This application is the U.S. national phase of International Application No. PCT/EP2007/062234, filed 12 Nov. 2007, which designated the U.S. and claims priority to French Application No. 06 09905, filed 14 Nov. 2006, the entire contents of each of which are hereby incorporated by reference.
The present invention relates to fluid dispensers, commonly called atomizers, that are used to accurately diffuse, by means of piezoelectric members, fluids in the form of micro-droplets or aerosols.
In many applications, fluids or liquids, whatever their nature (oily, aqueous or alcoholic), whether they are solutions or suspensions (particles suspended in a liquid), are dispensed by micronization, atomization, vaporization or aerosol generation. The main applications that use these fluid dispensing devices relate to the administration of medicines (pharmacy), the diffusion of cosmetic products (in particular perfumes), disinfection, odor generation, humidification of air or media (paper, fabrics, etc.) and the dispensing of biological reagents.
Regarding medical applications, nebulizers have been employed for decades to deliver medicines by inhalation. The devices used for tins purpose can include a mechanical dosing pump, a pneumatic or ultrasound nebulizer. Until recently, these devices were designed to deliver medicines through respiratory pathways, at a relatively superficial level. For some years, the pharmaceutical industry has been addressing the administration of medicines in the form of aerosols as deep as possible into the lungs in order to reach the bronchioles. By being able to do this, it would be possible to administer systemic medicines or genes by respiratory pathway.
For this, it is necessary to develop new technologies to enhance the efficiency, the accuracy and the uniformity of the aerosols intended to be deposited in the bronchioles. The conventional devices are generally limited either by an excessively fast expulsion of the aerosol, or by excessive consumption, or by degradation of the medicinal products, or by excessively large droplets, or by noise.
To satisfy the new conditions demanded by the delivery of medicines by respiratory pathway, a number of manufacturers of aerosol generators have developed devices based on vibrating micro-perforated grids or membranes. These manufacturers include Nektar (Aeroneb), Odem (TouchSpray), Pari (e-Flow), Pfeiffer (MicroHaler), Omron (NE-UO22), Sheffield Pharmaceutical (Premaire), Alexza (Staccato).
The first studies concerning ultrasound atomizers including a vibrating micro-perforated membrane were carried out by the Matsushita research laboratory in the 1980s. The principle of the ejection of liquid in fine droplets through a micro-perforated vibrating membrane subject to vibration is developed in particular in the following publications: Ueha S., et al. Mechanism of ultrasonic atomisation using a multi-pinhole plate. Acoust. Soc. Jpn. (E) 6, 1:21 (1985). Maehara N., et al. Influence of the vibrating system of a multipinhole-plate ultrasonic nebutizer on its performance. Review of scientific instruments, 57 (11), November 1986, pp. 2870-2876. Maehara N., et al. A pinhole-plate ultrasonic atomizer. Ultrasonics November 1984.
All of these studies have formed the subject of a number of patents, in particular U.S. Pat. No. 4,533,082 (1985) and U.S. Pat. No. 4,605,167 (1986) which describe an atomizer that uses a vibrating membrane perforated with micro-holes. The membrane includes a curved part protuberance or dome) at its center causing the droplets generated to diverge. The membrane includes micro-perforations of 30 to 100 μm diameter. The vibrating member is an annular piezoelectric ceramic with an external diameter of 5 to 15 mm, an internal diameter of 2 to 8 mm. The vibrating membrane that is 30 to 120 μm thick is glued to the annular ceramic. This piezoelectric ceramic is excited at frequencies between 30 and 200 kHz on its radial deformation mode. Bespack U.S. Pat. No. 5,152,456 (1992), see also the corresponding European application, EP 0 432 992 A1, takes up the principle proposed by Matsushita. However, the vibrating member (or vibrator) comprises an annular disk of aluminum that is 22 mm in diameter. The piezoelectric ceramic is fixed to this aluminum disk. The operating mode of the piezoelectric ceramic corresponds to a radial deformation. The central opening of the aluminum disk is 4 mm. The nickel membrane has 1500 perforations (or holes) of 3 μm diameter.
The Toda U.S. Pat. No. 5,297,734 (1994) refers to a vibrating-plate-type atomizer of square geometry allowing throughputs up to 1 l/hour. The atomizer comprises a nickel membrane 50 μm thick glued to a piezoelectric ceramic disk with an external diameter of 24 mm, an internal diameter of 12 mm and a thickness of 6 mm. The membrane has tapered holes with an internal diameter of 1 mm and external diameter of 20 μm.
The Technology Transfer Partnership (TTP) U.S. Pat. No. 5,261,601 (1993) describes an atomizer based on the abovementioned Bespack patent. The TTP U.S. Pat. No. 5,518,179 (1996) refers to a disk atomizer in which the perforated membrane is made of electroformed nickel. The TTP atomizer requires no liquid chamber behind the membrane and the liquid is fed by capillarity (use of wick or porous material). The TTP atomizer highlights its bimorphic structure specifying the flexing mode of the assembly consisting of the piezoelectric ceramic and the micro-perforated membrane. The membrane has a rigidity comparable to that of the annular piezoelectric ceramic. The reference atomizer comprises a brass ring with an external diameter of 20 mm and a thickness of 200 μm. The piezoelectric ceramic ring has an external diameter of 20 mm, an internal diameter of 6 mm and a thickness of 200 μm. The Aerogen U.S. Pat. No. 6,085,740 (2000) mentions a means for atomizing a liquid in fine droplets by using a micro-grid. The membrane, provided with micro-holes of 1 to 6 μm diameter, is vibrated by a piezoelectric bimetallic strip operating at 45 kHz. The liquid is fed by capillarity and the membrane can be dissociated from the vibrator.
The Aerogen U.S. Pat. No. 6,427,682 (2002) describes the use of a medicine diffusing appliance that uses a vibrating membrane. Its principle is very close to that of Matsushita. It comprises a part made of aluminum vibrated by flexing using an annular piezoelectric ceramic. The vibrating membrane provided with micro-holes is produced by electroforming. A chamber containing the liquid is in contact with the membrane.
Moreover, Omron has developed an ultrasound pump technology making it possible to atomize a liquid through a micro-perforated membrane. This technology is described in U.S. Pat. No. 6,901,926 (2005). In the Omron technology, the micro-perforated membrane is not vibrated directly by the vibrating member. The droplets are formed by ejection of the liquid through the holes when the pressure varies dynamically due to the ultrasound pump.
The piezoelectric or ultrasound atomizers of the state of the art (frequency greater than 20 μm) that include a micro-perforated membrane that is subjected to vibration all operate by flexing of the membrane and the piezoelectric ceramic associated therewith. In fact, it involves combining in different ways an annular piezoelectric ceramic and a thin metallic membrane that includes a large number of micro-perforations. This type of structure benefits from a small thickness.
The devices of the state of the art do, however, have a number of drawbacks.
A first drawback lies in the fact that the micro-perforated membrane contributes strongly to the resonance mode of the atomizer. The effect of this phenomenon is that the atomizer is itself greatly damped in its resonance by the liquid that is in contact with the membrane. The operation of the atomizer depends strongly on the quantity of liquid or the pressure exerted by the liquid behind the membrane. This creates a complication in the control of the atomizer's excitation frequency. Furthermore, this damping leads to an overheating of the vibrating member and of the membrane. This overheating causes the operating time of the atomizer to be limited, the electrical consumption required for the latter to operate to be increased and can lead to a degradation of the properties of the liquid to be atomized. Moreover, in this type of structure, the deformation of the membrane by flexing does not make it possible to obtain a uniform displacement over the entire surface of the membrane. Depending on the positioning of the micro-holes on the membrane, the latter do not have the same throughput and the aerosol generation can be unstable (threshold effect). Also, the sensitivity of the vibrating structure to the mechanical fixings and the liquid seals (spurious damping) make the technological solutions for industrially implementing such structures in large quantities and at low cost both complex and costly.
There is therefore a need to remedy these various drawbacks and propose devices that are more robust, easier to control electronically, more energy-efficient, easier to industrialize in large quantities and at low cost.
The present invention sets out to remedy in particular the problems explained in the preceding section.
To this end, its subject is an atomizer as defined in the main claim.
Preferred embodiments are the subject of the dependent claims.
In the present text, the term “transducer” should be understood to mean a member comprising a piezoelectric transducer body, at least one piezoelectric member and, optionally, a rear mass.
The term “section” should be understood to mean a geometrical figure comprising the intersection of a plane and a volume. Thus, considering the example of a cylindrical object with a variable internal diameter, it will be said that it has a section that varies over its length.
The transducer body has a symmetry axis.
A number of the advantages offered by the atomizer according to the present invention result from the fact that the piezoelectric transducer body to which the membrane is fixed vibrates in a longitudinal mode, that is, in a direction parallel to the symmetry axis of the piezoelectric transducer body.
One or more piezoelectric members can be provided.
Preferably, the section of the piezoelectric transducer body varies over its length.
According to one embodiment, the section varies discontinuously.
Advantageously, the section varies abruptly at a single point.
Such a section variation is illustrated in the following embodiment in which the piezoelectric transducer body has two parts with different external diameters. The deformation amplification zone, the end of which includes the membrane, has the smallest diameter. In this configuration, called “horn” in this text, the longitudinal ultrasound waves are amplified in displacement at the change of section of the transducer. The tubular member acts as a micronic longitudinal displacement amplifier.
According to another embodiment of the invention, the membrane at least partially forms a dome that provides a number of functions. Commonly in the prior art, the micro-perforated membrane is designed to retain the liquid in the atomizing chamber behind the membrane and contain its static pressure. The balance of the pressures, the shape of the holes and the nature of the material used for the membrane is such that the liquid does not seep out of the membrane and that no “dripping” or liquid loss phenomenon occurs. Moreover, the dome shape provides for a better distribution of the micro-droplet or aerosol mist by causing the jet to diverge by simple geometrical effect. Also, the vibratory speed associated with the displacement of the membrane makes it possible to eject the micro-droplets through the holes. In the case of the present invention, the dimensions of the dome and of the micro-perforated membrane are such that the dome provides a vibratory motion amplification effect while retaining a vibratory speed distribution that is uniform over the surface of the membrane. Unlike in the prior art, the membrane does not affect the vibratory behavior of the transducer. Whatever the thickness of the membrane (for example from 20 to 200 μm), the piezoelectric member retains its dynamic characteristics and its vibratory performance. More specifically, the resonance frequency and the vibratory displacements of the transducer are not modified by the mechanical coupling of the membrane. This gives the atomizer advantages in as much as the transducer (frequencies, vibratory displacements, deformation modes, coupling coefficient and mechanical quality factor) can be designed without taking into account the membrane (geometry and material).
This property of the present invention advantageously makes it possible to optimize the structure of the transducer (or converter) in order to favor either the aerosol output speed, or the throughput, or the resonance frequency, or the consumption or the efficiency of the transducer. In this way, it is possible to produce vibrating membrane atomizers that allow aerosols to be produced at almost zero speed (medical application) up to ejection speeds for example of the order of 30 m/s (cosmetic application). Similarly, the atomization throughput is no longer directly linked to the surface area of the piezoelectric ceramic but to the length of the piezoelectric transducer making it possible to adapt throughputs from 1 μl/s to 300 μl/s. It is this same length that directly governs the resonance frequency of the atomizer. The atomizer operating mode is not a flexing mode but a longitudinal elongation mode. This makes it possible to work at high frequencies (50 to 200 kHz) with piezoelectric ceramics of small diameter without compromising the liquid throughput and above all with very low losses. These mechanical losses which correspond to an energy that is dissipated in heat in the transducer increase strongly according to the operating frequency of the transducer. In the present invention, the latter are reduced because the efficiencies of the longitudinal-transducer-type structures are far better than the “bimetallic strip” type structures that operate by flexing.
The low losses in the transducer lead to the design of atomizers with low electrical consumption. This advantage is considerable in as much as the atomizers of the prior art are limited in their application by the atomization time and the lifetime of the power supply cells or batteries. In practice, the advantageous applications of the vibrating micro-perforated membrane atomizers mainly relate to “hand-held” devices operating on cells or batteries. The structure that is the subject of the present invention is less damped by the liquid behind the membrane. This property provides for less heating of the liquid to be atomized. In the applications in which the atomizers deliver medical formulations, heating of the liquid can be prohibitive and greatly limit the benefit of such atomizers.
Moreover, according to a preferred embodiment the present invention is characterized by the fact that the vibration nodes can be accessed to enable the atomizer to be mechanically fixed easily. The atomizers of the prior art that operate by flexing of the annular ceramic are difficult to fix mechanically without disturbing and greatly damping the vibration mode. In the case of the present invention, the atomizer is preferably mechanically fixed or overmolded in the area of the vibration node (this node is unique) and allows for very simple and very inexpensive mechanical assembly and sealing solutions.
Another characteristic of the invention is that the liquid can be placed directly in contact with the rear face of the membrane. In practice, the vibration mode of the atomizer in a longitudinal mode has little sensitivity to the presence of a liquid and to the weight of the column of this liquid.
This property enables the atomizer to operate equally at any angle from the vertical to the horizontal. The liquid can also be guided to the membrane by capillarity by using ducts, wicks or appropriate porous materials. In this way, the liquid reservoir can be located above, around or below the atomizer. According to a variant of the invention, the structure of the atomizer comprises a rear mass, also called dynamic mass, the role of which is to prevent the transducer from vibrating backward, two piezoelectric ceramics linked by common connections, a vibratory movement amplifier including a cavity and a micro-perforated membrane of varied shape but preferably dished forming a protuberance or dome.
According to another variant of the invention, a pre-stressing mechanism like a screw can be used to mechanically link the rear mass, the ceramics and the amplifier. The amplifier is metallic and preferably made of stainless steel, titanium or aluminum. The micro-perforated membrane is glued to the vibratory amplifier. The membrane, which has little effect on the vibratory behavior of the atomizer, can be made of a variety of materials such as plastic, silicon, ceramic, but is preferably made of metal. The micro-perforations can be produced by different means but preferably by electroforming or by laser. The quantity of micro-perforations can range from one hole for the dispensing of liquid on demand, to several thousands of holes. The size of the micro-holes or the mesh of the grids can range from 1 μm to 100 μm in equivalent diameter according to the applications of the atomizer. It has been demonstrated that the throughput and uniformity performance of the jet of droplets from the atomizer were greatly dependent on the displacement mode of the membrane. These performance levels are enhanced if the membrane is displaced in “piston” mode without deformation by flexing. In the state of the art, the atomizers operate by flexing and therefore lead to one or more vibration nodes inside the membrane. In the present invention, the membrane is not involved in the vibration mode of the transducer and it is possible to engineer and optimize the geometry of the membrane in order for the latter to be deformed in “piston” mode. For this, modelings and test results show that the diameter of the protuberance (or dome) must be close to the diameter of the cavity containing the liquid (or chamber). This means that the maximum height of the dome must be close to half the internal diameter of the cavity.
The displacement of the membrane in “piston” mode means that the vibratory speed on the surface of the membrane can be made uniform. The result of this is that the micro-perforations (or holes) eject micro-droplets of sizes that are better calibrated and with an identical throughput when they are compared with each other.
Other embodiments of the invention are briefly described below:
It follows that the invention is not limited to the embodiments described hereinabove. The latter are only examples.
It will also be noted that, in addition to the introduction of a longitudinal vibration mode, it is possible to provide a radial vibration mode.
The invention will be better understood in this section by means of a detailed description and nonlimiting examples illustrated by the figures.
The atomizer illustrated in
In the atomizers illustrated in
One or more piezoelectric members, preferably comprising a single-piece 2 or multilayer 9 piezoelectric ceramic, are located in the top part of the atomizer, at the level of the stress concentration zone 1a.
The rear mass 5 (dynamic mass) makes it possible to reduce the deformations at the rear of the piezoelectric ceramics. The prestressing screw 6 makes it possible to mechanically link all of this stack. This assembly constitutes a piezoelectric transducer which is an electromechanical converter which vibrates according to a longitudinal mode. A longitudinal mode is defined by the fact that the transducer is deformed along its symmetry axis by elongation or contraction of its section. The vibratory behavior of this type of transducer is governed essentially by its length so that the ratio of the overall length of the transducer to the diameter or width of the piezoelectric ceramic is, preferably, greater than or equal to 1.
The micro-perforated membrane 3 or a grid of small thickness (20 to 200 μm) is mechanically fixed to the end of the piezoelectric transducer body 1 where its vibratory speed is maximum. The fixing of the membrane 3 is such that the latter is acoustically coupled to the transducer in the zone 1b. In a first deformation mode and by way of example, this transducer is deformed and vibrates according to its half-wavelength.
In the embodiment of
In the configuration of
This configuration offers the advantage of not having the ceramic 2 in contact with the liquid and of not posing problems of seal-tightness with the reservoir. The section variation of the body of the transducer 1 still makes it possible to amplify the vibratory displacement at the level of the membrane 3.
In this specific case, the body of the transducer 1 is made of stainless steel. The internal cavity containing the liquid 4 has a diameter of 6 mm and the stress concentration zone 1a has an external diameter of 16 mm.
The deformation amplification zone 1b has an external diameter of 8 mm. The single-piece piezoelectric ceramic 2 is a PIC 255 (Physic Instruments) ceramic with an internal diameter of 8 mm, an external diameter of 16 mm and a thickness of 1 mm.
The lengths of the transducer 1 and of the deformation amplification zone 1b are respectively 16 mm and 12 mm. The microperforated membrane 3 has been made of electroformed nickel provided with 800 holes with a diameter of 5 μm. The thickness of the membrane is 50 μm and it has an external diameter of 8 mm. The dome has a height of 0.8 mm for a diameter of 5 mm. The membrane is fixed to the transducer by gluing. The longitudinal modes concerned have respectively resonance frequencies of 77 kHz and 120 kHz.
In the embodiment according to
The electrode 7 for electrically connecting the single-piece piezoelectric ceramic 2 is foil of stainless steel measuring 30 mm in diameter and 50 μm in thickness. The electroformed nickel membrane 3 comprises 10 800 2 μm holes for a thickness of 20 μm. The atomizer has made it possible to obtain droplets with a size of 2 μm for a throughput of 0.6 ml/min for an operating frequency of 80 kHz.
The electrode 7 for electrically connecting the single-piece piezoelectric ceramic 2 is made of stainless steel 30 mm in diameter and 50 μm thick. The electroformed nickel membrane 3 comprises 45 300 2 μm holes for a thickness of 20 μm. The atomizer has made it possible to obtain droplets with a size of 2 μm for a throughput of 2.5 ml/min for an operating frequency of 70 kHz.
The invention is obviously not limited to the examples discussed hereinabove. Similarly, it is not limited to the medical field. The atomizer according to the invention can also be used as a diffuser of odors and perfume and/or in the application of cosmetic products. The invention also covers the diffusion of various liquid mists for local use (humidifiers or lubricators) or liquid handling devices for biotechnologies or reagents.
Number | Date | Country | Kind |
---|---|---|---|
06 09905 | Nov 2006 | FR | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/EP2007/062234 | 11/12/2007 | WO | 00 | 6/16/2009 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO2008/058941 | 5/22/2008 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
2855244 | Camp | Oct 1958 | A |
2949900 | Bodine | Aug 1960 | A |
3103310 | Lang | Sep 1963 | A |
4153201 | Berger et al. | May 1979 | A |
4300546 | Kruber | Nov 1981 | A |
4326275 | Butler | Apr 1982 | A |
4337896 | Berger | Jul 1982 | A |
4479609 | Maeda et al. | Oct 1984 | A |
4496101 | Northman | Jan 1985 | A |
4533082 | Maehara et al. | Aug 1985 | A |
4541564 | Berger et al. | Sep 1985 | A |
4585167 | Kholin | Apr 1986 | A |
4655393 | Berger | Apr 1987 | A |
4723708 | Berger et al. | Feb 1988 | A |
4850534 | Takahashi et al. | Jul 1989 | A |
4978067 | Berger et al. | Dec 1990 | A |
5134993 | Van der Linden et al. | Aug 1992 | A |
5170782 | Kocinski | Dec 1992 | A |
6357671 | Cewers | Mar 2002 | B1 |
6394363 | Arnott et al. | May 2002 | B1 |
6640804 | Ivri et al. | Nov 2003 | B2 |
6651650 | Yamamoto et al. | Nov 2003 | B1 |
7883031 | Collins et al. | Feb 2011 | B2 |
20020129812 | Litherland et al. | Sep 2002 | A1 |
20020162898 | Klimowicz et al. | Nov 2002 | A1 |
20050034719 | Feiner et al. | Feb 2005 | A1 |
20050056274 | Kunschir | Mar 2005 | A1 |
20050224076 | Pfichner et al. | Oct 2005 | A1 |
20060102172 | Feiner et al. | May 2006 | A1 |
20060243277 | Denyer et al. | Nov 2006 | A1 |
Number | Date | Country |
---|---|---|
0 432 992 | Jun 1991 | EP |
1 386 672 | Feb 2004 | EP |
58-067374 | Apr 1983 | JP |
58-67374 | Apr 1983 | JP |
61-141955 | Jun 1986 | JP |
5-277188 | Oct 1993 | JP |
A 5-277188 | Oct 1993 | JP |
2003-265994 | Sep 2003 | JP |
A 2005-537870 | Dec 2005 | JP |
A 2006-506150 | Feb 2006 | JP |
A 2006506150 | Apr 2006 | JP |
9310910 | Jun 1993 | WO |
WO 2004022132 | Mar 2004 | WO |
Entry |
---|
International Search Report for PCT/EP2007/062234, mailed Apr. 10, 2008. |
English Translation of International Search Report for PCT/EP2007/062234, mailed Apr. 10, 2008. |
Japanese Office Action dated May 8, 2012 for applicant's Japanese Patent Application No. 2009-536715 corresponding to PCT/EP2007/062234 filed Nov. 12, 2007, and its English translation. |
Japanese Office Action dated Jan. 28, 2014, for applicant's Japanese Patent Application No. 2009-536715 corresponding to PCT/EP2007/062234 filed Nov. 12, 2007, and its English translation. |
Berger, Harvey L., “Coating Drug-Eluting Arterial Stents Using Ultrasonic Spray Nozzles,” ILASS Americas, 19th Annual Conference on Liquid Atomization and Spray Systems, Toronto, Canada, May 2006, 6 pp. |
Japanese Office Action mailed Jun. 3, 2014 issued in Japanese Patent Application No. 2013-185297, 3 pp. |
Japanese Office Action mailed Jun. 10, 2014 issued in Japanese Patent Application No. 2013-17255, 3 pp. |
Maehara, Naoyoshi et al., “Influence of the Vibrating System of a Multipinhole-Plate Ultrasonic ebulizer on its Performance,” Rev. Sci. Instrum. 57 (11), Nov. 1986, pp. 2870-2876. |
Maehara, N. et al., “A Pinhole-Plate Ultrasonic Atomizer,” Ultrasonics, Nov. 1984, pp. 259-260. |
Peskin, Richard L. et al., “Ultrasonic Atomization of Liquids,” The Journal of the Acoustical Society of America, vol. 35, No. 9, Sep. 1963, pp. 1378-1381. |
Number | Date | Country | |
---|---|---|---|
20100044460 A1 | Feb 2010 | US |