JPS59226377A - Progressive wave generator - Google Patents
Progressive wave generatorInfo
- Publication number
- JPS59226377A JPS59226377A JP10070883A JP10070883A JPS59226377A JP S59226377 A JPS59226377 A JP S59226377A JP 10070883 A JP10070883 A JP 10070883A JP 10070883 A JP10070883 A JP 10070883A JP S59226377 A JPS59226377 A JP S59226377A
- Authority
- JP
- Japan
- Prior art keywords
- spherical
- damper
- wave
- waves
- wave generator
- 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.)
- Granted
Links
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
本発明はつる巻ばねと球状重@号を用いた波動実験装置
を改良し、進行波の生成を可能にしたものである。従来
つる巻ばねと球状重錘を用いた波動実験装置では、進行
波の生成が出来なかった。DETAILED DESCRIPTION OF THE INVENTION The present invention improves a wave experiment device using a helical spring and a spherical gravity beam, thereby making it possible to generate traveling waves. Conventional wave experiment devices using helical springs and spherical weights have not been able to generate traveling waves.
本発明は一直勝上に等間隔に配列された球状重錘1を、
その直径よりもやや直径の小さな伸張されたつる巻ばね
2の綿線間にそう人して綿線の弾力によって両側から締
めつけてがん着し、つる巻ばね2の軸心方向を水平とし
た波動実験装置に於て。The present invention uses spherical weights 1 arranged at equal intervals on a straight line,
Place a person between the cotton wires of the stretched helical spring 2, which has a diameter slightly smaller than that diameter, and tighten it from both sides using the elasticity of the cotton wires, so that the axial direction of the helical spring 2 is horizontal. In the wave experiment equipment.
その一端より数個の球状重錘1の下部に球状の制振子3
を取付け、これを粘性の大きな液中にひたし1割振度を
端より段階的に減する様にした進行波生成装置である。A spherical damper 3 is attached to the bottom of several spherical weights 1 from one end.
This is a traveling wave generating device in which a 100% oscillator is attached and immersed in a highly viscous liquid, and the degree of oscillation is gradually reduced from the end.
今割振装置の取付けられた一端の反対側の端の球状重錘
にパルス波を与えると。Now apply a pulse wave to the spherical weight at the opposite end of the attached end of the allocator.
波動は制振子に吸収されて反射波はなく、連続的な単振
動を与えると正弦波形の進行波が生成される。この場合
制振子3の割振1隻が端に向って段階的に強くなる様に
構成したことが重要で+ tlill振子3の制振度を
ほぼ等しくするときは、(夜の粘性又は液中の制振子3
0体積を少しずつ変えても、パルス波に対する反射波の
生T1+y、はさけられない。すなわち制低度が弱いと
きも強いときも反射波が生成され、その中間の反射波の
ない状態が作れないのである。今一実施例をあげると、
鉛製球状重錘の質量402直径18胴9球状重錘IWj
の距離40crn球状1(錘を紐で一本つりとし、その
長さ600m球状車錘の重重5個、(11径03間のピ
アノ線製つる巻ばねの綿線の直径16咽で1球状重錘間
の綿線の巻数8(球状重錘をがん着する2巻を除く)。The wave is absorbed by the damper and there is no reflected wave, and when continuous simple harmonic motion is applied, a traveling wave with a sinusoidal waveform is generated. In this case, it is important that the damping force of the damper 3 is configured so that it becomes stronger stepwise toward the end.When the damping degree of the damping pendulum 3 is made almost equal, (viscosity at night or Dampener 3
Even if the zero volume is changed little by little, the reflection wave T1+y of the pulse wave cannot be avoided. In other words, reflected waves are generated both when the control level is weak and strong, and it is impossible to create a state in which there are no reflected waves in between. To give an example,
Mass of lead spherical weight 402 Diameter 18 Body 9 Spherical weight IWj
Distance: 40 crn Spherical 1 (The weight is suspended by a string, and its length is 600 m.) 5 weights of spherical wheel weights, The number of turns of cotton wire between the weights is 8 (excluding the 2 turns that securely attach the spherical weight).
球状制振子の直径2 (l mm +制振子の数4個で
ある。The diameter of the spherical damper is 2 (l mm + the number of dampers is 4).
粘性の大きな液としては、水治水ガラス潤滑油などが適
当である。液の粘性は気温によって異なるので、第3図
に示す減衰曲線は大体適当な値であり、この様に液の粘
性及び液中のtlill振子の体積を;a整する。液の
粘性が強すき′るとき(l−1,Y閏滑油は石油でうす
め9弱いときけワセリンをとかす。水飴水ガラスは水で
うすめたり煮つめたりする。液中にある1lill振子
の体積を変えるには9球状重錘との間隔を球状重錘と制
振子をつなぐねじで変えてもよ(、つるす紐の長さで調
整してもよく、そのためばねの1lqll心が多少変わ
っても差支えない。この様に調整してパルス波に対する
反射波のない状態を作り1割振装置のない端の球状重錘
につる巻ばねの軸心方向、これと直角な方向に連続的な
単振動を与えると、それぞれ連続的な縦波横波の進行波
が得られる。又単振動でなく連続的な円運動を与えると
9割振装置のない場合のパルス波と異なり各振子ともよ
く円運動をし9表面波相当の波動が得られる。As the highly viscous liquid, water control water glass lubricating oil or the like is suitable. Since the viscosity of the liquid varies depending on the temperature, the attenuation curve shown in FIG. 3 is approximately an appropriate value, and in this way the viscosity of the liquid and the volume of the trill pendulum in the liquid are adjusted. When the viscosity of the liquid is strong (l-1, Y), dilute the lubricant oil with petroleum and dissolve the vaseline when it is weak. Dilute or boil the water syrup with water. The volume of a 1 liter pendulum in the liquid. To change the distance between the spherical weight and the damper, you can change the distance between the spherical weight and the damper using the screw that connects the spherical weight and the damper. No problem. Adjust in this way to create a state in which there is no reflected wave for the pulse wave, and apply continuous simple harmonic motion to the spherical weight at the end without the oscillation device in the direction of the axis of the helical spring and in the direction perpendicular to this. When given, continuous traveling waves of longitudinal waves and transverse waves are obtained.Also, when continuous circular motion is given instead of simple harmonic motion, each pendulum moves well in a circular motion, unlike the pulse wave when there is no oscillation device. Waves equivalent to surface waves can be obtained.
本発明の効果は、1)制振子の制振朋を端より段階的に
減することにより、パルス波に対する反射波をなくする
ことが出来る。2)連続的な111振動を制振子のある
端と反対の端から力え、正弦波形の進行波が生成される
。3)制振子が球状であるため。The effects of the present invention are as follows: 1) By gradually reducing the damping force of the damper from the end, reflected waves for pulse waves can be eliminated. 2) Continuous 111 vibrations are applied from one end of the damper and the other end to generate a traveling wave in the form of a sine wave. 3) Because the damper is spherical.
液から受ける抵抗力が方向によらず均一であり。The resistance force received from the liquid is uniform regardless of direction.
円滑な割振が出来る。4)一本づりでけ硝:波横波表囲
波相当の波が、調整を変えずに生成出来る。Smooth allocation is possible. 4) Single-stranded glass: Waves equivalent to transverse waves and surface waves can be generated without changing the adjustment.
比較例として固体摩擦による減衰装置を述べると、他の
条件を上記実施例と同じにし+ jlill掘子たけ球
状のスポンジとし、端よりl1lI(次とれが摩擦する
床面との間の減衰度を減じたものを作ると、大体パルス
波に対する反射波のない状態が作れるが一周整がむずか
しく、一本づりで1l−j:!till 4Xi子の−
Hの球状重錘及び紐に小振動が入ってくる。As a comparative example, a damping device using solid friction is described.The other conditions are the same as in the above example, and a spherical sponge is used. If you create a reduced version, you can create a state where there is no reflected wave for the pulse wave, but it is difficult to adjust the cycle, and with one line, 1l-j:!till 4Xi child's -
A small vibration enters H's spherical weight and string.
第1図は本発明の一実施例を示す立面図、第2図は割振
装(6,の部分の拡犬立曲図、第3図は各制振子の適当
な制振jWを不す減衰曲線の一例である。
■・・・・・・球状重錘、2・・・・・・っる巻ばね、
3 ・・・・球状の制振子、4・・・°液槽
引用文献
特 公昭35−7932Fig. 1 is an elevational view showing one embodiment of the present invention, Fig. 2 is an enlarged elevational view of the allocation device (6), and Fig. 3 is an elevation view showing an appropriate damping jW of each damper. This is an example of a damping curve. ■... Spherical weight, 2... Round coil spring,
3... Spherical vibration damper, 4...°Liquid tank cited literature special publication 1977-7932
Claims (1)
りもやや泊耗の小さな伸張されたつる巻ばね2の螺勝間
にそう人して綿線の弾力によって両側から締めつけてが
ん涜し、つる巻ばね2の軸心方向を水平とした波4■b
実験装置に於て、その一端より数個の球状型eIFの下
部に球状の制振子3を取付け、これを粘性の大きな液中
にひだし、制振吸を端より段階的に減する様にした進行
波生成装置。Spherical weights 1 arranged at equal intervals are placed between the threaded ends of stretched helical springs 2 whose wear is slightly smaller than their diameters, and tightened from both sides by the elasticity of the cotton wire. A wave 4b with the axial direction of the helical spring 2 horizontal
In the experimental apparatus, a spherical damper 3 was attached to the bottom of several spherical eIFs from one end, and this was swung into a highly viscous liquid, so that the damping and absorption was gradually reduced from the end. traveling wave generator.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10070883A JPS59226377A (en) | 1983-06-08 | 1983-06-08 | Progressive wave generator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP10070883A JPS59226377A (en) | 1983-06-08 | 1983-06-08 | Progressive wave generator |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS59226377A true JPS59226377A (en) | 1984-12-19 |
JPS6332386B2 JPS6332386B2 (en) | 1988-06-29 |
Family
ID=14281176
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP10070883A Granted JPS59226377A (en) | 1983-06-08 | 1983-06-08 | Progressive wave generator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59226377A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR101283640B1 (en) * | 2012-09-26 | 2013-07-08 | 주식회사 디브이씨 | A wave motion |
-
1983
- 1983-06-08 JP JP10070883A patent/JPS59226377A/en active Granted
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR101283640B1 (en) * | 2012-09-26 | 2013-07-08 | 주식회사 디브이씨 | A wave motion |
Also Published As
Publication number | Publication date |
---|---|
JPS6332386B2 (en) | 1988-06-29 |
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