JPS61172539A - X-ray diagnostic apparatus - Google Patents

X-ray diagnostic apparatus

Info

Publication number
JPS61172539A
JPS61172539A JP60013688A JP1368885A JPS61172539A JP S61172539 A JPS61172539 A JP S61172539A JP 60013688 A JP60013688 A JP 60013688A JP 1368885 A JP1368885 A JP 1368885A JP S61172539 A JPS61172539 A JP S61172539A
Authority
JP
Japan
Prior art keywords
ray
image
thickness
inspected
diagnostic apparatus
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
Application number
JP60013688A
Other languages
Japanese (ja)
Inventor
博司 筒井
末喜 馬場
大森 康以知
理 山本
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP60013688A priority Critical patent/JPS61172539A/en
Publication of JPS61172539A publication Critical patent/JPS61172539A/en
Pending legal-status Critical Current

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  • Analysing Materials By The Use Of Radiation (AREA)
  • Apparatus For Radiation Diagnosis (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 産業上の利用分野 この発明は厚さ測定機能を有するX線診断装置に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application This invention relates to an X-ray diagnostic apparatus having a thickness measurement function.

従来の技術 X線フィルムを含めて、従来よりX線診断に用いられる
X線画像は、被検査体を透過したX線の強度変化による
X線透過画像であシ、得られる情報には厚さの情報と単
位体積あたりの吸収の情報が重畳した情報となっている
Conventional technology X-ray images conventionally used for X-ray diagnosis, including X-ray film, are X-ray transmission images based on changes in the intensity of X-rays that have passed through the object being examined, and the information obtained includes thickness This information is a combination of information on absorption per unit volume and information on absorption per unit volume.

第5図において被検査体1を透過するX線について考え
る。被検査体1に入射するX線強度を工。。
In FIG. 5, consider the X-rays that pass through the object 1 to be inspected. Adjust the intensity of X-rays incident on the object to be inspected 1. .

被検査体を透過した後のX線強度をI、、I、、X線が
透過する被検査体1の厚さをx 1. x 2 e X
線が透過する部分の平均吸収係数をμm、μ2とすると
次式が成立する。
The X-ray intensity after passing through the object to be inspected is I, , I, and the thickness of the object 1 to be inspected through which the X-rays pass is x 1. x 2 e
Assuming that the average absorption coefficient of the portion through which the line passes is μm and μ2, the following equation holds true.

I 、 =Ioexp (−μm ・x、)    ・
”・・”(’)I  =I  exp(−μ ・I )
   ・・・・・・・・・(匂2  o       
 2  2 このように、通常のX線透過画像と呼ばれる画像の成分
として、X線が透過する経路の吸収係数と経路の長さの
積であるμ・Iというパラメータを有している。
I, = Ioexp (-μm ・x,) ・
"..."(') I = I exp (-μ ・I )
・・・・・・・・・(Smell 2 o
2 2 Thus, as a component of an image called a normal X-ray transmission image, it has the parameter μ·I, which is the product of the absorption coefficient of the path through which X-rays pass and the length of the path.

このようなパラメータを含む従来のX線透過画像の一例
を第6図に示す。第6図中aは胸部X線透過画像の概略
図である、A−にを結ぶ線上の透過X線強度分布をbK
示す。bに示すX線透過画像において、透過X線強度の
弱い部分が存在する場合、μ・Iの値が大きいというこ
とは分析できるが、吸収係数μが大きいのか、被検査体
の厚さIが厚いのか判別できない。そこで通常のX線透
過画像の読影(診断)を行なうには、医師の訓練による
人体(被検査体)の形状、形態パターンの記憶から、経
験的にX線透過画像を見ながら頭の中でパターン認識を
行なっている。
An example of a conventional X-ray transmission image including such parameters is shown in FIG. In Fig. 6, a is a schematic diagram of a chest X-ray transmission image, and bK shows the transmitted X-ray intensity distribution on the line connecting A-.
show. In the X-ray transmission image shown in b, if there is a part with weak transmitted X-ray intensity, it can be analyzed that the value of μ・I is large. I can't tell if it's thick or not. Therefore, in order to interpret (diagnose) a normal X-ray image, it is necessary to memorize the shape and morphological pattern of the human body (examined body) through medical training, and then to make a mental image while looking at the X-ray image from experience. Performing pattern recognition.

発明が解決しようとする問題点 近年、電気的に各種の画像処理が行なえるようになり、
X線透過画像も画像処理を行なうことにより診断能力を
高めるようになってきたが、上述のようにX線透過画像
そのものに被検査体の厚さ情報が含まれており、診断に
おいて最も重要なパラメータである吸収係数のみに関す
る情報を得ることができず、画像処理にも限度がある。
Problems to be solved by the invention In recent years, it has become possible to perform various types of image processing electrically.
The diagnostic ability of X-ray transmission images has also been improved through image processing, but as mentioned above, the X-ray transmission images themselves contain information on the thickness of the object being examined, which is the most important information in diagnosis. Information regarding only the absorption coefficient, which is a parameter, cannot be obtained, and image processing is also limited.

本発明は上記の欠点を解消するもので、X線透過画像か
ら被検査体の厚さのパラメータを除くことにより、被検
査体の平均吸収係数のみのパラメータからなる新しい画
像となり、被検査体の形態観察が容易な新しい診断機能
を有するX線診断装置を提供することを目的とする。
The present invention solves the above-mentioned drawbacks, and by removing the parameter of the thickness of the object to be inspected from the X-ray transmission image, a new image consisting of only the average absorption coefficient of the object to be inspected is created. It is an object of the present invention to provide an X-ray diagnostic apparatus having a new diagnostic function that facilitates morphological observation.

問題点を解決するための手段 この発明のX線診断装置は、被検査体の撮影部分の厚さ
を測定し、電気信号に変換されたX線透過画像を電気的
な画像処理により被検査体の厚さによるパラメータを除
去するものである。
Means for Solving the Problems The X-ray diagnostic apparatus of the present invention measures the thickness of the photographed portion of the object to be examined, and converts the X-ray transmission image into an electrical signal into an electrical image of the object to be examined. This method removes parameters depending on the thickness of the .

作  用 本発明は上記のような手段により、被検査体の厚さによ
るパラメータを除去することにより、従来の撮影によシ
得られるX線透過画像情報に含まれる被検査体の厚さに
よるパラメータと、被検査体を構成する物質のX線吸収
係数によるパラメータとを分離し、物質の平均吸収係数
のみからなる画像を得ることができる。
Effect of the present invention By using the above-described means to remove the parameter based on the thickness of the subject, the parameter based on the thickness of the subject included in the X-ray transmission image information obtained by conventional imaging is removed. By separating the X-ray absorption coefficient and the parameter based on the X-ray absorption coefficient of the substance constituting the object to be inspected, it is possible to obtain an image consisting only of the average absorption coefficient of the substance.

実施例;排芋 以下発明の原理について、図面を参照して説明する。Example: Potato The principle of the invention will be explained below with reference to the drawings.

第2図はX線が被検査体を透過するときの強度変化を示
す原理図である。図において、横軸Iは位置を示し、縦
軸d (x)は厚さを示す。位置Iにおける被検査体1
への入射X線強度を工。(り、被被検鉢体1らの透過X
線強度をI (x) 、被検査体1の位置XにおいてX
線の通過する厚さをd (z) ’ 、通過する部分(
図中射線部)の平均吸収係数をμ(I)とすると下記の
ような式が成立する。
FIG. 2 is a principle diagram showing changes in intensity when X-rays pass through an object to be inspected. In the figure, the horizontal axis I indicates position, and the vertical axis d(x) indicates thickness. Tested object 1 at position I
Manipulate the incident X-ray intensity. (Transmission of the tested pot body 1 etc.
The line intensity is I (x), and X at the position X of the inspected object 1
The thickness of the line passing through is d(z)', and the passing part (
If the average absorption coefficient of the ray part in the figure is μ(I), the following equation holds true.

I(”)=工0(x)exp(−μ0・dO)   −
−−(3)両辺対数をとると f(z)=μ(x)−d(x)          −
・・−・・−4吸収係数μ(I)と厚さd(りの積とし
て表わすことができる。従来のX線透過画像の信号は、
透過X線■ その画像信号の対数をとることにより、X線透過画像信
号は全て平均吸収係数μと厚さdの積からなる信号とな
る。ここで厚さdの情報を前もって測定し、X線透過画
像信号から被検査体の厚さの値を除すことによシ、X線
透過画像を、被検査体の厚さの情報を含まない平均吸収
係数の値のみからなる画像に変換することができる。
I(”)=Eng.0(x)exp(-μ0・dO) −
−−(3) Taking the logarithm on both sides, f(z) = μ(x)−d(x) −
...--4 It can be expressed as the product of absorption coefficient μ(I) and thickness d(ri).The signal of a conventional X-ray transmission image is
Transmitted X-ray ■ By taking the logarithm of the image signal, the X-ray transmitted image signal becomes a signal consisting of the product of the average absorption coefficient μ and the thickness d. Here, by measuring the information on the thickness d in advance and subtracting the value of the thickness of the object to be inspected from the X-ray transmission image signal, the It is possible to convert the image into an image consisting only of values of the average absorption coefficient.

以上のような本発明の原理を用いた実施例について、図
面を参照して説明する。第1図は本発明のX線診断装置
の構成図である。従来のX線透過画像を得るには、X線
制御器5によシ出力制御されたX線発生器2よシ出射し
たX線を被検査体1に照射し、透過したX線強度をX線
センサ3によシ検出し、メインコントローラ6、画像処
理器7を通してディスプレイ8によシ画像表示を行なう
Embodiments using the principles of the present invention as described above will be described with reference to the drawings. FIG. 1 is a configuration diagram of an X-ray diagnostic apparatus according to the present invention. To obtain a conventional X-ray transmission image, the inspected object 1 is irradiated with X-rays emitted from the X-ray generator 2 whose output is controlled by the X-ray controller 5, and the intensity of the transmitted X-rays is The line sensor 3 detects the image, and the image is displayed on the display 8 through the main controller 6 and image processor 7.

得られたX線透過画像から厚さのパラメータを除去する
ために、まず厚さ測定器4,4′を用いて被検査体の撮
影部位の厚さを測定する。次にメインコントローラ6、
画像処理器7を通して透過X線強度に含まれる厚さのパ
ラメータを除くことにより、平均吸収係数分布の画像を
得ることができる。
In order to remove the thickness parameter from the obtained X-ray transmission image, first, the thickness of the photographed region of the subject is measured using the thickness measuring devices 4, 4'. Next, the main controller 6,
By removing the thickness parameter included in the transmitted X-ray intensity through the image processor 7, an image of the average absorption coefficient distribution can be obtained.

この実施例に用いた厚さ測定器4,4′はモアレ画像か
ら厚さを測定する測定器であり、格子縞投光器と被検査
体上に生じたモアレ画像を撮影するカメラおよびモアレ
画像(すなわち等高線画像)から被検査体の2次元厚さ
分布を測定する処理部からなっている。この測定器によ
り得られる厚さ分布の一例を第3図に示す。図中aは得
られたモアレ画像であり、この等高線から被検査体の厚
さ分布が求まる。a中A−A’を結ぶ線上の厚さ分布は
、等高線を2次曲線近似で結ぶことにより、bに示すよ
うな厚さ分布が得られる。
The thickness measuring devices 4 and 4' used in this example are measuring devices that measure the thickness from a moire image, and include a checkered stripe projector, a camera that takes a moire image generated on the object to be inspected, and a moire image (i.e., a contour line). It consists of a processing section that measures the two-dimensional thickness distribution of the inspected object from the image). An example of the thickness distribution obtained by this measuring device is shown in FIG. In the figure, a is the obtained moiré image, and the thickness distribution of the object to be inspected can be determined from the contour lines. The thickness distribution on the line connecting A-A' in a is obtained by connecting the contour lines by quadratic curve approximation, as shown in b.

第4図に上記の方法による平均吸収係数分布の画像を得
る一例を示す。aは通常のX線透過画像であり、図中A
 −A/を結ぶ線上の透過X線強度分とると、その値は
平均吸収係数μ(x)と厚さd(りの積となる。次にc
 l/CA −A’を結ぶ線上の厚さ分布を示す。この
値d (りにより透過X線強度分布の対数値を除算する
ことにより、平均吸収係数からなる分布dを得ることが
できる。
FIG. 4 shows an example of obtaining an image of the average absorption coefficient distribution by the above method. A is a normal X-ray transmission image, and A in the figure
If we take the transmitted X-ray intensity on the line connecting -A/, its value is the product of the average absorption coefficient μ(x) and the thickness d
The thickness distribution on the line connecting l/CA-A' is shown. By dividing the logarithm value of the transmitted X-ray intensity distribution by this value d, a distribution d consisting of the average absorption coefficient can be obtained.

本発明に用いることのできるX線センサとしては、透過
X線強度を電気信号に変換できるセンサが使用できる。
As the X-ray sensor that can be used in the present invention, a sensor that can convert transmitted X-ray intensity into an electrical signal can be used.

例えばX線イメージインテンシファイアと撮像管の組合
せ(いわゆるX線テレビ)を用いれば、透過X線強度を
ビデオ信号として取出すことができる。また、S i 
、Go 、GaAs 。
For example, if a combination of an X-ray image intensifier and an image pickup tube (so-called X-ray television) is used, the transmitted X-ray intensity can be extracted as a video signal. Also, S i
, Go, GaAs.

CdTe、HgI等の半導体検出器を用いたX線センサ
アレイ、Xs電電離上センサアレイよび螢光体と光セン
サをもちいたセンサアレイ等をスキャンして透過X線強
度を測定し、電気信号に変換することができる。
The transmitted X-ray intensity is measured by scanning an X-ray sensor array using a semiconductor detector such as CdTe or HgI, an Xs ionization sensor array, a sensor array using a phosphor and an optical sensor, etc., and converted into an electrical signal. can be converted.

また本発明に用いる厚さ測定器としては、前述のモアレ
画像測定器以外に、レーザ光により被検査体上をスキャ
ンし、その反射光から被検査体までの距離を検出して厚
さを計測する測定器等を用いることもできる。
In addition to the above-mentioned moiré image measuring device, the thickness measuring device used in the present invention can be used to measure the thickness by scanning the object to be inspected with a laser beam and detecting the distance to the object from the reflected light. It is also possible to use a measuring device etc.

発明の効果 本発明はX線診断装置に被検査体の厚さ測定器を備え、
従来の撮影により得られるX線透過画像情報に含まれる
被検査体の厚さのパラメータを除くことにより被検査体
の吸収係数のみのパラメータからなる画像情報に変換す
ることができ、被検査体の吸収による情報のみを直接視
認できるために診断の能率を非常に高めることができる
Effects of the Invention The present invention includes an X-ray diagnostic apparatus equipped with a thickness measuring device for an object to be inspected,
By removing the parameter of the thickness of the object contained in the X-ray transmission image information obtained by conventional radiography, it is possible to convert it into image information consisting only of the absorption coefficient of the object. Diagnosis efficiency can be greatly increased because only information from absorption can be directly viewed.

さらに、この装置を医学上のみならず、被破壊検査等に
用いれば、被検査体の形状を画像から取除くことにより
、物体内の形状のみならず、物質の同定測定も行なえ、
また、例えば両部に空洞等が存在する場合、従来は空洞
の奥行が不明であったのが、物体の厚さのパラメータを
取除くことにより、逆に空洞の奥行の測定も可能となり
、きわめて有用である。
Furthermore, if this device is used not only for medical purposes but also for destructive inspection, by removing the shape of the object to be inspected from the image, it is possible to identify not only the shape inside the object but also the substance.
In addition, for example, when there is a cavity in both parts, the depth of the cavity was previously unknown, but by removing the parameter of the thickness of the object, it is now possible to measure the depth of the cavity, which is extremely useful. Useful.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明のX線診断装置の構成の概略を示す断面
図、第2図はX線が物体を透過するときの強度変化を示
す原理図、第3図は厚さ測定器によシ得られる厚さ分布
の一例を示す図、第4図は平均吸収係数分布の画像を得
る方法を示す図、第6図は被検査体を透過するX線の変
化を示す図、第6図は胸部X線透過画像を示す概略図で
ある。 、  1・・・・・・被検査体、2・・・・・・X線発
生器、3・・・・・・X線センサ、4,41・・・・・
・厚さ測定器、6・旧・・メインコントローラ。 代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図 第2図 I(χ2 第3図 ((ス・ン Q                  χ第4図 第5図 ■。■。 −I、I2
Fig. 1 is a sectional view showing the outline of the configuration of the X-ray diagnostic device of the present invention, Fig. 2 is a principle diagram showing the change in intensity when X-rays pass through an object, and Fig. 3 is a diagram showing how the Figure 4 is a diagram showing an example of the obtained thickness distribution. Figure 4 is a diagram showing a method for obtaining an image of the average absorption coefficient distribution. Figure 6 is a diagram showing changes in X-rays passing through the object to be inspected. is a schematic diagram showing a chest X-ray transmission image. , 1...Object to be inspected, 2...X-ray generator, 3...X-ray sensor, 4, 41...
・Thickness measuring device, 6. Old... Main controller. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 Figure I (χ2 Figure 3 ((S・N Q Figure 4 Figure 5 ■.■. -I, I2

Claims (4)

【特許請求の範囲】[Claims] (1)X線を発生するX線発生器と、被検査体を透過し
たX線を検出して電気信号に変換するX線検出器と、被
検査体の厚さを測定する厚さ測定器とを備え、前記X線
検出器により得られたX線透過像信号を前記厚さ測定器
の出力信号を係数として補正する機能を有することを特
徴とするX線診断装置。
(1) An X-ray generator that generates X-rays, an X-ray detector that detects the X-rays that have passed through the object to be inspected and converts them into electrical signals, and a thickness measuring device that measures the thickness of the object to be inspected. An X-ray diagnostic apparatus comprising: a function of correcting an X-ray transmission image signal obtained by the X-ray detector using an output signal of the thickness measuring device as a coefficient.
(2)X線検出器が、半導体X線検出器、半導体X線検
出器アレイまたは半導体X線面検出器からなることを特
徴とする特許請求の範囲第1項記載のX線診断装置。
(2) The X-ray diagnostic apparatus according to claim 1, wherein the X-ray detector comprises a semiconductor X-ray detector, a semiconductor X-ray detector array, or a semiconductor X-ray surface detector.
(3)X線検出器がガス電離箱検出器またはガス電離箱
検出器アレイからなることを特徴とする特許請求の範囲
第1項記載のX線診断装置。
(3) The X-ray diagnostic apparatus according to claim 1, wherein the X-ray detector comprises a gas ionization chamber detector or a gas ionization chamber detector array.
(4)X線検出器がイメージインテンシファイヤーおよ
び撮像管からなることを特徴とする特許請求の範囲第1
項記載のX線診断装置。
(4) Claim 1, wherein the X-ray detector comprises an image intensifier and an image pickup tube.
The X-ray diagnostic device described in Section 1.
JP60013688A 1985-01-28 1985-01-28 X-ray diagnostic apparatus Pending JPS61172539A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60013688A JPS61172539A (en) 1985-01-28 1985-01-28 X-ray diagnostic apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60013688A JPS61172539A (en) 1985-01-28 1985-01-28 X-ray diagnostic apparatus

Publications (1)

Publication Number Publication Date
JPS61172539A true JPS61172539A (en) 1986-08-04

Family

ID=11840126

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60013688A Pending JPS61172539A (en) 1985-01-28 1985-01-28 X-ray diagnostic apparatus

Country Status (1)

Country Link
JP (1) JPS61172539A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5516330A (en) * 1978-07-20 1980-02-05 Fuji Elelctrochem Co Ltd Enclosed type cell
JP2020014801A (en) * 2018-07-27 2020-01-30 株式会社日立製作所 X-ray imaging device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5516330A (en) * 1978-07-20 1980-02-05 Fuji Elelctrochem Co Ltd Enclosed type cell
JPS585509B2 (en) * 1978-07-20 1983-01-31 富士電気化学株式会社 sealed battery
JP2020014801A (en) * 2018-07-27 2020-01-30 株式会社日立製作所 X-ray imaging device

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