US3696259A - Device for distributing vibratory energy - Google Patents

Device for distributing vibratory energy Download PDF

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Publication number
US3696259A
US3696259A US86928A US3696259DA US3696259A US 3696259 A US3696259 A US 3696259A US 86928 A US86928 A US 86928A US 3696259D A US3696259D A US 3696259DA US 3696259 A US3696259 A US 3696259A
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Prior art keywords
transmission element
input
flange
transducers
displacement
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US86928A
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English (en)
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Eiji Mori
Katsuhiko Ito
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Panasonic Holdings Corp
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Individual
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    • BPERFORMING OPERATIONS; TRANSPORTING
    • B06GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS IN GENERAL
    • B06BMETHODS OR APPARATUS FOR GENERATING OR TRANSMITTING MECHANICAL VIBRATIONS OF INFRASONIC, SONIC, OR ULTRASONIC FREQUENCY, e.g. FOR PERFORMING MECHANICAL WORK IN GENERAL
    • B06B3/00Methods or apparatus specially adapted for transmitting mechanical vibrations of infrasonic, sonic, or ultrasonic frequency
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04RLOUDSPEAKERS, MICROPHONES, GRAMOPHONE PICK-UPS OR LIKE ACOUSTIC ELECTROMECHANICAL TRANSDUCERS; DEAF-AID SETS; PUBLIC ADDRESS SYSTEMS
    • H04R17/00Piezoelectric transducers; Electrostrictive transducers
    • H04R17/04Gramophone pick-ups using a stylus; Recorders using a stylus
    • H04R17/08Gramophone pick-ups using a stylus; Recorders using a stylus signals being recorded or played back by vibration of a stylus in two orthogonal directions simultaneously

Definitions

  • This invention relates to devices for distributing vibratory energy of the type having longitudinal vibrations, and more particularly to a device for distributing vibratory energy from one or more transducers or for combining energy from a plurality of transducers.
  • the direction of propagation of the vibrational energy is turned through substantially 90 at the junction.
  • the effect can be applied, not only to change the direction of propagation, but also to distribute the energy from a single transducer, or a number of transducers, to a number of positions (or even uniformly around the circular boundary of a flange-like element), or to combine the energy from a number of transducers and feed it to one or more positions.
  • any element connected by an intermediate portion thereof should be formed so that the junction is at a displacement node for longitudinal vibrations in the parts of the element separated thereby.
  • FIG. 1 is a cross sectional view of an electro-acoustical transducer coupled to a transmission element
  • FIG. 2 is an elevation view of a device according to the invention for distributing vibratory energy around the periphery of a circular flange provided as the second of the transmission elements;
  • FIG. 3 is a plan view of the device of FIG. 2;
  • FIGS. 4 and 5 show two further devices in perspective
  • FIG. 6 is an elevation of a device for combining the energy from a set of transducers
  • FIG. 7 is a plan view of the device of FIG. 6;
  • FIGS. 8 and 9 are perspective views of two further devices for combining the energy from a set of transducers
  • FIG. 10 is a perspective view showing the transmission elements of one form of the device according to the invention.
  • FIG. 13 shows a correlation between two vibratory displacements at an entrance end-face and an exit endface of the device of FIG. 12;
  • FIG. 14 is an elevation view of the elements of a device which is a modification of that shown in FIG. 6;
  • FIG. 15 is an end elevation view of the elements of FIG. 14 with transducers added thereto;
  • FIG. 16 is a graph illustrating a correlation between two vibratory displacements at one entrance end-face and one exit end-face of the device shown in FIG. 14;
  • FIG. 17 illustrates a test set-up for the device for FIG. 14.
  • FIG. 18 is a graph illustrating the correlation between input power and output vibration.
  • electro-acoustical transducers especially magnetostrictive and electro-strictive transducers, may be employed in the device of the present invention.
  • a preferred form of transducer has been developed and is shown in FIG. 1. It gives an adequate level of acoustical energy and is stable in operation.
  • the transducer 1 consists of metallic supporting members 2 and 3 and a vibrator of the electro-stn'ctive type sandwiched between the two members. The parts are joined together by a threaded bolt 5 which passes through the vibrator and gives the transducer adequate stability and strength. A satisfactory mounting of the transducer upon a transmission element 6 is obtainable by a double-ended bolt 7, as is shown in FIG. 1.
  • the transducer should be as small as possible for the power handled thereby.
  • an aluminium-base alloy having relatively low density such as duralumin
  • lead zirconate titanate is used as the electrostrictive type material in the vibrator, or transducer 4.
  • a multilayer construction is recommended for the transducer 4.
  • the transducer 4 shown in FIG. 1 is composed of four layers of electrostrictive material.
  • the transducer may be activated by a power supply of appropriate frequency (not shown) fed in at the terminals 8 and 9. All of the devices to be described hereinafter may incorporate a transducer or transducers according to FIG. 1.
  • the specification of a convenient transducer is as follows:
  • Electrostrictive vibrator or transducer Material lead zirconate titanate Size: diameter 40 mm thickness 5 mm Arrangement: four layers total thickness mm Supporting Members Material: duralumin Diameter: 40 mm Length: resonance length of 20 kHz, viz.,
  • transducer assembly is shown in FIG. 1, and has a total overall length of 120 mm.
  • the power input of this transducer may be up to 300 watts. If the intended frequency of operation is different from 20 kHz the above-mentioned dimensions must, of course, be changed. The re-designing is readily achieved in accordance with known techniques.
  • FIG. 11 The results of a practical experiment are shown in FIG. 11.
  • the vibration from the transducer is transmitted to the output end-faces by means of resonance.
  • the vibration amplitude at each of the output faces is substantially equal to the input amplitude, and the output energy at each of the output faces is about one third of the input vibrational energy.
  • the input energy is diverged in three directions in the embodiment of FIG. 10.
  • the device'of FIG. 4 is a modification of that of FIG. 10 and has a third transmission element perpendicular to the other two.
  • Energy from the transducer 1 is distributed in four different directions at right angles to its original direction to pass along transmission elements located at a distance of one-quarter wavelength from the junction between the transducer 1 and transmission element 12.
  • Vibratory energy is received at each of the end-faces 13, 14, 15 and 16 which are one-quarter wavelength from the center of the structure. If the above end-faces are correctly loaded, the vibratory energy from the one simple transducer may be utilized at each of them.
  • the divergent structure is potentially useful in many fields of industry.
  • FIG. 9 shows transducers l fixed to end-faces corresponding to end'faces 13, l4, l5 and 16 of FIG. 4 and the energy from these transducers is discharged from one end-face of the element 26, while the other end-face of the element 26 is fitted with a reflection plate 22 for the frequency concerned.
  • the total vibratory energy discharged from the end-face of element 26 is about four times that generated by a single transducer.
  • Such a convergence device may be utilized for industrial applications requiring large amounts of vibratory energy to be applied at a single position-
  • FIG. 12 there is shown another form of divergence structure consisting of a rod-shaped transmission element and a circular flange. This fiangeis located at a distance of one quarter wavelength from one end-face of the rod-shaped element and is at about right angles thereto.
  • the vibratory energy is discharged radially from the peripheral face R of the flange.
  • the radius of said flange may be calculated from the following equation.
  • Input Power 20 watts The vibratory energy from the transducer, which is fixed to face L or L, is shifted through 90 at the junction of the rod and flange which is one-quarter wavelength long from the transducer, and is then radially diverged from face R.
  • the vibration of output face R has less amplitude than that of input face L under these no load conditions. This is a characteristic of this embodiment.
  • FIGS. 2 and 3 vibratory energy transmitted from a transducer 1 to a rod-shaped transmission element is radially diverged from a circular flange l1 placed at a distance of one-quarter wavelength from the transducer.
  • FIG. 5 shows an extension of the principle.
  • the device of FIG. 5 has three flanges 18, 19 and 20 on a transmission rod 17. The flanges are spaced one-half wavelength apart and the distance between each end-face of the rod 17 and the neighboring flange is one-quarter wavelength.
  • the power from the transducer 1 is diverged to the peripheries of the three flanges.
  • a flange can be used for convergence instead of divergence of the vibratory energy.
  • the flange of FIG. 12 is given a regular polygonal periphery and the transducer is fixed to one flat peripheral face of the flange, the correlation between the vibration amplitude of the driven face and that of the discharge face is similar to that shown in FIG. 13. If transducers are placed on several flat peripheral sides of the flange, the energy from the transducers converges to the ends-of the rod element. Under no load conditions in an ideal case without losses, energy which is about equal to the total energy from the transducers, is discharged at 90 to its original directions at the output face.
  • the device of FIGS. 6 and 7 has a flange of regular octagonal shape.
  • a transducer is fixed to every alternate side of the flange shown in FIG. 7.
  • the vibratory energy from the four transducers is converged into the flange and then is discharged from one end-face of transmission element 21 after a change of direction.
  • the discharged energy is about four times that given by a single transducer and is about equal to the combined energy given by the four transducers.
  • the end-face of said transmission rod 21 is fitted with a reflection plate 22 as is shown in FIG. 9.
  • a reflection plate 22 as is shown in FIG. 9.
  • the device of FIG. 8 is a modification of that of FIGS. 6 and 7.
  • a circular flange is positioned onehalf wavelength from the octagonal flange 24.
  • the vibratory energy converged into the regular octagonal flange 24 is turned through 90 along transmission rod 23, and is then, after being shifted through 90 by circular flange 25, diverged radially.
  • the dimensions of the flange 25 are chosen as hereinbefore described.
  • FIG. 14 there is shown a structure suitable for obtaining a high output power for use in heavy industry.
  • This transmission body is made up of a rod-shaped transmission element 33 having a resonant length at the operating frequency.
  • Two supports 32 and 40 are located one-quarter wavelength from each end-face of the rod 33, and two flanges, and 31, of regular l2- sides polygonal periphery are spaced one-half wavelength apart and one-half wavelength from the supporters 40 and 32, respectively.
  • Twelve transducers are fixed to each flange by holes such as the holes 34, 35, 36, 37, 38 and 39.
  • the dimensions and operating conditions are as follows:
  • each of supporters 32 and 40 is the form of a small circular flange.
  • the dimensions of these flanges are made as small as possible since they lie on the length of a transmission element. Typically they may be about 8 mm in both width and height. It will be observed that they are positioned at displacement nodes in order to minimize disturbance of the operation of the device and that they are deliberately made non-resonant.
  • the correlation between the vibration amplitude at input face R and that of output face L, under no load conditions, is as shown in FIG. 16, it is seen that the ratio of output vibration amplitude to input vibration amplitude is more than 3 to I. This ratio is of particular importance for the purpose of most efficient utilization of the vibration energy.
  • the device of FIG. 14 facilitates synthesis of vibration energy by means of resonance vibration based upon the relation between the transducers and the transmission element. Both in input and output, the following equation applies:
  • the output vibration amplitude grows together with output vibration energy, which inturn, grows together with input vibration energy.
  • the ratio of output vibration amplitude to input vibration amplitude is about 3 to 1. This has been verified by actual no load tests, the results of which are shown in FIG. 16.
  • an output power of about 4,800 watts can theoretically be obtained with an input power of about 200 watts per transducer. In actual practice, however, the full theoretical output of 4,800 watts will not be obtained due to losses, etc. If the number of the flanges is increased, an even greater output can be obtained.
  • FIG. 18 An actual no load test was carried out to show the relationship between input power and output vibration amplitude and the results are shown in FIG. 18.
  • the device of FIG. 14 shown generally by 30, 31, 33
  • the plug 41 is connected to face L via an intermediary element 43.
  • the output vibration amplitude was measured as the input power to the transducers on flanges 30 and 31 was set at 80, 160, 200 and 240 volts.
  • the amplitudes were measured with a pickup 44 and the results thereof indicated by mV.
  • FIG. 18 shows the output with input energy supplied to transducers on each flange 30 and 31. An actual no load efficiency of about 85 percent was obtained.
  • the devices of the present invention may, of course, utilize tubular transmission elements in place of the solid elements described above.
  • the electro-strictive material lead zirconate titanate
  • a transducer component in the foregoing description.
  • Other materials which can be used are, for example, magnetrostrictive or piezoelectric materials such as Ferrite, nickel, nickel-iron alloy, crystals, barium titanate and the like.
  • a device for transmitting virbratory energy comprising:
  • At least one input transmission element and an output transmission element said at least one input transmission element being joined to said output transmission element with said at least one input transmission element substantially perpendicular to said output transmission element;
  • At least two input vibration transducers producing longitudinal vibrations of the same frequency, said input vibration transducers being connected to at least one of said at least one input transmission element;
  • said transducers being positioned with respect to said at least one input transmission element to which they are connected, such that, at a vibrational frequency at which said transducers are operable a displacement node of a standing wave is formed at a junction of said transmission elements, and such that, said output transmission element has said frequency as a standing wave frequency for which there is a displacement node at said junction and a displacement antinode at an extremity of said output transmission element remote from said junction.
  • a device wherein said transmission elements are elongate in the direction of the vibrations and have a regular cross section, said atleast one input transmission element being connected to an intermediate position of said output transmission element and said output transmission element being dimensioned to have displacement antinodes at each of its ends.
  • a device including at least first and second input transmission elements, said output transmission element being connected to an intermediate portion of said first input transmission element to divide same into said two parts, said second input transmission element being connected to said first input transmission element and to said output transmission element in the vicinity of said junction therebetween, said second input transmission element being of such length that a displacement node is located at said junction and a displacement antinode is located at an extremity of said second input transmission element remote from said junction.
  • a device wherein said at least two transducers are connected with said input transmission elements at the position of a displacement antinode, said extremity of said output transmission element being located at a displacement antinode and being free to receive vibrational energy from more than one of said transducers.
  • a device further comprising a reflector, and wherein at least one of said transducers is connected to an input transmission element at a displacement antinode, at least one transmission element is connected to said reflector and has an extremity positioned at a displacement antinode and at least an output transmission element has an extremity positioned at a displacement antinode and which is free to receive vibrational energy from at least two transducers.
  • said at least one input transmission element includes a regularly polygonal flange, one of said at least two transducers being connected to respective peripheral faces of said flange, said flange being dimensioned such that the longitudinal vibrations from each transducer have a common displacement antinode at the center of said flange, said output transmission element being connected with said flange transmission element at said center.
  • said output transmission element is a bar and further comprising a second flange connected at its center to said bar, said second flange being dimensioned such that a displacement antinode is formed around its periphery.
  • said second flange has a regularly polygonal shape, each peripheral face thereof being connected to a respective transducer, all of said transducers on said flanges being operable at the same frequency.
  • a device wherein said barshaped input transmission element extends beyond said flange-shaped output transmission element and further comprising at least a second generally circular flangeshaped output transmission element connected concentrically with said extended portion of said barshaped input transmission element, said second flangeshaped output transmission element being positioned at displacement antinodes of said bar-shaped input transmission element.
  • a device for transmitting vibratory energy comprising:
  • At least one input transmission element and at least two output transmission faces on at least one output transmission element said at least one input transmission element being joined to said at least one output transmission element with said at least one input transmission element substantially perpendicular to said at least one output transmission element;
  • At least one input vibration transducer producing longitudinal vibrations said input vibration transducers being connected to at least one of said at least one input transmission element;
  • said transducers being positioned with respect to said at least one input transmission element to which they are connected, such that, at a vibrational frequency at which said transducers are operable a displacement node of a standing wave is formed at a junction of said transmission elements, and such that, said at least one output transmission element has said frequency as a standing wave frequency for which there is a displacement node at said junction and a displacement antinode at an extremity of said output transmission element remote from said junction, the input vibrations from said at least one transducer being distributed to said output transmission faces.
  • a device for transmitting vibratory energy comprising:
  • At least one elongated, generally bar-shaped, input transmission element and a generally circular flange-shaped output transmission element said at least one input transmission element being 'oined to sald flange-shaped output transmission e ement substantially centrally of said flange-shaped output transmission element with said at least one input transmission element substantially perpendicular to said flange-shaped output transmission element;
  • At least one input vibration transducer producing longitudinal vibrations said at least one input vibration transducer being connected to at least one of said at least one input transmission element;
  • said transmission elements being dimensioned, and said at least one transducer being positioned with respect to said at least one input transmission element, such that, at a vibrational frequency at which said transducers are operable a displacement node of a standing wave is formed at a junction of said transmission elements, and such that, said flange-shaped output transmission element has said frequency as a standing wave frequency for which there is a displacement node at said junction and a displacement antinode formed around the periphery of said flange-shaped output transmission element, energy from said at least one vibration transducer being distributed around said periphery.

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  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Apparatuses For Generation Of Mechanical Vibrations (AREA)
US86928A 1967-12-25 1970-11-04 Device for distributing vibratory energy Expired - Lifetime US3696259A (en)

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JP8285567 1967-12-25
JP1895468 1968-03-25

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CH (1) CH485496A (cs)
CS (1) CS153488B2 (cs)
DE (1) DE1810406C3 (cs)
FR (1) FR1599285A (cs)
GB (1) GB1242603A (cs)
NL (1) NL144499B (cs)
SE (1) SE342154B (cs)

Cited By (21)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3749947A (en) * 1971-08-28 1973-07-31 Denki Onkyo Co Ltd Switch devices
US3946829A (en) * 1973-09-17 1976-03-30 Nippon Tokushu Togyo Kabushiki Kaisha Ultrasonic device
US3999433A (en) * 1974-10-23 1976-12-28 The United States Of America As Represented By The Secretary Of The Air Force Mechanically tuned buffer rod for ultrasonic temperature sensor
US4302709A (en) * 1978-12-14 1981-11-24 Office National D'etudes Et De Recherche Aerospatiales Vibrating device with motionless frame
WO1986004737A1 (en) * 1985-02-01 1986-08-14 American Hospital Supply Corporation Ultrasonic horn assembly
EP0394958A2 (en) * 1989-04-25 1990-10-31 Idemitsu Kosan Company Limited Method of plasticizing molding material and apparatus therefor
FR2651693A1 (fr) * 1989-09-08 1991-03-15 Mecasonic Sa Dispositif pour la mise en vibration d'un element inerte a l'aide d'une tete ultrasonique accordee .
FR2669561A1 (fr) * 1990-11-22 1992-05-29 Dominique Dubruque Dispositif de pulverisation ultrasonique de fluide.
US5172020A (en) * 1990-12-18 1992-12-15 Kabushiki Kaisha Toshiba Magnetic core for AC electrical equipments
US5203362A (en) * 1986-04-07 1993-04-20 Kaijo Denki Co., Ltd. Ultrasonic oscillating device and ultrasonic washing apparatus using the same
EP0584670A1 (en) * 1992-08-28 1994-03-02 Societe Des Produits Nestle S.A. Ultrasonic cutting device
DE4238384C1 (de) * 1992-11-13 1994-05-11 Erosonic Ag Wattwil Sonotrode für ein Ultraschall-Bearbeitungsgerät
US5426341A (en) * 1992-10-21 1995-06-20 Durr Dental Gmbh & Co. Kg Sonotrode for ultrasonic machining device
US6979936B1 (en) * 1999-10-31 2005-12-27 Nanomotion Ltd. Piezoelectric motors and motor driving configurations
US20060186126A1 (en) * 2005-02-19 2006-08-24 Browne Alan L Active material node based reconfigurable structures
US20070075607A1 (en) * 2003-09-29 2007-04-05 Jiromaru Tsujino High-capacity ultrasonic composite oscillating device
FR2910825A1 (fr) * 2007-01-02 2008-07-04 Sodeva Sa Dispositif de pulverisation ultrasonique industriel.
WO2015116587A1 (en) * 2014-01-28 2015-08-06 Frito-Lay North America, Inc. Ultrasonic sonotrode for transversely aligned transducer
EP2267765A4 (en) * 2008-04-07 2016-09-14 Adwelds Corp SUPPORT DEVICE FOR A RESONATOR
JP2017504301A (ja) * 2014-01-24 2017-02-02 ヘルマン ウルトラシャルテクニーク ゲーエムベーハー ウント コー.カーゲーHerrmann Ultraschalltechnik Gmbh & Co.Kg コンバーターユニット
US10029409B2 (en) 2014-01-28 2018-07-24 Ewi, Inc. (Edison Welding Institute, Inc.) Transverse sonotrode design for ultrasonic welding

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JPS5025899B1 (cs) * 1971-02-25 1975-08-27
IT1139730B (it) * 1980-11-18 1986-09-24 Usm Corp Dispositivo a trompa per la trasmissione di vibrazioni ultrasoniche e metodo per il fissaggio della sua parte terminale
FR2500336A1 (fr) * 1981-02-23 1982-08-27 Legrand Sa Organe de transmission a interposer entre un organe menant et un organe mene, en particulier outil vibrant
FR2526335A1 (fr) * 1982-05-04 1983-11-10 Legrand Sa Organe de transmission a noyau flottant propre notamment a l'assistance ultrasonique d'un quelconque traitement, et application en particulier au compactage et au trefilage
DE102021113875A1 (de) 2021-05-28 2022-12-01 Herrmann Ultraschalltechnik Gmbh & Co. Kg Konvertereinheit mit mehreren Konverterelementen

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US2948867A (en) * 1958-11-17 1960-08-09 Oskar E Mattiat Piezoelectric ceramic resonators
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US3435250A (en) * 1967-08-18 1969-03-25 Us Army Solid state microwave acoustic delay line and frequency converter
US3546498A (en) * 1969-06-13 1970-12-08 Univ Ohio Curved sonic transmission line

Cited By (34)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3749947A (en) * 1971-08-28 1973-07-31 Denki Onkyo Co Ltd Switch devices
US3946829A (en) * 1973-09-17 1976-03-30 Nippon Tokushu Togyo Kabushiki Kaisha Ultrasonic device
US3999433A (en) * 1974-10-23 1976-12-28 The United States Of America As Represented By The Secretary Of The Air Force Mechanically tuned buffer rod for ultrasonic temperature sensor
US4302709A (en) * 1978-12-14 1981-11-24 Office National D'etudes Et De Recherche Aerospatiales Vibrating device with motionless frame
WO1986004737A1 (en) * 1985-02-01 1986-08-14 American Hospital Supply Corporation Ultrasonic horn assembly
US4607185A (en) * 1985-02-01 1986-08-19 American Hospital Supply Corporation Ultrasonic horn assembly
US5203362A (en) * 1986-04-07 1993-04-20 Kaijo Denki Co., Ltd. Ultrasonic oscillating device and ultrasonic washing apparatus using the same
EP0394958A2 (en) * 1989-04-25 1990-10-31 Idemitsu Kosan Company Limited Method of plasticizing molding material and apparatus therefor
EP0394958A3 (en) * 1989-04-25 1991-11-13 Idemitsu Kosan Company Limited Method of plasticizing molding material and apparatus therefor
FR2651693A1 (fr) * 1989-09-08 1991-03-15 Mecasonic Sa Dispositif pour la mise en vibration d'un element inerte a l'aide d'une tete ultrasonique accordee .
US5632445A (en) * 1990-11-22 1997-05-27 Dubruque; Dominique Ultrasonic fluid spraying device
WO1992009373A1 (fr) * 1990-11-22 1992-06-11 Dominique Dubruque Dispositif de pulverisation ultrasonique de fluide
FR2669561A1 (fr) * 1990-11-22 1992-05-29 Dominique Dubruque Dispositif de pulverisation ultrasonique de fluide.
US5172020A (en) * 1990-12-18 1992-12-15 Kabushiki Kaisha Toshiba Magnetic core for AC electrical equipments
EP0584670A1 (en) * 1992-08-28 1994-03-02 Societe Des Produits Nestle S.A. Ultrasonic cutting device
US5426341A (en) * 1992-10-21 1995-06-20 Durr Dental Gmbh & Co. Kg Sonotrode for ultrasonic machining device
DE4238384C1 (de) * 1992-11-13 1994-05-11 Erosonic Ag Wattwil Sonotrode für ein Ultraschall-Bearbeitungsgerät
US7199507B2 (en) 1999-10-31 2007-04-03 Nanomotion Ltd. Piezoelectric motors and motor driving configurations
US6979936B1 (en) * 1999-10-31 2005-12-27 Nanomotion Ltd. Piezoelectric motors and motor driving configurations
US20060006764A1 (en) * 1999-10-31 2006-01-12 Nanomotion Ltd. Piezoelectric motors and motor driving configurations
US20070075607A1 (en) * 2003-09-29 2007-04-05 Jiromaru Tsujino High-capacity ultrasonic composite oscillating device
US7474036B2 (en) * 2003-09-29 2009-01-06 Jiromaru Tsujino High-capacity ultrasonic composite oscillating device
US7638921B2 (en) * 2005-02-19 2009-12-29 Gm Global Technology Operations, Inc Active material node based reconfigurable structures
US20060186126A1 (en) * 2005-02-19 2006-08-24 Browne Alan L Active material node based reconfigurable structures
FR2910825A1 (fr) * 2007-01-02 2008-07-04 Sodeva Sa Dispositif de pulverisation ultrasonique industriel.
WO2008080887A1 (en) * 2007-01-02 2008-07-10 Heraeus Psp France Sas Industrial ultrasonic spraying device
TWI421129B (zh) * 2007-01-02 2014-01-01 Sodeva 工業超音波噴灑裝置
EP2267765A4 (en) * 2008-04-07 2016-09-14 Adwelds Corp SUPPORT DEVICE FOR A RESONATOR
JP2017504301A (ja) * 2014-01-24 2017-02-02 ヘルマン ウルトラシャルテクニーク ゲーエムベーハー ウント コー.カーゲーHerrmann Ultraschalltechnik Gmbh & Co.Kg コンバーターユニット
US10220413B2 (en) 2014-01-24 2019-03-05 Herrmann Ultraschalltechnik Gmbh & Co. Kg Converter unit
US9205596B2 (en) 2014-01-28 2015-12-08 Frito-Lay North America, Inc. Ultrasonic sonotrode for transversely aligned transducer
WO2015116587A1 (en) * 2014-01-28 2015-08-06 Frito-Lay North America, Inc. Ultrasonic sonotrode for transversely aligned transducer
US10029409B2 (en) 2014-01-28 2018-07-24 Ewi, Inc. (Edison Welding Institute, Inc.) Transverse sonotrode design for ultrasonic welding
US10399274B2 (en) 2014-01-28 2019-09-03 Edison Welding Institute, Inc. Method for using transverse sonotrode in ultrasonic welding

Also Published As

Publication number Publication date
NL6817811A (cs) 1969-06-27
DE1810406B2 (de) 1973-08-16
FR1599285A (cs) 1970-07-15
DE1810406C3 (de) 1974-03-28
CH485496A (fr) 1970-02-15
SE342154B (cs) 1972-01-31
GB1242603A (en) 1971-08-11
NL144499B (nl) 1975-01-15
DE1810406A1 (de) 1969-07-10
CS153488B2 (cs) 1974-02-25

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