JPH05200028A - Ultrasonic diagnosing device - Google Patents

Ultrasonic diagnosing device

Info

Publication number
JPH05200028A
JPH05200028A JP4012372A JP1237292A JPH05200028A JP H05200028 A JPH05200028 A JP H05200028A JP 4012372 A JP4012372 A JP 4012372A JP 1237292 A JP1237292 A JP 1237292A JP H05200028 A JPH05200028 A JP H05200028A
Authority
JP
Japan
Prior art keywords
delay time
ultrasonic
delay
time curve
quantization
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
JP4012372A
Other languages
Japanese (ja)
Other versions
JPH0773579B2 (en
Inventor
Shuji Abe
周二 阿部
Shuji Otani
修司 大谷
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.)
Hitachi Ltd
Original Assignee
Aloka 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 Aloka Co Ltd filed Critical Aloka Co Ltd
Priority to JP4012372A priority Critical patent/JPH0773579B2/en
Publication of JPH05200028A publication Critical patent/JPH05200028A/en
Publication of JPH0773579B2 publication Critical patent/JPH0773579B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Ultra Sonic Daignosis Equipment (AREA)
  • Investigating Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)

Abstract

PURPOSE:To provide an ultrasonic diagnosing device giving an ultrasonic tomographic image in which a delay time is quantized and the quantizing width is varied in a position of a group of receiving piezoelectric transducers to reduce circuit elements and prevent the ultrasonic image from degrading the quality. CONSTITUTION:A delay time setting circuit has a delay line 20 and input/output circuit 22. The delay line 20 is provided with 48 output taps 20-1-20-48 and the input/output circuit 22 provided in 4X8 with 48 matrix circuits 22-101-22-806. A delay time curve is quantized to approximate a quantization delay time curve 112 by setting such delay line 20. Then, the quantization delay time curve 112a on both ends of a group of vibrators having a small absolute valve of the delay time is equalized to the prior quantization delay time curve. On the other hand, the quantization delay time curve 112b in the central part is different from the prior one, while the quality of the tomographic image is not remarkably degraded since the influence of both ends of the receiving vibration group on the bundle of ultrasonic wave beams is large.

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、被検体に超音波を送受
信し、受信された反射波に基づき超音波断層画像を得る
超音波診断装置であって、特に電子フォーカス制御の超
音波診断装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an ultrasonic diagnostic apparatus which transmits and receives ultrasonic waves to and from a subject and obtains an ultrasonic tomographic image based on the received reflected waves, and more particularly, an ultrasonic diagnostic apparatus of electronic focus control. Regarding

【0002】[0002]

【従来の技術】従来、複数個の振動子を有する超音波探
触子により超音波を送受信し、断層画像を得る超音波診
断装置において、複数の振動子から送信される超音波ビ
ームは1点で集束される。
2. Description of the Related Art Conventionally, in an ultrasonic diagnostic apparatus which obtains a tomographic image by transmitting and receiving ultrasonic waves by an ultrasonic probe having a plurality of transducers, one ultrasonic beam is transmitted from a plurality of transducers. Be focused on.

【0003】図3で説明すると、直線状に配列された振
動子列10は10-1ないし10-32の32個の振動子を
有している。この振動子列10から距離S0 の点F0 に
超音波ビームを集束させる場合、中心付近の振動子10
-16 ,10-17 から点F0 までの距離S0 と、端部の振
動子10-1,10-32 から点F0 までの距離S1 との経
路差が生じる。この経路差S1 −S0 により生じる超音
波の到達時間の差を予め各振動子の超音波パルスの送信
タイミングの遅延時間(td)として設定することによ
り、点F0 において超音波パルスの位相が揃い焦点が結
ばれる。図4に示すように焦点(F0 )までの距離の長
い端部の振動子に対し、中心付近の振動子の超音波の送
信タイミングを遅くし、またこの中間の各振動子につい
ても焦点(F0 )までの距離に応じて送信タイミングを
遅らせることで、超音波パルスが点F0 に到達した際に
位相が揃い点F0 を焦点とすることができる。この各振
動子に与えるべき遅延時間量を示した曲線が図4に示す
遅延時間曲線100となる。
Explaining with reference to FIG. 3, the transducer array 10 arranged linearly has 32 transducers 10-1 to 10-32. When focusing the ultrasonic beam on the point F0 at a distance S0 from the transducer array 10, the transducers 10 near the center are
A path difference occurs between the distance S0 from -16, 10-17 to the point F0 and the distance S1 from the end vibrators 10-1, 10-32 to the point F0. By setting the difference in the arrival time of the ultrasonic waves caused by this path difference S1 -S0 as the delay time (td) of the transmission timing of the ultrasonic pulse of each transducer in advance, the phase of the ultrasonic pulse is uniform at the point F0. Are tied together. As shown in FIG. 4, the transmission timing of ultrasonic waves of the vibrator near the center is delayed with respect to the vibrator at the end portion where the distance to the focus (F0) is long, and the focus (F0 By delaying the transmission timing in accordance with the distance up to), when the ultrasonic pulse reaches the point F0, the point where the phases are aligned can be focused on the point F0. A curve showing the amount of delay time to be given to each transducer is the delay time curve 100 shown in FIG.

【0004】また、受信においても点F0 からの反射波
が各振動子に到達する時間に時間差が生じる。この時間
差を補正し、位相を揃えるように図5に示す遅延時間設
定回路11を設けている。このときの遅延時間を示す曲
線101が受信時の遅延時間曲線である。
Further, in reception, there is a time difference in the time required for the reflected wave from the point F0 to reach each transducer. The delay time setting circuit 11 shown in FIG. 5 is provided to correct this time difference and align the phases. A curve 101 showing the delay time at this time is a delay time curve at the time of reception.

【0005】以上のような遅延時間の設定は、例えば図
6に示す遅延時間設定回路により行われる。遅延時間設
定回路はディレーライン30と入出力回路32より構成
され、ディレーライン30は80個の出力タップ群(3
0-1、30-2、…、30-80)を有し、入出力回路は4
×8のマトリクス回路80個により構成される。
The setting of the delay time as described above is performed by, for example, the delay time setting circuit shown in FIG. The delay time setting circuit is composed of a delay line 30 and an input / output circuit 32, and the delay line 30 has a group of 80 output taps (3
0-1, 30-2, ..., 30-80) and 4 I / O circuits
It is composed of 80 × 8 matrix circuits.

【0006】ディレーライン30の出力タップは各々2
0n秒(ナノ秒)間隔の遅延時間を出力する。図6にお
いては出力タップ30-1は20n秒、出力タップ30-2
は40n秒、…、出力タップ30-80 は1600n秒の
遅延時間が設定されている。つまりこの場合の量子化幅
は20n秒であり、前述の図5に示す遅延時間曲線10
1をこの量子化幅にて量子化し、近似している(11
1)。この遅延時間設定回路により図7に示すように各
振動子に遅延時間を設定し、超音波パルスを集束させ
る。
Each delay line 30 has two output taps.
The delay time of 0 nsec (nanosecond) is output. In FIG. 6, the output tap 30-1 is 20 ns, and the output tap 30-2 is
, 40 ns, ..., The output tap 30-80 has a delay time of 1600 ns. That is, the quantization width in this case is 20 nsec, and the delay time curve 10 shown in FIG.
1 is quantized with this quantization width and approximated (11
1). This delay time setting circuit sets a delay time for each transducer as shown in FIG. 7 to focus the ultrasonic pulse.

【0007】[0007]

【発明が解決しようとする課題】以上のように遅延時間
設定回路は80個の出力端子を備えたディレーライン3
0と80個のマトリクス回路を有しているが、受信の振
動子群の中央部における各振動子の遅延時間は隣接する
振動子のそれと大きくは変わらない。したがって、受信
の振動子群の中央部付近では量子化幅を小さくする必要
がない。これとは逆に、受信の振動子群の両端部で遅延
時間曲線101を再現するためには、隣接する振動子の
各々に与える遅延時間の差が大きいために細かく量子化
する必要がある。
As described above, the delay time setting circuit includes the delay line 3 having 80 output terminals.
Although it has 0 and 80 matrix circuits, the delay time of each transducer in the central portion of the transducer group for reception is not much different from that of the adjacent transducer. Therefore, it is not necessary to reduce the quantization width near the center of the receiving transducer group. On the contrary, in order to reproduce the delay time curve 101 at both ends of the transducer group for reception, it is necessary to finely quantize because the difference in delay time given to each adjacent transducer is large.

【0008】つまり、1つの遅延曲線を再現するために
必要な量子化幅は受信の振動子群の両端部と中央部にお
いて異なっており、量子化幅を小さく設定すれば受信の
振動子群の中央部にて不必要に小さな量子化幅となって
しまい、量子化幅を大きく設定すれば受信の振動子群の
両端部で遅延曲線の再現性が悪いという問題点があっ
た。
That is, the quantization width required to reproduce one delay curve is different at both ends and the central portion of the receiving transducer group, and if the quantization width is set to be small, the receiving transducer group's There is a problem that the quantization width becomes unnecessarily small in the central portion, and if the quantization width is set large, the reproducibility of the delay curve is poor at both ends of the transducer group for reception.

【0009】さらに、量子化幅を小さくした場合、ディ
レーラインの出力タップ数が増え、マトリクス回路の数
が増加するという問題もあった。
Further, when the quantization width is reduced, there is a problem that the number of delay line output taps increases and the number of matrix circuits increases.

【0010】本発明は、前述の問題を解決するためにな
されたもので、画質を低下させずに回路素子を減少させ
ることのできる超音波診断装置を得ることを目的とす
る。
The present invention has been made to solve the above problems, and an object thereof is to obtain an ultrasonic diagnostic apparatus capable of reducing the number of circuit elements without degrading the image quality.

【0011】[0011]

【課題を解決するための手段】本発明に係る超音波診断
装置においては、超音波パルスの遅延時間を量子化し、
かつ量子化の際に受信の振動子群の部位に応じて異なっ
た量子化幅を設定する。
In the ultrasonic diagnostic apparatus according to the present invention, the delay time of the ultrasonic pulse is quantized,
In addition, when quantizing, different quantizing widths are set according to the parts of the transducer group for reception.

【0012】[0012]

【作用】探触子の部位に応じて異なる遅延時間曲線の傾
きが小さい部位では量子化幅を大きく設定することによ
り、対応する回路素子を減少させることができる。
The circuit element corresponding to the probe can be reduced by setting a large quantization width in the portion where the slope of the delay time curve which differs depending on the portion of the probe is small.

【0013】[0013]

【実施例】以下、本発明の好適な実施例を図面に基づき
説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT A preferred embodiment of the present invention will be described below with reference to the drawings.

【0014】図1に本実施例の超音波探触子の遅延時間
設定回路を示す。遅延時間設定回路はディレーライン2
0と入出力回路22を有し、ディレーライン20は出力
タップ20-1、20-2、…、20-48 の48個を備え、
入出力回路22は4×8にマトリクス回路22-101,
…,22-806の48個のマトリクス回路を備えている。
図2に示す遅延時間の特性から遅延時間の絶対値が大き
い領域、つまり受信の振動子群の中央付近の振動子に与
える遅延時間は、隣り合う振動子で大きく変化しないこ
とが読み取れる。言い換えれば、この領域において遅延
時間曲線101の振動子配列方向の変化割合(遅延時間
曲線の傾き)が小さい。したがって、従来技術で示した
ディレーライン30の出力タップ群において遅延時間の
長い側のタップを間引いて量子化幅を40n秒として
も、従来技術とほぼ同等に遅延時間曲線を量子化でき
る。実施例においては、出力タップ20-1から20-16
までを20n秒間隔で、出力タップ20-17 から20-4
8 までを40n秒間隔で遅延時間を設定している。具体
的には20-1は20n秒、20-2は40n秒、…、20
-16 は320秒に設定され、20-17 は360n秒、2
0-18 は400n秒、…、20-48 は1600n秒に設
定されている。
FIG. 1 shows a delay time setting circuit of the ultrasonic probe of this embodiment. Delay time setting circuit is delay line 2
0 and an input / output circuit 22, and the delay line 20 includes 48 output taps 20-1, 20-2, ..., 20-48,
The input / output circuit 22 is a 4 × 8 matrix circuit 22-101,
, 22-806, 48 matrix circuits are provided.
From the characteristics of the delay time shown in FIG. 2, it can be seen that the area where the absolute value of the delay time is large, that is, the delay time given to the transducer near the center of the transducer group for reception does not change significantly between the adjacent transducers. In other words, the change rate of the delay time curve 101 in the transducer array direction (the slope of the delay time curve) is small in this region. Therefore, the delay time curve can be quantized almost in the same manner as in the prior art, even if the quantization width is set to 40 ns by thinning out the tap with the long delay time in the output tap group of the delay line 30 shown in the prior art. In the embodiment, the output taps 20-1 to 20-16
Output taps 20-17 to 20-4 at 20nsec intervals
The delay time is set up to 8 every 40 ns. Specifically, 20-1 is 20 ns, 20-2 is 40 ns, ..., 20
-16 is set to 320 seconds, 20-17 is 360n seconds, 2
0-18 is set to 400 nsec, and 20-48 is set to 1600 nsec.

【0015】このようなディレーラインの設定により遅
延時間曲線101は量子化によって量子化遅延時間曲線
112と近似される。このとき遅延時間の絶対値が小さ
い受信の振動子群の両端部の量子化遅延時間曲線112
aは前述の量子化遅延時間曲線111と等しくなる。一
方、受信の振動子群の中央部の量子化遅延時間曲線11
2bは前述の量子化遅延時間曲線111とは異なるが、
超音波ビームの集束に対しては受信の振動子群の両端部
の影響が大きいので断層画像の画質を著しく落とすこと
はない。
By setting such a delay line, the delay time curve 101 is approximated to the quantized delay time curve 112 by quantization. At this time, the quantized delay time curve 112 at both ends of the transducer group for reception whose absolute value of delay time is small
a becomes equal to the above-mentioned quantization delay time curve 111. On the other hand, the quantization delay time curve 11 at the center of the transducer group for reception
2b is different from the quantization delay time curve 111 described above,
Since the influence of both ends of the transducer group on reception is large with respect to the focusing of the ultrasonic beam, the image quality of the tomographic image is not significantly deteriorated.

【0016】以上のように遅延時間を設定することによ
って、マトリクス回路素子の数を従来の遅延回路の80
個に比して48個に減少することが可能となる。
By setting the delay time as described above, the number of matrix circuit elements is set to 80 of that of the conventional delay circuit.
It is possible to reduce the number to 48 compared to the number.

【0017】本実施例において、受信の最小遅延時間が
常にディレーラインの最小時間タップになるように補正
している。この時、画像の表示開始位置を一定にするた
めには、送信と受信の最大遅延時間の合計が常に一定に
なるようにしなければならないため、受信での最小時間
タップを使うようにするための補正遅延時間を送信の遅
延時間に振分けている。送信の開始時間は、ある一定周
期の時間をカウントしているだけなので、送信の最大遅
延時間を多くすることは簡単にできる。
In this embodiment, the minimum delay time of reception is always corrected to the minimum time tap of the delay line. At this time, in order to make the display start position of the image constant, the sum of the maximum delay times of transmission and reception must always be constant, so the minimum time tap for reception is used. The correction delay time is distributed to the transmission delay time. Since the transmission start time only counts a certain period of time, it is easy to increase the maximum transmission delay time.

【0018】このように遅延時間を送信時と受信時に振
り分けることにより最小遅延時間が常にディレーライン
の最小出力タップにすることができ、これにより、遅延
時間曲線の再現性が良くなるため、量子化による誤差を
大きくしないようにすることができる。
By thus dividing the delay time at the time of transmission and at the time of reception, the minimum delay time can always be set to the minimum output tap of the delay line, which improves the reproducibility of the delay time curve, and thus the quantization It is possible to prevent the error due to the error from increasing.

【0019】また、本実施例においてはディレーライン
の間引きは1つ飛びに設定し、量子化幅は20n秒と4
0n秒の2種類にて設定したが、量子化幅を20n秒、
40n秒、60n秒の3種類に設定することも可能であ
る。例えば、出力タップ20-1から20-24 までが20
n秒間隔で、出力タップ20-25 から20-40 までが4
0n秒間隔で、出力タップ20-41 から20-48 までが
60n秒間隔で設定することも可能である。
In this embodiment, the delay lines are thinned out by one and the quantization width is 20 nsec.
Although it was set with two types of 0 ns, the quantization width was 20 ns,
It is also possible to set three types of 40 ns and 60 ns. For example, output taps 20-1 to 20-24 are 20
Output taps 20-25 to 4 are 4 at n-second intervals.
It is also possible to set the output taps 20-41 to 20-48 at 60 ns intervals at 0 ns intervals.

【0020】さらに、出力タップの数が48個の場合に
ついて示したが、これに限られるものではない。
Further, the case where the number of output taps is 48 is shown, but the number is not limited to this.

【0021】[0021]

【発明の効果】以上のように受信のディレーラインの出
力タップを間引いて使用したので、回路素子を減じるこ
とが可能となり、また超音波ビームの集束に影響の大き
い受信の振動子群の端部の量子化幅は従来と同様に設定
したために超音波断層画像の画質を低下させることはな
い。
As described above, since the output taps of the reception delay line are thinned out and used, it becomes possible to reduce the number of circuit elements and the end portion of the reception transducer group which greatly affects the focusing of the ultrasonic beam. Since the quantization width of is set as in the conventional case, the image quality of the ultrasonic tomographic image is not deteriorated.

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

【図1】本発明に係る超音波診断装置の遅延時間設定回
路の構成図である。
FIG. 1 is a configuration diagram of a delay time setting circuit of an ultrasonic diagnostic apparatus according to the present invention.

【図2】本発明に係る量子化された遅延時間曲線を示す
図である。
FIG. 2 is a diagram showing a quantized delay time curve according to the present invention.

【図3】複数個の超音波振動子を備えた超音波探触子の
集束方法を示す図である。
FIG. 3 is a diagram showing a method of focusing an ultrasonic probe including a plurality of ultrasonic transducers.

【図4】送信時に設定する遅延時間の説明図である。FIG. 4 is an explanatory diagram of a delay time set at the time of transmission.

【図5】受信時に設定する遅延時間の説明図である。FIG. 5 is an explanatory diagram of a delay time set at the time of reception.

【図6】従来の遅延時間設定回路の構成図である。FIG. 6 is a configuration diagram of a conventional delay time setting circuit.

【図7】従来の量子化された遅延時間曲線を示す図であ
る。
FIG. 7 is a diagram showing a conventional quantized delay time curve.

【符号の説明】[Explanation of symbols]

10 振動子列 11 ディレーライン(機能) 20 ディレーライン(素子) 22 入出力回路 10 Transducer array 11 Delay line (function) 20 Delay line (element) 22 Input / output circuit

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】複数個の振動子で構成された探触子により
超音波パルスを送信し、被検体より反射した前記超音波
パルスを受信し、さらに前記複数個の振動子ごとに受信
信号に所定の遅延時間量を設定し、超音波パルスを集束
させ超音波断層画像を得る超音波診断装置において、 前記遅延時間は量子化され、かつ前記受信の振動子群の
部位により量子化幅が異なることを特徴とする超音波診
断装置。
1. An ultrasonic wave pulse is transmitted by a probe composed of a plurality of transducers, the ultrasonic wave pulse reflected from a subject is received, and further, a received signal is obtained for each of the plurality of transducers. In an ultrasonic diagnostic apparatus that sets a predetermined delay time amount and focuses an ultrasonic pulse to obtain an ultrasonic tomographic image, the delay time is quantized, and the quantization width differs depending on the part of the transducer group for reception. An ultrasonic diagnostic apparatus characterized by the above.
JP4012372A 1992-01-27 1992-01-27 Ultrasonic diagnostic equipment Expired - Fee Related JPH0773579B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4012372A JPH0773579B2 (en) 1992-01-27 1992-01-27 Ultrasonic diagnostic equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4012372A JPH0773579B2 (en) 1992-01-27 1992-01-27 Ultrasonic diagnostic equipment

Publications (2)

Publication Number Publication Date
JPH05200028A true JPH05200028A (en) 1993-08-10
JPH0773579B2 JPH0773579B2 (en) 1995-08-09

Family

ID=11803438

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4012372A Expired - Fee Related JPH0773579B2 (en) 1992-01-27 1992-01-27 Ultrasonic diagnostic equipment

Country Status (1)

Country Link
JP (1) JPH0773579B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010081965A (en) * 2008-09-29 2010-04-15 Toshiba Corp Ultrasonic diagnostic apparatus
WO2012108344A1 (en) * 2011-02-07 2012-08-16 株式会社 東芝 Ultrasound diagnostic apparatus

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010081965A (en) * 2008-09-29 2010-04-15 Toshiba Corp Ultrasonic diagnostic apparatus
WO2012108344A1 (en) * 2011-02-07 2012-08-16 株式会社 東芝 Ultrasound diagnostic apparatus
JP2012161445A (en) * 2011-02-07 2012-08-30 Toshiba Corp Ultrasonic diagnostic apparatus
CN103298411A (en) * 2011-02-07 2013-09-11 株式会社东芝 Ultrasound diagnostic apparatus
US9629611B2 (en) 2011-02-07 2017-04-25 Toshiba Medical Systems Corporation Ultrasound diagnosis apparatus for substantially reducing tap concentration

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