JPS6324896Y2 - - Google Patents
Info
- Publication number
- JPS6324896Y2 JPS6324896Y2 JP14483080U JP14483080U JPS6324896Y2 JP S6324896 Y2 JPS6324896 Y2 JP S6324896Y2 JP 14483080 U JP14483080 U JP 14483080U JP 14483080 U JP14483080 U JP 14483080U JP S6324896 Y2 JPS6324896 Y2 JP S6324896Y2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- gain
- gain control
- scanning line
- control voltage
- 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.)
- Expired
Links
- 230000005540 biological transmission Effects 0.000 claims description 5
- 238000003325 tomography Methods 0.000 claims description 5
- 238000002592 echocardiography Methods 0.000 description 8
- 238000010586 diagram Methods 0.000 description 6
- 230000001360 synchronised effect Effects 0.000 description 2
- 239000000523 sample Substances 0.000 description 1
- 229920006395 saturated elastomer Polymers 0.000 description 1
Landscapes
- Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
- Ultra Sonic Daignosis Equipment (AREA)
Description
【考案の詳細な説明】
本考案は電子走査形超音波断層装置、特にそれ
に用いられる高周波増幅器の利得制御装置に関す
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an electronic scanning ultrasonic tomography apparatus, and particularly to a gain control device for a high frequency amplifier used therein.
超音波断層装置において、生体からの反射エコ
ーのダイナミツクレンジは100dB以上と広いた
め、強力反射エコーが入力した場合、特に高周波
増幅器の飽和、バイアス点の移動などが生じ、近
傍の微弱エコーがマスクさせる欠点がある。 In ultrasonic tomography devices, the dynamic range of reflected echoes from living organisms is wide, at over 100 dB, so when strong reflected echoes are input, the high-frequency amplifier becomes saturated, the bias point moves, etc., and nearby weak echoes are masked. There are drawbacks to doing so.
そこで、従来、送波パルスに同期して、時間と
ともに利得を制御する時間利得制御(Time
Gain Control略してTGC)が実施されている。
すなわち第1図に示すように電子走査形リニアス
キヤンの場合、利得制御電圧は曲線1の如き、
TGC電圧となる。ここで、強力エコー(第1図
のPで示す部分)の存在する近傍では利得を減少
させてある。なお、第1図において、Sは体表位
置、Dは深部位置、SLは走査線を示す。 Therefore, conventionally, time gain control (Time gain control), which controls the gain over time in synchronization with the transmitted pulse, has been used.
Gain Control (abbreviated as TGC) is being implemented.
That is, as shown in FIG. 1, in the case of electronic scanning linear scan, the gain control voltage is as shown in curve 1.
Becomes TGC voltage. Here, the gain is reduced near the presence of strong echoes (the portion indicated by P in FIG. 1). In FIG. 1, S indicates a body surface position, D indicates a deep position, and SL indicates a scanning line.
しかし、配列素子の配列方向(x方向)に微細
エコー(第1図の斜線部分)が存在する場合、第
1図に示すような強力エコーのためにマスクされ
てしまう欠点がある。 However, if minute echoes (shaded areas in FIG. 1) exist in the arrangement direction (x direction) of the array elements, there is a drawback that they are masked by strong echoes as shown in FIG.
そこで本考案では、走査線方向(リニアスキヤ
ンの場合第1図のx方向、セクタスキヤンの場
合、角度方向)に走査線利得制御(Scanning
Line Gain Control)の機能を新たに追加せんと
するものである。 Therefore, in the present invention, scanning line gain control (scanning line gain control in the scanning line direction (in the case of linear scan, the x direction in Figure 1, in the case of sector scan, in the angular direction) is performed.
The aim is to add a new function (Line Gain Control).
すなわち第1図において、リニアスキヤンの走
査線幅をLとすれば距離xがx=0〜Lの範囲で
走査線利得制御(SLGC)の曲線を得て、断層像
の各点の増幅器の利得制御信号は曲線2の如き
TGCとSLGCの和または積とするのである。 That is, in Fig. 1, if the scanning line width of linear scan is L, a scanning line gain control (SLGC) curve is obtained for the distance x in the range of x = 0 to L, and the gain of the amplifier at each point of the tomographic image is calculated. The control signal is like curve 2
It is the sum or product of TGC and SLGC.
第2図は本考案の一実施例の構成を示すブロツ
ク図であり、1は高周波増幅器、2は時間利得制
御電圧発生器、3は走査線利得制御電圧発生器、
4は演算器で、和信号または積信号を得て、高周
波増幅器1の利得を制御する。5は超音波探触
子、6は高周波増幅器出力端子である。 FIG. 2 is a block diagram showing the configuration of an embodiment of the present invention, in which 1 is a high frequency amplifier, 2 is a time gain control voltage generator, 3 is a scanning line gain control voltage generator,
4 is an arithmetic unit which obtains a sum signal or a product signal and controls the gain of the high frequency amplifier 1; 5 is an ultrasonic probe, and 6 is a high frequency amplifier output terminal.
さらに第3図において、本考案を具体的なブロ
ツク図で詳細に説明する。 Further, referring to FIG. 3, the present invention will be explained in detail with a concrete block diagram.
第3図で、7は第1のクロツク信号cl1を発生
する。8は送波パルスを発生させるための分周器
(第3図の場合1/6)、9は第2のクロツク信号cl2
を発生させるための分周器(第3図の場合1/3)、
10はフレーム制御信号を発生させるための分周
器(第3図の場合、任意)、11−1および11
−2は後述の第4図の制御電圧発生回路であり、
InはTTL信号入力端子、cl1はクロツクパルス入
力端子、Outは制御電圧出力端子である。すなわ
ち、制御電圧発生回路11−1には送波信号繰り
返しパルスと同期した入力信号と、それより短い
周期のクロツク信号が供給され、また制御電圧発
生回路11−2には表示器のフレーム繰り返しパ
ルスに同期した入力信号と、表示器の複数走査線
(この場合には3走査線)の発生ごとに発せられ
るクロツク信号が供給される。12は演算器で和
または積の演算を実行する。13は出力端子であ
り、第2図の高周波増幅器1の制御電圧となる。 In FIG. 3, 7 generates the first clock signal cl1 . 8 is a frequency divider (1/6 in the case of Fig. 3) for generating the transmission pulse, and 9 is the second clock signal cl 2
A frequency divider (1/3 in the case of Figure 3) to generate
10 is a frequency divider (optional in the case of FIG. 3) for generating a frame control signal, 11-1 and 11
-2 is a control voltage generation circuit shown in FIG. 4, which will be described later;
In is a TTL signal input terminal, cl1 is a clock pulse input terminal, and Out is a control voltage output terminal. That is, the control voltage generation circuit 11-1 is supplied with an input signal synchronized with the transmission signal repetition pulse and a clock signal with a shorter cycle, and the control voltage generation circuit 11-2 is supplied with the frame repetition pulse of the display. A clock signal is provided which is synchronized to the input signal and which is generated on each occurrence of a plurality of scan lines (in this case three scan lines) of the display. 12 is an arithmetic unit that executes a sum or product operation. 13 is an output terminal, which serves as a control voltage for the high frequency amplifier 1 shown in FIG.
第3図の制御電圧発生回路11−1および11
−2について、さらに詳細に第4図を用いて説明
する。 Control voltage generation circuits 11-1 and 11 in FIG.
-2 will be explained in more detail using FIG. 4.
第4図において、20はシフトレジスタ、21
はオペアンプ、22は低域通過形フイルタ、TR
はトランジスタ、+Vは電源、R1,R2,R3は抵抗
である。シフトレジスタ20のInはTTL信号入
力端子、cl1はクロツク信号入力端子である。Out
は制御電圧の出力端子である。制御電圧発生回路
11−1の動作は、特願昭51−23541号(特開昭
52−107186)の発明と同一である。すなわち、シ
フトレジスタ20の内部では送波信号と同期して
入力された“1”の信号がクロツク入力にしたが
つて順次シフトする。(“1”のビツト以外はすべ
て“0”)したがつて、R1で示す複数の抵抗分圧
器の出力電圧に対応する電圧が順次切りかわりな
がら出力され、送波パルスに同期した曲線の制御
電圧が発生する。この曲線が深度方向の時間利得
制御(TGC)曲線となる。この曲線の設定は、
表示器の画面を観察しながら各抵抗分圧器を調整
することにより行なう。すなわち、従来のよう
に、ひとつの制御電圧発生回路しかない場合に
は、強力エコーの存在する深度で利得が低くなる
ように設定し、第1図の1のようなTGC曲線を
得るのである。一方、制御電圧発生回路11−2
も全く同様な回路構成を有しており、フレーム繰
り返しパルスに同期して“1”レベル信号がシフ
トレジスタに入力し、これがシフトレジスタ内を
シフトすることにより複数の抵抗分圧器の出力電
圧に対応する電圧が順次切りかわりながら出力さ
れ、もつて、走査線利得制御(SLGC)曲線が得
られる。2つの曲線が示す電圧の和または積が演
算器12でとられ、これにより表示利得が制御さ
れる。例えば制御電圧発生回路11−2に第1図
のSLGCのような曲線を設定し、制御電圧発生回
路11−1に第1図のTGCのうち2のような曲
線を設定すれば、第1図のPの位置の強力エコー
の表示出力を減少させながら、Pの近傍の走査線
を除く他の走査線における斜線部分の微少エコー
も表示することができる。すなわち、強力エコー
の位置の表示利得の制限を走査線方向、及び走査
線と直角方向のいずれか任意の一方、もしくは双
方で設定できるため、所望の位置の微弱エコーを
観察することができる。 In FIG. 4, 20 is a shift register, 21
is an operational amplifier, 22 is a low-pass filter, TR
is a transistor, +V is a power supply, and R 1 , R 2 , and R 3 are resistors. In of the shift register 20 is a TTL signal input terminal, and cl1 is a clock signal input terminal. Out
is the control voltage output terminal. The operation of the control voltage generating circuit 11-1 is described in Japanese Patent Application No. 51-23541.
52-107186). That is, inside the shift register 20, the "1" signal input in synchronization with the transmission signal is sequentially shifted in accordance with the clock input. (All bits are "0" except for the "1" bit) Therefore, the voltages corresponding to the output voltages of the multiple resistor voltage dividers shown by R1 are output while switching sequentially, and the curve is controlled in synchronization with the transmission pulse. Voltage is generated. This curve becomes the time gain control (TGC) curve in the depth direction. The settings for this curve are
This is done by adjusting each resistor voltage divider while observing the display screen. That is, when there is only one control voltage generating circuit as in the conventional case, the gain is set to be low at the depth where a strong echo exists, and a TGC curve like 1 in FIG. 1 is obtained. On the other hand, control voltage generation circuit 11-2
has exactly the same circuit configuration, and a “1” level signal is input to the shift register in synchronization with the frame repetition pulse, and by shifting within the shift register, it corresponds to the output voltage of multiple resistor voltage dividers. The output voltages are sequentially switched, and a scanning line gain control (SLGC) curve is obtained. The sum or product of the voltages shown by the two curves is calculated by the calculator 12, and the display gain is controlled thereby. For example, if the control voltage generation circuit 11-2 is set to a curve like SLGC in FIG. 1, and the control voltage generation circuit 11-1 is set to a curve like 2 of TGC in FIG. While reducing the display output of the strong echo at the position of P, it is also possible to display minute echoes in the shaded areas in other scanning lines other than the scanning line near P. That is, since the display gain limit for the position of a strong echo can be set in any one or both of the scanning line direction and the direction perpendicular to the scanning line, weak echoes at a desired position can be observed.
以上はリニアスキヤンについて説明したが、セ
クタスキヤンにも有効であることは明らかであ
る。 The above explanation has been about linear scan, but it is clear that sector scan is also effective.
このように本考案によれば、時間利得制御
(TGC)信号と走査線利得制御(SLGC)信号の
和または積信号を高周波増幅器の利得制御電圧と
することにより、超音波断層像の利得を2次元的
制御することが可能となり、超音波断層装置の高
性能化に寄与する所が大である。 As described above, according to the present invention, by using the sum or product signal of the time gain control (TGC) signal and the scanning line gain control (SLGC) signal as the gain control voltage of the high frequency amplifier, the gain of the ultrasonic tomographic image can be increased by 2. This makes it possible to perform dimensional control, which greatly contributes to improving the performance of ultrasonic tomography devices.
第1図は本考案の説明図、第2図は本考案の構
成を示すブロツク図、第3図は本考案の構成を示
すブロツク図、第4図は制御電圧発生回路の一例
を示す図である。
FIG. 1 is an explanatory diagram of the present invention, FIG. 2 is a block diagram showing the configuration of the present invention, FIG. 3 is a block diagram showing the configuration of the present invention, and FIG. 4 is a diagram showing an example of a control voltage generation circuit. be.
Claims (1)
信号繰り返しパルスに同期して利得制御信号を発
生する第1手段と、表示器のフレーム繰り返しパ
ルスに同期して走査線と直角方向の利得を制御す
る制御信号を発生する第2手段と具備し、上記第
1手段と第2手段のそれぞれの出力信号の和また
は積信号を受波の増幅器の利得制御信号とするこ
とを特徴とする超音波断層装置。 In an electronic scanning ultrasonic tomography apparatus, a first means for generating a gain control signal in synchronization with the repeated pulses of the transmission signal, and a first means for controlling the gain in a direction perpendicular to the scanning line in synchronization with the frame repetition pulses of the display device. An ultrasonic tomography apparatus comprising a second means for generating a control signal, the sum or product signal of the respective output signals of the first means and the second means being used as a gain control signal of a receiving amplifier. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14483080U JPS6324896Y2 (en) | 1980-10-13 | 1980-10-13 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP14483080U JPS6324896Y2 (en) | 1980-10-13 | 1980-10-13 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5768573U JPS5768573U (en) | 1982-04-24 |
| JPS6324896Y2 true JPS6324896Y2 (en) | 1988-07-07 |
Family
ID=29504514
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP14483080U Expired JPS6324896Y2 (en) | 1980-10-13 | 1980-10-13 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6324896Y2 (en) |
-
1980
- 1980-10-13 JP JP14483080U patent/JPS6324896Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5768573U (en) | 1982-04-24 |
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