JPH0439589Y2 - - Google Patents

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Publication number
JPH0439589Y2
JPH0439589Y2 JP1989018076U JP1807689U JPH0439589Y2 JP H0439589 Y2 JPH0439589 Y2 JP H0439589Y2 JP 1989018076 U JP1989018076 U JP 1989018076U JP 1807689 U JP1807689 U JP 1807689U JP H0439589 Y2 JPH0439589 Y2 JP H0439589Y2
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JP
Japan
Prior art keywords
excitation
vibrator
magnetostrictive
numbered
ultrasonic
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
Application number
JP1989018076U
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Japanese (ja)
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JPH01132987U (en
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Priority to JP1989018076U priority Critical patent/JPH0439589Y2/ja
Publication of JPH01132987U publication Critical patent/JPH01132987U/ja
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Expired legal-status Critical Current

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  • Transducers For Ultrasonic Waves (AREA)
  • Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)

Description

【考案の詳細な説明】 (産業上の利用分野) この考案は、円又は円弧上にほぼ等間隔に配列
される第1乃至第nの偶数個の磁歪振動子で構成
される振動子群を複数個、隣接する振動子群間が
ほぼ等間隔になるように複数層に積層して得られ
る円筒又は半円筒形状の超音波送受波器のそれぞ
れの振動子群に属する全ての振動子をそれぞれ同
時に励振して水中に超音波パルスを送波し、各磁
歪振動子により補捉される受信信号を別個に取り
出す水中探知用超音波送受信器に関する。水平面
に対する超音波パルスの送波方向、すなわちチル
ト角θを変化させることができる水中探知用超音
波送受信器に関する。
[Detailed description of the invention] (Field of industrial application) This invention uses a vibrator group consisting of an even number of first to n-th magnetostrictive vibrators arranged at approximately equal intervals on a circle or arc. All the transducers belonging to each transducer group of a cylindrical or semi-cylindrical ultrasonic transducer obtained by laminating multiple layers such that adjacent transducer groups are approximately equally spaced. The present invention relates to an ultrasonic transceiver for underwater detection that simultaneously excites and transmits ultrasonic pulses underwater and separately extracts received signals captured by each magnetostrictive vibrator. The present invention relates to an ultrasonic transceiver for underwater detection that can change the transmission direction of ultrasonic pulses with respect to a horizontal plane, that is, the tilt angle θ.

(従来の技術) 第1図において、Lo乃至L1o,乃至L2o,L31
至L3oは磁歪振動子の励磁コイルを示す。磁歪振
動子はいわゆる兀型磁歪振動子が用いられ、その
脚部に上記励磁コイルが巻回されている。
(Prior Art) In FIG. 1, L o to L 1o , L 2o to L 31 and L 31 to L 3o indicate excitation coils of a magnetostrictive vibrator. A so-called shoe-shaped magnetostrictive vibrator is used as the magnetostrictive vibrator, and the excitation coil is wound around the legs of the magnetostrictive vibrator.

第2図は上記励磁コイルL11乃至L1o,L21乃至
L2o,L31乃至L3oによつて励磁される磁歪振動子
を示し、磁歪振動子Z11乃至Z1oは励磁コイルL11
乃至L1oによつて励磁され、磁歪振動子Z21乃至
Z2oは励磁コイルL21乃至L2o、磁歪振動子Z31乃至
Z3oは励磁コイルL31乃至L3oによつてそれぞれ励
磁される。
Figure 2 shows the excitation coils L 11 to L 1o , L 21 to
The magnetostrictive oscillators are excited by L 2o , L 31 to L 3o , and the magnetostrictive oscillators Z 11 to Z 1o are excited by the exciting coil L 11
Excited by L 1o to magnetostrictive oscillators Z 21 to
Z 2o is the excitation coil L 21 to L 2o and the magnetostrictive vibrator Z 31 to
Z 3o is excited by exciting coils L 31 to L 3o , respectively.

磁歪振動子Z11乃至Z1o,Z21乃至Z2o,Z31乃至
Z3oは円形に3段配列され、各段間には遮音材1
が介在し、円形配列される振動子の隣接間にも遮
音材2を介在させて配列されている。そして、磁
歪振動子Z11乃至Z1oZ21乃至Z2o,Z31乃至Z3oは筐
体3,3間に支持され、支持軸4によつて船底に
固定される。
Magnetostrictive vibrators Z 11 to Z 1o , Z 21 to Z 2o , Z 31 to
Z 3o is arranged in three stages in a circle, with one piece of sound insulation material between each stage.
are interposed therebetween, and sound insulating materials 2 are also interposed between adjacent vibrators arranged in a circular manner. The magnetostrictive vibrators Z 11 to Z 1o Z 21 to Z 2o and Z 31 to Z 3o are supported between the casings 3 and 3 and fixed to the bottom of the ship by the support shaft 4.

第1図において、励磁コイルL11乃至L1oは一端
が共通接続されて接地され、他端はそれぞれ別個
に、送受信切換回路T11乃至T1oを経て出力変成
器51の出力コイルL01に接続される。出力変成
器51は励振電源61から励振電力が導かれ、こ
の励振電力によつて励磁コイルL11乃至L1oが同時
に励磁される。従つて、励磁コイルL11乃至L1o
同方向に巻回されているとき、第2図の磁歪振動
子Z11乃至Z1oは同相で励振される結果、円周方向
に超音波パルスが同時に送波される。なお、超音
波パルスの送波後、探知物体から帰来する反射波
は、各々の帰来方向の磁歪振動子に受波された
後、送受信切換回路T11乃至T1oからそれぞれの
受信器に導かれるがこれについては省略する。
In FIG. 1, the excitation coils L 11 to L 1o are commonly connected at one end and grounded, and the other ends are individually connected to the output coil L 01 of the output transformer 51 via transmission/reception switching circuits T 11 to T 1o . be done. Excitation power is led to the output transformer 51 from an excitation power source 61, and the excitation coils L11 to L1o are simultaneously excited by this excitation power. Therefore, when the excitation coils L 11 to L 1o are wound in the same direction, the magnetostrictive vibrators Z 11 to Z 1o in FIG. 2 are excited in the same phase, so that ultrasonic pulses are simultaneously generated in the circumferential direction. Waves are transmitted. Note that after the ultrasonic pulse is transmitted, the reflected waves returning from the detected object are received by the magnetostrictive vibrators in each returning direction, and then guided to the respective receivers from the transmitting/receiving switching circuits T11 to T1o . However, this will be omitted.

他方、励磁コイルL21乃至L2o,L31乃至L3oも上
記と同様にして、それぞれの励磁電源62,63
によつて励磁される。従つて、励振電源61,6
2,63が同相であるとき、第2図の磁歪振動子
Z11乃至Z1oZ21乃至Z2o,Z31乃至Z3oが同相で励振
されるから、水平面の広範囲方向に超音波パルス
が送波される。
On the other hand, the excitation coils L 21 to L 2o and L 31 to L 3o are also connected to the respective excitation power supplies 62 and 63 in the same manner as above.
Excited by. Therefore, the excitation power sources 61, 6
When 2 and 63 are in phase, the magnetostrictive vibrator in Figure 2
Since Z 11 to Z 1o , Z 21 to Z 2o , and Z 31 to Z 3o are excited in the same phase, ultrasonic pulses are transmitted in a wide range of directions on the horizontal plane.

この場合、各段の振動子Z11乃至Z1o,Z21乃至
Z2o,Z31乃至Z3oの励振位相を変化させると、水
平面に対する超音波パルスの送波方向、すなわち
チルト角θを変化させることができる。チルト角
θの調整は、周知のように、位相調節器7によつ
て励振電源61,62,63の各励振出力の位相
を調節することにより行なわれる。
In this case, each stage of vibrators Z 11 to Z 1o , Z 21 to
By changing the excitation phase of Z 2o , Z 31 to Z 3o , it is possible to change the transmission direction of the ultrasonic pulse with respect to the horizontal plane, that is, the tilt angle θ. The tilt angle θ is adjusted, as is well known, by adjusting the phase of each excitation output of the excitation power sources 61, 62, and 63 using the phase adjuster 7.

(従来装置の欠点) 第1図において、励磁コイルL11乃至L1o,L21
乃至L2o,L31乃至L3oは、第2図の振動子筐体3,
3内に設けられ、励振電源61,62,63等は
船体内に設けられる。そして各励振電源61,6
2,63と励磁コイルとは給電線により接続され
る。この場合、接続する給電線の線数をできるだ
け減らすため、励磁コイルL11乃至L1o,L21乃至
L2o,L31乃至L3oの片方を共通接続して接地する
方式が多く用いられる。そのため、励磁コイル
L11乃至L1oL21乃至L2o,L31乃至L3oの電流が同相
で流れ、送信時の各励磁コイルの励振電流は比較
的大電流であるため、接地電流は非常に大きな電
流が流れる。そして、この接地電流は第2図の筐
体3、支持軸4を経て船体を通つて出力変成器5
1,52,53へ導かれる。そのため、従来は、
この接地電流のために送受波器筐体、船体の接地
電流路に電触が発生し種々の弊害を生じさせる。
又、大電流の接地電流によつて、振動子相互間に
相互誘導を生じさせ、送受信特性を劣化させる原
因にもなる。
(Disadvantages of the conventional device) In Fig. 1, the excitation coils L 11 to L 1o , L 21
L 2o to L 3o and L 31 to L 3o are the transducer housing 3 in FIG.
The excitation power sources 61, 62, 63, etc. are provided inside the hull. And each excitation power source 61, 6
2, 63 and the excitation coil are connected by a power supply line. In this case, in order to reduce the number of connected feeder lines as much as possible, the excitation coils L11 to L1o , L21 to
A method in which one of L 2o , L 31 to L 3o is commonly connected and grounded is often used. Therefore, the excitation coil
The currents L 11 to L 1o , L 21 to L 2o , and L 31 to L 3o flow in the same phase, and the excitation current of each exciting coil during transmission is a relatively large current, so a very large ground current flows. . This ground current then passes through the casing 3, support shaft 4, and the hull of the ship to the output transformer 5 in Fig. 2.
It will lead you to 1, 52, 53. Therefore, conventionally,
This ground current causes electrical contact in the ground current path of the transducer housing and the ship's hull, causing various problems.
Further, the large ground current causes mutual induction between the vibrators, which causes deterioration of transmission and reception characteristics.

(考案が解決しようとする課題) この考案は、上記欠点を解消するもので送受波
器筐体に接地電流を流さないようにすることを目
的とする。
(Problems to be Solved by the Invention) This invention is intended to eliminate the above-mentioned drawbacks, and aims to prevent ground current from flowing through the transducer housing.

(課題を解決するための手段) この考案に係る水中探知用超音波送受信器は、
円又は円弧上にほぼ等間隔に配列される第1乃至
第nの偶数個の磁歪振動子で構成される振動子群
を複数個、隣接する振動子群間がほぼ等間隔にな
るように複数層に積層して得られる円筒又は半円
筒形状の超音波送受波器のそれぞれの振動子群に
属する全ての振動子をそれぞれ同時に励振して水
中に超音波パルスを送波し、各磁歪振動子により
補捉される受信信号を別個に取り出すもので、上
記複数層のそれぞれの層の第1乃至第nの磁歪振
動子のうち奇数番目振動子の励磁コイルに対して
偶数番目振動子の励磁コイルを逆方向に巻回し、 奇数番目振動子の各励磁コイルの終端(始端)
を共通接続すると共に、偶数番目振動子の終端
(始端)を共通接続し、 上記共通接続部を上記超音波送受波器の筐体に
接地すると共に、上記各層の第1乃至第nの磁歪
振動子の励磁コイルの上記共通接続されていない
端を送受信切替回路を経て励振電源に導くように
構成する。
(Means for solving the problem) The ultrasonic transmitter/receiver for underwater detection according to this invention has the following features:
A plurality of vibrator groups each consisting of an even number of first to n-th magnetostrictive vibrators arranged at approximately equal intervals on a circle or an arc, and a plurality of vibrator groups such that adjacent vibrator groups are approximately equally spaced apart. All the oscillators belonging to each oscillator group of the cylindrical or semi-cylindrical ultrasonic transducer obtained by laminating layers are simultaneously excited to transmit ultrasonic pulses into the water, and each magnetostrictive oscillator is The received signal captured by the above-mentioned plurality of layers is separately taken out, and the excitation coil of the even-numbered vibrator is separated from the excitation coil of the odd-numbered vibrator among the first to n-th magnetostrictive vibrators in each of the plurality of layers. Winding in the opposite direction, the end (starting end) of each excitation coil of the odd-numbered vibrator
At the same time, the terminal ends (starting ends) of the even-numbered transducers are commonly connected, and the common connection part is grounded to the casing of the ultrasonic transducer, and the first to nth magnetostrictive vibrations of each layer are connected in common. The ends of the secondary excitation coils that are not commonly connected are configured to be led to the excitation power source via a transmission/reception switching circuit.

(考案の原理) 第3図において、L1,L2は第1図と同様な励
磁コイルで、励磁コイルL2は励磁コイルL1に対
してその巻回方向が逆方向になされている。
(Principle of the invention) In FIG. 3, L 1 and L 2 are excitation coils similar to those in FIG. 1, and the excitation coil L 2 is wound in the opposite direction to the excitation coil L 1 .

そして、励磁コイルL1とL2はその終端が互いに
接続されて接地されている。又、励磁コイルL1
とL2の終端は励振電源E1.E2の一端に接続され
る。励振電源E1,E2は直列接続され、同相で同
じ出力電圧を送出する。
The excitation coils L 1 and L 2 have their terminal ends connected to each other and grounded. Also, excitation coil L 1
and the terminal of L 2 is the excitation power source E 1 . Connected to one end of E 2 . The excitation power supplies E 1 and E 2 are connected in series and output the same output voltage in the same phase.

従つて、励磁コイルL1とL2が同じ特性のとき、
励磁コイルL1とL2の接続点Qと励振電源E1,E2
の接続点Pとの間は電位が平衡するから、P,Q
点を接地しても接地電流は流れない。又、励磁コ
イルL1とL2を逆方向に巻回することにより、同
方向の磁束を発生させることができるから、振動
子から同相の超音波を発生させることができる。
Therefore, when exciting coils L 1 and L 2 have the same characteristics,
Connection point Q between excitation coils L 1 and L 2 and excitation power supplies E 1 and E 2
Since the potential is balanced with the connection point P, P, Q
Even if the point is grounded, no ground current will flow. Furthermore, by winding the excitation coils L 1 and L 2 in opposite directions, it is possible to generate magnetic flux in the same direction, so that ultrasonic waves in the same phase can be generated from the vibrator.

(考案の実施例) 第4図において、第1図と同じ番号は同一の動
作を行なう。
(Embodiment of the invention) In FIG. 4, the same numbers as in FIG. 1 perform the same operations.

L′11乃至L′1oは第1図と同様な励磁コイルで偶
数個配列されている。そして、奇数番目励磁コイ
ルL′11,L′13,L′15……に対して偶数番目励磁コ
イルL′12,L′14,L′16……はその巻回方向が逆方
向になされ、それぞれの励磁コイルL′11乃至L′1o
は終端が共通接続されて接地されている。又、奇
数番目励磁コイルL′11,L′13,L′15……の各々の
始端はそれぞれに対応して設けられた送受信切換
回路T11,T13,T15……を経て出力変成器51の
出力コイルL01の片方の端子に導かれる。そして、
偶数番目励磁コイルL′12,L′14,L′16……の各々
の始端はそれぞれに対応して設けられた送受信切
換回路T12,T14,T16……を経て出力変成器51
の他方の端子に導かれる。なお、各励磁コイル
L′11乃至L′1oの始端が導かれる送受信切換回路
T11乃至T1oは周知のごとくして送信信号と受信
信号とを切換えるもので、各励磁コイルL′11乃至
L′1oに生じる受信信号は、接地に対する受信信号
が各々の送受信切換回路T11乃至T1oから受信器
に導かれる。
L' 11 to L' 1o are excitation coils similar to those shown in FIG. 1, and an even number of them are arranged. The even-numbered excitation coils L' 12 , L' 14 , L' 16 . . . are wound in the opposite direction to the odd-numbered excitation coils L' 11 , L' 13 , L' 15 . Each excitation coil L′ 11 to L′ 1o
have their ends connected together and grounded. Furthermore, the starting ends of each of the odd-numbered excitation coils L ' 11 , L ' 13 , L ' 15 . . . It is led to one terminal of the output coil L 01 of No. 51. and,
The starting ends of each of the even-numbered excitation coils L ' 12 , L ' 14 , L ' 16 .
is led to the other terminal of In addition, each excitation coil
Transmission/reception switching circuit where the starting ends of L′ 11 to L′ 1o are led
T 11 to T 1o are for switching between a transmitting signal and a receiving signal as is well known, and each excitation coil L′ 11 to
The received signal generated at L' 1o is directed to the receiver from each of the transmission/reception switching circuits T 11 to T 1o .

上記において、励磁コイルL′11乃至L′1oは奇数
番目励磁コイルと偶数番目励磁コイルが一対ずつ
組合されて第3図と同様にして送信電流が出力変
成器51から供給される。従つて、奇数番目励磁
コイルと偶数番目励磁コイルの接続点は、第3図
で説明したように電位が平衡するから、接続点を
接地しても接地電流は流れない。但し、各励磁コ
イルL′11乃至L′1oに生じる受波信号は、各励磁コ
イルの終端が接地され、接地電位に対する受波電
圧が送受信切換回路から送出される。従つて、受
波電圧による接地電流が流れるが、受波電圧は非
常に微弱な信号であるから、これによつて接地電
流が流れても前記説明のような弊害が生じること
はない。
In the above, the excitation coils L' 11 to L' 1o are combined into pairs of odd-numbered excitation coils and even-numbered excitation coils, and transmitting current is supplied from the output transformer 51 in the same manner as in FIG. Therefore, since the potential at the connection point between the odd-numbered excitation coil and the even-numbered excitation coil is balanced as explained in FIG. 3, no ground current flows even if the connection point is grounded. However, the receiving signal generated in each of the excitation coils L' 11 to L' 1o is grounded at its terminal end, and the receiving voltage relative to the ground potential is sent out from the transmission/reception switching circuit. Therefore, a ground current due to the received voltage flows, but since the received voltage is a very weak signal, even if the ground current flows due to this, the above-mentioned problem will not occur.

他の励磁コイルL′21乃至L′2o,L′31乃至L′3oも上
記励磁コイルL′11乃至L′1oと同様に接続されそれ
ぞれの出力変成器52,53によつて励磁され
る。
The other excitation coils L' 21 to L' 2o and L' 31 to L' 3o are connected in the same manner as the excitation coils L' 11 to L' 1o , and are excited by the respective output transformers 52 and 53.

(考案の効果) この考案は上記説明のように、接地電流を流す
ことなく送信電流を各々の励磁コイルに導くこと
ができる。
(Effects of the invention) As explained above, this invention can lead the transmission current to each excitation coil without flowing a ground current.

従つて、接地電流によつて各振動子に相互誘導
を生じさせることなく送受信を行うことができる
から、送受波器の送受信特性を向上させることが
できる。又、接地電流による電触を防止すること
ができる。
Therefore, transmission and reception can be performed without causing mutual induction in each vibrator due to the ground current, so that the transmission and reception characteristics of the transducer can be improved. Further, electrical contact due to ground current can be prevented.

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

第1図は従来装置の動作を説明するための図、
第2図は超音波送受波器の一例を示す図、第3図
はこの考案の原理を説明するための図、第4図は
この考案の実施例を示す。
FIG. 1 is a diagram for explaining the operation of a conventional device.
FIG. 2 is a diagram showing an example of an ultrasonic transducer, FIG. 3 is a diagram for explaining the principle of this invention, and FIG. 4 is a diagram showing an embodiment of this invention.

Claims (1)

【実用新案登録請求の範囲】 円又は円弧上にほぼ等間隔に配列される第1乃
至第nの偶数個の磁歪振動子で構成される振動子
群を複数個、隣接する振動子群間がほぼ等間隔に
なるように複数層に積層して得られる円筒又は半
円筒形状の超音波送受波器のそれぞれの振動子群
に属する全ての振動子をそれぞれ同時に励振して
水中に超音波パルスを送波し、各磁歪振動子によ
り補捉される受信信号を別個に取り出す水中探知
用超音波受信器において、 上記複数層のそれぞれの層の第1乃至第nの磁
歪振動子のうち奇数番目振動子の励磁コイルに対
して偶数番目振動子の励磁コイルを逆方向に巻回
し、 奇数番目振動子の各励磁コイルの終端(始端)
を共通接続すると共に、偶数番目振動子の終端
(始端)を共通接続し、 上記共通接続部を上記超音波送受波器の筐体に
接地すると共に、上記各層の第1乃至第nの磁歪
振動子の励磁コイルの上記共通接続されていない
端を送受信切替回路を経て励振電源又はその一の
入力端子を船体に接地される受信器に導くように
したことを特徴とする水中探知用超音波送受信
器。
[Claims for Utility Model Registration] A plurality of vibrator groups each consisting of an even number of first to n-th magnetostrictive vibrators arranged at approximately equal intervals on a circle or an arc, with distance between adjacent vibrator groups. All the transducers belonging to each transducer group of a cylindrical or semi-cylindrical ultrasonic transducer obtained by laminating multiple layers at approximately equal intervals are simultaneously excited to emit ultrasonic pulses into the water. In an ultrasonic receiver for underwater detection that transmits waves and separately extracts received signals captured by each magnetostrictive vibrator, an odd-numbered vibration of the first to n-th magnetostrictive vibrators in each of the plurality of layers is used. The excitation coil of the even-numbered vibrator is wound in the opposite direction to the excitation coil of the child, and the end (starting end) of each excitation coil of the odd-numbered vibrator is wound.
At the same time, the terminal ends (starting ends) of the even-numbered transducers are commonly connected, and the common connection part is grounded to the casing of the ultrasonic transducer, and the first to nth magnetostrictive vibrations of each layer are connected in common. Ultrasonic transmitter/receiver for underwater detection, characterized in that the ends of the excitation coils that are not commonly connected are guided through a transmitter/receiver switching circuit to an excitation power source or one input terminal thereof to a receiver grounded to the hull. vessel.
JP1989018076U 1989-02-17 1989-02-17 Expired JPH0439589Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1989018076U JPH0439589Y2 (en) 1989-02-17 1989-02-17

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1989018076U JPH0439589Y2 (en) 1989-02-17 1989-02-17

Publications (2)

Publication Number Publication Date
JPH01132987U JPH01132987U (en) 1989-09-11
JPH0439589Y2 true JPH0439589Y2 (en) 1992-09-16

Family

ID=31232394

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1989018076U Expired JPH0439589Y2 (en) 1989-02-17 1989-02-17

Country Status (1)

Country Link
JP (1) JPH0439589Y2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55149593A (en) * 1979-04-20 1980-11-20 Furuno Electric Co Ltd Transmitting and receiving unit of ultrasonic wave
JPS5625080A (en) * 1979-08-06 1981-03-10 Toshiba Corp Package type generator equipment

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55149593A (en) * 1979-04-20 1980-11-20 Furuno Electric Co Ltd Transmitting and receiving unit of ultrasonic wave
JPS5625080A (en) * 1979-08-06 1981-03-10 Toshiba Corp Package type generator equipment

Also Published As

Publication number Publication date
JPH01132987U (en) 1989-09-11

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