JPS5951346A - Code conversion circuit of ultrasonic tomographic imaging apparatus - Google Patents

Code conversion circuit of ultrasonic tomographic imaging apparatus

Info

Publication number
JPS5951346A
JPS5951346A JP57144106A JP14410682A JPS5951346A JP S5951346 A JPS5951346 A JP S5951346A JP 57144106 A JP57144106 A JP 57144106A JP 14410682 A JP14410682 A JP 14410682A JP S5951346 A JPS5951346 A JP S5951346A
Authority
JP
Japan
Prior art keywords
transducer
scanning line
conversion circuit
code conversion
transducers
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.)
Granted
Application number
JP57144106A
Other languages
Japanese (ja)
Other versions
JPH0215027B2 (en
Inventor
Keiichi Murakami
敬一 村上
Yuichi Sugiyama
雄一 杉山
Nobushiro Shimura
孚城 志村
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.)
Fujitsu Ltd
Original Assignee
Fujitsu 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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP57144106A priority Critical patent/JPS5951346A/en
Publication of JPS5951346A publication Critical patent/JPS5951346A/en
Publication of JPH0215027B2 publication Critical patent/JPH0215027B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G10MUSICAL INSTRUMENTS; ACOUSTICS
    • G10KSOUND-PRODUCING DEVICES; METHODS OR DEVICES FOR PROTECTING AGAINST, OR FOR DAMPING, NOISE OR OTHER ACOUSTIC WAVES IN GENERAL; ACOUSTICS NOT OTHERWISE PROVIDED FOR
    • G10K11/00Methods or devices for transmitting, conducting or directing sound in general; Methods or devices for protecting against, or for damping, noise or other acoustic waves in general
    • G10K11/18Methods or devices for transmitting, conducting or directing sound
    • G10K11/26Sound-focusing or directing, e.g. scanning
    • G10K11/34Sound-focusing or directing, e.g. scanning using electrical steering of transducer arrays, e.g. beam steering
    • G10K11/341Circuits therefor
    • G10K11/345Circuits therefor using energy switching from one active element to another
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/52Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S15/00
    • G01S7/52017Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S15/00 particularly adapted to short-range imaging
    • G01S7/5205Means for monitoring or calibrating

Landscapes

  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Acoustics & Sound (AREA)
  • Multimedia (AREA)
  • Ultra Sonic Daignosis Equipment (AREA)
  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Radiography Using Non-Light Waves (AREA)

Abstract

PURPOSE:To correct the shift of a tomographic image, by adding an offset amount to information related to the position and the direction of the display scanning line of each vibrator when the shift of the tomographic image is generated by the attaching errors of a plurality of ultrasonic vibrators in a single probe. CONSTITUTION:The reference slot pulse from the rotary encoder 2 attached to the rotary shaft of a single probe having two vibrators assembled therein is subjected to the shaping of a wave form by a wave form shaping circuit 3 to generate an initiating pulse which in turn initiate a counter 4 and the pulse P2 subjected to wave form shaping is clocked to generate a display scanning line number M prior to correction. From the count value, a scanning judging circuit 5 judges whether either one of two vibrators is used in the transmission or the reception of ultrasonic waves and a selection signal S (a) is used as the selection input of a data selector 6 while either one of offset amount A, B indicated by SWA, SWB is selected to add a correction amount to a scanning line number M' prior to correction in an adder 9. By this mechanism, the shift of a tomographic image is corrected.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は超音波断層撮像装置に係シ、特に1同−探触子
内に複数の超音波振動子を持ち、それらの振動子を機械
的に回転又は揺動させる事により超音波ビームの送受信
方向を変えて断層像を得る装置において、振動子取付の
機棹的精度の低さを電子回路で救済するための符号変換
回路に関する。
[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to an ultrasonic tomographic imaging apparatus, and in particular has a plurality of ultrasonic transducers in one probe, and mechanically converts the transducers. The present invention relates to a code conversion circuit for using an electronic circuit to remedy the low mechanical precision of mounting a transducer in an apparatus that obtains tomographic images by changing the transmission and reception direction of an ultrasonic beam by rotating or swinging the ultrasonic beam.

〔発明の従来技術〕[Prior art to the invention]

従来、同−探触子内に複数の振動子を紹み込んだ例とし
て、例えば第1図(a)に示す様に、1つの回転中心1
の周囲に、同一回転半径r上で且つ回転中心を通る直線
上に2つの振動子A、  Bを平行に配列したものがあ
る。これらの振動子を回転させ、第1図(b)に示す如
く超音波送受信方向を変え、送受信の方向に対応してデ
ィスプレイの表示走査線の方向を変化させると、第1(
9)(c)の如き扇状の表示走査線が得られる。この時
超音波ビーム送受信の方向は、例えば第1図(d)に示
す如き、円周上に等間隔に配置されたスロットS1と基
準位置を示すスロットS2とを持つロータリエンコーダ
2を回転軸1に取シ付け、スロット毎にパルスを発生す
る光学的スロット検出回路の出力をクロックとして、カ
ウンタkit作させる事によシ、カウンタの値として得
る事ができる。このカウンタは、基準位置スロット検出
回路の出力を用いて、ロータリエンコーダが1回転する
毎に特定の値に初期化する場合もある事は言う寸でも々
い。以下、第1図に示したロータリエンコーダ形式の位
置検出機構を用いた機械的回転式探触子を例にとって、
本発明の詳細を述べる。
Conventionally, as an example of introducing multiple transducers into the same probe, for example, as shown in Fig. 1(a), one rotation center 1
There is a device in which two vibrators A and B are arranged in parallel around the same radius of rotation r and on a straight line passing through the center of rotation. When these transducers are rotated to change the direction of ultrasonic transmission and reception as shown in FIG.
9) A fan-shaped display scanning line as shown in (c) is obtained. At this time, the direction of ultrasonic beam transmission and reception is determined by moving a rotary encoder 2, which has slots S1 arranged at equal intervals on the circumference and slots S2 indicating a reference position, to a rotating shaft 1, as shown in FIG. 1(d), for example. The counter value can be obtained by attaching the output to the optical slot detection circuit that generates a pulse for each slot as a clock and operating the counter kit. Suffice it to say, this counter may be initialized to a specific value each time the rotary encoder rotates once, using the output of the reference position slot detection circuit. Below, we will take as an example a mechanical rotary probe using a rotary encoder type position detection mechanism shown in Figure 1.
The details of the present invention will be described.

今、2つの振動子A、Bが第2図(a)に示す如く機械
的に正確に回転軸の周囲に取り付けられていたとする。
Assume now that two vibrators A and B are mechanically accurately attached around the rotation axis as shown in FIG. 2(a).

この時、例えば同図の如く回転中心を通る直線上に並ん
だターゲットT1.T2があったとすると、振動子A又
はBによる断層像はそれぞれ第2図(b)又は(C)の
様にな9、この2つの断層像ヲ重ね合わせてもターゲッ
トの像はズレる事がないO これに対し、第3図(a)に示す如く、例えば振動子A
は正しく取や付けられているが振動子Bの取シ付は角度
が狂っていた場合を考えてみると、振動子Aによる断層
像は第3図(b)の如く正しいものが得られる。ところ
が、振動子Bによる像は、例3− えば第3図(c)の如く、エンコーダの出力から求めら
れた表示走査線の番号(図の場合l)と、実際の超音波
ビームの送受信方向(表示走査線番号に換算してi−△
N)との間にズレ(走査線番号に換算してΔN)が発生
する。この結果、実際には第3図(c)の破線の方向に
表示されるべき像が、実線の方向に表示される事になる
0N図(d)(e)も回転角度が変化した時の同様の例
を示してあシ、結局、振動子Bによる像は、同図(f)
の様になり、ターゲットは本来表示されるべき表示走査
線からΔN本だけズした表示走査線に表示される。従っ
て、振動子A及びBによる像’t−3ifね合わせると
、第3図(ロ))の如く、ターゲットが2重に見える事
になる。
At this time, for example, as shown in the figure, targets T1. If there is T2, the tomographic images produced by transducer A or B will be as shown in Figure 2 (b) or (C),9 respectively, and even if these two tomographic images are superimposed, the image of the target will not shift. O On the other hand, as shown in FIG. 3(a), for example, the vibrator A
If we consider a case where the transducer B is installed correctly but the angle of the transducer B is incorrect, the correct tomographic image obtained by the transducer A will be obtained as shown in FIG. 3(b). However, as shown in Example 3 - Figure 3(c), the image produced by transducer B is based on the display scanning line number (l in the figure) obtained from the encoder output and the actual transmission and reception direction of the ultrasound beam. (Converted to display scanning line number, i-△
N), a deviation (ΔN in terms of scanning line number) occurs. As a result, the image that should actually be displayed in the direction of the broken line in Figure 3(c) is displayed in the direction of the solid line.The 0N diagrams (d) and (e) also show when the rotation angle changes. A similar example is shown.In the end, the image produced by transducer B is shown in the same figure (f).
The target is displayed on a display scan line that is shifted by ΔN lines from the display scan line where it should originally be displayed. Therefore, when the images 't-3if' from the oscillators A and B are combined, the target will be seen twice as shown in FIG. 3(b).

この問題は、振動子を取シ付ける際の機械的精度を充分
に向上させれば解決する問題ではあるが、価格的にそれ
が困難な場合もある0 〔発明の目的〕 本発明による符号変換回路は、例えば上に述べたA、 
、B 2つの振動子を用いる場合の問題に対し、Aの一
表示走査線番号に対しでは何の修正もしない4− が、Bの表示走査線番号としては、エンコーダパルスカ
ウント回路から出力された値からΔNを減じた値を用い
る、という方法によシ、第3図(f)の像を同図(h)
の如く修正し、同図(b)に示す様な振動子Aの像と重
ねても、2Nに見える事がない様にするものである。
This problem can be solved by sufficiently improving the mechanical precision when mounting the vibrator, but it may be difficult to do so in terms of cost.0 [Object of the Invention] Code conversion according to the present invention The circuit is, for example, A mentioned above,
, B To solve the problem when using two transducers, no correction is made for one display scanning line number of A4- However, as the display scanning line number of B, the display scanning line number output from the encoder pulse count circuit is By using the value obtained by subtracting ΔN from the value, the image in Fig. 3(f) can be converted to the image in Fig. 3(h).
This is done so that even if the image is superimposed on the image of the vibrator A as shown in FIG. 3(b), it will not look like 2N.

〔発明の実施例〕[Embodiments of the invention]

本発明の一実施例を第4図によシ説明する。 An embodiment of the present invention will be explained with reference to FIG.

第4図において、カウンタ4は、ロータリエンコーダ2
0基準スロツトパルスを波形整形した初期化パルスによ
って初期化(たとえば0にセット)された後、ロータリ
エンコーダの円周上スロットパルスを波形整形したパル
スP2をクロックとして、修正前の表示走査線番号Mを
発生する。
In FIG. 4, the counter 4 is connected to the rotary encoder 2.
After being initialized (for example, set to 0) by an initialization pulse that is a waveform-shaped 0 reference slot pulse, the display scanning line number M before correction is set using a pulse P2 that is a waveform-shaped waveform of the circumferential slot pulse of the rotary encoder. Occur.

□走査線番号判定回路5は、カウンタの値から、第3図
(a)の2つの振動子のうちA、 Bいずれが超音波ビ
ームの送受信に使われているかを判定し、判定出力St
−発生する。信号Sは、データセレクタ6の選択入力と
な、9、SWA、SWBで指定されるオフセット量0F
FSETA、0FFSETBのいずれかを選択する。
□The scanning line number determination circuit 5 determines from the value of the counter which of the two transducers A or B in FIG. 3(a) is used for transmitting and receiving the ultrasound beam, and outputs a determination output St
- occurs. The signal S is the selection input of the data selector 6, and the offset amount 0F specified by 9, SWA, and SWB.
Select either FSETA or 0FFSETB.

第3図の場合金側にとると、振動子Aに対する修正量0
FFSET A FiO振動子Bに対する修正前0FP
SET Bは一ΔNである。データセレクタ6で選択さ
れた修正出力ΔMは加算器9に送られ、修正前の走査線
番号M′と加算されて修正後の表示走査線番号M=M’
+ΔMが得られる。
In the case of Figure 3, if it is taken on the gold side, the amount of correction for vibrator A is 0.
FFSET A 0FP before correction for FiO resonator B
SET B is -ΔN. The modified output ΔM selected by the data selector 6 is sent to the adder 9, where it is added to the scanning line number M' before modification, and the display scanning line number after modification M=M'
+ΔM is obtained.

尚、以上で述べた方式の場合、例えば第3図(e)の場
合を考えてみると、第5図に示す如く、表示走査線の番
号として、Kの代わりにに一ΔNを用いると、表示走査
線の方向は正しく表現されるが、走査線の出発点が、実
際の超音波ビーム(第5図破a)の出発点Pではなく、
Qに移動してしまう。
In the case of the method described above, for example, considering the case of FIG. 3(e), if one ΔN is used instead of K as the number of the display scanning line as shown in FIG. Although the direction of the displayed scanning line is correctly expressed, the starting point of the scanning line is not the starting point P of the actual ultrasound beam (Fig. 5, broken a).
It moves to Q.

その結果、第5図の如く、本来表示されるべき位置に対
して、横方向に△X、*方向に△Yの誤差を持つ事にな
る。つまり、表示走査線の方向は正しく修正されるが、
位置は誤差を含む事になる。
As a result, as shown in FIG. 5, there is an error of ΔX in the horizontal direction and ΔY in the * direction with respect to the position where it should originally be displayed. This means that the direction of the display scan line is corrected, but
The position will include an error.

ΔNが小さい時はこの誤差は無視できる程度のものであ
るが、ΔNが大きくなった場合には、表示走査線の出発
点修正情報を各走査線毎に発生し、偏向信号発生部に送
る必要がある。第6図にこの時の構成図を示す。第6図
の2〜9は第4図の対応する番号のものと同じもの全表
わす。第6図では、コードコンバータ10が追加されて
いる。第5図の△X、△Yは、エンコーダによる表示走
査線番号の値M′及び修正量ΔMの両者に依存する。
When ΔN is small, this error is negligible; however, when ΔN becomes large, it is necessary to generate starting point correction information for each scanning line and send it to the deflection signal generator. There is. FIG. 6 shows a configuration diagram at this time. Numbers 2 to 9 in FIG. 6 represent all the same numbers as those in FIG. 4. In FIG. 6, a code converter 10 is added. ΔX and ΔY in FIG. 5 depend on both the value M' of the display scanning line number by the encoder and the correction amount ΔM.

第6図のコードコンバータ10はM9及び6Mから△X
及び△Yを発生するためのもので例えばROMやPLA
等を用いて実現される。M、ΔX。
The code converter 10 in FIG. 6 is from M9 and 6M to △X
and △Y, such as ROM or PLA.
It is realized using etc. M, ΔX.

△Yは偏向信号発生回路へ送られた5(xyディスプレ
イの場合)、あるいは座標計算回路に送られてメモリア
ドレスの計算に用いられたり(TV方式の場合)する。
ΔY is sent to the deflection signal generation circuit (in the case of an xy display), or is sent to the coordinate calculation circuit and used to calculate a memory address (in the case of a TV system).

第3図の説明において、振動子Aは機械的に正しく取付
けられていると仮定したが、第7図(a)に示す如く、
振動子A及びBの取付角度が、表示走査線番号に換算し
てそれぞれΔN人、ΔNBだけずれていた場合振動子A
及びBの表示走査線番号にそれぞれ−、ムNA及び−Δ
NBだけのオフセット量を与えれば良い事は明らかであ
るが△NA +ΔNBが=7= 小さい場合は、例えば振動子Aによる像を基準として、
振動子Bの表示走査線番号に−(ΔNB−△NA)だけ
のオフセットを与えて第7図(d) K示す如く表示す
れば、第7図(b)に示す振動子Aによる像とほぼ重な
る事は言うまでもない。
In the explanation of FIG. 3, it was assumed that the vibrator A was mechanically installed correctly, but as shown in FIG. 7(a),
If the mounting angles of transducers A and B differ by ΔN and ΔNB, respectively, in terms of display scanning line numbers, transducer A
-, MNA and -Δ for the display scanning line numbers of and B, respectively.
It is clear that it is sufficient to give an offset amount of only NB, but if △NA + △NB = 7 = small, for example, using the image by transducer A as a reference,
If the display scanning line number of transducer B is offset by -(ΔNB-ΔNA) and displayed as shown in FIG. 7(d) K, the image obtained by transducer A shown in FIG. 7(b) will be approximately Needless to say, they overlap.

この方法を用いた場合、像がダブって見える事は解消さ
れるが、全体として本来表示されるべき位置とけズした
位f)IJC表示される事になる。それが不都合な場合
は、上記の振動子Bに対するオフセット量(図−7の場
合−(ΔNB−ΔNA)だけを与えた後に、振動子A、
  Bの両者に対して等量(第7図の場合−△NA )
のオフセットff与えれば良い。この方法を用いる場合
の構成を第8図に示す。
If this method is used, the image will no longer appear double, but as a whole, the IJC will be displayed at the position where it should have been displayed and where it has been scratched. If this is inconvenient, after giving only the offset amount to the above-mentioned transducer B (in the case of Figure 7 - (ΔNB - ΔNA)),
Equal amounts for both B (in the case of Figure 7 - △NA)
It is sufficient to give the offset ff. FIG. 8 shows a configuration using this method.

第8図において2〜9は第4図の同一番号のものと同じ
ものであり、振動子Aを基準とした場合を考えているの
で、第4図におけるスイッチ7は除かれて、振動子Aに
対しては一定のオフセット針(0)が与えられている。
In FIG. 8, 2 to 9 are the same as those with the same numbers in FIG. A constant offset needle (0) is given for .

99出力をそのまま表示走査線番号として用いると、第
7図(b)と(d)を重ねた像が得られる。スイッチ1
1はその像を第7図8− (e)の如くするのに必要なオフセット量−△NA’r
作成するためのものであシ、これと加算器9との出力が
加算器12で加え合わされる事によシ、第7図(e)の
如き像が得られる。
If the 99 output is directly used as the display scanning line number, an image in which FIGS. 7(b) and 7(d) are superimposed is obtained. switch 1
1 is the offset amount -△NA'r necessary to make the image as shown in Fig. 7-8-(e)
By adding this and the output of adder 9 in adder 12, an image as shown in FIG. 7(e) is obtained.

この様に、2段階に分けてオフセット量を設定する利点
は以下の2点である。
The advantages of setting the offset amount in two stages in this manner are as follows.

第1に、複数の振動子による像がズレずに重なって見え
さえすれば良い。という場合は、全振動子に対して本来
の位置に表示される様に個別にオフセットを与える場合
に比べて、調整が少くてよい。第2に、一旦全ての振動
子の像が重なった後は、1ケ所の調整のみで全体像に対
する走査線番号のオフセットを調整できる。
First, it is only necessary that the images formed by the plurality of vibrators overlap without deviation. In this case, fewer adjustments are required than when giving individual offsets to all the vibrators so that they are displayed at their original positions. Second, once the images of all the transducers are superimposed, the offset of the scanning line number relative to the overall image can be adjusted by adjusting only one location.

以上の説明は2つの振動子が1つの探触子内に含まれた
場合についてのみ行なったが、3つ以上の振動子が1つ
の探触子内に含まれる場合についても、第4図の走を線
番号判定回路5からの出力を2ビット以上にし、オフセ
ット量設定5Wft7゜8の2つから更に増設し、デー
タセレクタ6の入カボート訪X17−憎課・手λ讃?)
口q kA +y口耐−↓呼事は明白である。
The above explanation was given only for the case where two transducers are included in one probe, but the case in which three or more transducers are included in one probe is also applicable as shown in Fig. 4. The output from the line number determination circuit 5 is set to 2 bits or more, the offset amount setting is increased from the two of 5Wft7°8, and the input port of the data selector 6 is changed to )
Mouth q kA + y mouth resistance − ↓ event is obvious.

又、以上の説明は、位置検出機構としてロータリエンコ
ーダを用いた場合についてのみ行なったが、ポテンショ
メータを用いて角度を検出したーリ、回転運動を直糾運
動に変換した上で差動トランスを用いる事により角度を
検出したりして位置検出を行なう場合についても適用で
きる。これらの場合、検出された角度信号(アナログ)
をA/D変換する時は、第4図の構成において、カウン
タ4の出力式わシに、A/D変換器の出力あるいはその
出力をしかるべく符号変換して表示走査線番号に直した
ものを用いればよい。アナログ信号のままで処理する場
合はカウンタ4の代わりにボテンシ目メータ又は差動ト
ランスの出力を、振動子番号判定判定回路5の代わ勺に
電圧比較器としかるべき比較電圧源を、データセレクタ
60代わシにアナログマルチプレクサを、スイッチ7.
8の代わ夛に可変電圧源を、ディジタル加算器9の代わ
りにアナログ加算器を、それぞれ置けば良い。
Also, the above explanation was given only for the case where a rotary encoder is used as the position detection mechanism, but if the angle is detected using a potentiometer, then a differential transformer is used after converting rotational motion into linear motion. It can also be applied to cases where position detection is performed by detecting an angle. In these cases, the detected angle signal (analog)
When performing A/D conversion, in the configuration shown in Fig. 4, the output of the A/D converter or the output of the A/D converter is converted into a display scanning line number by appropriate sign conversion. You can use When processing analog signals as they are, use the output of a potentiometer or differential transformer in place of the counter 4, a voltage comparator and appropriate comparison voltage source in place of the transducer number determination judgment circuit 5, and a data selector 60. Instead, use an analog multiplexer and switch 7.
A variable voltage source may be placed in place of 8, and an analog adder may be placed in place of digital adder 9.

〔発明の効果〕〔Effect of the invention〕

子を1つの探触子内に組み込む時、ある程度以上の機械
精度を祷る事が費用の点で困難な場合に、模様的精度の
不足を安価に回路的に救済する事ができる。
When incorporating the probe into one probe, if it is difficult to achieve a certain level of mechanical precision due to cost, the lack of pattern precision can be compensated for at low cost using a circuit.

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

第1図、第2図は一般の探触子の動作説明図、第3図は
本発明の一実施例の動作説明図、第4図は本発明の一実
施例ブロック図、第5図と第6図は夫々本発明の第2の
実施例の動作説明図とブロック図、第7図と第8図は夫
々本発明の第3の実施例の動作d−図とブロック図であ
る。 躬 2 図 (C) 第 5 図 AXAY     M 第 6 図 (α)(1))、(C) (i)                    Ce
)   −第7図
Figures 1 and 2 are diagrams explaining the operation of a general probe, Figure 3 is a diagram explaining the operation of an embodiment of the present invention, Figure 4 is a block diagram of an embodiment of the invention, and Figure 5. FIG. 6 is an operational explanatory diagram and a block diagram of the second embodiment of the present invention, and FIGS. 7 and 8 are an operational diagram and a block diagram of the third embodiment of the present invention, respectively. 2 Figure (C) Figure 5 AXAY M Figure 6 (α) (1)), (C) (i) Ce
) -Figure 7

Claims (3)

【特許請求の範囲】[Claims] (1)単一の探触子内で複数の超音波振動子を機械的に
回転又は揺動させながら超音波を送受信し、ディスプレ
イ上に輝度変調又はカラー変調圧よって断層像を表示す
る超音波断層撮像装置で、現に送受信を行なっている振
動子の機械的な位置又は方向又はその両者を機−的又は
光学的エンコーダ又は差動トランス又はボテンシ田メー
タ等の機械的位置検出機構によって検出し、表示走査線
の位置又は方向又はその両者を決定する超音波断層撮像
装置において、上記機械的位置検出機構の出力から直接
に得られた各振動子の位置又は方向又はその両者に関す
る情報に、各振動子に対して独立に任意のオフセラ)i
ie加えて、各振動子に対する表示走査線の位置又は方
向又はその両者に関する情報を修正する事10徴とする
超音波断層撮像装置の符号変換回路。
(1) Ultrasound that transmits and receives ultrasound while mechanically rotating or swinging multiple ultrasound transducers within a single probe, and displays tomographic images on a display using brightness modulation or color modulation pressure. In a tomographic imaging device, the mechanical position and/or direction of the transducer currently performing transmission and reception is detected by a mechanical position detection mechanism such as a mechanical or optical encoder, a differential transformer, or a potentiometer, In an ultrasonic tomography apparatus that determines the position and/or direction of a display scanning line, each vibration is added to the information regarding the position and/or direction of each vibrator obtained directly from the output of the mechanical position detection mechanism. any offseller)i independently for the child
ie, a code conversion circuit for an ultrasonic tomographic imaging apparatus, which additionally modifies information regarding the position and/or direction of a display scanning line for each transducer;
(2)複数の超音波振動子の取付精度の機械的誤差によ
シ、異る振動子によって得られた断層像にズレが生じる
場合、第1項記載のオフセット量として、ある特定の振
動子による断層像を基準として他の振動子による断層像
が基準断層像に丁度型なり合う様なオフセット量を基準
とした振動子以外の振動子の光示走査線の位置又は方向
又はその両者を決定するために与える事を特徴とする特
許請求の範囲第(1)項記載の超音波断層撮像装置の符
号変換回路。
(2) If a deviation occurs in tomographic images obtained by different transducers due to mechanical errors in the mounting accuracy of multiple ultrasonic transducers, the amount of offset described in paragraph 1 may be determined by using a certain transducer. Determining the position or direction of the optical scanning line of a transducer other than the transducer, or both, based on the amount of offset such that the tomographic image produced by the other transducer exactly conforms to the reference tomographic image, using the tomographic image obtained by the transducer as a reference. A code conversion circuit for an ultrasonic tomographic imaging apparatus according to claim 1, wherein the code conversion circuit is provided to perform the following steps.
(3)上記基準とした振動子自身も取付に機械的な誤差
を含む場合、その機械的誤差を補正するために表示走査
線番号に付与すべきオフセット量を、当該探触子内の全
ての振動子に対して等しく与える事を特徴とする特許請
求の範囲第(2)項記載の超音波断層撮像装置の符号変
換回路。
(3) If the transducer itself, which is based on the above standard, includes mechanical errors in its installation, the amount of offset that should be added to the display scanning line number in order to compensate for the mechanical errors should be applied to all of the transducers in the probe. A code conversion circuit for an ultrasonic tomographic imaging apparatus according to claim (2), characterized in that the code conversion circuit applies equal power to the transducers.
JP57144106A 1982-08-20 1982-08-20 Code conversion circuit of ultrasonic tomographic imaging apparatus Granted JPS5951346A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57144106A JPS5951346A (en) 1982-08-20 1982-08-20 Code conversion circuit of ultrasonic tomographic imaging apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57144106A JPS5951346A (en) 1982-08-20 1982-08-20 Code conversion circuit of ultrasonic tomographic imaging apparatus

Publications (2)

Publication Number Publication Date
JPS5951346A true JPS5951346A (en) 1984-03-24
JPH0215027B2 JPH0215027B2 (en) 1990-04-10

Family

ID=15354322

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57144106A Granted JPS5951346A (en) 1982-08-20 1982-08-20 Code conversion circuit of ultrasonic tomographic imaging apparatus

Country Status (1)

Country Link
JP (1) JPS5951346A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61146247A (en) * 1984-12-19 1986-07-03 松下電器産業株式会社 Ultrasonic diagnostic apparatus
WO2004034911A1 (en) * 2002-10-18 2004-04-29 Matsushita Electric Industrial Co., Ltd. Ultrasonic probe

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61146247A (en) * 1984-12-19 1986-07-03 松下電器産業株式会社 Ultrasonic diagnostic apparatus
JPH0414579B2 (en) * 1984-12-19 1992-03-13 Matsushita Electric Ind Co Ltd
WO2004034911A1 (en) * 2002-10-18 2004-04-29 Matsushita Electric Industrial Co., Ltd. Ultrasonic probe
US7431697B2 (en) 2002-10-18 2008-10-07 Matsushita Electric Industrial Co., Ltd. Ultrasonic probe

Also Published As

Publication number Publication date
JPH0215027B2 (en) 1990-04-10

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