This application is a filing under 35 U.S.C. §371 of International Patent Application PCT/AU2007/000502, filed Apr. 18, 2007, which claims priority to Australian application no. AU 2006902034, filed Apr. 19, 2006.
The present invention relates to an ultrasonic transducer and components for such a transducer wherein there is an attempt to match impedance between the transducer and a medium into which the ultrasound is transmitted. The invention extends to methods of usage of such transducers, which receive ultrasonic energy from a piezo-electric driver to which the transducer is coupled.
A problem in the propagation of ultrasound into a fluid arises because of the large mismatch between the acoustic impedance of conventional transducer materials and that of the fluid. The acoustic impedance of lead zirconium titanate (PZT) is 30×10 6 rayls and of titanium, 27.3×106 rayls, whereas that of water is 1.49×106 and of air is 413. The mismatch between PZT and water is a factor of 20 and this can be alleviated by placing a material with an intermediate acoustic impedance e.g. plastic, between the PZT and water. Often, in medical applications, a jelly or oil is applied to the surface of a transducer to ensure good contact between the body and the transducer by eliminating any air layer. Clearly, the mismatch between a solid transducer and air, almost 105, substantially reduces the propagation of ultrasound.
While there are many uses of high power ultrasound, normally in the frequency range of 15 kHz to 1 MHz, these involve the propagation of ultrasound into solid or liquid media. A particular useful region is around 20 kHz.
The best propagation of sound is believed to occur where the change in acoustic impedance is gradual. For example, matching layers are used in medical ultrasound applications where a plastic layer of a thickness equal to ¼ the wavelength of the sound in the plastic is intermediate between the impedances of the solid transducer and tissue (or water). A series of matching layers may be used and the efficiency of the energy flow will be determined by the number, acoustic impedance and thickness of these layers. This approach is not feasible with propagation from a solid into air because of the magnitude of the change.
Accordingly, there is a need for new and useful approaches to propagate ultrasound into a gaseous medium at power levels at which useful effects can be achieved.
In one aspect, the present invention provides an apparatus for generating an ultrasonic field into a gaseous medium, the apparatus comprising a transducer body operable to provide an ultrasonic output field and an ultrasound transmitter portion adapted to provide a substantial degree of impedance matching with the gaseous medium, the transmitter portion having at least one horn shaped cavity having a throat of relatively reduced dimension transverse to the axis of the cavity and a discharge aperture through which ultrasound is emitted into the gaseous medium and having a relatively enlarged dimension transverse to the axis of the cavity, the arrangement being characterised by the transducer body and the transmitter portion being substantially integral by either having (a) a unitary construction or (b) a face of the transmitter portion being intimately engaged with a corresponding face of the transducer body portion so that in substance there is no gap, whereby a high degree of impedance matching is achieved by the device.
There may be a multiplicity (e.g. 4 per square cm) of such cavities in a closely packed array.
The profile of the horn shape cavities may be exponential or of similar profile.
Embodiments of the invention are especially applicable to the field of high power ultrasonic emitters i.e. those having a power of the order of hundreds of watts.
The surface of the device from which ultrasound is emitted into the gaseous medium can extend over a substantial area e.g. many square centimeters. The device could be circular or could be elongated to distribute the ultrasonic field along a path for a purpose such as defoaming liquid products. For example, filled bottles of carbonated beverage may be defoamed as they move along a conveyer in a fraction of a second.
The present invention in another embodiment subsists in a method of treating in a gaseous medium material by using an apparatus according to the first aspect of the invention and driven to provide an ultrasonic field at sufficient power to affect the material in the medium.
A more specific methodology is defoaming the foam above a liquid body, such as a carbonated beverage which generally will foam when filled into containers. Rapid reduction of the foam to ensure correct filling to a prescribed level can be achieved using embodiments of the invention.
The present invention facilitates embodiments which may be in the form of a compact device for defoaming (and other airborne high power ultrasonic applications). This is exemplified by a transducer having an array of exponentially tapered holes provided in a conventional titanium transducer horn. For simplified explanation for the operation of this transducer one can consider sections through the horn end. As the acoustic wave that is propagating through the device along the cylindrical axis reaches a cross-section immediately before the start of the holes, it is confronted with an acoustic impedance that is the product of the density and velocity of sound in titanium. When the wave reaches the tip of the device, the acoustic impedance is that of air, a factor of 7000 different. If the tapered holes have the right dimensions and appropriate degree of taper, the wave will propagate through the remaining solid around the holes without interference. The density and the velocity of sound at any cross-section along the holes can be approximated by
p=ps·As/At+pa·Aa/At
and
c=cs·As/At+ca·Aa/At
where As and Aa are the cross-sectional areas of the solid and air, At is the total horn area, p and c are the density and velocity of sound. Since As/At at the tip of the device is 0.392 and Aa/At is 0.608, the effective acoustic impedance at the horn tip is 4.62 Mrayls. With careful machining, one could reduce the effective acoustic impedance to 1.21 Mrayls, gaining a factor of 20 compared with solid titanium.
If a ¼ wavelength matching layer of a plastic (e.g. methacrylate) is butted to the conventional titanium horn and the tapered holes are made in this material, a further reduction in the acoustic impedance by a factor of approximately 12 can be achieved.
For illustrative purposes only an embodiment of the invention will be described with reference to the accompanying drawings of which,
The system in
The sonotrode 12 is shown in more detail in
The left hand end of the body 13 has a screw-threaded line bore 17 for screw threadably being fixed onto a corresponding threaded element at the tip of the transducer 11. A rigid connection occurs so that there is efficient transfer from solid to solid of the ultrasonic field developed in the transducer.
This embodiment could be mounted with the axes of the horn shaped cavities 26 directed vertically downwardly and thus spaced along a horizontal path under which product to be treated can be moved. For example, in a soft drink beverage plant the ultrasonic field can be used to quell foaming very quickly so bottles can be filled accurately and consistently and eliminate the current substantial wastage in most plants due to inadequately filled bottles being rejected.
Referring now to
The Y axis of the diagram represents distance in millimeters from the end face 16.
Contour lines indicate boundaries of different intensities of the measured ultrasonic field. Substantially 100% value is achieved in the shaded area marked “X” and the next area around it has a boundary representing 83.25% of maximum value. Other contour lines show the measured field strength. It will be apparent that the ultrasound field transmitted into air has been efficiently transferred over an extended zone suitable for any industrial processing requiring such high strength ultrasonic fields.
One application of the invention is to defoaming products on a production line such as a container filling line for carbonated beverages. When a container is filled before closure a considerable problem is dissolved carbon dioxide coming out of solution and causing a foam which if efficiently quelled would permit reliable and precise filling of the container to the desired volume of the liquid prior to closure of the container.
Other potential applications are dealing with fog, mist or smoke dispersion and acceleratory drying of moist solids eg as they are moved on conveyor belts.
Number | Date | Country | Kind |
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2006902034 | Apr 2006 | AU | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/AU2007/000502 | 4/18/2007 | WO | 00 | 1/21/2009 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2007/118285 | 10/25/2007 | WO | A |
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4437497 | Enander | Mar 1984 | A |
4999976 | Smith | Mar 1991 | A |
6744899 | Grunberg | Jun 2004 | B1 |
6925187 | Norris et al. | Aug 2005 | B2 |
20010033124 | Norris et al. | Oct 2001 | A1 |
20020128328 | Varadaraj | Sep 2002 | A1 |
Number | Date | Country |
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0885641 | Dec 1998 | EP |
2341742 | Mar 2000 | GB |
07-046693 | Feb 1995 | JP |
10-85509 | Apr 1998 | JP |
WO 9118486 | Nov 1991 | WO |
Entry |
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International Preliminary Report on Patentability and Written Opinion of the International Search Authority for PCT Application No. PCT/AU2007/000502, 5 pages, Jul. 24, 2007. |
Search Report for PCT Application No. PCT/AU2007/000502, 3 pages, Jul. 24, 2007. |
Extended European Search Report dated May 14, 2012 for corresponding European Application No. 07 718 749.0, 6 pages. |
Number | Date | Country | |
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20090308487 A1 | Dec 2009 | US |