JPS58166278A - Separating method of time series signal - Google Patents
Separating method of time series signalInfo
- Publication number
- JPS58166278A JPS58166278A JP57047463A JP4746382A JPS58166278A JP S58166278 A JPS58166278 A JP S58166278A JP 57047463 A JP57047463 A JP 57047463A JP 4746382 A JP4746382 A JP 4746382A JP S58166278 A JPS58166278 A JP S58166278A
- Authority
- JP
- Japan
- Prior art keywords
- signal
- pulse
- reflected
- received
- response
- 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.)
- Pending
Links
- 238000000034 method Methods 0.000 title claims abstract description 14
- 238000000926 separation method Methods 0.000 claims description 3
- 230000035945 sensitivity Effects 0.000 abstract description 3
- 238000010586 diagram Methods 0.000 description 3
- 238000001028 reflection method Methods 0.000 description 3
- 230000003111 delayed effect Effects 0.000 description 2
- 239000000470 constituent Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 239000011159 matrix material Substances 0.000 description 1
- 230000002269 spontaneous effect Effects 0.000 description 1
- 238000003325 tomography Methods 0.000 description 1
- 230000017105 transposition Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO 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
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/02—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
- G01S7/28—Details of pulse systems
- G01S7/285—Receivers
Landscapes
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Ultra Sonic Daignosis Equipment (AREA)
- Radar Systems Or Details Thereof (AREA)
- Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
Abstract
Description
【発明の詳細な説明】
この発明はパルス反射法を用いた超音波断層写真装置等
における距離分解能改善方法に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for improving distance resolution in an ultrasonic tomography apparatus using a pulse reflection method.
この方法として送受波器のQを極力小さくLqiい音響
パルスを発生する方法か−・般に用いらhている5、こ
のようなQを小さくする方法は、送受波器の非放射面に
吸収体を設けて実現さrIる1、シ、かじ、この方法で
Qを小さくすると確かに匂い音響パルスを発生できるが
、その反面送受波器の感電は低下する。One method for this is to minimize the Q of the transducer and generate a high Lqi acoustic pulse.This method is commonly used5. If Q is reduced using this method, it is certainly possible to generate odor acoustic pulses, but on the other hand, the electric shock of the transducer is reduced.
この発明は比較的Qが大きく尚感変な送受波器を用いた
パルス反射法で、複数の反射波が重なり合った場合の距
離分解能改善方法として、受波信号をコンボリューショ
ン演算で処理し各反射波を分離する方法により、所期の
目的を達し得るようにしたものである。This invention is a pulse reflection method using a transducer with a comparatively large Q and a relatively strange shape.As a method for improving distance resolution when multiple reflected waves overlap, the received signal is processed by convolution calculation, and each reflected wave is This method achieves the desired purpose by separating the waves.
以下、この発明におけるQの大きい送受波器を用いた時
に生ずる反射波の重なりを分離する処理系の設計方法に
ついて述べる。Hereinafter, a method of designing a processing system for separating overlapping reflected waves that occurs when a transducer with a large Q according to the present invention is used will be described.
第1図にパルス反射法を用いた基本システムを示す。第
1図に示す様に、入力信号をf、受波信号をy1音響系
のインパルス応答をhとする。また処理系、つまりコン
ボルバのインパルス応答をgとし最終的に得られる信号
をdとする。・つまり、信号発生器1でパルス波の入力
信号fを発生して送波器4に4え、反射体6、例えば樹
木の年輪2人体の構成層などエリ音響系のインパルス応
答りを得て、これを受波器5より受波信号yとしてコン
ボルバ2に与え、これとコンボルバのインパルス応答g
とをたたみ込み演算処理して得た結果信号dを表示器3
に与えて表示像を得る・1イイ1′f彼1析層写真装置
とした構成例の場合を示すものである。Figure 1 shows a basic system using the pulse reflection method. As shown in FIG. 1, the input signal is f, the received signal is y1, and the impulse response of the acoustic system is h. Further, let g be the impulse response of the processing system, that is, the convolver, and let d be the signal finally obtained.・In other words, the signal generator 1 generates a pulse wave input signal f, sends it to the transmitter 4, and obtains the impulse response of the acoustic system of the reflector 6, such as the growth rings of a tree, the constituent layers of the human body, etc. , this is given to the convolver 2 as a received signal y from the receiver 5, and this and the impulse response g of the convolver are
The result signal d obtained by convolving and processing is displayed on the display 3.
This figure shows an example of a configuration in which a display image is obtained by applying 1'f to 1' to obtain a display image.
この場合dは次式で与えられる。J
d=f*h*g=FHg ・・・・・・・・・・
・・・・・・・(1)ただし、*はたたみ込みを示し、
FとHはその演算を行う行列であり次式となる
ここで反射波が1個の場合で距離分解能を改善し得る希
望波形としてKを仮定し、dとKの2乗誤差をδとする
と、δは次式で与えられる。In this case, d is given by the following equation. J d=f*h*g=FHg ・・・・・・・・・・・・
・・・・・・・・・(1) However, * indicates convolution,
F and H are the matrices that perform the calculation, and are given by the following equation.Here, assuming that K is the desired waveform that can improve the distance resolution when there is only one reflected wave, and the squared error of d and K is δ, then , δ is given by the following equation.
δ=(d−K) (d−K)t
=gtHtFtFHg−2gtHtF’に+KtK
・・・・・・(2)ただし、右肩のtは行列等の転置を
示す1、以上より式(2)のδを特徴とする請求め複数
の反射波が重なった受波信号とgをたたみ込み各反射波
を分離することにより距離分解能を改善できる。またg
は次式で求められる。δ=(d-K) (d-K)t =gtHtFtFHg-2gtHtF'+KtK
......(2) However, t on the right shoulder is 1 indicating the transposition of a matrix, etc. From the above, δ in equation (2) is a received signal in which multiple reflected waves overlap, and g Distance resolution can be improved by convolving and separating each reflected wave. Also g
is calculated using the following formula.
HtFtFHg=HtFtK ・・・・・・
・・・・・・・・・・・(3)このように、入力信号f
および音響系のインパルス応答りを求め、また希望波形
Kを仮定することにより式(3)から処理系gを容易に
設計できる。HtFtFHg=HtFtK ・・・・・・
・・・・・・・・・・・・(3) In this way, the input signal f
By determining the impulse response of the acoustic system and assuming the desired waveform K, the processing system g can be easily designed from equation (3).
また、この種の処理系はBBD等の遅延素子を用いたF
IRフィルタで容易に実現できる。In addition, this type of processing system uses a delay element such as a BBD.
This can be easily achieved with an IR filter.
計算は、正弦波を3波長ゲートした信号をfとし、送受
波器のQを10として行ない、またgの段数を64とし
、正弦波を1波長ゲートした信号をKとした。The calculation was carried out by setting f to be a signal obtained by gated a sine wave with three wavelengths, setting Q of the transducer to 10, setting the number of stages of g to 64, and setting K to a signal obtained by gated a sine wave by one wavelength.
まず希望波形Kが音響系の伝搬時興経過後さらにNサン
プル時間遅れた時の最小2乗誤差δを求めた。この結果
を第2図に示す。この図からδはNの増加に伴い減少し
Nが56の時最小となることがわかる。またこの時のg
を第3図に示す。First, the minimum square error δ was calculated when the desired waveform K is further delayed by N sample time after the propagation of the acoustic system. The results are shown in FIG. From this figure, it can be seen that δ decreases as N increases and becomes minimum when N is 56. G at this time again
is shown in Figure 3.
次に4個の反射波が重なり合った受波信号の分離につい
て検討する。ます受波信号として、各反射波の振幅比が
l: o、s : 0.7 : t で、各反射波の間
隔が50 、20 、30の波形を仮定し、この時の波
形を第4図に示す。Next, we will consider separating a received signal in which four reflected waves overlap. Assume that the received signal has a waveform in which the amplitude ratio of each reflected wave is l: o, s: 0.7: t, and the intervals between each reflected wave are 50, 20, and 30, and the waveform at this time is As shown in the figure.
一般に反射波の間隔が短いと第4図に示す様な重なりが
生じその結果得られる反射像の距離分解能は低下する。Generally, when the interval between reflected waves is short, overlapping occurs as shown in FIG. 4, and as a result, the distance resolution of the resulting reflected image is reduced.
また第4図の信号と第3図のgとをたたみ込んだ結果を
第5図に示す。この結果から、4個の反射波が分離し、
その振幅比も保存されていることがわかる。ただ先に説
明した様に、分離した各反射波は56サンプル時間だけ
遅れて現われる。Further, FIG. 5 shows the result of convolving the signal in FIG. 4 with g in FIG. 3. From this result, four reflected waves are separated,
It can be seen that the amplitude ratio is also preserved. However, as previously explained, each separate reflected wave appears delayed by 56 sample times.
この発明によれば、以上のように、比較的Qが大きく高
い送受波感度を持つ送受波器を用いた場合でも、受波信
号に適宜な数列gをたたみ込ませることにエリ重なった
複数の反射波を分離することができ、距離分解能を改善
できる、2この方法は、反射波が弱く高感度の送受波器
を必要とする場合や反射波の間隔が短い場合の距離分解
能改善方法として有効である、。According to the present invention, as described above, even when using a transducer with a relatively large Q and high transmitting/receiving sensitivity, multiple The reflected waves can be separated and the distance resolution can be improved.2 This method is effective as a distance resolution improvement method when the reflected waves are weak and a highly sensitive transducer is required or when the intervals between the reflected waves are short. It is.
図面は実施例を示し、第1図は紹音波断層写^、装置の
場合の要部構成略図、第2図は・イ延i+Ii1.2東
誤差の線図、第3図〜第5図は信号波形であり、第3図
はコンボルバの応答g1第4図は受波信号h1第5図は
処理された結果信号dの波形を示す。
1・・・信号発生器、2・・・コンボルバ、3・・・表
示器、4・・・送波器、5・・・受波器、6・・・反射
体。
特許出願人
ヤ 2記
半30
IME
第4口
木5k
IME
手続補正書(自発)
昭和57年9月3を日
特許庁長官 殿
1、 事件の表示
特願昭57−47465
2、発明の名称
時系列信号の分離方法
3、補正をする者
事件との関係 特許出願人
マ141 東京部品用区上太崎2−10−45明細書
・図面
5、補正の内容
明細書・図面の浄書
(内容に変更なし)The drawings show examples, and Fig. 1 is a sonic tomography^, a schematic diagram of the main part configuration of the device, Fig. 2 is a line diagram of ・Ien i + Ii 1.2 east error, and Figs. 3 to 5 are diagrams. FIG. 3 shows the response g of the convolver, FIG. 4 shows the received signal h, and FIG. 5 shows the waveform of the processed signal d. DESCRIPTION OF SYMBOLS 1... Signal generator, 2... Convolver, 3... Display device, 4... Wave transmitter, 5... Wave receiver, 6... Reflector. Patent applicant Ya 2 and a half 30 IME 4th opening 5k IME Procedural amendment (spontaneous) September 3, 1980 Director General of the Japan Patent Office 1. Indication of case Patent application 1984-47465 2. Title of the invention Separation method of series signals 3, relationship with the case of the person making the amendment Patent applicant Ma141 2-10-45 Kamitasaki, Tokyo Parts Industry Specification/Drawing 5, Contents of amendment No change)
Claims (1)
として、受波信号をコンポリューンヨン演算で処理し各
反射波を分離する時系列信けの分離方法。As a method for improving separation resolution when multiple reflected waves overlap, a time-series signal separation method that processes the received signal using a convolution calculation and separates each reflected wave.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57047463A JPS58166278A (en) | 1982-03-26 | 1982-03-26 | Separating method of time series signal |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57047463A JPS58166278A (en) | 1982-03-26 | 1982-03-26 | Separating method of time series signal |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS58166278A true JPS58166278A (en) | 1983-10-01 |
Family
ID=12775842
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57047463A Pending JPS58166278A (en) | 1982-03-26 | 1982-03-26 | Separating method of time series signal |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58166278A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008524623A (en) * | 2004-12-21 | 2008-07-10 | ウニヴェルシテテート・イ・オスロ | Channel impulse response estimation method |
-
1982
- 1982-03-26 JP JP57047463A patent/JPS58166278A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008524623A (en) * | 2004-12-21 | 2008-07-10 | ウニヴェルシテテート・イ・オスロ | Channel impulse response estimation method |
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