JPS59226342A - X-ray photographing device - Google Patents
X-ray photographing deviceInfo
- Publication number
- JPS59226342A JPS59226342A JP58101294A JP10129483A JPS59226342A JP S59226342 A JPS59226342 A JP S59226342A JP 58101294 A JP58101294 A JP 58101294A JP 10129483 A JP10129483 A JP 10129483A JP S59226342 A JPS59226342 A JP S59226342A
- Authority
- JP
- Japan
- Prior art keywords
- level
- video signal
- ray
- aperture
- voltage
- 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.)
- Pending
Links
- 238000001514 detection method Methods 0.000 claims abstract description 8
- 238000003384 imaging method Methods 0.000 claims description 13
- 238000010586 diagram Methods 0.000 description 6
- NJPPVKZQTLUDBO-UHFFFAOYSA-N novaluron Chemical compound C1=C(Cl)C(OC(F)(F)C(OC(F)(F)F)F)=CC=C1NC(=O)NC(=O)C1=C(F)C=CC=C1F NJPPVKZQTLUDBO-UHFFFAOYSA-N 0.000 description 6
- 238000003745 diagnosis Methods 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 1
- 238000002405 diagnostic procedure Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 238000002834 transmittance Methods 0.000 description 1
- 238000004804 winding Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03B—APPARATUS OR ARRANGEMENTS FOR TAKING PHOTOGRAPHS OR FOR PROJECTING OR VIEWING THEM; APPARATUS OR ARRANGEMENTS EMPLOYING ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ACCESSORIES THEREFOR
- G03B15/00—Special procedures for taking photographs; Apparatus therefor
- G03B15/003—Apparatus for photographing CRT-screens
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Analysing Materials By The Use Of Radiation (AREA)
- Radiography Using Non-Light Waves (AREA)
- Apparatus For Radiation Diagnosis (AREA)
Abstract
Description
【発明の詳細な説明】
本発明はXls撮影装置に関し、特にX線の照射野を変
更しながらX線間接撮影を行う装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an Xls imaging apparatus, and more particularly to an apparatus that performs indirect X-ray imaging while changing the X-ray irradiation field.
X@テレビジョン装置の医学診断への応用と実用化は従
来のX線診断法に画期的な進歩と発展をもたらしたもの
でX線診断医の暗室作業からの開放とX線被ばく量の軽
減という大きな利点から現在では欧米諸国においてはも
ちろんわが国においても多数の装置が日常のX線診断業
務に使用されており、今後ますます増加するものと思わ
れる。The application and practical use of X@television equipment to medical diagnosis has brought revolutionary progress and development to conventional X-ray diagnostic methods, freeing X-ray diagnosticians from darkroom work and reducing X-ray exposure. Because of the great advantage of reducing radiation exposure, a large number of devices are now used in daily X-ray diagnostic work not only in Western countries but also in Japan, and the number of devices is expected to increase in the future.
一方、この透視診断時や、診断状態によってはX線フィ
ルムに撮影する場合、部位により、観察し易い画調選択
や、被検体に対し必要部位以外へのX線被ばくを避ける
目的で鉛の可動絞りを用い、適宜X線照射野を調節する
のが哲通である。On the other hand, during this fluoroscopic diagnosis or when taking images on X-ray film depending on the diagnostic condition, depending on the part, the image tone may be selected to make it easier to observe, or the lead may be moved to avoid X-ray exposure to areas other than the necessary parts of the subject. Tetsumitsu uses an aperture to adjust the X-ray irradiation field as appropriate.
すなわち第1図で、1はX線発生器で、2は鉛の絞りで
あり、6は絞りの調節器である。調節器3から絞り2を
開閉するとX線の照射角度は変化し、照射野(像変換面
上のX&lが入射する領域)の変更が可能となる。4は
被検体、例えば人体で度増幅して出力する。6aは投影
レンズで、出力像光を平行光に変換する機能を持ち、6
bと60はそれぞれ、平行光を結像するだめの結像レン
ズである。7は光路切換鏡で、切換鏡7を斜設もしくは
退去させることにより撮影レンズ6aからの光束を結像
レンズ6bもしくは6Cへ誘導する。That is, in FIG. 1, 1 is an X-ray generator, 2 is a lead aperture, and 6 is an aperture adjuster. When the diaphragm 2 is opened or closed by the adjuster 3, the irradiation angle of the X-rays changes, and the irradiation field (the area on the image conversion surface where X&l is incident) can be changed. 4 is amplified by a subject, for example, a human body, and outputted. 6a is a projection lens which has a function of converting output image light into parallel light;
b and 60 are respectively imaging lenses for imaging parallel light. Reference numeral 7 denotes an optical path switching mirror, which guides the light beam from the photographing lens 6a to the imaging lens 6b or 6C by installing or removing the switching mirror 7 obliquely.
8はビデオカメラ、9はビデオ受像器であり、10はカ
メラ、11はロールフィルム、12はコント四−ラ、1
6はアパーチャ絞りである。8 is a video camera, 9 is a video receiver, 10 is a camera, 11 is a roll film, 12 is a controller, 1
6 is an aperture stop.
ここで、被検体4を通してX線を照射するとイメージイ
ンテンシファイア5の入力面に被検体のX線像が入則し
、出力面に可現像として形成される。Here, when X-rays are irradiated through the subject 4, an X-ray image of the subject enters the input surface of the image intensifier 5, and is formed as a developable image on the output surface.
切換鈴7を破線の位置に設定しておくと、ビデオカメラ
8の撮像面には被検体の透過像が再結像され、ビデオ受
像器2にそれが映出される。検者(医師)はその映保を
確3,3シてレリーズすると、切換鏡7は実線の位置に
切換わり、結像レンズ6Cによる透過像がロールフィル
ム11上に形成され、これを露光する。その際、検者は
調節器6により絞り2の絞り風を変えながら撮影を行っ
ているが、絞り量を変えて照射野を変更すると、ビデオ
受像器9の画面の左右端には絞りの影が現われ、その間
の照射野に透過像が映出される。When the switching bell 7 is set at the position indicated by the broken line, a transmitted image of the subject is re-formed on the imaging surface of the video camera 8 and displayed on the video receiver 2. When the examiner (doctor) secures the image and releases it, the switching mirror 7 is switched to the position shown by the solid line, and an image transmitted by the imaging lens 6C is formed on the roll film 11, which is exposed. . At that time, the examiner takes pictures while changing the aperture wind of the aperture 2 using the adjuster 6, but when the irradiation field is changed by changing the amount of aperture, the shadow of the aperture appears on the left and right edges of the screen of the video receiver 9. appears, and a transmitted image is projected in the irradiation field between them.
従って実際に画保の現われる範囲が変化するにもかかわ
らず、ロールフィルムの送りfikが一定であると、画
eE囲が狭いときにはその分のフィルムが無駄になる。Therefore, if the roll film feed fik is constant even though the range in which the image cover actually appears changes, when the image area eE is narrow, the corresponding amount of film will be wasted.
これに対処する為に、コントローラ12を設けて、ビデ
オ信号を検査し、右側の絞りの影と左側の絞りの影の間
口即ち照射野の長さを検知して、その検知量をカメラの
フィルム巻取機構へ入力する。このとき像のカブリを防
ぐよう絞り2に応じてアパーチャ絞り16は開口幅が変
化している。ここでビデオ信号よりX線絞りの影の間隔
を検知することを第2図に示す。第2図(ハ)は透視像
のNff1目の走査線に係わる信号であり、第2図(1
3)はモニタに写し出されるX DA m視伶を示す。To deal with this, a controller 12 is provided to inspect the video signal, detect the width of the shadow of the right aperture and the shadow of the left aperture, that is, the length of the irradiation field, and calculate the detected amount to the camera film. Input to the winding mechanism. At this time, the opening width of the aperture stop 16 is changed according to the stop 2 to prevent fogging of the image. FIG. 2 shows how the distance between the shadows of the X-ray diaphragm is detected from the video signal. FIG. 2(C) is a signal related to the Nff1st scanning line of the perspective image, and FIG.
3) shows the X DA m view displayed on the monitor.
図に示される如く、X線が直接照射されている部分は、
最大電圧Vp を示し、X線絞りによりX線が照射さ
れない部分すなわち画像が形成されない部分は■φ (
ペデスタル電圧)を示す。なおSけ同期信号である。こ
こで従来はX線絞りの影を判別するため、X線照射部の
最大電圧Vpに、定数P(0,2≦μ≦0.6)を乗じ
たμVpを閾値(スレッシュホールド)とし、その電圧
より低い部分をX KBA絞りの影と判別してその影に
相当するカメラのアパーチャ部までカメラの絞り幕を閉
じていた。As shown in the figure, the area directly irradiated with X-rays is
It shows the maximum voltage Vp, and the part where X-rays are not irradiated by the X-ray aperture, that is, the part where no image is formed, is ■φ (
pedestal voltage). Note that S is a synchronization signal. Conventionally, in order to distinguish the shadow of the X-ray diaphragm, μVp, which is the maximum voltage Vp of the X-ray irradiation unit multiplied by a constant P (0, 2≦μ≦0.6), is used as a threshold. The area lower than the voltage was identified as the shadow of the X KBA aperture, and the camera's aperture curtain was closed to the aperture area of the camera that corresponded to that shadow.
この方式であると、第6図の如く最大電圧Vpが低い時
には検出レベルとしての閾値μVpは忠実にX線絞りの
範囲を検出する。しかし第4図の如く被検体にX M透
過率の非常に良く表示器上の輝度を高める領域があって
最大電圧Vpが非常に高い場合、閾値μVpも高くなっ
てしまい図より明らかなように実際のX線絞りより小さ
い範囲を検出してしまう。この為、カメラ側のアパーチ
ャ絞りがこの検出情報により内側まで絞り込まれ、必要
な像を欠損してしまうという欠点があった。With this method, when the maximum voltage Vp is low as shown in FIG. 6, the threshold μVp as the detection level faithfully detects the range of the X-ray aperture. However, as shown in Fig. 4, if the subject has a region with very good XM transmittance that increases the brightness on the display and the maximum voltage Vp is very high, the threshold value μVp also becomes high, as is clear from the figure. A range smaller than the actual X-ray aperture is detected. For this reason, the aperture diaphragm on the camera side is narrowed down to the inside based on this detection information, resulting in the disadvantage that a necessary image is lost.
本発明は斯かる従来例の欠点を除去したX線撮影装置を
提供することを目的とする。An object of the present invention is to provide an X-ray imaging apparatus that eliminates the drawbacks of the conventional example.
この目的を達成するため、本発明においては、最大電圧
Vpが成る電圧以上となった場合には閾値レベルを一定
の値にすることを特徴とする。In order to achieve this object, the present invention is characterized in that the threshold level is set to a constant value when the maximum voltage Vp exceeds the voltage.
第5図は本発明の原理図を示す。FIG. 5 shows a principle diagram of the present invention.
第5図において、最大電圧Vpが成る一定電圧VC以上
になると閾値はμVpでな(p V cとなる。In FIG. 5, when the maximum voltage Vp exceeds a constant voltage VC, the threshold value becomes μVp (pVc).
すなわち最大電圧VpがVcより小さい時は閾値はμV
pであり、VCを超えるとvpの値に拘らず〜一定値μ
Vcとなる。That is, when the maximum voltage Vp is smaller than Vc, the threshold value is μV.
p, and when it exceeds VC, it becomes a constant value μ regardless of the value of vp.
It becomes Vc.
これにより、最大電圧Vpが高い場合にも、正規のX線
絞りの開き範囲を検出できる。Thereby, even when the maximum voltage Vp is high, the normal opening range of the X-ray diaphragm can be detected.
第6図は本発明を実施する電気検出系のブロック図例で
ある。FIG. 6 is an example of a block diagram of an electrical detection system implementing the present invention.
図中Pはビデオ信号のピーク電圧を検出する系で、ピー
クレベルクランプ回路によりピーク電圧をある一定値V
c以下に制限する。P in the figure is a system that detects the peak voltage of the video signal, and the peak voltage is set to a certain value V by a peak level clamp circuit.
Limit to less than c.
このクランプレベルは可変抵抗vR1により自由に設定
できる。これにより閾値レベルは、バッファ1′、可変
抵抗VRを介してピーク電圧がVc以内であれば、μV
pに、またピーク電圧がVcを超えるとμVcに設定さ
れる。そしてコンパレータによりビデオ信号におけるx
6絞りの開口幅が検出される。This clamp level can be freely set by variable resistor vR1. As a result, the threshold level is set to μV if the peak voltage is within Vc via the buffer 1' and the variable resistor VR.
p, and when the peak voltage exceeds Vc, it is set to μVc. Then, a comparator determines x in the video signal.
The aperture width of 6 stops is detected.
なお、ピークレベルクランプ回路において、クランプ電
圧は可変抵抗va−1により予め設定されルカ、ペデス
タルレベル■φに応じて自動的に可変とする回路を設け
ることもできる。In the peak level clamp circuit, a circuit may be provided in which the clamp voltage is set in advance by the variable resistor va-1 and is automatically varied in accordance with the pedestal level φ.
またこのクランプ電圧をビデオ信号の最大電圧Vpに応
じて何段階かに選択的に設定する回路を設けることもで
きる。Further, a circuit may be provided to selectively set this clamp voltage to several levels depending on the maximum voltage Vp of the video signal.
これによりXi絞りの開口幅を種々のピーク電圧Vpの
値に拘らず、正規に検出できる。Thereby, the aperture width of the Xi aperture can be normally detected regardless of the various values of the peak voltage Vp.
なお以上の説明において、ピーク電圧Vpはブランキン
グレベルを基準に検出していたが、測定基準レベルをブ
ランキングレベルでなく、ヘテ゛スタルレベルとするこ
とも可能である。In the above explanation, the peak voltage Vp was detected based on the blanking level, but it is also possible to set the measurement reference level to a hetal level instead of the blanking level.
すなわちペデスタルレベルを基準としてビデオ信号の最
大電圧■p′を測定し、最大電圧■p′がペデスタルレ
ベルを基準とした成る一部値Vc’以内であれば、閾値
をペデスタルレベルを基準としてμVp / に設定し
、一定値Vc’を超える場合には閾値をペデスタルレベ
ルを基準としてμVc ” にすることもできる。That is, the maximum voltage ■p' of the video signal is measured with the pedestal level as a reference, and if the maximum voltage ■p' is within the partial value Vc' with the pedestal level as a reference, the threshold value is μVp / with the pedestal level as a reference. , and if it exceeds a certain value Vc', the threshold value can be set to μVc'' with the pedestal level as a reference.
以上、本発明によれば、ビデオ信号よりX線絞り位置を
決定する際、閾値を成る一部11L圧レベル以下とする
ことで画像の一部が非常に明るいX線透視像の場合でも
、フィルム上のX線伶をカメラのアパーチャ絞りが大き
く欠損することなく正Cζ7よ撮影範囲とすることがで
きる。As described above, according to the present invention, when determining the X-ray diaphragm position from the video signal, by setting the threshold to be less than or equal to the 11L pressure level for a portion of the image, even if a portion of the image is a very bright X-ray fluoroscopic image, the film can be The imaging range of the upper X-ray beam can be set to the normal Cζ7 without causing a large loss in the aperture diaphragm of the camera.
第1図は、本発明に係わるX線(Jν影装置の実施例の
図。
第2図(5)、@は、各々ビデオ信号、X線酋視像を示
す図。
第6図、第4図は、従来例のX線絞りの開口幅を測定す
るための説明図。
第5図は、本発明の原理図。
第6図は、本発明を実施する電気検出系のブロック図。
図中1はX線発生器、2は絞り、6は絞りW11¥J1
器、4は被検体、8はビデオカメラ、9はビデオ受像器
、10はカメラ、11はロールフィルム、12はコント
ローラ、13はアパーチャ絞りである。
出願人 ギヤノン株式会社FIG. 1 is a diagram of an embodiment of the X-ray (Jν) imaging device according to the present invention. FIG. The figure is an explanatory diagram for measuring the aperture width of a conventional X-ray diaphragm. Figure 5 is a principle diagram of the present invention. Figure 6 is a block diagram of an electrical detection system implementing the present invention. 1 is the X-ray generator, 2 is the aperture, 6 is the aperture W11\J1
4 is a subject, 8 is a video camera, 9 is a video receiver, 10 is a camera, 11 is a roll film, 12 is a controller, and 13 is an aperture stop. Applicant: Gyanon Co., Ltd.
Claims (1)
のフィルム送り、アパーチャ絞りを可変とする装置にお
いて。 ビデオ信号の最大電圧が成るレベル以上は検出レベルを
一定とすることを特徴とするX線撮影装置。 2、検出レベルをビデオ信号の最大電圧に応じて複数段
階に設定する特許請求の範囲第1項記載のX線撮影装置
。 3、検出レベルを、X線絞り部位に相当するペテ゛スタ
ルレベルの変動に応じて自動的に可変とする特許請求の
範囲第1項記載のX線撮影装置。[Claims] 1. In a device that detects the opening amount of an X-ray diaphragm using a video signal and makes film advance and aperture diaphragm of a camera variable. An X-ray imaging apparatus characterized in that a detection level is kept constant above a level at which a maximum voltage of a video signal occurs. 2. The X-ray imaging apparatus according to claim 1, wherein the detection level is set in multiple stages depending on the maximum voltage of the video signal. 3. The X-ray imaging apparatus according to claim 1, wherein the detection level is automatically varied according to fluctuations in the petal level corresponding to the X-ray aperture region.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58101294A JPS59226342A (en) | 1983-06-07 | 1983-06-07 | X-ray photographing device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP58101294A JPS59226342A (en) | 1983-06-07 | 1983-06-07 | X-ray photographing device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59226342A true JPS59226342A (en) | 1984-12-19 |
Family
ID=14296815
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP58101294A Pending JPS59226342A (en) | 1983-06-07 | 1983-06-07 | X-ray photographing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59226342A (en) |
-
1983
- 1983-06-07 JP JP58101294A patent/JPS59226342A/en active Pending
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