JPH01104251A - Ultrasonic diagnostic apparatus - Google Patents

Ultrasonic diagnostic apparatus

Info

Publication number
JPH01104251A
JPH01104251A JP63232574A JP23257488A JPH01104251A JP H01104251 A JPH01104251 A JP H01104251A JP 63232574 A JP63232574 A JP 63232574A JP 23257488 A JP23257488 A JP 23257488A JP H01104251 A JPH01104251 A JP H01104251A
Authority
JP
Japan
Prior art keywords
vibration elements
reception
transmission
ultrasonic
elements
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
JP63232574A
Other languages
Japanese (ja)
Other versions
JPH026533B2 (en
Inventor
Akira Sasaki
明 佐々木
Kenichi Hirayae
平八重 謙一
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 Healthcare Manufacturing Ltd
Original Assignee
Hitachi Medical Corp
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 Hitachi Medical Corp filed Critical Hitachi Medical Corp
Priority to JP63232574A priority Critical patent/JPH01104251A/en
Publication of JPH01104251A publication Critical patent/JPH01104251A/en
Publication of JPH026533B2 publication Critical patent/JPH026533B2/ja
Granted legal-status Critical Current

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

Abstract

PURPOSE:To obtain a homogeneous ultrasonic image having no density variation between scanning lines, by changing the number of vibrators to be used between at the time of transmission from a vibration element and at the time of reception from the specimen and setting a scanning pitch to 1/2 and bringing directionality to synthetic one of transmission and reception. CONSTITUTION:At the first time, ultrasonic waves are transmitted by vibration elements 1, 2, 3...n and received by vibration elements 1, 2, 3...n-1. At the second time, ultrasonic waves are also transmitted by the vibration elements 1, 2, 3...n and received by vibration elements 2, 3...n. On and after, the vibration elements are shifted by one to similarly execute the operations of the first and second transmitting and receiving cycles by (n) vibration elements 2, 3...n+1. That is, in the first cycle, ultrasonic waves are transmitted by the vibration elements 2, 3...n+1 and received by the vibration elements 2, 3...n and, in the second cycle, ultrasonic waves are transmitted by the vibration elements 2, 3...n+1 and received by the vibration elements 3, 4...n+1. For example, when the number (n) of the vibration elements are set to n=10, transmission is always performed using 10 vibration elements and reception is always performed using 9 vibration elements and the scanning pitch at that time becomes 1/2. Therefore, the enhancement of accuracy and the uniformization of the sensitivity difference between ultrasonic beams adjacent to each other can be achieved.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、超音波診断装置に係り、特に超音波走査線密
度をあげて画質の向上を計った、所謂1/2ピッチ走査
方式の超音波診断装置に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to an ultrasonic diagnostic apparatus, and particularly to an ultrasonic diagnostic apparatus using the so-called 1/2 pitch scanning method, which aims to improve image quality by increasing the ultrasonic scanning line density. The present invention relates to a sound wave diagnostic device.

[従来の技術] 超音波診断装置として、探触子の任意の個数の振動素子
数を、繰り返しパルス毎に、あるいは任意の一定周期毎
に変化させて超音波走査線密度を向上させる1/2ピッ
チ走査方式のものが特開昭52−68775号公報によ
って公知である。
[Prior Art] As an ultrasonic diagnostic device, an arbitrary number of vibrating elements of a probe is changed for every repetitive pulse or every arbitrary fixed period to improve the ultrasonic scanning line density by 1/2. A pitch scanning method is known from Japanese Patent Laid-Open No. 52-68775.

[g!明が解決しようとする例題コ 前記公報に記載された1/2ピッチ走査方式のものは、
相隣り合う超音波ビームに出力および受信感度差がでる
ため、均質な画像を得るのが困難である。その原理説明
を第1図において説明する。
[g! The example problem that Akira is trying to solve is that of the 1/2 pitch scanning method described in the above publication.
Since there are differences in output and reception sensitivity between adjacent ultrasound beams, it is difficult to obtain a homogeneous image. The principle will be explained with reference to FIG.

第2図において、1,2,3.・・・、n−1,nは等
間隔に配設された振動素子を示す、49口。
In FIG. 2, 1, 2, 3. ..., n-1, n indicate vibrating elements arranged at equal intervals, 49 holes.

ハ、二、ホ、へは、振動素子による超音波送信。C, 2, HO, HE: Ultrasonic wave transmission using a vibrating element.

受信の回数を示し、それぞれ、イにおいては1゜2.・
・・、n−1の振動素子により、口においては1.2.
・・・、nの振動素子により、さらにハにおいては2,
3.・・・、nの振動素子により超音波の送受信を行な
うようにしである。したがって、各振動素子の中心間隔
を1ピツチ(IP)とすると。
Indicates the number of receptions, 1°2.・
..., n-1 vibration elements in the mouth, 1.2.
..., n vibration elements further increase 2,
3. ..., n vibrating elements transmit and receive ultrasonic waves. Therefore, if the center spacing of each vibrating element is 1 pitch (IP).

1回毎の超音波送受信は超音波ビームが1/2(1/2
F)ピッチずつずれるように振動素子が選択使用される
ことになる。
For each ultrasonic transmission/reception, the ultrasonic beam is 1/2 (1/2
F) Vibration elements are selectively used so as to be shifted by pitch.

すなわち、上記従来技術は、振動素子数n=10とする
と、第1表に示すように、超音波送受順位第1表 1と2.3と4.5と6は振動素子数が9個と10個の
ように相違するため、振動素子での送受感度が違い、そ
の受信信号をそのまま表示すると、超音波走査線の1本
おきに濃淡差が生じることになり、当然のことながら均
一な画像を得ることができないという問題点を有してい
るものであった。
That is, in the above conventional technology, when the number of vibrating elements is n=10, as shown in Table 1, the ultrasonic transmission/reception order of Table 1, 1, 2.3, 4.5, and 6 has 9 vibrating elements. Because there are 10 different ultrasonic scanning lines, the transmitting and receiving sensitivity of the vibrating element is different, and if the received signal is displayed as it is, there will be a difference in density between every other ultrasonic scanning line, which naturally results in a uniform image. The problem was that it was not possible to obtain

本発明の目的は゛、超音波走査線密度を向上させ、かつ
相隣り合う超音波ビームの感度差をなくし、表示された
走査線間の濃淡のない均質な超音波画像が得られる超音
波診断装置を提供することにある。
The object of the present invention is to provide an ultrasonic diagnostic apparatus that improves the density of ultrasonic scanning lines, eliminates sensitivity differences between adjacent ultrasonic beams, and obtains homogeneous ultrasonic images with no shading between displayed scanning lines. Our goal is to provide the following.

[課題を解決するための手段] 上記目的は、複数(m個)の振動子を有する探触子と、
n個の振動子(但し、n<m)#1〜#nを、振動素子
1個毎にずらしながら順次選択し、各選択したn個の振
動子に対して第1.第2の送受波サイクルを設定し、第
1の送受波サイクルにあってはn個の選択振動子#1〜
#n全体を駆動して送波を行わせ、受波に際しては振動
子#1〜#(n+α)(但し、α=+1又は−1)を選
択して受波を行わせ、第2の送受波サイクルにありでは
n個の選択振動子#1〜#n全体を駆動して送波を行わ
せ、受波に際しては振動子#2〜#(n+1+β)(但
し、第1の送受波サイクルにあってα=+1の場合はβ
=+1とし、第1の送受波サイクルにあってα=−1の
場合はβ=−1とする)を選択して受波を行わせる振動
素子選択手段を設けた超音波診断装置によって解決され
る。
[Means for solving the problem] The above purpose is to provide a probe having a plurality of (m) transducers;
n vibrators (where n<m) #1 to #n are sequentially selected while shifting each vibrating element, and the first... A second wave transmission/reception cycle is set, and in the first wave transmission/reception cycle, n selected oscillators #1 to
#n is driven as a whole to transmit waves, and when receiving waves, select transducers #1 to #(n+α) (however, α = +1 or -1) to perform wave reception, and the second transmitting/receiving In the wave cycle, all n selected oscillators #1 to #n are driven to perform wave transmission, and when receiving waves, oscillators #2 to #(n+1+β) (however, in the first wave transmission/reception cycle If α=+1, then β
= +1, and if α = -1 in the first wave transmission/reception cycle, β = -1) to perform wave reception. Ru.

[作用コ 振動素子#1〜#nを選択したとき、第1の送受信サイ
クルでは#1〜#nのn個で送波し、#1〜#(n−1
)で受信する。このとき送波の指向送波と受波の指向性
は−ピッチずれる。送受信のn−1 総合指向特性は−と□との中間にある。すなわち<n 
 1ピツチ)上に送受信の総合指向特性がくる。
[When the active vibration elements #1 to #n are selected, in the first transmission/reception cycle, waves are transmitted by n pieces #1 to #n, and #1 to #(n-1
). At this time, the directivity of the transmitted wave and the directivity of the received wave are shifted by -pitch. The n-1 overall directional characteristics of transmission and reception are between - and □. That is, <n
1 pitch) is the overall directional characteristic of transmitting and receiving.

次に第2の送受信サイクルでは、第1の送受信サイクル
と同じく、#1〜#nのn個で送波し、#2〜#nで受
信する。このときの送波の指向性したがって、第1の送
受信サイクルと第2の送受信サイクルとの間で総合指向
特性は1/2ピツチずれたことになる。そして振動素子
を順次1個ずらして走査すると、1/2ピツチずつの走
査が行なわれる。そして、各送受信サイクルでの送波と
受波の振動素子数は送波がn個、受波が(n −1)個
との関係が保たれるため、各送受信サイクルでの感度差
は均一となる。
Next, in the second transmission/reception cycle, as in the first transmission/reception cycle, waves are transmitted by n waves #1 to #n and received by waves #2 to #n. The directivity of the transmitted wave at this time Therefore, the overall directivity characteristic is shifted by 1/2 pitch between the first transmission/reception cycle and the second transmission/reception cycle. When the vibrating elements are sequentially shifted one by one and scanned, scanning is performed in 1/2 pitch increments. The number of vibrating elements for transmitting and receiving waves in each transmitting/receiving cycle is maintained at n for transmitting and (n - 1) for receiving, so the sensitivity difference in each transmitting and receiving cycle is uniform. becomes.

[実施例] 第1図は本発明の原理説明をする図であって、第2図と
同一符号を付しであるものは同一のものを示しその説明
は省略する。すなわち、第1回目の超音波の送受波サイ
クルにおいては、振動素子1.2,3.・・・、nで送
波し、振動素子1,2゜3、・・・、n−1で受波する
。第2回目の送受波サイクルにおいては、第1回目と同
様に振動素子1゜2.3.・・・、nで送波し、振動素
子2,3.・・・。
[Example] Fig. 1 is a diagram for explaining the principle of the present invention, and the same reference numerals as in Fig. 2 indicate the same parts, and the explanation thereof will be omitted. That is, in the first ultrasonic wave transmission/reception cycle, the vibration elements 1.2, 3. . . , n is transmitted, and the wave is received by the vibrating elements 1, 2° 3, . . . , n-1. In the second wave transmission/reception cycle, the vibration element 1° 2.3. ..., n, and vibrating elements 2, 3 . ....

nで受波する。以下、振動素子を1個ずらして、同じく
n個の振動素子2,3.・・・、n+1で第1゜第2の
送受波サイクルの動作を実行する。即ち、第1サイクル
では振動素子2,3.・・・、n+1で送波し、振動素
子2,3.・・・、nで受波し、第2サイクルでは振動
素子2,3.・・・、n+1で送波し、振動素子3,4
.・・・、n+1で受波する。例えば、振動素子n=1
0とすると、常に送波は10個、受波は9個の振動素子
を使用することになり、そのときの走査ピッチは1/2
となる。これをもう少し具体的に説明すると第2表に示
す如くである。
Receive at n. Hereinafter, by shifting the vibrating element by one, the same number of n vibrating elements 2, 3, . ..., the operation of the 1st and 2nd wave transmission/reception cycles is executed at n+1. That is, in the first cycle, the vibration elements 2, 3 . . . , transmits waves with n+1, and vibrates the vibration elements 2, 3 . ..., n, and in the second cycle, the vibration elements 2, 3, . ..., wave is transmitted by n+1, and vibration elements 3 and 4
.. ..., the wave is received at n+1. For example, vibration element n=1
If it is set to 0, 10 vibrating elements are always used for transmitting waves and 9 vibrating elements for receiving waves, and the scanning pitch at that time is 1/2.
becomes. This will be explained in more detail as shown in Table 2.

第  2  表 尚、振動素子の番号は、素子番号で示したが、絶えず、
n個の素子を選んでいく故に、そのn個の素子を#1.
#2.・・・、#nとの相対番号で示してもよい。
In Table 2, the numbers of the vibrating elements are shown as element numbers, but
Since n elements are selected, the n elements are #1.
#2. ..., may be indicated by a relative number with #n.

また、第3図は上述の原理に基づいて送受波時の指向特
性を示したもので、同図からもわかるように、送波時の
振動子数をn、受波時の振動子数をn−1とすると、振
動子数が充分に大きいとき(探触子口径が大きいとき)
は、総合の指向性は、送波時の指向特性Xと受波時の指
向特性Yとの中心である総合指向特性Zとなる。ここで
、総合指向特性Zとは、Z=XXYである。第3図では
In addition, Figure 3 shows the directivity characteristics during wave transmission and reception based on the above-mentioned principle.As can be seen from the figure, the number of oscillators during wave transmission is n, and the number of oscillators during wave reception is If n-1, when the number of transducers is sufficiently large (when the probe diameter is large)
The overall directivity is the overall directivity Z, which is the center of the directivity X during transmission and the directivity Y during reception. Here, the overall directional characteristic Z is Z=XXY. In Figure 3.

総合指向特性Zの出現場所は示しであるが具体的形態は
省略し七なる。z=xxyより当然に予想可能だからで
ある。
The location where the general directional characteristic Z appears is shown, but the specific form is omitted. This is because it is naturally predictable from z=xxy.

そこで、本実施例のように、n個の振動素子#1.82
.・・・、#nを順次選択し、且つ各n個の振動素子に
対して第1.第2の送受波サイクルを採用することによ
り、総合指向特性Zは、1/2ピツチずつ平行移動する
。この1/2ピツチずっの平行移動とは、走査線が17
2ピツチずつ設定できることを意味し、1ピツチの走査
線に比べて高精細な像が得られたことになる。更に、各
送受波は、必ずn個と(n−1)個との振動素子からの
ものとなり、各送受信による素子数の変動が全くなく、
感度差はなくなる。
Therefore, as in this embodiment, n vibration elements #1.82
.. . . , #n are sequentially selected, and the first . By employing the second wave transmission/reception cycle, the overall directional characteristic Z is translated by 1/2 pitch. This parallel movement of 1/2 pitch means that the scanning line is 17
This means that the scanning line can be set in 2-pitch increments, which means that a higher-definition image can be obtained than with a 1-pitch scanning line. Furthermore, each transmission and reception is always from n and (n-1) vibrating elements, and there is no change in the number of elements due to each transmission and reception.
There will be no difference in sensitivity.

次に上述の超音波走査方法に基づく具体的な回路を第4
図に示し説明する。
Next, a specific circuit based on the above-mentioned ultrasonic scanning method will be described in the fourth section.
It is shown and explained in the figure.

第4図において11は多数個の振動素子(1,2゜〜I
n?・・・、m)を有して成る探触子、12はタイミン
グクロック信号発生器、13は高圧パルス発生器、14
はマルチプレクサ切替制御回路、15はそのマルチプレ
クサで超音波の送、受波系を切替えるためのものである
。16はマルチプレクサ15によって受信側に切替えら
れたとき反射超音波を受波する受波回路、17は受波回
路16の出力部に設けた受波出力増幅器、18は受波出
力を表示する表示器(CRT)を示し、19はその表示
器18のX軸偏向回路、20はY軸偏向回路である。
In Fig. 4, 11 is a large number of vibration elements (1,2°~I
n? ..., m); 12 is a timing clock signal generator; 13 is a high-voltage pulse generator; 14;
1 is a multiplexer switching control circuit, and 15 is a multiplexer for switching between ultrasonic transmission and reception systems. 16 is a receiving circuit that receives reflected ultrasound when switched to the receiving side by the multiplexer 15, 17 is a receiving output amplifier provided at the output section of the receiving circuit 16, and 18 is a display that displays the receiving output. (CRT), 19 is an X-axis deflection circuit of the display 18, and 20 is a Y-axis deflection circuit.

第4図に示す回路の各部め入出力波形は第5図に示す如
くであるが、同波形図と共に第4図の動作を説明する。
The input/output waveforms of each part of the circuit shown in FIG. 4 are as shown in FIG. 5, and the operation of FIG. 4 will be explained with reference to the waveform diagram.

タイミングクロック信号発生D 12よりのクロック信
号aの入力により高圧パルス発生器13からはパルス波
すが出方されるが、その出力パルス波すはそのとき制御
回路14がらの[I]」レベル信号Cによりマルチプレ
クサ15を介して探触子11の各振動素子(1,2,・
・・、n)に入力される。これによって超音波が発射さ
れ、被検体より反射波が得られるが、波形すで示す超音
波送信が終了した直後(P点)にマルチプレクサ15を
制御信号Cにより制御し、1〜n−1個の各振動素子が
受けた反射波dだけを受信回路16に入力する。
A pulse wave is output from the high-voltage pulse generator 13 in response to the input of the clock signal a from the timing clock signal generator D 12, and the output pulse wave is then an [I] level signal from the control circuit 14. C, each vibrating element (1, 2, . . .
..., n). As a result, ultrasonic waves are emitted and reflected waves are obtained from the subject. Immediately after the ultrasonic wave transmission shown in the waveform is completed (point P), the multiplexer 15 is controlled by the control signal C, and the multiplexer 15 is controlled by the control signal C. Only the reflected wave d received by each vibrating element is input to the receiving circuit 16.

そして、増幅器17を介して、X、Y軸偏向回路19゜
20により偏向しである表示器18に超音波画像を表示
する。
Then, the ultrasonic image is displayed on the display 18 via the amplifier 17 and deflected by the X and Y axis deflection circuits 19 and 20.

そしてまた、次、のクロック信号入力により高圧パルス
が発生する直前において、制御回路14はマルチプレク
サ15を制御して1〜n個の振動素子にだけ高圧パルス
を印加する。以下同様に制御回路I4の制御によりマル
チプレクサ15を切替え、2〜n個の各振動素子が受け
た反射波dだけを受信回路16に入力し、表示器18に
表示する。このようにして、振動素子からの超音波送信
時と被検体からの超音波受信時の使用振動子数を変え、
走査ピッチを1/2とし指向性を超音波送受信を総合し
たものとしたものであるから、超音波ビームの密度は向
上し、かつ相隣り合う超音波ビームの感度差はなくなる
Immediately before a high voltage pulse is generated by the next clock signal input, the control circuit 14 controls the multiplexer 15 to apply the high voltage pulse only to 1 to n vibration elements. Thereafter, the multiplexer 15 is similarly switched under the control of the control circuit I4, and only the reflected waves d received by each of the 2 to n vibration elements are input to the receiving circuit 16 and displayed on the display 18. In this way, the number of transducers used when transmitting ultrasonic waves from the transducer element and when receiving ultrasonic waves from the subject is changed,
Since the scanning pitch is 1/2 and the directivity is a combination of ultrasonic transmission and reception, the density of the ultrasonic beam is improved and there is no difference in sensitivity between adjacent ultrasonic beams.

なお、上述の実施例においては、受波時に使用する振動
素子数を、送波時に使用する振動素子数より1個少なく
する場合について述べたが、これに限らす受波時に使用
する振動素子数の方を多くしても同様の作用、効果が得
られる。即ち、1個多い受波振動素子の選択によっても
実現可能である。−膜化すれば、送波振動子を#1.#
2.・・・。
In addition, in the above-mentioned embodiment, a case was described in which the number of vibrating elements used during wave reception is one less than the number of vibrating elements used during wave transmission, but the number of vibrating elements used during wave reception is limited to this. The same action and effect can be obtained even if the amount is increased. That is, it can also be realized by selecting one more receiving vibration element. - If it is made into a film, the transmitting oscillator #1. #
2. ....

#nとした場合、第1送受波サイクルにあっては$1.
#2.・・・、# (n+α) (但し、α=+1又は
α=−1)による受渡となり、第2送受波サイクルにあ
っては#2.#3.・・・、 11 (n+1+β)(
但し、第1送受波サイクルにあってα=+1の場合はβ
=+1、第1送受波サイクルにあってα=−1の場合は
β=−1とする)となる。この結果α=+1.又はα=
−1のいずれであろうと、1/2ピツチ走査となり、か
つα=−1では必ず(n−1)個の受波素子、α=+1
の場合は必ず(n+1)個の受波素子となる。
#n, $1.00 in the first wave transmission/reception cycle.
#2. ..., #(n+α) (however, α=+1 or α=-1), and in the second transmission/reception cycle, #2. #3. ..., 11 (n+1+β)(
However, if α=+1 in the first transmission/reception cycle, β
=+1, and when α=-1 in the first wave transmission/reception cycle, β=-1). This result α=+1. or α=
-1, it is 1/2 pitch scanning, and when α=-1, there are always (n-1) receiving elements, α=+1
In this case, there are always (n+1) receiving elements.

[発明の効果] 以上の説明からも明らかなように本発明によれば、1/
2ピツチ走査での高精細化及び相隣り合う超音波ビーム
の感度差の均一化を達成でき、均質な超音波画像が得ら
れると共に、超音波ビームの密度の向上が図れるという
効果がある。
[Effect of the invention] As is clear from the above explanation, according to the present invention, 1/
It is possible to achieve high definition in two-pitch scanning and to equalize the difference in sensitivity between adjacent ultrasound beams, resulting in the effect that a homogeneous ultrasound image can be obtained and the density of ultrasound beams can be improved.

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

第1図は本発明による超音波走査方式を説明するための
原理図、第2図は従来例による超音波走査方式を説明す
るための原理図、第3図は第2図の走査方式による超音
波指向特性図、第4図は本発明の一実施例を示す回路構
成図、第5図は第4図の動作説明をする入出力波形図で
ある。 11・・・超音波振動素子、15・・・マルチプレクサ
。 第1図 イ  ロ 第2図 第4図
FIG. 1 is a principle diagram for explaining the ultrasonic scanning method according to the present invention, FIG. 2 is a principle diagram for explaining the conventional ultrasound scanning method, and FIG. 4 is a circuit configuration diagram showing an embodiment of the present invention, and FIG. 5 is an input/output waveform diagram illustrating the operation of FIG. 4. 11... Ultrasonic vibration element, 15... Multiplexer. Figure 1 A Figure 2 Figure 4

Claims (1)

【特許請求の範囲】[Claims] 1、複数(m個)の振動子を有する探触子と、n個の振
動子(但し、n<m)#1〜#nを、振動素子1個毎に
ずらしながら順次選択し、各選択したn個の振動子に対
して第1、第2の送受波サイクルを設定し、第1の送受
波サイクルにあってはn個の選択振動子#1〜#n全体
を駆動して送波を行わせ、受波に際しては振動子#1〜
#(n+α)(但し、α=+1又は−1)を選択して受
波を行わせ、第2の送受波サイクルにあってはn個の選
択振動子#1〜#n全体を駆動して送波を行わせ、受波
に際しては振動子#2〜#(n+1+β)(但し、第1
の送受波サイクルにあってα=+1の場合はβ=+1と
し、第1の送受波サイクルにあってα=−1の場合はβ
=−1とする)を選択して受波を行わせる振動素子選択
手段とを備えたことを特徴とする超音波診断装置。
1. Sequentially select a probe having multiple (m) transducers and n transducers (where n<m) #1 to #n while shifting each transducer, and select each The first and second wave transmission/reception cycles are set for the n number of selected oscillators, and in the first wave transmission/reception cycle, all of the n selected oscillators #1 to #n are driven to transmit waves. When receiving waves, vibrator #1 ~
#(n+α) (however, α=+1 or -1) is selected to perform wave reception, and in the second wave transmission/reception cycle, all of the n selected oscillators #1 to #n are driven. When transmitting waves, when receiving waves, oscillators #2 to #(n+1+β) (however, the first
If α=+1 in the first transmission/reception cycle, β=+1, and β if α=−1 in the first transmission/reception cycle.
1. An ultrasonic diagnostic apparatus comprising: a transducer selection means for selecting a transducer (=-1) to perform wave reception.
JP63232574A 1988-09-19 1988-09-19 Ultrasonic diagnostic apparatus Granted JPH01104251A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63232574A JPH01104251A (en) 1988-09-19 1988-09-19 Ultrasonic diagnostic apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63232574A JPH01104251A (en) 1988-09-19 1988-09-19 Ultrasonic diagnostic apparatus

Publications (2)

Publication Number Publication Date
JPH01104251A true JPH01104251A (en) 1989-04-21
JPH026533B2 JPH026533B2 (en) 1990-02-09

Family

ID=16941479

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63232574A Granted JPH01104251A (en) 1988-09-19 1988-09-19 Ultrasonic diagnostic apparatus

Country Status (1)

Country Link
JP (1) JPH01104251A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5332987A (en) * 1976-09-08 1978-03-28 Hitachi Medical Corp Method of controlling ultrasonic vibrator
JPS5552746A (en) * 1978-10-16 1980-04-17 Aloka Co Ltd Electronic scanning signal processor in ultrasoniccwave disgnosis device

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5332987A (en) * 1976-09-08 1978-03-28 Hitachi Medical Corp Method of controlling ultrasonic vibrator
JPS5552746A (en) * 1978-10-16 1980-04-17 Aloka Co Ltd Electronic scanning signal processor in ultrasoniccwave disgnosis device

Also Published As

Publication number Publication date
JPH026533B2 (en) 1990-02-09

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