JPH0194282A - Wave transmitting and receiving apparatus - Google Patents
Wave transmitting and receiving apparatusInfo
- Publication number
- JPH0194282A JPH0194282A JP62251554A JP25155487A JPH0194282A JP H0194282 A JPH0194282 A JP H0194282A JP 62251554 A JP62251554 A JP 62251554A JP 25155487 A JP25155487 A JP 25155487A JP H0194282 A JPH0194282 A JP H0194282A
- Authority
- JP
- Japan
- Prior art keywords
- pattern
- wave
- vibrator
- transmitting
- cylindrical
- 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
- 230000005540 biological transmission Effects 0.000 claims description 6
- 238000005259 measurement Methods 0.000 abstract description 7
- 239000012212 insulator Substances 0.000 abstract 1
- 239000002131 composite material Substances 0.000 description 10
- 238000010586 diagram Methods 0.000 description 6
- 230000004323 axial length Effects 0.000 description 5
- 230000000694 effects Effects 0.000 description 3
- 239000011810 insulating material Substances 0.000 description 3
- 239000012774 insulation material Substances 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 230000000644 propagated effect Effects 0.000 description 1
Landscapes
- Measurement Of Levels Of Liquids Or Fluent Solid Materials (AREA)
- Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)
- Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は波動送受波装置、特に受波器受信出力のサイ
ドロープ・レベルの低減化に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a wave transmitting/receiving device, and in particular to reducing the sidelobe level of the received output of a wave receiver.
[従来の技術]
従来、超音波式距離測定装置、超音波レベル計等に使用
される波動送受波装置としては第5図に示すものがある
。[Prior Art] Conventionally, there is a wave transmitting/receiving device used in ultrasonic distance measuring devices, ultrasonic level meters, etc. as shown in FIG.
第5図において1は時間軸発生機能を有し、時間計測の
基準となる基準信号を発生する駆動部、2は駆動部1で
発生した基準信号を受けて、ほぼ一定の周波数の電気振
動を発生させる発振器、3は発振器2から送られる電気
振動を超音波に変換して送信する送波用の円筒形振動子
(以下、送波用振動子という)、4aは送波用振動子3
て送信した超音波を受信する受波器の円筒形振動子(以
下、受波用振動子という)、5は送波用振動子3と受波
用振動子4aとの間に設けられた音響絶縁材、6は中心
角が直角の円錐状をした波動反射用筒である。送波用振
動子3と受波用振動子4aは第6図に示すように外径、
内径、長さp 、ρ2及び材質がそれぞれ同じ振動子が
用いられ、その中心軸が波動反射用筒6の中心軸と一致
するように波動反射用筒6に取付けられている。In Fig. 5, numeral 1 has a time axis generation function and generates a reference signal that serves as a reference for time measurement, and numeral 2 receives the reference signal generated by the drive portion 1 and generates electrical vibrations at a nearly constant frequency. 3 is a cylindrical wave transmitting oscillator (hereinafter referred to as a wave transmitting oscillator) that converts the electric vibrations sent from the oscillator 2 into ultrasonic waves and transmitting the same; 4a is a wave transmitting oscillator 3;
A cylindrical transducer (hereinafter referred to as a receiving transducer) of the receiver receives the ultrasonic waves transmitted by the receiver, and 5 is an acoustic transducer provided between the transmitting transducer 3 and the receiving transducer 4a. The insulating material 6 is a conical wave reflecting tube with a right angle center angle. As shown in FIG. 6, the transmitting transducer 3 and the receiving transducer 4a have an outer diameter of
A vibrator having the same inner diameter, length p, ρ2, and material is used, and is attached to the wave reflecting tube 6 so that its center axis coincides with the center axis of the wave reflecting tube 6.
7は送波用振動子3から放射されて波動反射用筒6の反
射面で反射して波動反射用筒6の中心軸に対して平行に
進む送信波、8は超音波の伝達媒体中に存在する反射物
、9は反射物8で反射し送信波7と平行・逆向きに進む
反射波、10は増幅器、11は増幅器10から送られる
電気振動の振幅比較等の信号処理を行なう処理部である
。7 is a transmitted wave emitted from the wave transmitting transducer 3, reflected by the reflecting surface of the wave reflecting tube 6, and traveling parallel to the central axis of the wave reflecting tube 6; 8 is a transmitted wave in the ultrasonic transmission medium. 9 is an existing reflecting object; 9 is a reflected wave that is reflected by the reflecting object 8 and travels parallel to and in the opposite direction to the transmitted wave 7; 10 is an amplifier; 11 is a processing unit that performs signal processing such as amplitude comparison of electric vibrations sent from the amplifier 10. It is.
上記のように構成された波動送受波装置において、駆動
部1から送られる基準信号に同期して発振部2て電気振
動を発生させ、この電気振動が送波用振動子3に送られ
てパルス状の超音波に変換される。この超音波は送波用
振動子3の側面から放射され、波動反射用筒6の反射面
のうち送波用振動子3の長さΩ 1に対応する内径φ1
1と外径φ1oで定まる領域内で反射して送信される。In the wave transmitting/receiving device configured as described above, the oscillating unit 2 generates electrical vibrations in synchronization with the reference signal sent from the driving unit 1, and the electrical vibrations are sent to the wave transmitting oscillator 3 to generate pulses. is converted into ultrasonic waves. This ultrasonic wave is radiated from the side surface of the wave transmitting transducer 3, and the inner diameter φ1 of the reflecting surface of the wave reflecting cylinder 6 corresponds to the length Ω1 of the wave transmitting transducer 3.
1 and the outer diameter φ1o and is transmitted.
この送信波7が媒体中を伝播し測定対象物である反射物
8て反射して波動反射用筒6の反射面のうち受波用振動
子4aの長さρ2に対応する内径φ21と外径φ2o内
で定まる領域内で反射した後、受波用振動子4aて受波
されて受波用振動子4て電気振動に変換される。This transmitted wave 7 propagates through the medium and is reflected by a reflecting object 8, which is the object to be measured.The inner diameter φ21 and outer diameter of the reflecting surface of the wave reflecting tube 6 correspond to the length ρ2 of the wave receiving vibrator 4a. After being reflected within a region determined within φ2o, the wave is received by the wave receiving vibrator 4a and converted into electric vibration by the wave receiving vibrator 4.
この電気振動は増幅器10で増幅され、あらかじめ超音
波の送信時に駆動部1で発生する基準信号を受けて計時
を開始している処理部11に送られる。This electric vibration is amplified by an amplifier 10 and sent to a processing unit 11 which has started time measurement in response to a reference signal generated by the drive unit 1 in advance when transmitting the ultrasonic wave.
この電気振動の振幅があらかじめ定められたしきい値と
比較され、電気振動の振幅がしきい値を超えた時点で計
時を終了し計測信号を送りだす。The amplitude of this electric vibration is compared with a predetermined threshold, and when the amplitude of the electric vibration exceeds the threshold, timekeeping is stopped and a measurement signal is sent.
第7図は上記波動送受波装置の指向性パターンの一例を
示し、図においてdは送波用振動子3と波動反射用筒6
が形成する指向性パターン(以下、第1のパターンとい
う)を示し、eは受波用振動子4aと波動反射用筒6が
形成する指向性パターン(以下、第2のパターンという
)を示す。なお、eが第1のパターン、dが第1のパタ
ーンであっても良い。FIG. 7 shows an example of the directivity pattern of the above-mentioned wave transmitting/receiving device.
indicates a directivity pattern (hereinafter referred to as a first pattern) formed by the wave receiving vibrator 4a and a directivity pattern formed by the wave reflection cylinder 6 (hereinafter referred to as a second pattern). Note that e may be the first pattern and d may be the first pattern.
第7図に示すように第1のパターンdを有する超音波を
送信し、この超音波の反射波9を第2のパターンeを有
する波動反射用筒6と受波用振動子4aで受信すると、
受波用振動子4aの受信出力は第1のパターンdと第2
のパターンeを相乗した値に見合う合成パターンfとし
て得られる。この合成パターンfの第1サイドロープ・
レベルは互いにレベルが高いロープの部分で合成されて
いるため第7図に示す場合は約−20dBとなっている
。As shown in FIG. 7, when an ultrasonic wave having a first pattern d is transmitted and a reflected wave 9 of this ultrasonic wave is received by the wave reflecting tube 6 and the wave receiving transducer 4a having a second pattern e, ,
The receiving output of the wave receiving transducer 4a is divided into the first pattern d and the second pattern d.
A composite pattern f corresponding to the value obtained by adding the pattern e is obtained. The first side rope of this composite pattern f
Since the levels are combined in the rope parts where the levels are mutually high, the level is about -20 dB in the case shown in FIG. 7.
[発明が解決しようとする問題点]
上記従来の波動送受波装置においては、第1のパターン
dと第2のパターンeの互いにレベルが高いロープの部
分で相乗して合成パターンfのサイドロープを形成して
いるため、合成パターンfのサイドロープ・レベルが高
く、このため本来の= 4 −
主ロープによる計測等に障害を与えるという問題点があ
った。[Problems to be Solved by the Invention] In the above-mentioned conventional wave transmitting/receiving device, the side ropes of the composite pattern f are synergized by the rope portions of the first pattern d and the second pattern e whose levels are high. Because of this, the side rope level of the composite pattern f is high, which poses a problem in that it interferes with measurements using the original = 4 - main rope.
この発明はかかる問題点を解決するためになされたもの
であり受波器受信出力のサイドロープ・レベルを低減し
て高確度に計測等を行なうことができる波動送受波装置
を得ることを目的とするものである。The present invention was made to solve this problem, and its purpose is to provide a wave transmitting and receiving device that can reduce the sidelobe level of the received output of a wave receiver and perform measurements with high accuracy. It is something to do.
[問題点を解決するための手段]
この発明に係る波動送受波装置は第1の円筒形振動子と
波動反射用筒が形成する指向性パターン、または第2の
円筒形振動子と波動反射用筒が形成する指向性パターン
の強度が大きいサイドロープが存在する範囲内で、一方
の指向性パターンのロープ間の極小値の方向が他方の指
向性パターンの極大値の近傍方向に存在するようにした
ことを特徴とする。[Means for Solving the Problems] The wave transmitting/receiving device according to the present invention has a directivity pattern formed by a first cylindrical vibrator and a wave reflecting tube, or a directivity pattern formed by a first cylindrical vibrator and a wave reflecting cylinder. Within the range where the directional pattern formed by the cylinder has side ropes with high strength, the direction of the minimum value between the ropes of one directional pattern is in the vicinity of the maximum value of the other directional pattern. It is characterized by what it did.
[作用]
この発明においては、第1の円筒形振動子と波動反射用
筒が形成する指向性パターンと、第2の円筒形振動子と
波動反射用筒が形成する指向性バターンのサイドロープ
の方向に相違をもたせ、−方の指向性パターンのロープ
間の極小値と他方の指向性パターンのサイドロープの極
大値もしくはその近傍の値を相乗じることにより受波器
受信出力のサイドロープ・レベルを低減させる。[Function] In this invention, the directional pattern formed by the first cylindrical vibrator and the wave reflecting tube, and the side rope of the directional pattern formed by the second cylindrical vibrator and the wave reflecting tube. The side lobe level of the receiver's received output is determined by adding the local minimum value between the ropes of the - side directional pattern and the local maximum value of the side lobe of the other directional pattern, or a value in the vicinity thereof, with a difference in direction. Reduce.
[実施例コ
第1図はこの発明の一実施例を示すブロック図であり、
図において1〜3.5〜11は第5図に示した従来例と
全く同じものである。4は送波用振動子3から送信され
た超音波の反射物8で反射した反射波9を受信して電気
振動に変換する受波器の振動子(以下、受渡用振動子と
いう)である。[Embodiment FIG. 1 is a block diagram showing an embodiment of the present invention.
In the figure, numbers 1 to 3.5 to 11 are exactly the same as the conventional example shown in FIG. Reference numeral 4 denotes a receiver transducer (hereinafter referred to as a delivery transducer) that receives reflected waves 9 reflected by an ultrasonic reflector 8 transmitted from the transmitting transducer 3 and converts them into electrical vibrations. .
送波用振動子3と受渡用振動子4との間には音響絶縁材
5が挿入され、送波用振動子3と受波用振動子4は第2
図に示すように中心軸が波動反射用笠6の中心軸と一致
するように波動反射用笠6に取付けられている。An acoustic insulating material 5 is inserted between the wave transmitting vibrator 3 and the wave receiving vibrator 4, and the wave transmitting vibrator 3 and the wave receiving vibrator 4 are
As shown in the figure, it is attached to the wave reflecting shade 6 so that its central axis coincides with the central axis of the wave reflecting shade 6.
この受渡用振動子4の軸方向長さρ2は送波用振動子3
の軸方向長さplより短かくなっており、送波用振動子
3と波動反射用笠6で形成する指向性パターン(以下、
第1のパターンという)と、受波用振動子4と波動反射
用笠6で形成する指向性パターン(以下、第2のパター
ンという)は−定の関係で相違させである。The axial length ρ2 of the transmission transducer 4 is the transmission transducer 3.
is shorter than the axial length pl, and the directivity pattern (hereinafter referred to as
The directivity pattern formed by the wave receiving transducer 4 and the wave reflecting shade 6 (hereinafter referred to as the second pattern) are different from each other in a constant relationship.
第3図は第1のパターンと第2のパターンの一例を示し
、第3図においてaは第1のパターン、bは第2のパタ
ーンである。第3図に示すように第1のパターンaと第
2のパターンbの主ロープ中央部はほぼ一致し、第1の
パターンaの主ロープと第1のサイドロープ間の極小値
を示す位置に第2のパターンbの第1サイドロープの極
大値の位置がくるように受波用振動子4の軸方向長さρ
2が定めである。FIG. 3 shows an example of the first pattern and the second pattern, and in FIG. 3, a is the first pattern and b is the second pattern. As shown in Fig. 3, the central portions of the main ropes of the first pattern a and the second pattern b almost coincide, and the center portions of the main ropes of the first pattern a and the first side ropes are located at the minimum value. The axial length ρ of the wave receiving transducer 4 is adjusted so that the position of the maximum value of the first side rope of the second pattern b is located.
2 is the standard.
上記のように構成した波動送受波装置において、送波用
振動子3から放射された超音波は波動反射用笠6の反射
面で反射し第1のパターンaに示す送信波7として媒体
中に送信される。この送信波7が媒体中を伝播し反射物
8で反射して反射波9となる。この反射波9が波動反射
用笠6の反射面のうち受波用振動子4の長さΩ2に対応
する内径φ21と外径φ2o内で定まる領域内で反射し
て受渡用振動子4で受波されて電気振動に変換される。In the wave transmitting/receiving device configured as described above, the ultrasonic waves emitted from the wave transmitting transducer 3 are reflected by the reflecting surface of the wave reflecting shade 6 and enter the medium as transmitted waves 7 shown in the first pattern a. Sent. This transmitted wave 7 propagates through the medium, is reflected by a reflecting object 8, and becomes a reflected wave 9. This reflected wave 9 is reflected within the area defined by the inner diameter φ21 and the outer diameter φ2o corresponding to the length Ω2 of the wave receiving vibrator 4 on the reflecting surface of the wave reflecting shade 6, and is received by the delivery vibrator 4. The waves are converted into electrical vibrations.
この超音波を受波した受渡用振動子4の受信出力は第1
のパターンaと第2のパターンbを相乗じた合成パター
ンCとして得られる。この場合第1のパターンaと第2
のパターンbの主ロープ中央部はほぼ一致しているため
雨上ロープの中央部を相乗して得られる合成パターンC
の主ロープ・レベルを一定レベルに保持することができ
る。−方、第1のパターンaの主ロープと第1サイドロ
ープ間の極小値の方向が第2のパターンbの第1サイド
ロープの極大値の方向とほぼ一致しているため、これら
を相乗して得られた合成パターンCの実用上支障となる
次数の低い方のサイドロープ・レベルを低減することが
できる。すなわち第3図に示す場合には合成パターンC
の第1サイドロープ・レベルは一25dB程度となり、
第7図に示した従来例と比べて約5dB程度改善するこ
とができる。この場合、合成パターンCの主ロープは第
7図に示した従来例の場合と比べて少し広くなるが、=
8 −
実用上特に支障は生じない。The receiving output of the delivery transducer 4 that received this ultrasonic wave is the first one.
A composite pattern C is obtained by combining the pattern a and the second pattern b. In this case, the first pattern a and the second pattern
Since the central parts of the main ropes in pattern B are almost the same, a composite pattern C can be obtained by combining the central parts of the rain ropes.
main rope level can be maintained at a constant level. - On the other hand, since the direction of the minimum value between the main rope and the first side rope of the first pattern a is almost the same as the direction of the maximum value of the first side rope of the second pattern b, these are synergized. It is possible to reduce the side lobe level of the lower order which is a practical problem in the composite pattern C obtained by the method. In other words, in the case shown in FIG. 3, the composite pattern C
The first side rope level of is about -25 dB,
This can be improved by about 5 dB compared to the conventional example shown in FIG. In this case, the main rope of composite pattern C is slightly wider than that of the conventional example shown in Fig. 7, but =
8 - There are no particular problems in practical use.
なお、上記実施例においては送波用振動子3の軸方向長
さplと受渡用振動子4の軸方向長さΩ2とを変えて第
1のパターンaと第2のパターンbを相違させた場合に
ついて説明したが、送波用振動子3と受波用振動子4の
内、外径や両振動子3,4間の距離、すなわち音響絶縁
材5の厚さを変えても上記実施例と同様の作用を奏する
ことができる。In the above embodiment, the first pattern a and the second pattern b were made different by changing the axial length pl of the wave transmitting vibrator 3 and the axial length Ω2 of the delivery vibrator 4. Although the case has been explained, even if the inner and outer diameters of the wave transmitting vibrator 3 and the wave receiving vibrator 4, the distance between both vibrators 3 and 4, or the thickness of the acoustic insulating material 5 are changed, the above-mentioned embodiments will work. The same effect can be achieved.
また、上記実施例においては反射物8で反射した超音波
の反射波を受渡用振動子4で受信する場合について説明
したが、第4図に示すように超音波の伝達媒体中に反射
物8が存在しない場合であっても、送波用とは別に受波
器の波動反射用笠6aと受渡用振動子4を組合せて、送
波用振動子3から送信した送信波7を直接受波用振動子
4で受信することにより、上記実施例と同様の作用を奏
することができる。Further, in the above embodiment, a case has been described in which the reflected wave of the ultrasonic wave reflected by the reflecting object 8 is received by the delivery transducer 4, but as shown in FIG. Even if there is no transmitting wave, the transmitting wave 7 transmitted from the transmitting vibrator 3 can be directly received by combining the receiver's wave reflection shade 6a and the delivery vibrator 4 in addition to the wave transmitting one. By receiving the signal using the digital vibrator 4, the same effect as in the above embodiment can be achieved.
なお、上記各実施例において送波用振動子3と受渡用振
動子4の形状1寸法を異ならせても、振動子はある程度
の周波数帯域を有しているから、送受同一周波数での使
用には実用上支障を生じない。In each of the above embodiments, even if the transmitting transducer 3 and the delivery transducer 4 have different shapes and dimensions, the transducers have a certain frequency band, so they cannot be used at the same frequency for transmitting and receiving. does not cause any practical problems.
また、上記各実施例においては超音波を伝搬させる場合
について説明したが、超音波以外の波動伝播に対しても
上記各実施例と同様に適用することができる。Further, in each of the above embodiments, the case where ultrasonic waves are propagated has been described, but the present invention can also be applied to wave propagation other than ultrasonic waves in the same manner as in each of the above embodiments.
〔発明の効果]
この発明は以上説明したように第1の円筒形振動子と波
動反射用筒が形成する指向性パターンと、第2の円筒形
振動子と波動反射用筒が形成する指向性パターンとのサ
イドロープの位置に相違をもたせ、一方の指向性パター
ンのロープ間の極小値と他方の指向性パターンのサイド
ロープの極大値を相乗じることにより受波器受信出力の
低次数のサイドロープ・レベルを低減するようにしたの
で、受信出力のサイドロープが測定等に与える障害を防
止することができる。[Effects of the Invention] As explained above, the present invention has a directivity pattern formed by the first cylindrical vibrator and the wave reflecting tube, and a directivity pattern formed by the second cylindrical vibrator and the wave reflecting tube. By making a difference in the position of the side ropes from the pattern and multiplying the minimum value between the ropes of one directional pattern and the maximum value of the side ropes of the other directional pattern, the low-order side of the receiver's received output is Since the rope level is reduced, it is possible to prevent side ropes of the received output from interfering with measurements, etc.
第1図はこの発明の実施例を示すブロック図、第2図は
上記実施例の送受波器を示す断面図、第3図は上記実施
例の指向性パターンを示す状態図、第4図は他の実施例
を示すブロック図、第5図は従来例を示すブロック図、
第6図は従来例の送受波器を示す断面図、第7図は従来
例の指向性パターンを示す状態図である。
1・・・駆動部、2・・・発振器、3・・・送波用振動
子、4.4a・・・受波用振動子、5・・・音響絶縁材
、6.8a・・・波動反射用筒、10・・・増幅器、1
1・・・処理部、a、d・・・第1のパターン、b、e
・・・第2のパターン、c、f・・・合成パターン。FIG. 1 is a block diagram showing an embodiment of the present invention, FIG. 2 is a sectional view showing the transducer of the above embodiment, FIG. 3 is a state diagram showing the directivity pattern of the above embodiment, and FIG. A block diagram showing another embodiment, FIG. 5 is a block diagram showing a conventional example,
FIG. 6 is a sectional view showing a conventional transducer, and FIG. 7 is a state diagram showing a directivity pattern of the conventional example. DESCRIPTION OF SYMBOLS 1... Drive part, 2... Oscillator, 3... Vibrator for wave transmission, 4.4a... Vibrator for wave reception, 5... Acoustic insulation material, 6.8a... Wave motion Reflection tube, 10...Amplifier, 1
1... Processing section, a, d... First pattern, b, e
... second pattern, c, f... composite pattern.
Claims (2)
の円筒形振動子と、第1の円筒形振動子から送信した波
動を受信する第2の円筒形振動子と、中心角が直角の円
錐状をなし送・受共用または送・受個別に設けられた波
動反射用笠とを備え、第1の円筒形振動子と第2の円筒
形振動子が、その中心軸をそれぞれ波動反射用笠の中心
軸と共有になるように配置された波動送受波装置におい
て、第1の円筒形振動子と波動反射用笠が形成する指向
性パターン(以下、第1のパターンという)、または第
2の円筒形振動子と波動反射用笠が形成する指向性パタ
ーン(以下、第2のパターンという)の強度が大きいサ
イドロープが存在する範囲内で、一方の指向性パターン
のロープ間の極小値の方向が他方の指向性パターンのサ
イドロープの極大値の近傍方向に存在するようにしたこ
とを特徴とする波動送受波装置。(1), the first transmitting wave having a nearly constant frequency
A cylindrical oscillator, a second cylindrical oscillator that receives the waves transmitted from the first cylindrical oscillator, and a conical shape with a right angle center angle, and are provided for both transmission and reception or separately for transmission and reception. A wave transmitting/receiving device comprising: a wave reflecting shade; the first cylindrical oscillator and the second cylindrical oscillator are arranged so that their respective central axes are shared with the central axis of the wave reflecting shade; In the wave device, the directivity pattern formed by the first cylindrical vibrator and the wave reflecting shade (hereinafter referred to as the first pattern), or the directivity formed by the second cylindrical vibrator and the wave reflecting shade Within the range where side ropes with high strength exist in the pattern (hereinafter referred to as the second pattern), the direction of the minimum value between the ropes of one directional pattern is near the maximum value of the side ropes of the other directional pattern. A wave transmitting/receiving device characterized in that the wave transmitting/receiving device exists in a direction.
プの方向を、第1の円筒形振動子と第2の円筒形振動子
の中心軸方向の長さ、外径、内径のうち少なくとも1つ
を相違させることにより異ならせる特許請求の範囲第1
項記載の波動送受波装置。(2) The direction of the side ropes of the first pattern and the second pattern is determined by at least the length in the central axis direction, the outer diameter, and the inner diameter of the first cylindrical vibrator and the second cylindrical vibrator. Claim 1 that differs by making one thing different
The wave transceiver device described in .
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62251554A JPH0194282A (en) | 1987-10-07 | 1987-10-07 | Wave transmitting and receiving apparatus |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62251554A JPH0194282A (en) | 1987-10-07 | 1987-10-07 | Wave transmitting and receiving apparatus |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0194282A true JPH0194282A (en) | 1989-04-12 |
Family
ID=17224552
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62251554A Pending JPH0194282A (en) | 1987-10-07 | 1987-10-07 | Wave transmitting and receiving apparatus |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0194282A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100709779B1 (en) * | 2006-11-23 | 2007-04-19 | 주식회사 씨케이 테크피아 | A ultrasonic level sensor and a measuring method using wherein ultrasonic level sensor |
-
1987
- 1987-10-07 JP JP62251554A patent/JPH0194282A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100709779B1 (en) * | 2006-11-23 | 2007-04-19 | 주식회사 씨케이 테크피아 | A ultrasonic level sensor and a measuring method using wherein ultrasonic level sensor |
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