JPS63209632A - Ultrasonic wave receiver - Google Patents

Ultrasonic wave receiver

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Publication number
JPS63209632A
JPS63209632A JP62043589A JP4358987A JPS63209632A JP S63209632 A JPS63209632 A JP S63209632A JP 62043589 A JP62043589 A JP 62043589A JP 4358987 A JP4358987 A JP 4358987A JP S63209632 A JPS63209632 A JP S63209632A
Authority
JP
Japan
Prior art keywords
delay line
frequency signal
delay
signal
local oscillation
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
JP62043589A
Other languages
Japanese (ja)
Other versions
JPH0321178B2 (en
Inventor
島崎 通
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.)
GE Healthcare Japan Corp
Original Assignee
Yokogawa Medical Systems 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 Yokogawa Medical Systems Ltd filed Critical Yokogawa Medical Systems Ltd
Priority to JP62043589A priority Critical patent/JPS63209632A/en
Publication of JPS63209632A publication Critical patent/JPS63209632A/en
Publication of JPH0321178B2 publication Critical patent/JPH0321178B2/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)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (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) 本発明は、複数の受波高周波信号を局部発振周波数信号
と混合して中間周波信号に周波数変換して整相加算する
超音波受信装置に関する。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) The present invention relates to an ultrasonic receiving device that mixes a plurality of received high frequency signals with a local oscillation frequency signal, converts the frequency into an intermediate frequency signal, and adds the phased signal. .

(従来の技術) 超音波診Ili装置としては断層像を得るBモード装置
が多く用いられている。この装置のスキャンの方式とし
て各種あるが、その内型子セクタ走査は電子式に走査す
る方式であって、機械的な走査がなく、走査速度を速く
することができ、機械的な摩耗がなく、機械音がしない
等の利点があって、近時良く用いられている。この電子
セクタ走査方式の一例を第3図に示す。(イ)図は送波
時、(ロ)図は受波時の状態を示す図である。図におい
て、1は撮動子エレメントで、遅延線2により各振動子
エレメント1の位相を制御して電音波ビームを矢印の方
向に放射し、又、受波に際しては(ロ)図のように各振
動子エレメント1から得られた受波信号を遅延線2を通
して遅らせ、(イ)図の放射された超音波ビームと同一
方向に位相が合うように合成するものである。尚、図中
の遅延wA2の長さは遅延時間に比例している。
(Prior Art) B-mode devices that obtain tomographic images are often used as ultrasonic diagnostic Ili devices. There are various scanning methods for this device, but the internal mold sector scanning is an electronic scanning method that does not involve mechanical scanning, can increase the scanning speed, and is free from mechanical wear. It has the advantage of not making mechanical noise, and has been widely used in recent years. An example of this electronic sector scanning method is shown in FIG. Figure (a) shows the state when transmitting waves, and figure (b) shows the state when receiving waves. In the figure, reference numeral 1 denotes a camera element, which controls the phase of each transducer element 1 using a delay line 2 to emit an electrosonic beam in the direction of the arrow. The received signals obtained from each transducer element 1 are delayed through a delay line 2 and synthesized so that they are in phase in the same direction as the emitted ultrasonic beam shown in FIG. Note that the length of the delay wA2 in the figure is proportional to the delay time.

(発明が解決しようとする問題点) ところで、遅延線を用いて複数の受渡信号を整相加算す
ることはパルス超音波法では不可欠であるが、遅延線は
本質的には低域濾波器(LPF)なので長い遅延線を用
いると受波高周波信号(RF)のロスが大きくなり、使
用できる遅延線の長さには限界がある。従って、受波^
周波信号を周波数変換して中間周波信号(IF)にして
遅延線を用いれば、ロスについては相当改善されるので
長い遅延線を用いることができる。更に、遅延時間のス
テップを高周波の場合と同じにした時は高周波の場合よ
りも正確な整相加算ができる。しかし、複数の受波高周
波信qに局部発掘周波数を掛は口してそれぞれの中間周
波信号を求めるとき、局部発振周波数信号(しF)に対
する各受波高周波信号の位相は、その到来遅延時間によ
ってまちまらなために、得られた中間周波信号を遅延線
に通しても正しい整相加算が行われない。中間周波信号
の正しい整相加算を行うためには、局部発振周波数信号
の位相を各受渡高周波信号ごとにrA整する必要がある
が、各受渡高周波信号の位相は超音波ビームの方位角に
よって変化するので、それに合わせて中間周波信号の位
相を調整することは厄介なことである。
(Problem to be Solved by the Invention) Incidentally, it is essential in the pulsed ultrasound method to perform phasing and addition of multiple delivered signals using a delay line, but the delay line is essentially a low-pass filter ( (LPF), if a long delay line is used, the loss of the received radio frequency signal (RF) will increase, and there is a limit to the length of the delay line that can be used. Therefore, the received wave ^
If a frequency signal is frequency-converted into an intermediate frequency signal (IF) and a delay line is used, the loss is considerably improved and a long delay line can be used. Furthermore, when the delay time step is the same as in the high frequency case, more accurate phasing and addition can be performed than in the high frequency case. However, when multiplying multiple received high-frequency signals q by the local excavation frequency to obtain each intermediate frequency signal, the phase of each received high-frequency signal with respect to the local oscillation frequency signal (shiF) is determined by its arrival delay time. Because of this, correct phasing and addition cannot be performed even if the obtained intermediate frequency signal is passed through a delay line. In order to perform correct phasing and addition of intermediate frequency signals, it is necessary to adjust the phase of the local oscillation frequency signal to rA for each delivered high-frequency signal, but the phase of each delivered high-frequency signal changes depending on the azimuth of the ultrasound beam. Therefore, it is troublesome to adjust the phase of the intermediate frequency signal accordingly.

本発明は上記の点に鑑みてなされたもので、その目的は
、複数の受波高周波信号を中間周波信号に変換して遅延
線で整相加算する場合、複数の受波高周波信号の各々に
対する位相の調整が容易にできる超音波受信装置を実現
することにある。
The present invention has been made in view of the above points, and an object of the present invention is to convert a plurality of received high-frequency signals into intermediate frequency signals and perform phasing and summation of the received high-frequency signals using a delay line. The object of the present invention is to realize an ultrasonic receiving device in which the phase can be easily adjusted.

(問題点を解決するための手段) 前記の問題点を解決する本発明は、複数の受波高周波信
号を局部発振周波数信号と混合して中間周波信号に変換
して遅延線で整相加算する超音波受信装置において、遅
延線の始端に局部発振周波数信号を入力する手段、複数
の受波1%周波信号のそれぞれの到来遅延時間に対応し
た遅延線上の遅延点から局部発振周波数信号をそれぞれ
取り出す手段、これらの局部発振周波数信号を用いて対
応する受波高周波信号をそれぞれ中間周波信号に周波数
変換する手段、変換された各中間周波信号を遅延線上の
各局部発振周波数信号取り出し点にそれぞれ入力する手
段、及び遅延線の終端から中間周波整相加算信号を出力
する手段を具備することを特徴とするものである。
(Means for Solving the Problem) The present invention which solves the above problem mixes a plurality of received high frequency signals with a local oscillation frequency signal, converts the signal into an intermediate frequency signal, and performs phasing and addition using a delay line. In an ultrasonic receiver, means for inputting a local oscillation frequency signal to the starting end of a delay line, and extracting each local oscillation frequency signal from a delay point on the delay line corresponding to the arrival delay time of each of the plurality of received 1% frequency signals. means for frequency converting the corresponding received high frequency signals into intermediate frequency signals using these local oscillation frequency signals; and means for inputting each converted intermediate frequency signal to each local oscillation frequency signal extraction point on the delay line. and means for outputting an intermediate frequency phasing and addition signal from the terminal end of the delay line.

(作用) 中間周波信号を整相加算するための遅延線が、局部発振
周波数信号の位相調整のための遅延線としても利用され
るので、局部発振周波数信号の位相が常に受信高周波信
号の位相に一致する。
(Function) The delay line for phasing and adding intermediate frequency signals is also used as a delay line for adjusting the phase of the local oscillation frequency signal, so the phase of the local oscillation frequency signal always matches the phase of the received high frequency signal. Match.

(実施例) 以下、図面を参照して本発明の実施例を詳細に説明する
(Example) Hereinafter, an example of the present invention will be described in detail with reference to the drawings.

第1図は本発明の一実施例のブロック図である。FIG. 1 is a block diagram of one embodiment of the present invention.

図において、RFl、RF2.RF3は被検体内から反
射された超音波を受波した各振動子エレメントからの受
波高周波信号である。受波高周波信号入内の数は実際に
は多数であるが、便宜上受波高周波信号入力が前記の3
個であるものとして説明する。3は各振動子エレメント
からの受波信号を被検体内の各方向等からの距離に応じ
て所定の遅延を与える総遅延時間がTの遅延線である。
In the figure, RF1, RF2. RF3 is a received high frequency signal from each transducer element that received the ultrasound reflected from inside the subject. The number of receiving high-frequency signal inputs is actually large, but for convenience, the receiving high-frequency signal inputs are the three mentioned above.
This will be explained assuming that there are 1. Reference numeral 3 denotes a delay line having a total delay time of T for giving a predetermined delay to the received signal from each transducer element according to the distance from each direction within the subject.

遅延線3は両端のa、e間にす、c、dのタップを有し
、各タップ間の遅延時間は次のように設定されている。
The delay line 3 has taps c and d between a and e at both ends, and the delay time between each tap is set as follows.

a−b ;r1’   b −e :rta −c :
r2/   c −e ;τ2a −d ;r3’  
 d −e ;r3ここで、τ1’+ τ2′、τ3′
は受波高周波信号RF1.RF2.EF3の到来遅延時
間に等しい遅延時間で、τ1.τ2.τ3は前記受波高
周波信号に基づく中間周波信号が遅延線3の終端eにお
いて整相加算されるに必要な遅延時間である。
a-b; r1' b-e: rta-c:
r2/c −e; τ2a −d; r3'
d −e ; r3 where τ1'+ τ2', τ3'
is the received high frequency signal RF1. RF2. With a delay time equal to the arrival delay time of EF3, τ1. τ2. τ3 is a delay time necessary for the intermediate frequency signal based on the received high frequency signal to be phased and added at the terminal end e of the delay line 3.

4は前記受波高周波信号のRFl、RF2.RF3をミ
キサ6A、6B、6Cにおいて中間周波信号に変換する
ための局部発振周波数信号を発1辰する局部周波数発振
器(LO)で、その出力の局部発振周波数信号は3co
aωLtで表わされる信号である。5は遅延線の特性イ
ンピーダンスZOに等しい抵抗値を有する抵抗で、遅延
線3の一端aに接続されている。7A、7B、7Gは局
部周波敗発振器4の出力の局部発振周波数信号を増幅す
るバッファアンプで、出力信号を帯域濾波器(BPF)
8A、8B、8Cを経て、ミキサ6A、6B、6Cに入
力する。9A、9B、9Cはミキサ6A、6B、6Gに
よって入力高周波信号がダウンコンバートされた中間周
波信号のみを通過させ。
4 are the received high frequency signals RFl, RF2 . A local frequency oscillator (LO) that generates a local oscillation frequency signal for converting RF3 into an intermediate frequency signal in mixers 6A, 6B, and 6C.The output local oscillation frequency signal is 3co
This is a signal represented by aωLt. A resistor 5 has a resistance value equal to the characteristic impedance ZO of the delay line, and is connected to one end a of the delay line 3. 7A, 7B, and 7G are buffer amplifiers that amplify the local oscillation frequency signal output from the local frequency loss oscillator 4, and the output signal is passed through a bandpass filter (BPF).
It passes through 8A, 8B, and 8C and is input to mixers 6A, 6B, and 6C. 9A, 9B, and 9C pass only intermediate frequency signals obtained by down-converting input high frequency signals by mixers 6A, 6B, and 6G.

高周波信号や局部発振周波数信号を遮断する低域浦波器
で、その出力信号は増幅器10A、10B。
This is a low frequency wave generator that blocks high frequency signals and local oscillation frequency signals, and its output signal is sent to amplifiers 10A and 10B.

10Cにおいて増幅され、遅延線3のタップb。10C and tap b of delay line 3.

C,dにそれぞれ入力されている。11は遅延線3の出
力端に接続された遅延線3の特性インピーダンスZoに
等しい抵抗値の終端抵抗である。遅延線3のI端eから
は全中間周波信号の整相加算された信号が増幅器12で
増幅されて出力される。
They are input to C and d, respectively. Reference numeral 11 denotes a terminating resistor connected to the output end of the delay line 3 and having a resistance value equal to the characteristic impedance Zo of the delay line 3. From the I terminal e of the delay line 3, a signal obtained by phasing and adding all the intermediate frequency signals is amplified by the amplifier 12 and output.

次に上記のように構成された実施例の動作を説明する。Next, the operation of the embodiment configured as described above will be explained.

受波高周波信号のRFlはミキサ6Δに入力される。一
方、局部周波数発振器4の出力の局部発振周波数信号は
抵抗5を軽で遅延線3に入力され、τl′の遅延を受け
てタップbから出力される。この出力信号をLFlとす
る。この出力信号LF1はバッファアンプ7Aで増幅さ
れ、帯域濾波器8Aを経てミキサ6Aに入力される。ミ
キサ6AはRFlとLFlとの乗算を行い、受波高周波
信号を中間周波信号に周波数変換する。前記ミキサ6△
の出力信号は、低域浦波器9Aにより上側波帯信号を除
去されて下側波帯のみの中間周波信号IF1となり、増
幅器10Aを経て、再び遅延線3のタップbに入力され
る。帯域濾波器8Aはこの中間周波信号のミキサ6Aへ
の逆流を防止している。遅延線3に入力された中間周波
信号IF1はτ1の遅延を受けて終端eに達する。
The received high frequency signal RFl is input to the mixer 6Δ. On the other hand, the local oscillation frequency signal output from the local frequency oscillator 4 is input to the delay line 3 through a resistor 5, and is output from tap b after being delayed by τl'. Let this output signal be LFl. This output signal LF1 is amplified by a buffer amplifier 7A, and is input to a mixer 6A via a bandpass filter 8A. The mixer 6A multiplies RFl and LFl to convert the received high frequency signal into an intermediate frequency signal. The mixer 6△
The output signal has the upper sideband signal removed by the low frequency waveform generator 9A to become an intermediate frequency signal IF1 of only the lower sideband, which is inputted again to the tap b of the delay line 3 via the amplifier 10A. Bandpass filter 8A prevents this intermediate frequency signal from flowing back to mixer 6A. The intermediate frequency signal IF1 input to the delay line 3 is delayed by τ1 and reaches the terminal e.

受信信号RF2.RF3が遅延$113のタップC。Received signal RF2. RF3 is tap C with a delay of $113.

タップdから出力された局部発掘周波数信号しF2.1
F3により周波数変換され、中間周波信号IF2.IF
3が遅延線3の終端eから出力される動作はRFIの場
合と同じなので説明を省略する。前記3つのそれぞれの
遅延を受けた中間周波信号は遅延a3の末端eにおいて
整相加算され増幅器12において増幅される。
The local excavation frequency signal output from tap d is F2.1
The frequency is converted by F3, and the intermediate frequency signal IF2. IF
The operation in which signal 3 is output from the terminal e of the delay line 3 is the same as in the case of RFI, so a description thereof will be omitted. The intermediate frequency signals subjected to the three respective delays are phased and summed at the terminal e of the delay a3 and amplified in the amplifier 12.

次に上記の回路の動作における整相加算の状況を計算に
より説明する。
Next, the state of phasing and addition in the operation of the above circuit will be explained by calculation.

各振動子エレメントからの周波数ω0の高周波信号をそ
れぞれ次のように表わす。
The high frequency signals of frequency ω0 from each vibrator element are expressed as follows.

RFl:A+CO3ωo  (t+τt  T)RF2
:A2cosωo  (j+τ2−T)RF3:AtC
O3ω3 (j+τ3−■)・・・(1) 8部周波数発振器4の出力信号の遅延線3のタップb、
c、dにおける信号LF1.LF2.LF3は、遅延m
3でそれぞれで1′、τ /、τ3′の遅延を受けて次
式のようになる。
RFl:A+CO3ωo (t+τt T)RF2
:A2cosωo (j+τ2−T)RF3:AtC
O3ω3 (j+τ3−■)...(1) Tap b of the delay line 3 of the output signal of the 8-part frequency oscillator 4,
Signals LF1.c, d. LF2. LF3 has a delay m
3, each receives a delay of 1', τ/, and τ3', resulting in the following equation.

LFl:acosωc、  (j−τ1′ )LF2;
BcosωL  (を−τ2′ )LF3:3cosω
L  (t−τ3′ )・・・(2) 遅延時間の関係は第1図の遅延線3の構成から明らかな
ように次式に示す通りである。
LFl: acosωc, (j−τ1′)LF2;
BcosωL (−τ2′)LF3:3cosω
L (t-τ3')...(2) As is clear from the configuration of the delay line 3 in FIG. 1, the relationship between the delay times is as shown in the following equation.

τ1+τ1′富τ2+τ2′冒τ3+τ3′−T   
             ・・・(3)ミキサ6A、
68.6Cで受波高周波信号と局部発振周波数信号の乗
算を行い、低域浦波器9A。
τ1+τ1′ Wealth τ2+τ2′ Expansion τ3+τ3′−T
...(3) Mixer 6A,
68.6C multiplies the received high frequency signal and the local oscillation frequency signal, and the low frequency wave generator 9A.

9B、9Cで下側波帯のみを取り出すと、次式のIFl
、IF2.TF3が1’?られる。
If only the lower sideband is taken out at 9B and 9C, IFl of the following formula
, IF2. TF3 is 1'? It will be done.

ミキサ6Aにおいて、(1)、(2)、(3)式%式% ))] 開襟にして lF2 − (A2 B/2 ) cos  (ω rF (t
 +τ2−下)) IF3 = (A3 B/ 2 ) CO8((t)  IF 
 (t +で3−T)) ・・・ (4) (4)式(7)rFl、[F2.HF3は更にl延線3
によってそれぞれで1.τ2.τ3の遅延を受けた後加
算されるため、出力のΣIFはΣI F= (A+ 8
/2)cos  (cc+ HF(t −T) )+ 
(A2 B/ 2 ) COS  (ωIF  (t 
−T) )+ (A3 B/2)cos  (ωIF 
 (t −T) )−(A!+△2 +A! )  (
B/2)cos(ωI+−(t −T) ) となる。このようにして1本の遅延線を局部発振周波数
信号の遅延と受波高周波信号を変換した中間周波信号の
遅延とに共用することにより、正しく整相加算された中
間周波信号を得ることができる。
In the mixer 6A, (1), (2), (3) formula% formula% ))] IF2 − (A2 B/2 ) cos (ω rF (t
+τ2-lower)) IF3 = (A3 B/2) CO8((t) IF
(3-T at t+)) ... (4) (4) Formula (7) rFl, [F2. HF3 is further l wire extension 3
1. τ2. Since they are added after receiving a delay of τ3, the output ΣIF is ΣIF=(A+8
/2) cos (cc+ HF(t −T) )+
(A2 B/2) COS (ωIF (t
-T) )+ (A3 B/2)cos (ωIF
(t −T) )−(A!+△2 +A!) (
B/2)cos(ωI+-(t-T)). In this way, by using one delay line for both the delay of the local oscillation frequency signal and the delay of the intermediate frequency signal obtained by converting the received high frequency signal, it is possible to obtain an intermediate frequency signal that is correctly phased and summed. .

この信号のタイミングチャートを第2図に示す。A timing chart of this signal is shown in FIG.

図において、第1図と同じ部分、同じ信号には同じ符号
を付しである。図中、LFOは局部周波数発振器4の出
力信号であって、遅延線3の始端aにおける遅延Oのと
きの位相をθとする。図に示すようにRFIは τs’(−T−τt )、RF2はτ2’(=T−τz
>、RF3はτs’  (−T−A3)の遅れを持った
信号として入力されている。LFl、lF2、lF3は
LFOがそれぞれ遅延線3によりτ重′、τ2′、τ3
′の遅延を受けてタップb。
In the figure, the same parts and signals as in FIG. 1 are given the same reference numerals. In the figure, LFO is the output signal of the local frequency oscillator 4, and the phase when the delay O at the starting end a of the delay line 3 is θ. As shown in the figure, RFI is τs'(-T-τt) and RF2 is τ2'(=T-τz
>, RF3 is input as a signal with a delay of τs' (-T-A3). LFl, IF2, IF3 are LFOs with τ weights′, τ2′, τ3 due to the delay line 3, respectively.
Tap b after a delay of '.

c、dから出力される信号で、図に示すように、位相点
θはそれぞれで l 、τ2′、τ3′の遅延遅延を受
けていて、RFl、RF2.RF3に対して同位相の位
置を保っている。従って、RFl、RF2.RF3とL
Fl、lF2.lF3のそれぞれの積である1、Fl、
HF2.HF3もそれぞれ元の高周波信号と同じ遅延分
を有する信号として遅延線3のタップb、c、dに入力
される。
In the signals output from ports c and d, as shown in the figure, the phase points θ are delayed by l, τ2', and τ3', respectively, and are delayed by RFl, RF2. It maintains the same phase position with respect to RF3. Therefore, RFl, RF2. RF3 and L
Fl, IF2. 1, Fl, which are the respective products of lF3,
HF2. HF3 is also input to taps b, c, and d of the delay line 3 as signals having the same delay as the original high-frequency signal.

このIFl、HF2.IF3の信号は更に遅延線3の終
fNeの方にそれぞれでl、τ2.τ3の遅延を受け、
同じ遅延時間を有する位相の合った信号として整相され
、加算されてΣrFが得られる。
This IFl, HF2. The signal of IF3 is further transmitted to the terminal fNe of delay line 3 at l, τ2 . After a delay of τ3,
The signals are phased as in-phase signals having the same delay time and added to obtain ΣrF.

この各中間周波信号は受波高周波信号と等しい遅延分の
局部発振周波数信号でそれぞれ周波数変換され再び遅延
線3のそれぞれの位置に入力されたことにより各局部発
振周波数信号LF1.LF2゜1F3に特別の処理を施
さなくても正しく整相加算されることは第2図によって
明らかである。
Each of these intermediate frequency signals is frequency-converted using a local oscillation frequency signal with a delay equal to that of the received high-frequency signal and inputted again to each position of the delay line 3, so that each local oscillation frequency signal LF1. It is clear from FIG. 2 that phasing and addition can be performed correctly without any special processing on LF2°1F3.

第4図は本発明の他の実施例のブロック図である。この
実施例は短い遅延線を各ミキサ回路毎に挿入した例であ
る。図において、第1図と同等の部分には同じ符号を付
しである。図中、13Aは遅延時間τAの遅延線、13
Bは遅延時間τBの遅延線、13Gは遅延時間τCの遅
延線で、第1図の1本の遅延線3の遅延時間と対比すれ
ば第5図の通りになっている。即ち、次式に示す通りで
ある。
FIG. 4 is a block diagram of another embodiment of the invention. This embodiment is an example in which a short delay line is inserted in each mixer circuit. In the figure, parts equivalent to those in FIG. 1 are given the same reference numerals. In the figure, 13A is a delay line with delay time τA;
B is a delay line with a delay time τB, 13G is a delay line with a delay time τC, and when compared with the delay time of one delay line 3 in FIG. 1, they are as shown in FIG. That is, as shown in the following equation.

T−τA+τB+τC τ1−で^+τB+τC A2− τB + τC τ! 寓τC τl′−〇 A2 ′ =τ^ A3 ′ コτ^ +τB 第4図の回路は、抵抗5と遅延線13Aの間に遅延時間
0の遅延線が有るものと仮定すれば、第5図の遅延線の
配置から見ても明らかなように第1図の回路と同じもの
と見做すことができるので、第1図の回路と同じ結果を
得ることは明らかである。
T-τA+τB+τC τ1- and ^+τB+τC A2- τB + τC τ! If we assume that there is a delay line with a delay time of 0 between the resistor 5 and the delay line 13A, the circuit in Figure 4 will be as shown in Figure 5. As can be seen from the arrangement of the delay lines, this circuit can be regarded as the same as the circuit shown in FIG. 1, so it is clear that the same result as the circuit shown in FIG. 1 can be obtained.

以上説明したように局部発振周波数信号をそれぞれの受
波高周波信号の有する到来遅延時間に等  □しい遅延
線の遅延点から取り出し、受波高周波信号を周波数変換
し、得た中間周波信号を各局部発振周波数信号取り出し
点に入力したので、遅延線の終端において各信号の位相
が完全に合って、特別な手段を講じることなく整相加算
されるようになった。
As explained above, the local oscillation frequency signal is extracted from the delay point of the delay line equal to the arrival delay time of each received high-frequency signal, the received high-frequency signal is frequency-converted, and the obtained intermediate frequency signal is transmitted to each local Since the signals are input to the oscillation frequency signal extraction point, the phases of each signal match perfectly at the end of the delay line, and the signals can be phased and summed without any special measures.

尚、上記実施例において中間周波信号の周波数が単一周
波数ではあるが、かなり高い周波数(10MH2程度)
なので遅延線によって、遅延Wに対応する減衰を生じ、
ミキサの出力が局部発1辰周波数信号のレベルに依存す
るような状態になる場合は、見掛上遅延量による振幅誤
差を生ずるので、ミキサに入力する局部発振周波数信号
を波形整形するか、利得補償用増幅器を中間周波信号に
周波数変換した後に挿入する等の手段を講ずれば良い。
In addition, although the frequency of the intermediate frequency signal in the above embodiment is a single frequency, it is a fairly high frequency (about 10 MH2).
Therefore, the delay line causes attenuation corresponding to the delay W,
If the output of the mixer becomes dependent on the level of the local oscillation frequency signal, an amplitude error will occur due to the apparent amount of delay. It is sufficient to take measures such as inserting a compensation amplifier after converting the frequency into an intermediate frequency signal.

(発明の効果) 以上詳細に説明したように本発明によれば、複数の受波
高周波信号を中間周波信号に変換して遅延線で整相加算
する場合に、複数の受波高周波信号とそれぞれの局部発
振周波数信号との位相の調整が容易にできて、中間周波
帯による整相加算が正確に行えるようになり、実用上の
効果は大きい。
(Effects of the Invention) As described above in detail, according to the present invention, when converting a plurality of received high-frequency signals into intermediate frequency signals and performing phasing and addition on a delay line, each of the plurality of received high-frequency signals and The phase with the local oscillation frequency signal can be easily adjusted, and phasing and addition using the intermediate frequency band can be performed accurately, which has a great practical effect.

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

第1図は本発明の一実施例のブロック図、第2図は信号
のタイミングチャート、第3図は電子セクタ走査方式の
説明図、第4図は本発明の他の実施例の図、第5図は第
1図と第4図の実施例における遅延線の対比の図である
。 1・・・撮動子エレメント 2.3.13A、138.13G・・・遅延線4・・・
10 6A、6B、6C・・・ミキサ 7A、78.7G・・・バッファアンプ8Δ、8B、8
C・・・BPF 9A、9B、9C・・・LPF
FIG. 1 is a block diagram of one embodiment of the present invention, FIG. 2 is a signal timing chart, FIG. 3 is an explanatory diagram of an electronic sector scanning system, FIG. 4 is a diagram of another embodiment of the present invention, and FIG. FIG. 5 is a diagram comparing the delay lines in the embodiments of FIGS. 1 and 4. 1... Camera element 2.3.13A, 138.13G... Delay line 4...
10 6A, 6B, 6C...Mixer 7A, 78.7G...Buffer amplifier 8Δ, 8B, 8
C...BPF 9A, 9B, 9C...LPF

Claims (1)

【特許請求の範囲】[Claims] 複数の受波高周波信号を局部発振周波数信号と混合して
中間周波信号に変換して遅延線で整相加算する超音波受
信装置において、遅延線の始端に局部発振周波数信号を
入力する手段、複数の受波高周波信号のそれぞれの到来
遅延時間に対応した遅延線上の遅延点から局部発振周波
数信号をそれぞれ取り出す手段、これらの局部発振周波
数信号を用いて対応する受波高周波信号をそれぞれ中間
周波信号に周波数変換する手段、変換された各中間周波
信号を遅延線上の各局部発振周波数信号取り出し点にそ
れぞれ入力する手段、及び遅延線の終端から中間周波整
相加算信号を出力する手段を具備することを特徴とする
超音波受信装置。
In an ultrasonic receiving device that mixes a plurality of received high frequency signals with a local oscillation frequency signal, converts the mixture into an intermediate frequency signal, and performs phasing and summation using a delay line, means for inputting a local oscillation frequency signal to a starting end of a delay line; Means for extracting local oscillation frequency signals from delay points on the delay line corresponding to arrival delay times of respective received high frequency signals, and converting corresponding received high frequency signals into intermediate frequency signals using these local oscillation frequency signals. A means for converting the frequency, a means for inputting each converted intermediate frequency signal to each local oscillation frequency signal extraction point on the delay line, and a means for outputting an intermediate frequency phasing and addition signal from the terminal end of the delay line. Features of ultrasonic receiving device.
JP62043589A 1987-02-26 1987-02-26 Ultrasonic wave receiver Granted JPS63209632A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62043589A JPS63209632A (en) 1987-02-26 1987-02-26 Ultrasonic wave receiver

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62043589A JPS63209632A (en) 1987-02-26 1987-02-26 Ultrasonic wave receiver

Publications (2)

Publication Number Publication Date
JPS63209632A true JPS63209632A (en) 1988-08-31
JPH0321178B2 JPH0321178B2 (en) 1991-03-22

Family

ID=12667976

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62043589A Granted JPS63209632A (en) 1987-02-26 1987-02-26 Ultrasonic wave receiver

Country Status (1)

Country Link
JP (1) JPS63209632A (en)

Also Published As

Publication number Publication date
JPH0321178B2 (en) 1991-03-22

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