US3096080A

US3096080A - Apparatus for generating oscillations in fluid

Info

Publication number: US3096080A
Application number: US65163A
Authority: US
Inventors: Willems Peter
Original assignee: Individual
Current assignee: Individual
Priority date: 1959-10-30
Filing date: 1960-10-26
Publication date: 1963-07-02
Anticipated expiration: 1980-07-02

Description

P. wxLLx-:Ms 3,096,080

APPARATUS FOR GENERATING OSCILLATIONS IN FLUID July 2, 1963 vFiled Oct. 26, 1960 INVENTOR. efez' Mfems United States Patent O Peter This invention relates to an apparatus for generating oscillations at high sonic and ultrasonic frequencies in gaseous and liquid fluids.

Such oscillations when produced in air are commonly employed to transmit signals. They have a velocity of propagation of substantially 330 meters per second. Oscillations of the high sonic and ultrasonic frequency range are generated in liquids for the purpose of sounding distances between the generator and immersed objects, but also for mixing, homogenizing, emulsifying and the like, as is well known. Sound waves are propagated in liquids at velocities of more than 1400 meters per second. Sound waves directed against the surface of a solid body are partly reflected, and partly propagated in the body at velocities of the order of 5000 meters per second.

Known ultrasonic generators include Galton whistles, sirens, magnetostrictive and piezoelectric oscillators. Some of these oscillator types are capable of generating ultrasonic oscillations both in gaseous and in liquid uids, others are more limited in their applications. The known whistle type generators `are actuated by air under pressure and thus require equipment for producing such air.

Acoustic oscillations in air at an elevated level of enery (up approximately 50 watts of sound energy) have been produced by the so-called Hartmann generators. They rely on discharge of air from yan orice at supersonic velocities, and are not capable of being employed with liquids because it is not possible to induce ilow of a liquid at speeds greater than the speed of sound therein, that is, at speeds in excess of approximately 1,40() meters per second.

A Galton whistle is capable of operating in a liquid medium, at least at relatively low frequencies, but its e'iciency is low. At high frequencies a Galton whistle cannot operate in a liquid medium. The standing wave of relatively great amplitude which is required in the Galton whistle can be generated in a Ifluid filled cavity only when sound waves are totally reilected from the walls of the cavity. Whereas reection is substantially complete (about 99.99%) at air-metal interfaces, only approximately 86% of a sound wave is reflected into the liquid `at a liquid-metal interface. The resonance required for the operation of a Galton whistle thus is not available in a liquid lled space.

The ultrasonic whistle of Janowsky and Pohlmann is capable of operating in a liquid medium and may be ernployed for ultrasonic treatment of liquids which are fed to the whistle at a suitable high pressure. The whistle consists essentially of a nozzle orifice and of a lip adjustably mounted opposite the orifice. `It is limited to relatively small scale operations.

Oscillations of high frequency have been produced in air by sirens. They are equipped vwith a casing or stator provided with a plurality yof nozzles arranged about an axis and discharging axial streams of air at high pressure and velocity. A disc rotates about the stator axis and has openings which are sequentially axially aligned with the nozzle orilices as the disc rotates. As the openings pass over the nozzle orifices they release brief axial pulses of air at a high frequency which is a function of the rotary speed of the disc.

The known air sirens thus generate axial sound or ultrasound Waves. Their frequency and energy depend on the pressure and rate of air streaming through the noz- ICC zles, and on the frequency of interruption of the air streams by the imperforate portions of the rotary disc. The effects produced by the air sirens built so far are quite limited. At `an upper frequency limit of 4() kilocycles per second, a few kilowatts of energy can be generated.

It is an object of this invention to provide a mechanical oscillator capable of producing oscillations under many conditions of application at high levels of frequency and intensity.

Another object is the provision of a sonic and ultrasonic oscillator Iwhich is efective in both gaseous and liquid uids.

A further object is the provision of such oscillators which provide a directed stream of uid in which oscillations are propagated in the single direction 'of iluid flow.

With these and other objects in view, the invention mainly consists in a mechanical oscillator in which la rotor produces Aan axial flow of fluid through a housing. A plurality of lip means are mounted in the housing and capable yof oscillation transversely of the direction of Afluid ow.

In its more specific aspects, the invention contemplates providing the rotor with a plurality of ducts which extend helically about the axis. The ducts are arranged in a plurality of coaxial sets, each set having a corresponding plurality of entrance and discharge orices which are arranged in respective coaxial ring areas on a radial face of the rotor. A plurality of lip means are mounted in the housing, each set of lip means being axially adjacent the discharge orifices of one of the duct sets. When the rotor turns about its axis, fluid ows through the helical ducts and from the discharge orices against the lip means which are thereby caused to oscillate transversely of the direction of fluid ow.

Other features and many of the attendant advantages of this invention will be readily appreciated as the same becomes better understood by reference to the following detailed description when considered in connection with the accompanying drawings in which like reference numerals designate like pants throughout the iigures thereof, and wherein:

FIG. l shows an ultrasonic mechanical oscillator of the invention in side-elevation, partly sectional view; and

FlGS. 2, 3, and 4 show the oscillator of FIG. l in plan section on the lines lI-II, Ill-III, and lV-IV, respectively.

The working elements of the ultrasonic generator illustrated in the drawing are contained in a tubular casing 1 which is partly broken away in FIG. l in order to reveal the rotor 2 which is iixedly mounted on a shaft 9 for rotation in the direction of the arrow x (FIG. l), that is, clockwise as viewed in FlGS. 2, 3 and 4.

The casing 1 has a frusto-conical lead-in portion 12 the narrow end of which is joined by la cylindrical portion 13. A horn of parabolic cross section 14 is releasably attached to the discharge end of the cylindrical casing portion 13 and may be replaced by a differently shaped discharge nozzle.

A guide vane assembly 6 is iixedly mounted on the cylindrical casing portion 13 about the shaft 9. It consists essentially of three ishort coaxial cylinders 8, S', and 3" which are connected with each other and with the casing portion 13 by a plurality of

flat plates

7, 7', and 7" the major dimensions of which extend axially and radially in the `casing 1.

Axially adjacent the fixed guide vane `assembly 6 the rotor 2 carries three coaxial sets of

buckets

3, 3', and 3". The innermost set of buckets 3 is mounted on the rotor body 2 itself and the radially `outer sides of the bucket 3 are fastened to a cylindrical partition wall 11" which in turn carries an intermediate bucket set 3. A

aoeaoso partition wall 11 similarly divides the buckets 3 from an outer set of buckets 3 which are closely spaced from the housing 1. The main wall of each bucket is arranged -in a helix about the axis ofthe rotor 2 and is joined by a discharge portion 4 which is axially arranged and attached to the rotor 2 or the

partition walls

11, 11 over a part of its laxial length only. In the direction of liquid ilow through the apparatus, as indicated by the arrows y, the

rotary buckets

3, 3', 3" are followed by

stationary vanes

5, and 5 secured to Ithe casing 1 in an arrangement similar to that of the guide vane assembly 6. As best seen from FIG. 1, the

vanes

5, 5', and 5 are secured to the casing 1 and to interposed

partition Walls

16, 16 only over a part of their axial length. Each vane has a lip portion 17 axially adjacent the

buckets

3, 3', 3 which is free to oscillate in a tangential or circumferential direction. The afore-described apparatus operates as follows:

When the rotor 2 is rotated in the direction of the Yarrow x by a motor (not shown), iluid is drawn through the lead-in portion 12 of the casing 1 and the guide vane Y assembly `6. The

plates

7, 7', 7 ofthe latter reduce any turbulence that may haveexisted in the streaming fluid, and the ow of the uid is substantially laminar as it leaves the guide vane assembly 6.

- The

buckets

3, 3', and 3" carry the uid in a helical path toward the dischargeV end of the apparatus. Each bucket constitutes a Yhelically inclined duct which is open only at its axial entranceV and discharge orifices. The uid is driven at high speed against the lip portions 17 of the

vanes

5, 5', 5". Because of the axial orientation of the discharge portions 4 of the

buckets

3, 3', 3", the stream of fluid moves predominantly in an axial direction as it hits the edges of the lip portions 17. The lip portions 17 are made to oscillate, and these oscillations are transmitted to the owing iluid.

The oscillations of the lip portions 17 are due to two phenomena the eiects of which are superimposed. The passage of each bucket in a corresponding row on the rotor 2 imparts a pulse to the vane 5 and to its lip portion during rotation of the rotor. This pulse generates an oscillation the frequency of which depends on the eective free length of the lip 17. The initial amplitude of the oscillation is a function of the energy imparted to the lip portion by the bucket as it passes. The amplitude gradually decreases as the oscillation is damped by the sur.- rounding fluid, until passage of a succeeding bucket transmits a new pulse to the lip. Successive excitation of the lips bythe passing buckets establishes wave trains which are transmitted to the streaming fluid.

' The second type of oscillations is generated in the fluid itself as it is thrown at high speed against the edge of the lips 17 by the

buckets

3, 3', 3". These oscillations are in turn transmitted from the fluid to the

vanes

5, 5', and 5". Their frequency depends on the rotary speed of the rotor, on the Ynumber of circumferentially arranged buckets and vanes, and on the axial velocity of the liuid. j

Since the discharge portions 4 of the buckets are attached to the rotor 2 and to the partition walls 11, v11' only over a portion of their length, another set of lips capable of oscillations is formed opposite the lip portions 17. A third mode of oscillation is Ythus generated and superimposed on the oscillations generated by the aforedescribed mechanisms.

The relatively rigid assembly ofthe main portions of the vanes 5, 5', 5Y directs the sonic or ultrasonic waves generated in the fluid in the direction of the rotor axis. When a very intense directional effect is desired, the

vanes

5, 5', 5" and the

partition walls

16, 16 are axially elongated in such a manner that the axial length of each ofthe tubular ducts formed between the vanes and partitions is several times greater than the circumferential and radial width thereof. Each of the ducts then in eiect may form arresonant columnof iluid, or a column approaching conditions of resonance so as to increase the specific intensity of the sound waves traveling therethrough.

Whether a horn 14 or a differently shaped nozzle is employed at the discharge end of the mechanical oscillator of the invention will depend on the elfects that it is desired to achieve.

The apparatus illustrated is assembled from essentially at metallic elements which are joined along edges in the manner illustrated and described. It will be appreciated that a structurally equivalent machine may be built from integral blocks of material in which the several ducts and passages are formed by correspondingly arranged bores. The

flat plates

7, 7 7ll may thus be integral with the

cylinders

8, 8', 8" and the ducts defined therebetween may be formed by boring and have radial cross sections of arcuate shapes. The

buckets

3, 3', 3" and

partition Walls

11, 11 can be formed from a single piece of material by suitable machining operations, and

the same holds for the vanes 5, 5', S'f. The ducts formed between the

buckets

3, 3', and 3 are narrower at their entrance ends in a direction transverse to the direction of fluid ilow than at their discharge ends between the discharge portions 4, and similar dilferenccs in ilow section may be incorporated in elements of the generator of the invention when made from integral blocks of material by boring or other machining operations.

The effects of the two (or three) modes of oscillation generated by the apparatus of the invention in the fluid conveyed therethrough are superimposed. Interference and resonance phenomena are set up. Fluids passed through the apparatus show the effects associated with ultrasonic treatment'of high intensity and a broad range of frequencies. Mixtures of a liquid with a solid which only slowly dissolves therein wheny fed to the apparatus are dischraged as homogeneous solutions. Two immiscible liquids entering the machine emerge as colloidal dispersions of one in the other. Solids are suspended in liquids, and liquids may be finely distributed in a gaseous carrier by the apparatus illustrated.

The frequency and the amplitude of the oscillations generated can be varied at will within the limits set by the materials of construction. The apparatus is capable of being adapted to a wide range of applications without basic change. It is equally suitable for ultrasonic treatment of a system having a liquid as its main constituent or carrier phase, or one having a gaseous carrier phase.

It should be understood, of course, that the foregoing disclosure relates to only a preferred embodiment of the invention, and that it is intended to cover all changes and modifications of the example of the invention herein chosen for the purpose of the disclosure which do not constitute departures from the spirit and scope of the invention set forth in the appended claims.

What I claim is:

l. In a mechanical oscillator, in combination, a tubular housinghaving an axis; rotor means rotatable in said housing for actuating axial ow of a uid through said housing; and a plurality of lip means mounted in said housing for oscillation transversely of the Vdirection of iluid flow in contact with said flowing fluid, said lip means being angularly spaced about said axis and mounted for oscillation in respective paths tangential relative to a circle about said axis. v

2. In an oscillator as set forth in claim l, said rotor means defining a plurality of ducts axially extending in said housing, said fluid flowing through Said ducts when said rotor means rotates about said axis.

3. In an oscillator as set forth in claim 2, said ducts axis following said helically arranged portions in theY direction of fluid dow.

5. In an oscillator as set forth in claim 2, said ducts each having an entrance end and a discharge end, the polar moment of inertia of the cross section of said duct at the entrance end relative to said axis being smaller than the polar moment of the cross section of said duct at said discharge end.

6. in an oscillator as set forth in claim 2, said ducts each having a discharge end, said lip means dening a plurality of conduits therebetween, said conduits being alignable with said ducts for ow of said fluid from said discharge ends into said conduits.

7. In an oscillator as set forth in claim 6, the main direction of uid iiow in said discharge end and in said conduits being substantially the same.

8. in an oscillator as set forth in claim 2, guide vane means on said housing for directing flow of said fluid into said ducts.

9. In an oscillator as set forth in claim 2, said ducts being of arcuately shaped cross section.

10. ln a mechanical oscillator, in combination, a tubular housing having an axis; a rotor in said housing and defining therein a plurality of ducts helically extending about said axis in a plurality of coaxial sets, each set having a plurality of entrance and discharge orifices in a respective annular area of a radiai face on said rotor, said annular areas being coaxial; a plurality of lip means mounted in said housing in a plurality of coaxial annular sets, each set of lip means being axially adjacent the discharge orifices of one of said sets of ducts; and drive means for rotating said rotor about said axis for actuating flow of a fluid through said ducts in a direction from said entrance to said discharge orilices thereof and against said lip means as said rotor rotates, the lip means of each annular set being free to oscillate transversely of the direction of flow of said uid and tangentially relative to the respective set.

11. In an oscillator as set forth in claim 10, guide vane means for directing axial flow of said uid into said entrance orifices of said ducts.

12. In a mechanical oscillator, in combination, a tubular housing having an axis; rotor means rotatable in Said housing for actuating axial dow of a fluid through said housing, said rotor means defining a plurality 0f ducts axially extending in said housing, said fluid flowing through said ducts when said rotor means rotates about said axis, said ducts each having an entrance and a discharge end, a portion of said rotor at said discharge end being shaped to form a lip capable of oscillations transversely of the flow of fluid through said discharge end, and a plurality of lip means mounted on said housing for oscillation transversely of the direction of uid ow in contact with said flowing fluid.

13. In a mechanical oscillator, in combination, a tubular housing having an axis; rotor means rotatable in said housing about said axis for actuating flow of a fluid through said housing, said rotor means including a plurality of ducts each having an entrance portion and a discharge portion, said uid owing through said ducts from the respective entrance portions to the respective discharge portions thereof when said rotor means rotates about said axis; and a plurality of lip means mounted on said housing, said lip means being angularly spaced about said axis and closely adjacent said rotor means for sequential alignment with said discharge portions when said rotor means rotates, said lip means being free to oscillate in the fluid ilowing from said discharge portions in a direction transverse of luid flow and substantially parallel to the movement of the aligned discharge portions.

References Cited in the le of this patent UNITED STATES PATENTS 2,438,357 `Bloomberg Mar. 23, 1948 2,841,325 Weise July 1, 1958 2,947,312 Heinicke Aug. 2, 1960 2,956,733 Stalker Oct. 18, 1960 FOREIGN PATENTS 811,055 Germany Aug. 16, 1951

Claims

1. IN A MECHANICAL OSCILLATOR, IN COMBINATION, A TUBULAR HOUSING HAVING AN AXIS; ROTOR MEANS ROTATABLE IN SAID HOUSING FOR ACTUATING AXIAL FLOW OF A FLUID THROUGH SAID HOUSING; AND A PLURALITY OF LIP MEANS MOUNTED IN SAID HOUSING OF OSCILLATION TRANSVERSELY OF THE DIRECTION OF FLUID FLOW IN CONTACT WITH SAID FLOWING FLUID, SAID LIP MEANS BEING ANGULARLY SPACED ABOUT SAID AXIS AND MOUNTED FOR OSCILLATION IN RESPECTIVE PATHS TANGENTIAL RELATIVE TO A CIRCLE ABOUT SAID AXIS.