶解液の放射線計数値から上記気相又は液相中の放射性核種の濃度を測定する。
【0011】
所謂上記固体高分子物質を液体シンチレーション検出器に適用し、上記濃度測定を行う。
【0012】
上記発泡ポリスチレンに代表される固体高分子物質から成る放射性核種吸収体は、手軽に入手でき、極めて安価であり、且つ安全である。
【0013】
液体シンチレーターを入れた容器中に上記固体高分子物質から成る放射性核種吸収体を押し込むのみで、前記従来例の如き安全性を損なう機会を多く持つ操作を要することなく検体液が得られるから、これに既知の液体シンチレーション検出器を適用することにより、高信頼の濃度測定が安全且つ迅速に行える。測定コストも安価である。
【0014】
【発明の実施の形態】
以下本発明の実施の形態例について説明する。
【0015】
本発明に係る放射性核種吸収体1は発泡ポリスチレンに代表される固体高分子物質から成る。この固体高分子物質は計測容器2内に押し込むのに適した大きさのブロックにする。
【0016】
又はシート体、粉体として用い、粉体は通気・通水性を有する容器内に収容し、気相又は液相中に設置する。
【0017】
又ブロック又はシートは気相又は液相中にできるだけ全表面を露出した状態で支持し、静置する。
【0018】
図1A,Bに示すように、本発明に係る上記固体高分子物質から成る放射性核種吸収体1は例えば発泡ポリスチレンを柱体に形成し、好ましくは図1Aに示すように、円柱体に形成する。
【0019】
図2に示す液体シンチレーション検出器に適用する検体液を作る計測容器2は世界的に形状と大きさが規格化されており、その口径をR2とした場合、上記放射性核種吸収体1の柱体ブロック1′の口径R1はR2と略等しくし、口径内に緊密に接触させて徐々に押し込みながら計測容器2内の液体シンチレーター3(主としてトルエンやキシレンを溶媒として有機蛍光体を少量溶かし込んだ試液)中に浸漬し、徐々に溶解を促す。
【0020】
この時柱体ブロック1′の押し込みに従って液体シンチレーター3が溢出するのを防止するために、上記柱体ブロック1′の軸心に両端面において開口する貫通孔4を設ける。
【0021】
計測容器2内に柱体ブロック1′を押し込んで行くに従い、液体シンチレーター3は上記貫通孔4内に侵入し、貫通孔4内面から同ブロックから成る放射性核種吸収体1を溶解する。
【0022】
又貫通孔4内に液体シンチレーター3が押し上げられることにより、計測容器2の口部からの溢出を防止する。
【0023】
又他の好ましい例示として図1Bに示すように、円柱体から成る柱体ブロック1′を軸心方向において二分して半円柱形ブロックにし、適例としてその平面部に沿って長溝4′を有する形態にする。
【0024】
上記貫通孔4及び長溝4′は液体シンチレーター3との接触面積を増大し、均一なる溶解を促す手段であり、その変形例として複数の貫通孔4を柱体ブロック1′の一端面から他端面に亘って開設する場合を含み、同様に上記長溝4′を複数条形成する場合を含む。又その外径は多角柱体、平板状にすることができる。
【0025】
又上記長溝4′は液相中から柱体ブロック1′を引き上げた後、表面を拭掃するのに有利である。
【0026】
上記放射性核種吸収体1を形成する固体高分子物質としては、上記発泡ポリスチレンの他、非発泡ポリスチレン、ポリメタクリル酸メチル、ポリエチレン、ポリプロピレン等のポリビニル樹脂が適用可能であるが、汎用の液体シンチレーション検出器に適用する関係から、油溶性を有する発泡又は非発泡ポリスチレン、ポリメタクリル酸メチルが適性である。
【0027】
又上記放射性核種吸収体1は地中に埋め込んで、地中の放射性核種の検出に使用することができ、地中の水分度に応じ、気相又は液相の概念に含まれることとする。
【0028】
以下、放射性核種として水中ラドン、吸収物質、即ち固体高分子物質として、発泡ポリスチレンを用い、ラドンの濃度測定を行った実施例について説明する。この実施例は本発明を限定するものではない。
【0029】
10(縦)×10(横)×50(長さ)mmの角柱形ブロックに形成した発泡ポリスチレン吸収体をラドンを含有する水中に入れ、24時間以上設置した。
【0030】
ラドンを含有する水中に前記ポリスチレンを放置しておくと、24時間以上の放置時間でポリスチレンに吸収されたラドン量は一定値となり、ポリスチレンと水との間に分配律関係が成立することが明らかとなった(図3参照)。
【0031】
図3のグラフは縦軸にポリスチレン中ラドン濃度を示し、横軸に水中ラドン濃度を示しており、グラフは両者が原点を通る直線(正比例)関係にあること、即ち分配律関係が成立していることを示している。
【0032】
分配律関係が成立したポリスチレンの単位重量(1g)当たりのラドン吸収量(ベクレル/g)と水中ラドン濃度(ベクレル/g)は正比例した。この比例定数を広義のラドン分配係数と呼ぶ。
【0033】
以上の関係を利用してポリスチレンに吸収されたラドンの濃度から、水中ラドン濃度を算出することが可能となる。
【0034】
形状及び密度を一定にそろえた例えば前記大きさと形状を有するポリスチレンの柱状ブロック1′を標準吸収体として、そのラドン分配係数を定数として明らかにしておけば、標準吸収体を使用した計測値(ラドン濃度)を定数(分配係数)で除するだけで水中ラドン濃度が決定できる。
【0035】
即ち上記発泡ポリスチレン吸収体1を図2に示す如く、液体シンチレーター3の入った計測容器中2に押し込み、溶解させる。そしてこのラドンが溶解した液体シンチレーターの容器2を蓋で密閉し、液体シンチレーション検出器にかける。
【0036】
ここにおける液体シンチレーション検出器は、例えば「マグローヒル科学技術用語大辞典」や国際技術財団編の「科学大辞典」等に紹介されているように、放射線測定器として世界的に汎用されている。
【0037】
上記液体シンチレーション計測から得られた放射線計数値をラドン分配係数で除して水中ラドン濃度を算出した。
【0038】
発泡ポリスチレンのラドン分配係数は水に対して約130であった。この方法を用いて算出したラドン濃度の総合誤差は10%であった。
【0039】
発泡ポリスチレン2gを用いれば、従来の放射性核種吸収体としてトルエンを用いた溶媒抽出法に匹敵するラドン検出感度と精度を気相及び液相において達成することができる。
【0040】
上記した発泡ポリスチレンに代表される吸収性を有する発泡樹脂には、連通気泡構造のものと非連通気泡構造のものが存し、連通気泡構造の発泡樹脂は連通気泡内に液体シンチレーター3等の溶媒が浸入するので、溶媒との接触面積が大きく、溶解速度も大幅に向上する。又密度が少なく、溶解量も少ない。
【0041】
【発明の効果】
本発明によれば、発泡ポリスチレンの密度、形状及び質量を標準化する等し、そのラドン分配係数を値付けした材料を用いることで、実用的にもきわめて簡易に液相、気相中の放射性核種濃度を決定することが可能である。
【0042】
本発明は測定操作が簡易なだけでなく、上記発泡ポリスチレンに代表される固体高分子物質から成る放射性核種吸収体は、手軽に入手でき、極めて安価であり、且つ安全である。
【0043】
計測容器中に上記固体高分子物質から成る放射性核種吸収体を押し込むのみで、前記従来例の如き安全性を損なう機会を多く持つ操作を要することなく検体液が得られるから、これに既知の液体シンチレーション検出器を適用することにより、高信頼の濃度測定が安全且つ迅速に行える。測定コストも安価である。
【図面の簡単な説明】
【図1】Aは柱体ブロック形に形成した固体高分子物質から成る放射性核種吸収体の斜視図、Bは同柱体ブロック形に形成した固体高分子物質から成る放射性吸収体の他例を示す斜視図。
【図2】液体シンチレーション計測容器に上記柱体ブロック形の放射性核種吸収体を押し込んで溶解させている状態を示す断面図。
【図3】ポリスチレン中ラドン濃度と水中ラドン濃度の分配律関係を示すグラフ。
【符号の説明】
1 放射性核種吸収体
1′ 柱体ブロック
2 計測容器
3 液体シンチレーター
4 貫通孔
4′ 長溝[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to an absorber for a radionuclide existing in a gas phase or a liquid phase and a method for measuring the concentration of a radionuclide using the same.
[0002]
[Prior art]
Conventionally, toluene is used as a radionuclide absorber in a liquid, a solvent extraction method is used in which the toluene is added to a liquid in which a radionuclide is present to absorb the radionuclide, and the toluene in which the radionuclide is absorbed is removed from the liquid. A measurement method using a liquid scintillation detector for measuring the concentration of a radionuclide in a toluene solution in which the radionuclide is absorbed by liquid scintillation measurement is generally used. This radionuclide concentration measurement method is suitable for measuring the liquid phase.
[0003]
On the other hand, activated carbon is known as a radionuclide adsorbent in a gas phase, and this activated carbon (powder) is placed in a gas phase in which a radionuclide exists for a certain period of time to adsorb the radionuclide in the gas phase. A method is known in which toluene is used to absorb the radionuclide adsorbed on the activated carbon, and the presence or absence and relative concentration of the radionuclide are measured by measurement using a liquid scintillation detector similar to the above.
[0004]
Absorption means being taken up by another substance, and adsorption means being retained on the surface of a solid or liquid, and is different from absorption entering the solid or liquid.
[0005]
[Problems to be solved by the invention]
However, toluene used in the solvent extraction method is harmful to health, requires not only safety in handling, but also requires special measuring equipment for performing a measuring operation, and requires many man-hours. As described above, it is not suitable for measurement in a gas phase.
[0006]
Although the above activated carbon adsorption method can be measured in the gas phase, it can only measure the presence or absence and relative concentration of radionuclides, but has the fatal drawback that the absolute concentration is difficult to measure and accurate concentration measurement cannot be performed. are doing.
[0007]
[Means for Solving the Problems]
The present invention solves these problems appropriately, and a radionuclide absorber capable of easily and highly reliably measuring radionuclides present in a gas phase or a liquid phase, and a radionuclide using the same. It provides a method for measuring the concentration of nuclides.
[0008]
The radionuclide absorber according to the present invention is composed of an oil-soluble solid polymer substance represented by expanded polystyrene and other solid polymer substances.
[0009]
That is, the radionuclide absorber according to the present invention is an absorber of a radionuclide existing in a gas phase or a liquid phase, and is composed of a solid polymer substance used by being installed in the gas phase or the liquid phase.
[0010]
A solid polymer substance is placed in a gas phase or a liquid phase for a certain period of time to absorb radioactive nuclides, the solid polymer substance having absorbed the radionuclide is dissolved in a solvent, and the above-mentioned gas is determined from the radiation count value of the solution. The concentration of the radionuclide in the phase or liquid phase is measured.
[0011]
The so-called solid polymer substance is applied to a liquid scintillation detector to measure the concentration.
[0012]
The radionuclide absorber made of a solid polymer material represented by the expanded polystyrene is easily available, extremely inexpensive, and safe.
[0013]
By simply pushing the radionuclide absorber composed of the solid polymer substance into the container containing the liquid scintillator, the sample liquid can be obtained without the need for an operation having many opportunities to impair the safety as in the conventional example. By applying a known liquid scintillation detector to, a highly reliable concentration measurement can be performed safely and quickly. The measurement cost is also low.
[0014]
BEST MODE FOR CARRYING OUT THE INVENTION
Hereinafter, embodiments of the present invention will be described.
[0015]
The radionuclide absorber 1 according to the present invention is made of a solid polymer substance represented by expanded polystyrene. The solid polymer material is formed into a block having a size suitable for being pushed into the measuring container 2.
[0016]
Alternatively, the powder is used as a sheet or powder, and the powder is housed in a container having ventilation and water permeability, and is placed in a gas phase or a liquid phase.
[0017]
The block or sheet is supported and allowed to stand in a gas phase or a liquid phase with the entire surface exposed as much as possible.
[0018]
As shown in FIGS. 1A and 1B, the radionuclide absorber 1 made of the solid polymer material according to the present invention is formed, for example, of expanded polystyrene in a column, and preferably in a column, as shown in FIG. 1A. .
[0019]
The shape and size of the measurement container 2 for preparing the sample liquid applied to the liquid scintillation detector shown in FIG. 2 are standardized worldwide, and when the diameter is R2, the column of the
[0020]
At this time, in order to prevent the liquid scintillator 3 from overflowing as the column block 1 'is pushed in, through
[0021]
As the
[0022]
Further, since the liquid scintillator 3 is pushed up into the through
[0023]
As another preferred example, as shown in FIG. 1B, a column block 1 'composed of a column is bisected in the axial direction to form a semi-cylindrical block, and has a long groove 4' along its plane as a suitable example. Form.
[0024]
The through-
[0025]
The long groove 4 'is advantageous for wiping the surface after the column block 1' is pulled up from the liquid phase.
[0026]
As the solid polymer substance forming the
[0027]
The
[0028]
Hereinafter, an example in which radon concentration measurement was performed using radon in water as a radionuclide and expanded polystyrene as an absorbing substance, that is, a solid polymer substance, will be described. This example does not limit the invention.
[0029]
The expanded polystyrene absorber formed in a prismatic block of 10 (length) × 10 (width) × 50 (length) mm was placed in water containing radon and set for 24 hours or more.
[0030]
When the polystyrene is allowed to stand in water containing radon, the amount of radon absorbed by the polystyrene in the standing time of 24 hours or more becomes a constant value, and it is clear that a distribution law relationship is established between polystyrene and water. (See FIG. 3).
[0031]
The graph of FIG. 3 shows the concentration of radon in polystyrene on the vertical axis and the concentration of radon in water on the horizontal axis. The graph shows that the two are in a straight line (directly proportional) relationship passing through the origin, that is, the distribution rule relationship is established. It indicates that
[0032]
The radon absorption amount (becquerel / g) per unit weight (1 g) of polystyrene for which the distribution rule was established was directly proportional to the radon concentration in water (becquerel / g). This constant of proportionality is called the Radon distribution coefficient in a broad sense.
[0033]
Using the above relationship, the radon concentration in water can be calculated from the concentration of radon absorbed by polystyrene.
[0034]
If, for example, a columnar block 1 'of polystyrene having the same size and shape as described above is used as a standard absorber and its radon distribution coefficient is clarified as a constant, a measured value (Radon The concentration of radon in water can be determined simply by dividing the concentration) by a constant (partition coefficient).
[0035]
That is, as shown in FIG. 2, the expanded
[0036]
The liquid scintillation detector here is widely used as a radiation measuring instrument worldwide as introduced in, for example, "Maglow Hill Scientific and Technical Dictionary" and "Science Dictionary" edited by International Technology Foundation.
[0037]
The radon concentration in water was calculated by dividing the radiation count value obtained from the liquid scintillation measurement by the radon partition coefficient.
[0038]
The Radon partition coefficient of the expanded polystyrene was about 130 with respect to water. The total error in the radon concentration calculated using this method was 10%.
[0039]
When 2 g of expanded polystyrene is used, radon detection sensitivity and accuracy comparable to the solvent extraction method using toluene as a conventional radionuclide absorber can be achieved in the gas phase and the liquid phase.
[0040]
Absorbent foaming resins represented by the above-mentioned expanded polystyrene include those having a communicating cell structure and those having a non-communicating cell structure. The foaming resin having a communicating cell structure contains a solvent such as a liquid scintillator 3 in the communicating cells. As a result, the contact area with the solvent is large, and the dissolution rate is greatly improved. Also, the density is low and the amount of dissolution is small.
[0041]
【The invention's effect】
According to the present invention, the radionuclide in the liquid phase and the gaseous phase is very easily practically used by standardizing the density, shape and mass of the expanded polystyrene and using a material whose radon partition coefficient is valued. It is possible to determine the concentration.
[0042]
According to the present invention, not only the measurement operation is simple, but also a radionuclide absorber made of a solid polymer substance represented by the above-mentioned expanded polystyrene is easily available, extremely inexpensive, and safe.
[0043]
By simply pushing the radionuclide absorber composed of the solid polymer substance into the measurement container, the sample liquid can be obtained without the need for an operation having many chances of impairing the safety as in the conventional example. By applying the scintillation detector, highly reliable concentration measurement can be performed safely and quickly. The measurement cost is also low.
[Brief description of the drawings]
FIG. 1A is a perspective view of a radionuclide absorber composed of a solid polymer substance formed in a columnar block shape, and FIG. 1B is another example of a radioactive absorber composed of a solid polymer substance formed in a columnar block shape. FIG.
FIG. 2 is a cross-sectional view showing a state in which the column-shaped radionuclide absorber is pushed into and dissolved in a liquid scintillation measurement container.
FIG. 3 is a graph showing a distribution law relationship between a radon concentration in polystyrene and a radon concentration in water.
[Explanation of symbols]
DESCRIPTION OF
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| JP6108272B2 (en) * | 2012-12-05 | 2017-04-05 | 地方独立行政法人東京都立産業技術研究センター | Biomass origin discrimination method of plastic |
| KR101654711B1 (en) * | 2014-12-15 | 2016-09-08 | 한국수력원자력 주식회사 | Salt production year estimation method |
| JP7316108B2 (en) * | 2019-06-19 | 2023-07-27 | 東京インキ株式会社 | Radon radioactivity measurement method |
| KR102650229B1 (en) * | 2022-05-23 | 2024-03-21 | 한국원자력안전기술원 | Apparatus for collecting kit |
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