JPS5850478B2 - Chiyo Onpahon - Google Patents
Chiyo OnpahonInfo
- Publication number
- JPS5850478B2 JPS5850478B2 JP50127133A JP12713375A JPS5850478B2 JP S5850478 B2 JPS5850478 B2 JP S5850478B2 JP 50127133 A JP50127133 A JP 50127133A JP 12713375 A JP12713375 A JP 12713375A JP S5850478 B2 JPS5850478 B2 JP S5850478B2
- Authority
- JP
- Japan
- Prior art keywords
- horn
- throat
- diameter
- axis direction
- sound pressure
- 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
- 239000013078 crystal Substances 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
Landscapes
- Transducers For Ultrasonic Waves (AREA)
Description
【発明の詳細な説明】
従来の超音波ホーンは、第1図イの如く、喉部aから開
口部すに向うにつれ漸次口径が拡大して口径がほぼ楕円
であるホーンCの喉部a内に超音波発生源dを収納装着
してなり、ホーンCの口径の長軸方向の指向特性(即ち
、ホーンCの中心軸に対してホーンの喉部aにおいてホ
ーンの口径の長軸方向にα度の角度をなして交叉する線
分方向の音圧Hhと上記α度との関係)を実測すると、
第1図ハの如く、α度の絶対値の一定以下で音圧Hhは
大きくてα度の絶対値が上記一定値以上では音圧Hhが
小さくなるが、ホーンCのロ径ノ短軸方向の指向特性(
即ち、ホーンCの中心軸に対してホーンCの喉部a内に
おいてホーンの口径の短軸方向にβ度の角度をなして交
叉する線分方向の音圧Hvと上記β度の関係)を実測す
ると、第1図二の如く、β度の絶対値が一定値以上のと
き音圧Hvが大きくβ度の絶対値が上記一定値以上にお
いても音圧HVがβ度の絶対値の増加とともに大きく増
減し、ホーンCの口径の短軸方向の指向特性が乱れる欠
点があった。DETAILED DESCRIPTION OF THE INVENTION As shown in FIG. 1A, the conventional ultrasonic horn has a diameter that gradually increases from the throat a to the opening, and the diameter is approximately elliptical within the throat a of the horn C. The ultrasonic generation source d is housed and attached to the diaphragm, and the directivity characteristic is α in the longitudinal direction of the aperture of the horn C at the throat a of the horn with respect to the central axis of the horn C. When the relationship between the sound pressure Hh in the direction of line segments that intersect at a degree angle and the above α degree is actually measured,
As shown in FIG. The directional characteristic of (
That is, the relationship between the sound pressure Hv in a line segment that intersects the central axis of the horn C with an angle of β degrees in the short axis direction of the horn diameter in the throat a of the horn C and the above β degrees). When actually measured, as shown in Figure 1, 2, when the absolute value of β degree is above a certain value, the sound pressure Hv is large, and even when the absolute value of β degree is above the above fixed value, the sound pressure HV increases as the absolute value of β degree increases. There was a drawback that the directivity characteristics in the short axis direction of the aperture of the horn C were disturbed due to large increases and decreases.
本発明は上記のような従来の欠点を除去するものであっ
て、以下本発明の実施例を図面について説明すると、1
は喉部2から開口部3に向うにつれ漸次口径が拡大して
口径がほぼ楕円であるホーン、4は超音波発生源で、圧
電気結晶片に一対の電極を適当に装着してなり、一対の
電極間に高周波電圧を印加すると、圧電気結晶片は高周
波電圧に共振して弾性振動して超音波を発生する。The present invention eliminates the above-mentioned drawbacks of the conventional technology, and the embodiments of the present invention will be described below with reference to the drawings.
4 is a horn whose aperture gradually increases from the throat 2 toward the opening 3 and has an almost elliptical aperture; 4 is an ultrasonic wave generator, which is made up of a piezoelectric crystal piece with a pair of electrodes suitably attached thereto; When a high-frequency voltage is applied between the electrodes, the piezoelectric crystal piece resonates with the high-frequency voltage, vibrates elastically, and generates ultrasonic waves.
超音波発生源4はホーン1の喉部2内に配設される。An ultrasonic wave source 4 is disposed within the throat 2 of the horn 1 .
5は中心にほぼ楕円の孔6を有する板体で、超音波発生
源4の前方のホーン1の喉部2内に設げられ、孔6の長
軸方向はホーン1の口径の長軸方向と直交するようにな
されるものである。Reference numeral 5 denotes a plate having a substantially elliptical hole 6 in the center, which is provided in the throat 2 of the horn 1 in front of the ultrasonic wave generation source 4, and the long axis direction of the hole 6 is the long axis direction of the aperture of the horn 1. This is done perpendicularly to the
本発明は上記のような構成で、ホーン1の長軸方向の指
向特性(即ち、ホーン1の中心軸に対してホーン1の喉
部2においてホーン1の長軸方向にα度の角度をなして
交叉する線分方向の音圧Hhと上記α度との関係)を実
測すると、第5図の如く、α度の絶対値が一定値以下で
音圧Hhは大きくてα度の絶対値が上記一定値以上では
音圧Hhが小さくなって従来と同様であるが、ホーン1
の口径の短軸方向の指向特性(即ち、ホーン1の中心軸
に対してホーン1の喉部においてホーン10口径の短軸
方向にβ度をなして交叉する線分方向の音圧Hvと上記
β度の関係)を実測すると、第6図の如くβ度の絶対値
が一定値以下のとき音圧Hvは大きくβ度の絶対値が上
記一定値以上のとき音圧Hvは小さくなり、ホーン10
口径の短軸方向の指向特性の乱れが少なくなるものであ
る。The present invention has the above-described configuration, and has a directivity characteristic in the long axis direction of the horn 1 (that is, an angle of α degree is formed in the throat part 2 of the horn 1 in the long axis direction of the horn 1 with respect to the central axis of the horn 1). When we actually measure the relationship between the sound pressure Hh in the intersecting line segment direction and the above α degrees, we find that when the absolute value of α degrees is below a certain value, the sound pressure Hh is large and the absolute value of α degrees is Above the above certain value, the sound pressure Hh decreases and is the same as before, but the horn 1
(i.e., the sound pressure Hv in the direction of a line that intersects the short axis direction of the horn 10 diameter at an angle of β at the throat of the horn 1 with respect to the central axis of the horn 1, and the above As shown in Figure 6, when the absolute value of the β degree is below a certain value, the sound pressure Hv is large, and when the absolute value of the β degree is above the above certain value, the sound pressure Hv is small. 10
Disturbance in the directivity characteristics in the direction of the short axis of the aperture is reduced.
かように本発明は、喉部2から開口部3に向うにつれ漸
次口径が拡大して口径がほぼ楕円であるホーン1の喉部
2内に超音波発生源4を配設し、中心にほぼ楕円の孔6
を有する板体5を超音波発生源4の前方のホーン1の喉
部2内に設けて孔6の長軸方向をホーン10口径の長軸
方向に直交してなるものであるから、ホーンの口径の短
軸方向の指向特性が実測の結果乱れないようになる効果
があるものである。Thus, in the present invention, the ultrasonic wave generation source 4 is disposed within the throat 2 of the horn 1, which has an approximately elliptical diameter that gradually increases in diameter from the throat 2 toward the opening 3. Oval hole 6
A plate body 5 having a diameter is provided in the throat part 2 of the horn 1 in front of the ultrasonic wave generation source 4, and the long axis direction of the hole 6 is perpendicular to the long axis direction of the diameter of the horn 10. This has the effect of preventing the directivity characteristics in the short axis direction of the aperture from being disturbed as a result of actual measurements.
第1図は従来の超音波ホーンを示すもので、第1図イは
断面図、第1図中ま同上のX−X線における断面図、第
1図ハ、二は指向特性図である。
第2図乃至第6図は本発明の実施例を示すもので、第2
図は正面図、第3図は同上のY−Y線における断面図、
第4図は同上のZ−Z線における断面図、第6図及第6
図は指向特性図である。
1はホーン、2は喉部、3は開口部、4は超音波発生源
、5は板体、6は孔である。FIG. 1 shows a conventional ultrasonic horn, in which FIG. 1A is a sectional view, FIG. 2 to 6 show embodiments of the present invention.
The figure is a front view, and Figure 3 is a sectional view taken along the Y-Y line of the same as above.
Figure 4 is a cross-sectional view taken along the Z-Z line as above, Figures 6 and 6.
The figure is a directional characteristic diagram. 1 is a horn, 2 is a throat, 3 is an opening, 4 is an ultrasonic generation source, 5 is a plate, and 6 is a hole.
Claims (1)
て口径がほぼ楕円であるホーン1の喉部2内に超音波発
生源4を配設し、中心にほぼ楕円の孔6を有する板体5
を超音波発生源4の前方のホーン1の喉部2内に設けて
孔6の長軸方向をホーン10口径の長軸方向に直交して
なる超音波ホーン。1 An ultrasonic generation source 4 is disposed within the throat 2 of the horn 1, which gradually increases in diameter from the throat 2 toward the opening 3 and has an approximately elliptical diameter, and has an approximately elliptical hole 6 in the center. Plate body 5
is provided in the throat part 2 of the horn 1 in front of the ultrasonic wave generation source 4, and the long axis direction of the hole 6 is perpendicular to the long axis direction of the diameter of the horn 10.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50127133A JPS5850478B2 (en) | 1975-10-21 | 1975-10-21 | Chiyo Onpahon |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP50127133A JPS5850478B2 (en) | 1975-10-21 | 1975-10-21 | Chiyo Onpahon |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5250714A JPS5250714A (en) | 1977-04-23 |
| JPS5850478B2 true JPS5850478B2 (en) | 1983-11-10 |
Family
ID=14952420
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP50127133A Expired JPS5850478B2 (en) | 1975-10-21 | 1975-10-21 | Chiyo Onpahon |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5850478B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0430486U (en) * | 1990-07-05 | 1992-03-11 |
-
1975
- 1975-10-21 JP JP50127133A patent/JPS5850478B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5250714A (en) | 1977-04-23 |
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