JPS642905B2 - - Google Patents
Info
- Publication number
- JPS642905B2 JPS642905B2 JP7923983A JP7923983A JPS642905B2 JP S642905 B2 JPS642905 B2 JP S642905B2 JP 7923983 A JP7923983 A JP 7923983A JP 7923983 A JP7923983 A JP 7923983A JP S642905 B2 JPS642905 B2 JP S642905B2
- Authority
- JP
- Japan
- Prior art keywords
- pulse
- output
- circuit
- time
- clock
- 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
- 230000000630 rising effect Effects 0.000 claims description 5
- 230000005540 biological transmission Effects 0.000 claims description 4
- 238000004364 calculation method Methods 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000005259 measurement Methods 0.000 description 2
- 238000002604 ultrasonography Methods 0.000 description 2
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G04—HOROLOGY
- G04F—TIME-INTERVAL MEASURING
- G04F10/00—Apparatus for measuring unknown time intervals by electric means
- G04F10/04—Apparatus for measuring unknown time intervals by electric means by counting pulses or half-cycles of an ac
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Measurement Of Unknown Time Intervals (AREA)
- Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
Description
【発明の詳細な説明】
本発明は、送波器と受波器を一定距離だけ離し
て向い合わせて配設し、送波器から送出した超音
波パルスが受波器に到達するまでの時間間隔を測
定し、その計数結果に基づいて、風速や流速など
を演算する装置に用いる超音波の伝播時間を測定
する装置に関するものである。[Detailed Description of the Invention] The present invention provides a method for arranging a transmitter and a receiver facing each other with a certain distance apart, and the time it takes for an ultrasonic pulse sent from the transmitter to reach the receiver. The present invention relates to a device that measures the propagation time of ultrasonic waves used in devices that measure intervals and calculate wind speed, flow speed, etc. based on the counting results.
ここで超音波の伝播時間は、超音波パルスを送
信してから受信するまでの時間内に含まれるクロ
ツクパルスを計数して測定するものであるが、計
数の始めと終わりの時点では、極めて短い時間内
に処理しなければならないため、高度な設計技術
が必要であり、経済的面で不利であるとともに製
造面においても甚だ厄介である。 Here, the propagation time of ultrasound is measured by counting the clock pulses included in the time from transmitting the ultrasound pulse to receiving it, but at the beginning and end of counting, the time is extremely short. This requires advanced design technology, which is not only economically disadvantageous but also extremely complicated to manufacture.
本発明はかかる点に鑑み、できるだけ簡単な時
間間隔拡大の手段を取り入れ、任意のm倍に拡大
した時間で処理するようにし、測定を確実にする
とともに、測定精度の向上を計つたものである。 In view of this point, the present invention incorporates a means for expanding the time interval as simple as possible to perform processing in a time expanded by an arbitrary m times, thereby ensuring reliable measurement and improving measurement accuracy. .
次に実施例を示す図面を基にして説明する。 Next, an explanation will be given based on drawings showing examples.
第1図は実施例のブロツク図、第2図は作動説
明図であり、第1図の中で記号を付してある各部
に対応して示してある。 FIG. 1 is a block diagram of the embodiment, and FIG. 2 is an explanatory diagram of the operation, and the parts indicated by symbols in FIG. 1 are shown corresponding to each other.
第1図において1及び2はセツト・リセツト型
フリツプフロツプ回路、3はアンドゲート回路、
4はアツプ・カウンタ、5は減算器、6はOR回
路、7は積分器、8はアナログ・デジタル変換器
である。 In FIG. 1, 1 and 2 are set-reset flip-flop circuits, 3 is an AND gate circuit,
4 is an up counter, 5 is a subtracter, 6 is an OR circuit, 7 is an integrator, and 8 is an analog-to-digital converter.
Pは送信パルスの入力端子、Rは受信パルスの
入力端子、CLKはクロツクパルスの入力端子を
示す。 P indicates a transmitting pulse input terminal, R indicates a receiving pulse input terminal, and CLK indicates a clock pulse input terminal.
端子Pに入来する送信パルスP1(第2図イ参
照)と、端子Rからの受信パルスR1(第2図ロ参
照)とが、それぞれ第1のフリツプフロツプ回路
1のセツト端子Sとリセツト端子Rに印加する
と、回路1の出力は第2図のハに示す通り、送信
パルスP1と受信パルスR1の間がONとなり、この
出力はアンドゲート回路3の一方の端子に印加す
る。 The transmitted pulse P 1 (see FIG. 2 A) entering the terminal P and the received pulse R 1 from the terminal R (see FIG. 2 B) are connected to the set terminal S and the reset terminal of the first flip-flop circuit 1, respectively. When the voltage is applied to the terminal R, the output of the circuit 1 is turned ON between the transmission pulse P 1 and the reception pulse R 1 as shown in FIG. 2C, and this output is applied to one terminal of the AND gate circuit 3.
回路3の他方の端子には、端子CLKからのク
ロツクパルスが印加しており、回路3の出力は第
2図ニに示す通りとなり、この出力がアツプ・カ
ウンタ4に印加し、カウンタ4は入来するクロツ
クパルスの数Aを数える。 A clock pulse from terminal CLK is applied to the other terminal of circuit 3, and the output of circuit 3 is as shown in FIG. Count the number A of clock pulses.
一方第2のフリツプフロツプ回路2のセツト端
子Sには、OR回路6を介して送信パルスP1と受
信パルスR1が印加し、一方リセツト端子Rには
クロツクパルスが印加しており、出力には第2図
ホに示す通り、送信パルスP1の立上り時点から
始まり、送信パルスP1に続く第1発目のクロツ
クパルスの立上り時点までのt1時間だけONとな
る出力と、受信パルスR1に就ても受信パルスR1
に続く最初のクロツクパルスの立上り時点までの
t2時間だけONの出力が得られ、これらの出力は
積分器7の入力となり、両出力は積分されたあ
と、アナログ値はアナログ・デジタル変換器8で
デジタル値に変換されて減算器5に印加する。 On the other hand, the transmitting pulse P1 and the receiving pulse R1 are applied to the set terminal S of the second flip-flop circuit 2 via the OR circuit 6, while the clock pulse is applied to the reset terminal R, and the output is the first one. As shown in Figure 2E, the output is ON for t 1 hour starting from the rising edge of the transmitting pulse P1 and ending at the rising edge of the first clock pulse following the transmitting pulse P1 , and the output is ON for the receiving pulse R1 . Even if the received pulse R 1
up to the rising edge of the first clock pulse following
t Outputs that are ON for 2 hours are obtained, and these outputs become the inputs of the integrator 7. After both outputs are integrated, the analog value is converted to a digital value by the analog-to-digital converter 8, and then sent to the subtracter 5. Apply.
こゝでアナログ・デジタル変換器8の分解能を
適宜に選んでおくと、前記第2のフリツプフロツ
プ回路2で検出された時間t1とt2の出力を積分し
てデジタル化するとき、分解能によつて決まる拡
大率例えばm倍で、すなわちt1とt2をm倍してデ
ータを処理することができる。 If the resolution of the analog-to-digital converter 8 is selected appropriately, when the outputs at times t 1 and t 2 detected by the second flip-flop circuit 2 are integrated and digitized, the resolution will be reduced. The data can be processed with a magnification factor determined by the calculation, for example, m times, that is, t 1 and t 2 are multiplied by m.
一方減算器5には、前記第1のフリツプフロツ
プ回路1の出力(第2図ハ参照)が印加されるか
ら、減算器5の出力には前記mt1時間相当のデジ
タル値Bとmt2時間相当のデジタル値Cの差B−
Cが得られる。 On the other hand, since the output of the first flip-flop circuit 1 (see FIG. 2 C) is applied to the subtracter 5, the output of the subtracter 5 is the digital value B corresponding to mt 1 hour and the digital value B corresponding to mt 2 hours. The difference between the digital values C of B-
C is obtained.
このようにして求めた計数値Aと(B−C)
を、以下の演算処理すると、送信々号から受信々
号までの正しい時間間隔を示す計算値を求めるこ
とができる。 Count values A and (B-C) obtained in this way
By performing the following arithmetic processing on , it is possible to obtain a calculated value that indicates the correct time interval from the transmitted signal to the received signal.
A/D変換器のスケールをmに設定し、Aで得
られる1カウント相当の時間間隔でフルスケール
になるようにしておくと、(B−C)で得られた
1ビツトの値は1/mの時間間隔の重みを持つた
ものとなるので、両者を同一の時間単位に変換す
るためには、Aの計数値をm倍するか、或は(B
−C)の計数値を1/mにする必要がある。つま
り(B−C)の数値がm個集まつてAの時間単位
と同一になるのである。 If the scale of the A/D converter is set to m, and the time interval corresponding to 1 count obtained in A is set to full scale, the value of 1 bit obtained in (B-C) will be 1/ Since it has a weight of time interval m, in order to convert both to the same time unit, the count value of A must be multiplied by m, or (B
- It is necessary to set the count value of C) to 1/m. In other words, when m values of (B-C) are gathered, they become the same time unit as A.
したがつて、送受信間の時間間隔tは次の数式
に示す通りとなる。すなわち
時間間隔t=〔A×m+(B−C)〕×クロツクの1波
長に相当する時間/m
又は
=〔A+1/m(B−C)〕×(クロツクの
1波長に相当する時間)
上記の演算方法については具体的に触れない
が、デジタル演算やアナログ値に変換するなど、
周知の演算方法を用いればよい。 Therefore, the time interval t between transmission and reception is as shown in the following formula. That is, time interval t = [A x m + (B-C)] x time equivalent to one wavelength of the clock/m or = [A + 1/m (B-C)] x (time equivalent to one wavelength of the clock) Although we will not discuss the calculation methods in detail, we will use digital calculations, conversion to analog values, etc.
A well-known calculation method may be used.
本発明は以上説明した通りであり、従来は上記
のAの計数値だけを求め、この計数値を送受信間
の時間間隔としていたので、クロツクパルスの1
波長以下の部分については計数できないため誤差
を避けることができなかつたのに対し、時間間隔
拡大回路を利用することによつてクロツクパルス
の1波長をはずれた部分をも測定可能とし、正確
な時間間隔を測定でき、かつ、精度を向上させる
ためにクロツクパルスの周波数を徒らに高く上げ
る必要がなくなり、カウンタも特に高級なもので
なくとも充分であるなど、製造面は勿論、経済的
にも極めて有利となつて、実用面での効果は大き
い。 The present invention is as explained above. Conventionally, only the count value of A mentioned above was obtained and this count value was used as the time interval between transmission and reception.
Errors could not be avoided because parts below the wavelength cannot be counted, but by using a time interval expansion circuit, it is now possible to measure parts that are one wavelength away from the clock pulse, allowing accurate time intervals to be measured. It is extremely advantageous not only in terms of manufacturing but also economically, as it eliminates the need to raise the clock pulse frequency unnecessarily high to improve accuracy, and the counter does not need to be particularly high-class. Therefore, the practical effect is great.
第1図は実施例のブロツク図。第2図は第1図
の作動説明図。
1,2……フリツプフロツプ回路、3……アン
ドゲート回路、4……アツプ・カウンタ、5……
減算器、6……OR回路、7……積分器、8……
アナログ・デジタル変換器。
FIG. 1 is a block diagram of an embodiment. FIG. 2 is an explanatory diagram of the operation of FIG. 1. 1, 2...Flip-flop circuit, 3...AND gate circuit, 4...Up counter, 5...
Subtractor, 6...OR circuit, 7...Integrator, 8...
Analog to digital converter.
Claims (1)
間内に含まれるクロツクパルスを計数して、超音
波の伝播時間を測定する装置において、送信パル
スと受信パルスとが印加され、送信から受信まで
ONとなる第1のフリツプフロツプ回路と、 該回路の出力及びクロツクパルスとが印加され
るゲート回路と、 該ゲート回路の出力が印加され、出力の中に含
まれるクロツクパルスの数Aを計数するアツプカ
ウンタと、 OR回路を介して送られる前記送信パルス及び
受信パルスと、前記クロツクパルスとが印加され
て、前記送信パルスと受信パルスそれぞれの立上
り時点から始まり、送信パルスと受信パルスのそ
れぞれに続いて到来する初めてのクロツクパルス
の立上り時点までの時間t1及びt2の間だけONと
なるパルスを検出する第2のフリツプフロツプ回
路と、 該回路の出力が印加される積分回路と、該積分
回路の出力を前記t1及t2のm倍の拡大率でデジタ
ル化するアナログ・デジタル変換器と、 該アナログ・デジタル変換器の出力と、前記第
1のフリツプフロツプ回路の出力とが印加され、
該アナログ・デジタル変換器の出力に検出された
mt1の時間に相当するデイジタル数値Bと、mt2
に相当するデジタル数値Cとの差を(B−C)を
算出する減算器と、 を具備しており、送受信の時間間隔tの値をt=
[A+1/m(B−C)]×(クロツクの1波長に相当 する時間)として求めるように構成したことを特
徴とする超音波の伝播時間測定装置。[Claims] 1. A device that measures the propagation time of ultrasonic waves by counting clock pulses included in the time from when the ultrasonic pulses are transmitted to when they are received. , from sending to receiving
A first flip-flop circuit that is turned ON; a gate circuit to which the output of the circuit and clock pulses are applied; and an up counter to which the output of the gate circuit is applied and counts the number A of clock pulses included in the output. , the transmitting pulse and the receiving pulse sent through the OR circuit, and the clock pulse are applied, starting from the rising edge of the transmitting pulse and the receiving pulse, respectively, and arriving after the transmitting pulse and the receiving pulse, respectively. a second flip-flop circuit that detects a pulse that is ON only during times t1 and t2 up to the rising edge of the clock pulse; an integrating circuit to which the output of the circuit is applied; an analog-to-digital converter that digitizes at a magnification of m times 1 and t2 ; the output of the analog-to-digital converter and the output of the first flip-flop circuit are applied;
detected at the output of the analog-to-digital converter.
Digital value B corresponding to the time of mt 1 and mt 2
It is equipped with a subtracter that calculates the difference between the digital numerical value C corresponding to (B-C), and the value of the time interval t between transmission and reception as t=
1. An ultrasonic propagation time measuring device characterized in that the ultrasonic propagation time is determined as [A+1/m(B-C)]×(time corresponding to one wavelength of a clock).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7923983A JPS59204788A (en) | 1983-05-09 | 1983-05-09 | Propagation time measuring apparatus for ultrasonic wave |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7923983A JPS59204788A (en) | 1983-05-09 | 1983-05-09 | Propagation time measuring apparatus for ultrasonic wave |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59204788A JPS59204788A (en) | 1984-11-20 |
JPS642905B2 true JPS642905B2 (en) | 1989-01-19 |
Family
ID=13684305
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP7923983A Granted JPS59204788A (en) | 1983-05-09 | 1983-05-09 | Propagation time measuring apparatus for ultrasonic wave |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59204788A (en) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6271888A (en) * | 1985-09-25 | 1987-04-02 | Yokogawa Electric Corp | Time width measuring instrument |
JPS62144088A (en) * | 1985-12-18 | 1987-06-27 | Yokogawa Electric Corp | Time measuring apparatus |
JPS62288597A (en) * | 1986-06-06 | 1987-12-15 | Yokogawa Electric Corp | Time measuring device |
JPS63289482A (en) * | 1987-05-21 | 1988-11-25 | Yokogawa Electric Corp | Fraction time measuring apparatus |
Family Cites Families (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS49105568A (en) * | 1973-02-08 | 1974-10-05 | ||
JPS5139159A (en) * | 1974-09-30 | 1976-04-01 | Nippon Kokan Kk | Kijuntaisekikan oshoshita ryuryokeikenteisochi |
JPS524794A (en) * | 1975-06-30 | 1977-01-14 | Taiyo Musen Kk | Time interval automatic measuring unit |
JPS52135776A (en) * | 1976-05-08 | 1977-11-14 | Takeda Riken Ind Co Ltd | Pulse width measuring device |
-
1983
- 1983-05-09 JP JP7923983A patent/JPS59204788A/en active Granted
Also Published As
Publication number | Publication date |
---|---|
JPS59204788A (en) | 1984-11-20 |
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