JPH071308B2 - Fluorescent glass dosimeter - Google Patents
Fluorescent glass dosimeterInfo
- Publication number
- JPH071308B2 JPH071308B2 JP4223191A JP4223191A JPH071308B2 JP H071308 B2 JPH071308 B2 JP H071308B2 JP 4223191 A JP4223191 A JP 4223191A JP 4223191 A JP4223191 A JP 4223191A JP H071308 B2 JPH071308 B2 JP H071308B2
- Authority
- JP
- Japan
- Prior art keywords
- fluorescent glass
- dose equivalent
- dose
- filter
- glass element
- 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
- 239000011521 glass Substances 0.000 title claims description 53
- 238000001917 fluorescence detection Methods 0.000 claims description 13
- 230000005855 radiation Effects 0.000 claims description 8
- 230000005284 excitation Effects 0.000 claims description 4
- 230000005251 gamma ray Effects 0.000 claims description 3
- 229910052751 metal Inorganic materials 0.000 claims description 2
- 239000002184 metal Substances 0.000 claims description 2
- 238000002834 transmittance Methods 0.000 claims description 2
- 238000006243 chemical reaction Methods 0.000 description 8
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 description 6
- 229910052782 aluminium Inorganic materials 0.000 description 5
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 5
- 238000005259 measurement Methods 0.000 description 3
- 210000000695 crystalline len Anatomy 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 206010073306 Exposure to radiation Diseases 0.000 description 1
- 238000005452 bending Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000000084 gamma-ray spectrum Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 239000005365 phosphate glass Substances 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- -1 silver ions Chemical class 0.000 description 1
Landscapes
- Measurement Of Radiation (AREA)
Description
【発明の詳細な説明】Detailed Description of the Invention
【0001】[0001]
【産業上の利用分野】本発明は、個人被ばく線量の測定
等に利用される蛍光ガラス線量計に係わり、特に生体等
に影響を及ぼす複数種類の線量当量を直接測定する蛍光
ガラス線量計に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a fluorescent glass dosimeter used for measuring an individual exposure dose, and more particularly to a fluorescent glass dosimeter for directly measuring a plurality of types of dose equivalents affecting a living body.
【0002】[0002]
【従来の技術】一般に、蛍光ガラス線量計は、銀イオン
を含有したリン酸塩ガラスからなる蛍光線量計用ガラス
素子が用いられている。このガラス素子は、放射線の被
ばくによって活性された後、波長300〜400nmの
紫外線で励起すると蛍光を発するが、このときの蛍光強
度は被ばく放射線量に比例することから、この蛍光強度
を検出することにより被ばく放射線量を測定できる。2. Description of the Related Art Generally, as a fluorescent glass dosimeter, a glass element for a fluorescent dosimeter made of phosphate glass containing silver ions is used. This glass element emits fluorescence when excited by ultraviolet rays having a wavelength of 300 to 400 nm after being activated by exposure to radiation, and the fluorescence intensity at this time is proportional to the radiation dose to be exposed. Therefore, it is necessary to detect this fluorescence intensity. Can measure the radiation dose.
【0003】ところで、従来の個人被ばく線量測定用線
量計は、種々の波長の放射線を透過するための各種のフ
ィルタと蛍光ガラス素子との組合わせにより、1cm線
量当量の個人被ばく線量について直接測定することが行
われ、しかも自由空間中の照射線量に関してエネルギー
に依存せずに測定することが求められていた。By the way, conventional dosimeters for measuring individual exposure dose directly measure an individual exposure dose of 1 cm dose equivalent by combining various filters for transmitting radiation of various wavelengths and a fluorescent glass element. However, it has been required to measure the irradiation dose in free space without depending on energy.
【0004】[0004]
【発明が解決しようとする課題】ところで、平成元年度
に入ってから放射線防護関係法令が改正され、当該法令
によれば、個人被ばく線量の管理には、実効線量当量お
よび目の水晶体と皮膚以外の組織線量当量として1cm
線量当量、目の水晶体の組織線量当量として3mm線量
当量、皮膚の組織線量当量として70μm線量当量等で
求めることが規定されている。[Problems to be Solved by the Invention] By the way, since the act of radiation protection was amended since the beginning of the 1989 year, according to the act, the effective dose equivalent and the crystalline lens and the skin other than the eye should be used for the management of individual exposure dose. 1 cm as the tissue dose equivalent of
It is stipulated that the dose equivalent, the tissue dose equivalent of the crystalline lens of the eye be 3 mm dose equivalent, and the tissue dose equivalent of skin be 70 μm dose equivalent.
【0005】その結果、各種フィルタの組合わせによっ
て1cm線量当量の照射線量を測定することが実用化さ
れているものの、3mm線量当量および70μm線量当
量については直接測定するものが実用化されていなかっ
た。そこで、従来では、線量計で測定した1cm線量当
量と、他の測定器例えばγ線用スペクトルメータで測定
したエネルギー値とを用いて、1cm線量当量から換算
によって3mm線量当量および70μm線量当量を得る
ようにしている。As a result, although it has been put into practical use to measure the irradiation dose of 1 cm dose equivalent by combining various types of filters, those for direct measurement of 3 mm dose equivalent and 70 μm dose equivalent have not been put into practical use. . Therefore, conventionally, a 1 cm dose equivalent measured by a dosimeter and an energy value measured by another measuring device such as a γ-ray spectrum meter are used to obtain a 3 mm dose equivalent and a 70 μm dose equivalent by conversion from the 1 cm dose equivalent. I am trying.
【0006】しかしながら、30KeV以下の低エネル
ギー域では、70μm線量当量が1cm線量当量よりも
高感度であり、このため実際に低エネルギーの放射線を
取扱う事業所等では70μm線量当量を直接測定できる
線量計の実現が要望されていた。However, in the low energy region of 30 KeV or lower, the dose equivalent of 70 μm is more sensitive than the dose equivalent of 1 cm, and therefore, the dosimeter which can directly measure the dose equivalent of 70 μm in the offices handling low energy radiation. Was required.
【0007】本発明は上記実情にかんがみてなされたも
ので、1cm線量当量以外の線量当量,つまり3mm線
量当量、70μm線量当量をも直接測定でき、よって低
エネルギー放射線域の測定にも十分対処しうる蛍光ガラ
ス線量計を提供することを目的とする。The present invention has been made in view of the above situation, and it is possible to directly measure dose equivalents other than 1 cm dose equivalent, that is, 3 mm dose equivalent and 70 μm dose equivalent. The present invention aims to provide a fluorescent glass dosimeter.
【0008】[0008]
【課題を解決するための手段】本発明は上記課題を解決
するために、光子エネルギーの放射線に対する透過率の
異なる少なくとも2種類の金属フィルタおよびプラスチ
ックフィルタ等の組合せからなるフィルタ群と、これら
フィルタと対面する位置に配置される1個または複数個
の蛍光ガラス素子とを有し、励起光によって前記蛍光ガ
ラス素子のフィルタに対面する側の面部から得られる蛍
光検出量とこの蛍光検出量に対する線量当量の変換係数
とを用いて複数種類の線量当量を求める蛍光ガラス線量
計である。In order to solve the above problems, the present invention provides a filter group including a combination of at least two kinds of metal filters and plastic filters having different transmittances of photon energy to radiation, and these filters. A fluorescent detection amount obtained from the surface portion of the fluorescent glass device facing the filter by excitation light, and one or a plurality of fluorescent glass devices arranged at facing positions, and a dose equivalent to the detected fluorescence amount. It is a fluorescent glass dosimeter that obtains a plurality of types of dose equivalents using the conversion coefficient and.
【0009】[0009]
【作用】従って、本発明は以上のような手段を講じたこ
とにより、励起光によって蛍光ガラス素子の2つのフィ
ルタに対面する側の面部から得られるそれぞれの蛍光検
出量と予め定めた線量当量への換算係数とを用いて所定
の演算式(後記する(1)式および(2)式)に基づい
て1cm線量当量および70μm線量当量をを求め、さ
らにこれら2つの線量当量を用いて所定の演算式(後記
する(3)式)に基づいて3mm線量当量を求めること
により、他の測定器を用いることなく所要とする複数種
類の線量当量を直接測定するものである。Therefore, according to the present invention, by taking the above-mentioned means, the respective fluorescence detection amounts obtained from the surface portion of the fluorescent glass element facing the two filters by the excitation light and the predetermined dose equivalent can be obtained. The 1 cm dose equivalent and 70 μm dose equivalent are calculated based on the predetermined calculation formulas (equation (1) and formula (2) described later) using the conversion factor of and the predetermined calculation is performed using these two dose equivalents. By determining the 3 mm dose equivalent based on the equation (equation (3) described later), a plurality of required dose equivalents are directly measured without using other measuring instruments.
【0010】[0010]
【実施例】以下、本発明の一実施例について図面を参照
して説明する。図1ないし図3は蛍光ガラス素子とフィ
ルタとの関係を示す図であり、さらに詳細には図1は蛍
光ガラス素子とこの蛍光ガラス素子を支持する支持枠体
との関係を示す分解斜視図、図2は蛍光ガラス素子を支
持した支持枠体を収納するフィルタケースの断面図、図
3はフィルタケース内部の構成体の配置状態を示す断面
図である。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. 1 to 3 are views showing the relationship between the fluorescent glass element and the filter, and more specifically, FIG. 1 is an exploded perspective view showing the relationship between the fluorescent glass element and a support frame supporting the fluorescent glass element, FIG. 2 is a cross-sectional view of a filter case that accommodates a support frame that supports a fluorescent glass element, and FIG. 3 is a cross-sectional view showing an arrangement state of components inside the filter case.
【0011】この発明の蛍光ガラス線量計用の蛍光ガラ
ス素子としては、例えば4個の蛍光ガラス素子または図
に示す如く4個の蛍光ガラス素子に相当する長さを有す
る1個の蛍光ガラス素子11が用いられ、この蛍光ガラ
ス素子11は1組の支持枠体12、13によって支持さ
れる。As the fluorescent glass element for the fluorescent glass dosimeter of the present invention, for example, four fluorescent glass elements or one fluorescent glass element 11 having a length corresponding to four fluorescent glass elements 11 as shown in the figure. Is used, and the fluorescent glass element 11 is supported by a pair of support frames 12 and 13.
【0012】これら1組の支持枠体12、13のうち、
一方の支持枠体12は、例えば4個の開口部14a〜1
4dが形成され、さらに蛍光ガラス素子11の蛍光出力
光路となる部分を除き枠体外周縁部から垂直方向に素子
保持用突起15、…が設けられ、これら素子保持用突起
15、…にて図示矢印方向から嵌め込む蛍光ガラス素子
11を支持する構成となっている。Of these one set of support frames 12 and 13,
The one support frame 12 has, for example, four openings 14a to 1
4d is formed, and element holding protrusions 15, ... Are provided in the vertical direction from the outer peripheral edge of the frame except for the portion which becomes the fluorescence output optical path of the fluorescent glass element 11, and these element holding protrusions 15, ... It is configured to support the fluorescent glass element 11 fitted from the direction.
【0013】他方の支持枠体13は、蛍光ガラス素子1
1を支持する前記一方の支持枠体12を収納保持する役
割を有し、具体的には支持枠体12と同様に複数の開口
部16a〜16dが形成され、かつ、長手方向に対して
直交する方向の両端部を同一方向に向き合うように折り
曲げることによりコ字状部17、17が設けられ、さら
に前記開口部16a〜16dと対応する位置関係をもっ
て各コ字状17、17の面部に切欠部18a〜18dが
形成されている。また、支持枠体13の一端部には蛍光
ガラス素子11の種類や作業者のIDコードを光学的に
読み取るための番号孔19が設けられている。The other supporting frame 13 is a fluorescent glass element 1
1 has a role of accommodating and holding the one support frame body 12 that supports 1, specifically, a plurality of openings 16a to 16d are formed similarly to the support frame body 12 and are orthogonal to the longitudinal direction. U-shaped portions 17 and 17 are provided by bending both ends of the U-shaped portions 17 and 17 so as to face each other in the same direction, and notches are formed in the surface portions of the U-shaped portions 17 and 17 in a positional relationship corresponding to the openings 16a to 16d. Portions 18a to 18d are formed. Further, a number hole 19 for optically reading the type of the fluorescent glass element 11 and the ID code of the operator is provided at one end of the support frame 13.
【0014】そして、以上のような蛍光ガラス素子11
を支持する1組の支持枠体12、13は、図2に示す形
状のプラスチック製フィルタケース20に収納される。
このフィルタケース20は、図示右側から図示左側に順
次すずフィルタ21a、アルミニウムフィルタ21b、
プラスチックフィルタ21c,21dが配置されてい
る。従って、かかる1組の支持枠体12、13を収納し
たフィルタケース20を、各フイルタに跨がって切断し
たとき、図3に示すような断面となっている。Then, the fluorescent glass element 11 as described above is used.
The pair of support frames 12 and 13 for supporting the filter are housed in the plastic filter case 20 having the shape shown in FIG.
The filter case 20 includes a tin filter 21a, an aluminum filter 21b, and
Plastic filters 21c and 21d are arranged. Therefore, when the filter case 20 accommodating the set of support frames 12 and 13 is cut across the filters, the cross section is as shown in FIG.
【0015】さらに、例えばγ線またはX線の照射によ
って被ばくされた蛍光ガラス線量計から被ばく線量を読
み取る場合には、フィルタケース20から1組の支持枠
体12、13を取り出した後、各フィルタ21a〜21
dに対面する蛍光ガラス素子11の各面部が読取装置
側,つまり光電子増倍管31側を臨むように蛍光検出位
置に設置される。しかる後、図4に示すように励起紫外
線をダイアフラム30aを通して蛍光ガラス素子11に
入射し、このとき蛍光ガラス素子11の幅広面側から発
生する蛍光をダイアフラム30bを通して前記光電子増
倍管31で検出する構成となっている。Further, when reading the exposure dose from a fluorescent glass dosimeter exposed by, for example, γ-ray or X-ray irradiation, one set of support frames 12 and 13 is taken out from the filter case 20, and then each filter is removed. 21a-21
Each face of the fluorescent glass element 11 facing d is installed at the fluorescence detecting position so as to face the reader side, that is, the photomultiplier tube 31 side. Thereafter, as shown in FIG. 4, excited ultraviolet rays are made incident on the fluorescent glass element 11 through the diaphragm 30a, and at this time, the fluorescence generated from the wide surface side of the fluorescent glass element 11 is detected by the photomultiplier tube 31 through the diaphragm 30b. It is composed.
【0016】次に、本発明に係わる蛍光ガラス線量計を
用いて個人被ばく線量としての1cm線量当量、3mm
線量当量および70μm線量当量を求める例について説
明する。今、本発明に係わる蛍光ガラス線量計に関し、
実際の測定状態を模擬してその性能を評価すべく、ファ
ントム上に蛍光ガラス線量計を設置した後、γ線、X線
の各光子エネルギーを同じ照射線量で蛍光ガラス線量計
に照射して被ばくさせ、しかる後、励起紫外線を入射し
て励起したとき、蛍光ガラス素子11の各フィルタ21
a〜21dに対面する位置の面部から、図5に示すよう
な蛍光検出量の相対蛍光強度を測定することができる。
なお、同図においてAはすずフィルタ21a、Bはアル
ミニウムフィルタ21b、Cはプラスチックフィルタ2
1c,21dの各々に対面する蛍光ガラス素子11の面
部から得られた蛍光検出量である。すなわち、図5は各
光子エネルギーに対する蛍光検出量の相対蛍光強度の曲
線である。Next, using the fluorescent glass dosimeter according to the present invention, 1 cm dose equivalent as individual exposure dose, 3 mm
An example of obtaining the dose equivalent and the 70 μm dose equivalent will be described. Now, regarding the fluorescent glass dosimeter according to the present invention,
In order to simulate the actual measurement condition and evaluate its performance, a fluorescent glass dosimeter is installed on the phantom, and then the fluorescent glass dosimeter is irradiated with the same irradiation dose of each photon energy of γ-ray and X-ray. Then, when excitation ultraviolet rays are incident and excited, each filter 21 of the fluorescent glass element 11 is
The relative fluorescence intensity of the fluorescence detection amount as shown in FIG. 5 can be measured from the surface portion facing the a to 21d.
In the figure, A is a tin filter 21a, B is an aluminum filter 21b, and C is a plastic filter 2
It is the fluorescence detection amount obtained from the surface portion of the fluorescent glass element 11 facing each of 1c and 21d. That is, FIG. 5 is a curve of the relative fluorescence intensity of the fluorescence detection amount for each photon energy.
【0017】さらに、従来の測定単位であるレントゲン
照射線量から現在の線量当量に換算したときの換算係数
は既に周知の如く図6で示す通りとなっている。そこ
で、本蛍光ガラス線量計を用いて1cm線量当量、3m
m線量当量および70μm線量当量を求める場合、予め
メモリ等にγ線、X線の各照射エネルギーについて、図
6に示すような1cm線量当量、3mm線量当量および
70μm線量当量への換算係数を記憶しておくものとす
る。Further, as is well known, the conversion coefficient when converting the conventional X-ray irradiation dose, which is a unit of measurement, into the present dose equivalent is as shown in FIG. Therefore, using this fluorescent glass dosimeter, 1 cm dose equivalent, 3 m
When obtaining m dose equivalent and 70 μm dose equivalent, the conversion factors for 1 cm dose equivalent, 3 mm dose equivalent and 70 μm dose equivalent as shown in FIG. I will keep it.
【0018】そして、以上のような状態において1cm
線量当量H(1cm)を求める場合、すずフィルタ21
aおよびアルミニウムフィルタ21bと対面する蛍光ガ
ラス素子11の2ヶ所の面部より測定される蛍光検出量
をそれぞれR1、R2とすれば、下記の演算式から求め
ることができる。Then, in the above condition, 1 cm
When obtaining the dose equivalent H (1 cm), the tin filter 21
If the fluorescence detection amounts measured from the two surface portions of the fluorescent glass element 11 that face a and the aluminum filter 21b are R1 and R2, respectively, it can be calculated from the following arithmetic expression.
【0019】 H(1cm)=f・{r・R1+(1−r)R2} ……(1) 但し、上式においてrは分率であって0<r<1の関係
にある。fは蛍光検出量から線量当量への変換係数であ
る。よって、1cm線量当量H(1cm)は、蛍光検出
量R1、R2に最適な分率を用いて加算した後、線量当
量変換係数を乗じて求めるものである。H (1 cm) = f {rR1 + (1-r) R2} (1) However, in the above equation, r is a fraction and 0 <r <1. f is a conversion coefficient from the fluorescence detection amount to the dose equivalent. Therefore, the 1 cm dose equivalent H (1 cm) is obtained by adding the fluorescence detection amounts R1 and R2 using the optimum fraction and then multiplying by the dose equivalent conversion coefficient.
【0020】次に、70μm線量当量については、すず
フィルタ21aとプラスチックフィルタ21cまたは2
1dに対面する蛍光ガラス素子11の2ヶ所の面部より
測定される蛍光検出量をR1、R4とすれば、同様にR
1、R4に最適な分率を用いて加算し、かつ、線量当量
変換係数を乗ずることにより、 H(70μm)=f・{r・R1+(1−r)R2} ……(2) なる演算式で求めることができる。Next, for the 70 μm dose equivalent, the tin filter 21a and the plastic filter 21c or 2 are used.
If the fluorescence detection amounts measured from the two surface portions of the fluorescent glass element 11 facing 1d are R1 and R4, R will be the same.
The calculation of H (70 μm) = f {rR1 + (1-r) R2} (2) is performed by adding 1 and R4 using the optimum fraction and multiplying by the dose equivalent conversion coefficient. It can be obtained by a formula.
【0021】さらに、3mm線量当量H(3mm)は、
図6から明らかなように1cm線量当量と70μm線量
当量との間に位置して変化することから、次式に基づい
て求めれば近似値として得ることができる。Further, the 3 mm dose equivalent H (3 mm) is
As is clear from FIG. 6, since it is located between 1 cm dose equivalent and 70 μm dose equivalent and changes, it can be obtained as an approximate value if it is obtained based on the following equation.
【0022】 H(3mm)=H(1cm)+ {H(70μm)−H(1cm)}・0.85…(3) 従って、前記(1)式、(2)式および(3)式を用い
て求めた各線量当量について各光子エネルギーに対して
プロットしていけば、ほぼ図6に示すような曲線に近似
する曲線を得ることができる。H (3 mm) = H (1 cm) + {H (70 μm) −H (1 cm)} · 0.85 (3) Therefore, the above equations (1), (2) and (3) are By plotting each dose equivalent calculated using each photon energy, it is possible to obtain a curve that is approximately similar to the curve shown in FIG.
【0023】従って、以上のような実施例の構成によれ
ば、蛍光ガラス素子11における2つのフィルタの対面
する方向での蛍光検出量を測定した後、これら2つの蛍
光検出量と線量当量変換係数とを用いて所定の演算を行
うことにより、1cm線量当量および70μm線量当量
を求めることができ、さらに、1cm線量当量と70μ
m線量当量とを用いて所定の演算式を用いて演算すれ
ば、3mm線量当量を求めることができる。よって、特
別に他の測定器等によるエネルギー情報を必要とせず
に、1つの蛍光ガラス線量計を用いて1cm線量当量、
3mm線量当量および70μm線量当量に関する個人被
ばく線量を直接、かつ、容易に測定でき、低エネルギー
域の環境下でも70μm線量当量を直接測定でき、個人
被ばく線量の管理を適切に行うことができる。Therefore, according to the configuration of the above embodiment, after measuring the fluorescence detection amount in the facing direction of the two filters in the fluorescent glass element 11, these two fluorescence detection amounts and the dose equivalent conversion coefficient are measured. By performing a predetermined calculation using and, the 1 cm dose equivalent and 70 μm dose equivalent can be obtained, and further, 1 cm dose equivalent and 70 μm
If the m dose equivalent is used to perform a calculation using a predetermined calculation formula, the 3 mm dose equivalent can be obtained. Therefore, 1 cm dose equivalent can be obtained by using one fluorescent glass dosimeter without requiring energy information from other measuring devices.
It is possible to directly and easily measure the individual exposure dose related to the 3 mm dose equivalent and the 70 μm dose equivalent, and it is possible to directly measure the 70 μm dose equivalent even in an environment in a low energy region, and it is possible to appropriately manage the individual exposure dose.
【0024】なお、上記実施例では、すずフィルタ21
a、アルミニウムフィルタ21bおよびプラスチックフ
ィルタ21c、21dを用いたが、他の材質のフィルタ
を用いて実現してもよい。その他、本発明はその要旨を
逸脱しない範囲で種々変形して実施できる。In the above embodiment, the tin filter 21 is used.
Although a, the aluminum filter 21b, and the plastic filters 21c and 21d are used, they may be realized by using filters made of other materials. In addition, the present invention can be modified in various ways without departing from the scope of the invention.
【0025】[0025]
【発明の効果】以上説明したように本発明によれば、複
数種類の線量当量を直接測定でき、しかも低エネルギー
の放射線域の線量当量をも確実に測定でき、個人被ばく
線量の管理に適切に行える蛍光ガラス線量計を提供でき
る。As explained above, according to the present invention, it is possible to directly measure a plurality of types of dose equivalents, and moreover, it is possible to reliably measure dose equivalents in a low-energy radiation region, and it is possible to appropriately manage individual exposure doses. A fluorescent glass dosimeter can be provided.
【図1】 本発明の蛍光ガラス線量計における蛍光ガラ
ス素子と支持枠体との関係を示す分解斜視図。FIG. 1 is an exploded perspective view showing a relationship between a fluorescent glass element and a support frame in a fluorescent glass dosimeter of the present invention.
【図2】 蛍光ガラス素子を支持した支持枠体を収納す
るフィルタケースの断面図。FIG. 2 is a cross-sectional view of a filter case that houses a support frame that supports a fluorescent glass element.
【図3】 フィルタケース内部の状態を示す断面図。FIG. 3 is a cross-sectional view showing a state inside the filter case.
【図4】 蛍光ガラス素子、励起紫外線および蛍光検出
方向の相対的な位置関係を示す図。FIG. 4 is a diagram showing a relative positional relationship among a fluorescent glass element, excited ultraviolet rays, and fluorescence detection directions.
【図5】 各光子エネルギーに対する蛍光ガラス素子の
各フィルタに対面する位置での相対蛍光強度の曲線図。FIG. 5 is a curve diagram of relative fluorescence intensity at a position facing each filter of the fluorescent glass element with respect to each photon energy.
【図6】 各光子エネルギーに対する照射線量からの1
cm、3mm、70μm線量当量への換算係数の曲線
図。FIG. 6: 1 from the irradiation dose for each photon energy
The curve figure of the conversion factor to cm, 3 mm, and 70 micrometer dose equivalent.
11…蛍光ガラス素子、12、13…支持枠体、14a
〜14d、16a〜16d…開口部、18a〜18d…
切欠部、20…フィルタケース、21a…すずフィル
タ、21b…アルミニウムフィルタ、21c,21d…
プラスチックフィルタ。11 ... Fluorescent glass element, 12, 13 ... Support frame, 14a
-14d, 16a-16d ... Opening part, 18a-18d ...
Notch, 20 ... Filter case, 21a ... Tin filter, 21b ... Aluminum filter, 21c, 21d ...
Plastic filter.
Claims (2)
の異なる少なくとも2種類の金属フィルタおよびプラス
チックフィルタ等の組合せからなるフィルタ群と、これ
らフィルタと対面する位置に配置される1個または複数
個の蛍光ガラス素子とを有し、励起光によって前記蛍光
ガラス素子のフィルタに対面する側の面部から得られる
蛍光検出量とこの蛍光検出量に対する線量当量の変換係
数とを用いて複数種類の線量当量を求めることを特徴と
する蛍光ガラス線量計。1. A filter group composed of a combination of at least two kinds of metal filters and plastic filters having different transmittances of photon energy to radiation, and one or a plurality of fluorescent glasses arranged at a position facing these filters. And a plurality of types of dose equivalents using a fluorescence detection amount obtained from the surface of the fluorescent glass element facing the filter by excitation light and a conversion factor of the dose equivalent to the fluorescence detection amount. Fluorescent glass dosimeter characterized by.
の1cm線量当量、3mm線量当量、70μm線量当量
であることを特徴とする請求項1記載の蛍光ガラス線量
計。2. The fluorescent glass dosimeter according to claim 1, wherein the plurality of types of dose equivalents are 1 cm dose equivalent of γ-ray and X-ray, 3 mm dose equivalent, and 70 μm dose equivalent.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4223191A JPH071308B2 (en) | 1991-02-15 | 1991-02-15 | Fluorescent glass dosimeter |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4223191A JPH071308B2 (en) | 1991-02-15 | 1991-02-15 | Fluorescent glass dosimeter |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH052078A JPH052078A (en) | 1993-01-08 |
| JPH071308B2 true JPH071308B2 (en) | 1995-01-11 |
Family
ID=12630260
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4223191A Expired - Lifetime JPH071308B2 (en) | 1991-02-15 | 1991-02-15 | Fluorescent glass dosimeter |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH071308B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2014202689A (en) * | 2013-04-09 | 2014-10-27 | Agcテクノグラス株式会社 | Fluoroglass dosimeter measuring apparatus, and calibration method of fluoroglass dosimeter measuring apparatus |
| CN117042884A (en) * | 2021-03-31 | 2023-11-10 | 富士胶片株式会社 | Grinding method, polymer block manufacturing method and grinding device |
-
1991
- 1991-02-15 JP JP4223191A patent/JPH071308B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH052078A (en) | 1993-01-08 |
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