• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
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  • 优先权
    • 专利摘要:
    A method for promoting the sliding of at least one drop (15) onto a support (5), wherein an ultrasonic surface wave is generated in the support with a sufficient amplitude to cause the drop to deform in an inertial mode. capillary of clean vibration thus reducing the attachment of the drop to the support, so as to facilitate the displacement of the drop under the effect of an external force, the amplitude of the ultrasonic surface wave being insufficient to cause deformation asymmetric drop so as to cause it to move in the absence of the external force in the direction of propagation of the ultrasonic surface wave.
    公开号:FR3044937A1
    申请号:FR1562067
    申请日:2015-12-09
    公开日:2017-06-16
    发明作者:Adrien Bussonniere；Matar-Lacaze Olivier Bou；Michael Baudoin；Philippe Brunet
    申请人:De Lille 1, University of；Centre National de la Recherche Scientifique CNRS；Universite Lille 1 Sciences et Technologies；Lille Ecole Centrale de；
    IPC主号:
    专利说明:

    Method for promoting the sliding of at least one drop on a support
    The present invention relates to a method for facilitating the sliding of at least one drop of a liquid on a support.
    In various fields, it is necessary to overcome the effects of the accumulation of a liquid on a surface. For example, in the case of medical applications, it may be necessary to prevent or at least delay the coagulation of a drop of blood on a surface, without recourse to the addition of an anticoagulant agent. . In the optical field, the condensation of drops of water on a lens can prevent correct observation and then it is necessary to proceed with its cleaning, which proves tedious. As a further example, the accumulation of condensates of combustion products or fuel drops on some parts of an engine can reduce energy efficiency.
    It can also be useful to precisely control the movement of drops on a surface.
    To evacuate drops of liquid accumulated on a surface, it is well known to apply a mechanical force on the drops, for example by means of a wiper on a windshield of a motor vehicle. However, a windshield wiper limits the field of vision accessible to the driver. It also spreads the greasy particles deposited on the surface of the windshield. In addition, it is necessary to renew the seals of the wiper regularly. Furthermore, a mechanical force on the drops can not be easily applied in a large number of applications, for example in microfluidics for lack of available space to have suitable mechanical means that could further damage the surfaces.
    A known way to evacuate drops accumulated on a surface is to functionalize this surface. For example, US applications 2014/0817666 and US 2014/290732 describe a support covered with a porous body whose pores have a nanometric or micrometric size, thus forming a functionalized surface. When a drop of liquid is deposited on this functionalized surface, the porous body is impregnated with the liquid, thus forming a lubricating layer between the support and the droplet which can easily slide on the surface. However, the number of materials constituting supports adapted to surface functionalization is limited. In addition, surface functionalization can modify other surface properties than wettability. For example, it is of little interest for applications involving the optical properties of surfaces. Finally, after several cycles of imbibition and drying of the surface, the pores of the porous body are gradually filled by accumulation of the residual particles contained in the liquid, and the lubricating layer eventually no longer can be formed. The functionalized surface then loses its ability to promote the sliding of the drop.
    The implementation of an electric field to control the hydrophobicity of a surface is also known, particularly in the field of microfluidics. This technique, known by the acronym EWOD (for "Electro Wetting On Devices" in English) consists in applying a potential difference between two electrodes, so as to electrically polarize the surface to make it hydrophilic, thus loosening the drop of the surface . By controlling the location of the polarization, the drop can then be moved. However, few materials are suitable for this technique, which is also unsuitable for thick media. In addition, the EWOD technique requires a particularly precise positioning of the electrodes over the entire surface where it is desired to control the wetting properties.
    It is still known to evacuate drops by vibrating the support on which they rest, in particular by generating an ultrasonic surface wave so as to cause the displacement of the drops on the surface or to vaporize the drops. Ultrasonic surface waves have the advantage of being easily generated by means of a transducer. In addition, they are poorly attenuated and can spread over great distances. GB 2 387 107 and GB 1 037 787 respectively disclose a helmet visor and a windshield including a transducer for generating an ultrasonic wave for removing raindrops. These documents, however, are silent as to the characteristics of the ultrasonic wave. US 4,768,256 discloses a device for moving raindrops from a windshield, wherein an ultrasonic wave applied to the windshield causes the raindrops to move in the opposite direction to the direction of propagation of the ultrasonic wave longitudinal.
    In the article "Low power sessile droplets actuation via modulated acoustic surface", Mr. Baudoin, Brunet P., O. Bou Matar and E. Herth, Appl. Phys. Lett., Vol. 100, 154102 (2012), a method has recently been described in which an ultrasonic surface wave is applied to a support on which a drop of water is disposed, with a frequency and an amplitude such that the drop vibrates and deforms in an asymmetrical mode, causing its displacement in the direction of propagation of the ultrasonic surface wave. FR 1 308 877 and WO 2012/095643 describe a method for discharging raindrops from a windshield by ultrasonic vaporization. The amplitude and frequency of vibration are chosen so that the drops of rain falling on the windshield can not come into contact with the windshield, and are vaporized as soon as they enter the zone of vibratory movement of the surface of the windshield. broken.
    However, in order to obtain a vaporization or a displacement of a drop of liquid, the powers necessary for the vibration of one of the supports as described are particularly high, which limits their practical implementation, in particular for the development of autonomous devices. In particular, although FR 1 308 877 and WO 2012/095643 do not specify the amplitudes and frequencies of the waves generated to vaporize the drops, it is however well known that the vaporization requires energies greater than those necessary to move drops on a support.
    There is therefore a need for a process that can be easily implemented, allowing a drop of a liquid suspended on the surface of a support to be discharged, and applying to supports of shape, size and constituent material. varied. The invention aims to satisfy this need, and it achieves this by proposing a method for promoting the sliding of at least one drop on a support, in which process an ultrasonic surface wave is generated in the support with a sufficient amplitude to bring about the drop to be deformed according to an inertio-capillary mode of own vibration thus reducing the attachment of the drop to the support, so as to facilitate the displacement of the drop under the effect of an external force, the amplitude of Fonde de ultrasonic surface being insufficient to cause an asymmetrical deformation of the drop so as to cause it to move in the absence of the external force in the direction of propagation of ultrasonic surface wave.
    The method according to the invention is particularly remarkable in that the drop is released from the irregularities of the support which prevented its movement by means of an ultrasonic wave of lower power than that used in the methods of the prior art described above. . The drop can then be moved more easily via the application of the external force, in particular of low amplitude. By release of the drop, it is meant that the inertiocapillary vibrations of the drop make it possible to release the line of contact or triple line (in contact with both the support, the drop, and the surrounding gas, for example from the air) initially trapped in irregularities, especially chemical and mechanical surface.
    In addition, the method according to the invention is particularly robust in that it actively controls the vibrations of the surface and therefore of the drop. Therefore, it is possible to adapt the vibrations of the surface according to the state of the surface. The method according to the invention is thus less sensitive to pollution and surface defects of the support than the processes of the prior art.
    In addition, the method according to the invention also makes it possible to precisely control the displacement of the drop on the support.
    The higher energy efficiency of the method according to the invention can be attributed to the fact that in the prior art, the drop is moved to the surface of the support without vibration of the contact lines. It is therefore necessary to provide enough energy to the drop to exceed the so-called hysteresis angle, from which the contact lines come out of the traps formed by the irregularities, to move the drop. A higher energy input than with the method according to the invention is thus necessary to move it. In particular, the power of the surface ultrasonic wave used in the method according to the invention to promote the sliding of a drop can be at least 10 times, or even at least 30 times, lower than the power of a ultrasonic wave used in the prior art to move a drop.
    Moreover, as will become apparent later, the method according to the invention is particularly versatile. In particular, it can be implemented over a wide range of supports, micrometric or several tens of meters in length, as long as they have sufficient rigidity for an ultrasonic surface wave to propagate there, as well. purposes that thick. Likewise, the process according to the invention is not limited to a specific type of liquid. The invention is thus simplified implementation, and in particular does not require specific and complex treatment of the surface of the support.
    Surprisingly and until now unexplained, it has been observed that the vibration according to the inertio-capillary mode of the drop is carried out at a lower low frequency, in particular at least 60 000 times lower, or even 1 million times lower at the fundamental frequency of the ultrasonic surface wave. Moreover, it has been found that it is possible to bring drops of varying diameter to vibrate according to their inertio-capillary mode in soliciting the surface with a wave of the same fundamental frequency. Thus a wave of the same frequency can vibrate drops of very different sizes.
    An "inertio-capillary mode of clean vibration" of a drop is a mode of oscillation resonance of the drop resulting from a competition between the inertia of the drop and the surface tension of the drop. It has been demonstrated by J. Rayleigh, Proc. R. Soc. London, vol. 29, 71 (1879) and H. Lamb, "Hydrodynamics", Cambridge University Press, England (1932). It is also commonly referred to as Rayleigh-Lamb mode. The invention will be better understood on reading the following detailed description, non-limiting examples of implementation thereof, and on examining the appended drawing, in which FIGS. 1 and 4 show schematically different devices for implementing the method according to the invention.
    In the appended drawing, the actual proportions of the various constituent elements have not always been respected for the sake of clarity.
    FIGS. 1 to 4 illustrate devices la-d for implementing the method according to the invention, comprising a support 5 able to propagate an ultrasonic surface wave 10, a drop of liquid 15 and a means 20 for generating the wave ultrasonic surface.
    SUPPORT
    The support 5 may be of any material capable of propagating an ultrasonic surface wave 10. Preferably, it is made of a material having a modulus of elasticity greater than 0.1 MPa, for example greater than 10 MPa, or even greater than 100 MPa, or even greater than 1000 MPa, or even greater than 10000 MPa. A material having such a modulus of elasticity has a rigidity particularly suitable for propagation of ultrasonic surface waves.
    The support can be flexible, in the sense that it can deform, including elastically, without breaking under its own weight.
    In particular, it may be chosen from piezoelectric materials, polymers, in particular thermoplastics, glasses, metals and ceramics.
    The surface of the support on which longitudinal surface foundation propagates may be flat. It can also be curved, provided that the radius of curvature of the surface is greater than the wavelength of ultrasonic surface wave.
    The surface may be rough and have a roughness Ra less than the wavelength.
    The support may in particular be in the form of a flat plate, as is for example illustrated in Figure 1, or having at least one curvature in a direction, whose thickness e is less than 0.01 m. The length of the plate may be greater than 0.1 m, even greater than 1 m, or even greater than 10 m.
    By "thickness of the support", we consider the smallest dimension of the support measured in a direction perpendicular to the surface on which propagates ultrasonic background.
    As a variant, the support may have the shape of a block whose thickness is, for example, greater than 0.05 m, or even greater than 0.1 m, as is illustrated for example in FIG. 2.
    The support can be arranged flat with respect to the horizontal. As a variant, it may be inclined relative to the horizontal by an angle α greater than 10 °, even greater than 20 °, even greater than 45 °, or even greater than 70 °. It can be arranged vertically.
    In one embodiment, the support is made of an optically transparent material, in particular light in the visible. The method according to the invention is then particularly suitable for applications in which the improvement of the visual comfort of a user observing his environment through the medium is sought.
    An optically transparent material is particularly suitable for forming all or part of: - a glazing of a vehicle, in particular a windshield, a side glazing or a rear window of a motor vehicle, - a glass of a building, - a lens of an optical device selected from a spectacle lens, a long view, a telescope, a microscope, a photographic lens, a pair of binoculars, a rearview mirror.
    For applications where such supports are used, the method according to the invention makes it possible to reduce the surface density of drops in contact with the transparent material. As previously described, the process according to the invention releases the drops from the support, and discharges them by means of the external force. This avoids the formation of liquid clusters by cohesion of the drops moving in contact with the surface as in the processes of the prior art, these liquid clusters altering the optical properties of the support.
    In particular, the method according to the invention can be implemented so that the support is self-cleaning. Other types of support are possible. In particular, the support may be a substrate of a lab on a chip, in particular intended for microfluidic applications. It can be an internal wall of a combustion engine. The method according to the invention can thus improve the efficiency of the engine, effectively evacuating the drops forming on the wall by condensation of the combustion products or by deposition of unconsumed fuel drops. The support may be an element of a turbine, for example a blade, in particular an aircraft engine.
    It can be an electric cable. For example, in the variant where the support is an electric cable of a high-voltage power line and / or railroad supply, the method according to the invention, by promoting the sliding of raindrops settling on the electric cable, reduces the effects of vibrating by the rain of the electric cable and poles supporting it. In addition, in winter, the method according to the invention, by promoting the sliding of raindrops settling on the electric cable, limits the formation of ice or ice on the cables. Thus, the risk of damage or breaking of the cables is reduced.
    The support may be an element of the structure of an aircraft, for example a wing, a fuselage or an empennage. As described in the preceding paragraph, the method according to the invention, by promoting the sliding of the drops, on these elements, limits the formation of ice or ice on the structure of the aircraft.
    The support may be an element of a medical implant. In particular, the amplitude and the fundamental frequency of the surface ultrasonic wave can be chosen so as to promote the sliding of a drop of blood to prevent its coagulation, or of a biological fluid, to avoid the deposition of the biological material contained in the biological fluid on the surface.
    The support may further be selected from an element of a heat exchanger, a plumbing installation, an element of a ventilation system, an element of an oil extraction system of a well, for example a tube . Such supports generally have surfaces that are difficult to access to evacuate drops of liquid deposited thereon, for example by condensation. The method according to the invention is therefore particularly suitable for this type of support.
    The support may be a food storage element, for example an inner wall of a refrigerator, or a wall exposed to the condensation of a liquid. For example, in a refrigerator, the condensation of drops of water on a wall increases the heat exchange between the wall and the fresh air volume of the refrigerator, reducing its efficiency.
    As already illustrated above, the method according to the invention can be implemented in applications where high temperatures are encountered. Preferably then, the surface temperature of the support is greater than 100 ° C, or even greater than 300 ° C, or even greater than 500 ° C.
    LIQUID DROP
    In a preferred embodiment, the surface of the support is at least partially covered by a plurality of drops of liquid.
    The drop 15 of liquid may have a resting size Φ less than 5 mm, in particular between 0.1 mm and 1.5 mm, for example equal to 1 mm. By "resting size" of the droplet is meant the distance between the point of the drop farthest from the surface and the latter, without any longitudinal surface wave being applied to the support. In the present description, when reference is made to the size of the drop, it is the resting size of said drop, unless otherwise indicated.
    The support may be covered with a plurality of drops having a multimodal distribution of drop sizes. Preferably, a plurality of ultrasonic surface waves is generated in the support, with fundamental frequencies and amplitudes adapted to cause each drop of the plurality of drops to be deformed in an inertio-capillary mode of vibration.
    The process according to the invention is particularly versatile in that it makes it possible to promote the sliding of drops made of liquid with varied properties. By way of example, the viscosity of the liquid may be between 0.0001 and 2 Pa.s at 25 ° C.
    Preferably, the liquid constituting the droplet is chosen from water, in particular rainwater, a biological liquid, for example an animal or human blood, a liquid capable of cleaning the support, a chemical solution, a fuel and their mixtures.
    In one embodiment, the support is covered with drops consisting of a first liquid and drops consisting of a second liquid different from the first, without the efficiency of the process being reduced.
    In particular, the liquid may have a contact angle with the support of less than 180 °, in particular less than 120 °. The method according to the invention can thus promote the sliding of a drop disposed on a hydrophilic or hydrophobic support.
    The liquid may comprise particles, for example colloidal particles. It may include an active ingredient or a medicine.
    When it is caused to vibrate in an inertio-capillary mode, the drop vibrates by deforming at low frequency, which depends in particular on the properties, in particular the density, of the constituent liquid of the drop. Preferably, the vibration frequency according to the inertio-capillary mode of the drop is between 20 Hz and 10 kHz.
    ULTRASONIC SURFACE WAVE
    The fundamental frequency and the amplitude of the surface ultrasonic wave are preferably determined according to the properties of the support and the liquid.
    In particular, one skilled in the art knows how to determine the transmission length of the surface ultrasonic wave to a liquid placed on the support, as described in J. Campbell and W. Jones, IEEE Trans. Sonas Ultrason., 17: 71 (1970), preferably so that the ratio of the drop size over the transmission length of the surface ultrasonic wave is between 0.04 and 10. As for the amplitude ultrasonic surface wave, the person skilled in the art knows how to adapt it. For example, a drop of a liquid of higher surface tension than a drop in another liquid requires the application of a higher amplitude. The same goes for a drop of higher viscosity.
    Preferably, the fundamental frequency and the amplitude of the surface ultrasonic wave are adapted so that the ratio of the amplitude of oscillation of the drop to the resting size of the drop is less than or equal to 1.4, or even less than or equal to 1.3, or even less than or equal to 1.15. By "amplitude of oscillation" of the droplet is meant the largest diameter of the smallest sphere circumscribed to the drop, measured over a period of vibration of the drop, when a surface acoustic wave is applied to the support.
    Different types of ultrasonic surface waves can be generated and are particularly adapted to the geometry of the support.
    Preferably, the ultrasonic surface wave is a Lamb wave or a Rayleigh wave. In particular, it may be a Rayleigh wave when the support has a thickness greater than the wavelength of the ultrasonic surface wave. A Rayleigh wave is preferred because a maximum proportion of the energy of the wave is concentrated on the surface on which it propagates, and can be transmitted to the drop to make it vibrate.
    Preferably, the fundamental frequency of the ultrasonic surface ultrasonic wave is between 1 Mhz and 100 Mhz. In one embodiment, it may be between 5 Mhz and 40 Mhz, and in particular be equal to 20 Mhz.
    Furthermore, the fundamental frequency of the ultrasonic surface wave can be modulated at a modulation frequency of between 20 Hz and 10 kHz, in particular to optimize, according to the size of the drop, its vibratory regime in an inertio-capillary mode. Preferably, the fundamental frequency of the surface wave is modulated by the natural frequency of the inertio-capillary mode of vibration proper to the drop. The eigenfrequency of the drop can be determined approximately from the Rayleigh-Lamb formula, described in J. Rayleigh, Proc. R. Soc. London, vol. 29, 71 (1879) and H. Lamb, "Hydrodynamics", Cambridge University Press, England (1932): where:
    n denotes the order of the vibration mode, which is for example equal to 2 in the case of a quadripolar vibration mode, - σ is the surface tension, expressed in N.m'1, - p is the density of the liquid, expressed in kg.m'3, and - R is the radius of curvature of the drop which depends on its volume and the contact angle, expressed in m'3.
    Indeed the natural frequency fg above is calculated for a drop of low viscosity and levitation. For a laid drop, the calculation of the natural frequency must be adapted using the modifications proposed by M. Strani and F. Sabetta, J. Fluid Mech., 141: 233-247 and in the case of viscous liquids, corrections to the formula above described in the article by H. Lamb supra must be taken into account.
    The fundamental frequency can be modulated by means of a wave having a square-wave profile whose amplitude is 0 or 1, and whose frequency is equal to the modulation frequency, or via the product of two harmonic signals at the two frequencies considered. .
    Furthermore, the amplitude of the ultrasonic surface wave is sufficient to cause the drop to deform in an inertio-capillary mode of own vibration. Preferably, the amplitude of the surface ultrasonic wave, which corresponds to the normal displacement of the surface of the support on which the ultrasonic surface wave propagates and measured by laser interferometry, is less than 50 nm. In a particular mode of implementation of the method, it may be less than 5 nm, or even less than 1 nm, or even less than 0.5 nm.
    To generate the ultrasonic surface wave, different devices, powered by an electrical power source and optionally an amplifier 18, may be used. They can be selected from a laser, a sonotone, a transducer. Preferably, the ultrasonic surface wave is generated by means of a transducer connected to the support, preferably in contact with the support.
    In one embodiment, the transducer is an ultrasonic contact transducer, which is particularly suitable for applications where the area of the surface on which the ultrasonic surface area of propagation is greater than 10 -3 m 2. To optimize transducer wave propagation to the support surface, an impedance matched acoustic index transmission gel may be sandwiched between the acoustic transducer and the surface.
    In a first variant, as illustrated in FIG. 1, especially when the substrate has a thickness less than the length of the ultrasonic surface and / or the latter is a Lamb wave, the ultrasonic contact transducer 20a is preferably disposed at right angles to the surface on which ultrasound wave propagates. A second transducer of the same type may be disposed on the surface opposite to that on which the ultrasonic wave propagates.
    In a second variant, as illustrated in FIG. 2, especially when the substrate has a thickness greater than the length of the ultrasonic surface wave and / or the latter is a Rayleigh wave, the ultrasonic contact transducer 20b is disposed, for example by means of a shoe 25, so that the axis of the transducer forms an angle Θ with the normal to the surface on which the ultrasound surface wave propagates, less than 90 ° and whose value can be determined using the Snell-Descartes law.
    In another embodiment, especially for applications where the area of the surface on which the ultrasonic surface wave propagation is less than 10'3 m 2 and in particular microfluidic type applications, the transducer 20 preferably comprises interdigitated combs 30a, 30b arranged in direct contact with the support or in contact with an intermediate layer disposed on the support, the intermediate layer being made of a piezoelectric material, in particular chosen from the group formed by lithium niobate, the nitride of aluminum, lead titano-zircanate, and mixtures thereof. Figures 3 and 4 illustrate devices according to this embodiment. In FIG. 3, the support 5 is made of piezoelectric material and is covered by and in contact with the transducer. Alternatively, as illustrated in Figure 4, the support 5 is a non-piezoelectric material, and is covered by an intermediate layer 35 of a piezoelectric material. A transducer is disposed in contact with the intermediate layer.
    In the case of a medium having a high surface wave propagation area, for example greater than 10 3 m2, or where the surface is covered by a plurality of drops, a plurality of ultrasonic surface waves can be generated by means of a network of transducers. A network of transducers thus makes it possible to limit the effects of screening and wave diffusion by each individual drop of the plurality of drops. The person skilled in the art knows how to adapt the arrangement of the transducers of the array so as to generate ultrasonic surface waves having a sufficient amplitude to cause the drops to deform in an inertio-capillary mode.
    EXTERNAL FORCE
    The external force makes it possible to encourage the sliding of the drop which vibrates according to a specific inertio-capillary mode.
    In particular, sliding can be achieved with a small external force. Preferably, the external force is less than the force required to move the drop on the surface of the support when no ultrasonic wave is generated on the surface of the support.
    Preferably, the external force is chosen from gravitational, inertial, reaction, friction, magnetic, electrical forces, or may result from the setting in motion of a fluid, for example air, or may result from the contact of the drop with a moving body. Preferably, it is a gravitational force, particularly in the variant where the support is inclined. A gravitational force has the advantage of not requiring any particular device to be applied to gout. The external force may, of course, result from a combination of the external forces described in this paragraph. As an illustration, in the case where the support is an inclined windshield of a motor vehicle, the external force may have a gravitational component and an aerodynamic component resulting from the movement of the vehicle. At low speed, the aerodynamic component is weaker than the gravitational component, so that the external force acts to promote the sliding of the drop down. On the contrary, when the vehicle is traveling at high speed, the aerodynamic component can become predominant, and the drop then slides under the action of the external force on the windshield towards the roof of the vehicle.
    EXAMPLES
    A device as illustrated in Figure 3 is prepared to implement the method according to the invention.
    The support is inclined with respect to the horizontal angle α between 10 and 40 °.
    The support is in lithium niobate cut at 128 °, on which is disposed a transducer comprising interdigitated electrodes deposited by photolithography. These electrodes consist of a titanium support layer 20 nm thick and a gold conductive layer with a thickness of 100 nm. The width of the electrodes and their spacing a are both equal to 43.75 μm. They determine the resonant frequency fsaw of the transducer calculated as being equal to fsaw = y = ^ = 19.7 MHz where λ is the wavelength of the longitudinal wave and cs = 3484m / s is the propagation velocity of l Rayleigh wave along the Z crystallographic axis of lithium niobiate. An alternating voltage is applied by an IFR2023A generator and amplified by an Empower brand amplifier, model BBM0D3FE1 then generating Rayleigh waves propagating on the surface of the support. The generated acoustic sound power is calculated from the measurement of the normal displacement of the surface by laser interferometry and the background frequency.
    The transducer is positioned on the support such that the ultrasonic surface foundation propagates in the direction of inclination of the support upwardly.
    Furthermore, a monoatomic layer of octadecyltrichlorosilane is deposited on the surface of the support to make it hydrophobic and to control the contact angle of the drop with the support.
    For each test, a drop of water is deposited on the support.
    Different volumes of drop V are used for the tests: 2 μΐ, 5 μΐ, 10 μΐ and 15 μΐ.
    At rest, without application of a surface ultrasonic wave, the drop is immobile on the surface, regardless of the angle of inclination of the support.
    The waves are then generated continuously. The drop then starts to vibrate and its dynamics are recorded using a high-speed camera Photron SA3 equipped with a bellows and a macro lens with a focal length of 100 mm.
    The position of the contact lines is then determined by processing the images acquired by the camera with the imageJ software, which makes it possible to check whether the drop remains attached to the support or if it is released.
    For the various tests of the example, Weac acoustic Weber number waves less than 0.5 are generated.
    The Weber acoustic Weac number characterizes the ability of a surface ultrasonic wave to deform the surface. It is expressed according to the following equation:
    where: - p is the density of the liquid, expressed in kg.m'3, - As is the amplitude of the ultrasonic background, corresponding to the normal displacement of the surface area measured by laser interferometry, and expressed in m, - ü ) s is the pulsation of the ultrasonic wave, expressed in rad.s'1 (œs = 2nfs where fs is the fundamental frequency of the wave), is the equivalent radius of the drop calculated from the volume V of the drop , Express
    in m'3, - Qr is the Rayleigh angle, obtained from the Snell-Descartes law, which characterizes the direction of propagation of the acoustic wave within the constituent liquid of the drop, and - σ is the surface tension between the support and the drop of liquid, expressed in N.m'1.
    Whatever the inclination of the support, for an ultrasonic wave having an acoustic Weber number Weac of less than 0.2, the drop vibrates in an inertio-capillary mode and is released from its attachment to the support. It then slides along the support downwards, driven by the action of gravity. By way of comparison, when the Weber number is greater than 0.2, the asymmetrical deformation of the drop induced by the surface wave is sufficient for it to deform in the direction of propagation of the wave. For a low angle of inclination, it propagates in the direction of propagation of the wave, going up along the support. For a higher angle, it propagates in the opposite direction.
    For Weber numbers greater than 1, the asymmetrical deformation of the drop may be such that the drop splits. This division of the drop can be effected by atomization of the drop or because of the opposite effects of the gravitational and acoustic forces.
    Of course, the invention is not limited by the examples, provided for illustrative purposes only.
    权利要求:
    Claims (17)
    [1" id="c-fr-0001]
    1. Method for promoting the sliding of at least one drop (15) on a support (5), in which process an ultrasonic surface wave (10) is generated in the support with a sufficient amplitude to cause the drop to deform according to an inertio-capillary mode of clean vibration thus reducing the attachment of the drop to the support, so as to facilitate the displacement of the drop under the effect of an external force, the amplitude of the ultrasonic surface wave being insufficient to cause an asymmetrical deformation of the drop to cause it to move in the absence of the external force in the direction of propagation of the ultrasonic surface wave.
    [2" id="c-fr-0002]
    2. Method according to the preceding claim, wherein the fundamental frequency and the amplitude of the surface ultrasonic wave are adapted so that the ratio of the amplitude of oscillation of the drop on the resting size of the drop is less than or equal to 1.4, or even less than or equal to 1.3, or even less than or equal to 1.15.
    [3" id="c-fr-0003]
    3. Method according to one of the preceding claims, wherein the fundamental frequency of the ultrasonic surface wave is between 1 Mhz and 100 Mhz.
    [4" id="c-fr-0004]
    The method according to any of the preceding claims, wherein the fundamental frequency of the ultrasonic surface wave is modulated at a modulation frequency of between 20 Hz and 10 kHz.
    [5" id="c-fr-0005]
    5. Method according to the preceding claim, wherein the fundamental frequency of the surface wave is modulated by the natural frequency of the symmetrical inertio-capillary mode of vibration proper to the drop.
    [6" id="c-fr-0006]
    The method of any one of the preceding claims, wherein the surface wave is a Rayleigh wave or a Lamb wave.
    [7" id="c-fr-0007]
    7. Method according to any one of the preceding claims, wherein the drop has a size (Φ) less than 5 mm, in particular between 0.1 mm and 1.5 mm, for example equal to 1 mm.
    [8" id="c-fr-0008]
    8. Method according to any one of the preceding claims, wherein the natural frequency of the inertio-capillary mode of own vibration of the drop is between 20 Hz and 10 kHz.
    [9" id="c-fr-0009]
    9. Method according to any one of the preceding claims, wherein the support is of a material having a modulus of elasticity greater than 0.1 MPa.
    [10" id="c-fr-0010]
    10. A method according to any preceding claim, wherein the support is a material selected from piezoelectric materials, polymers, especially thermoplastics, glasses, metals and ceramics.
    [11" id="c-fr-0011]
    11. A method according to any one of the preceding claims, wherein the ultrasonic surface wave is generated by means of a transducer (20; 20a; 20b) connected to the support, preferably in contact with the support.
    [12" id="c-fr-0012]
    12. Method according to the preceding claim, wherein the transducer comprises interdigitated combs (30a, 30b) arranged in direct contact with the support or in contact with an intermediate layer (35) disposed on the support, the intermediate layer being made of a material piezoelectric, in particular chosen from the group formed by lithium niobate, aluminum nitride, lead titano-zircanate, and mixtures thereof.
    [13" id="c-fr-0013]
    13. The method as claimed in any one of the preceding claims, in which the external force is chosen from gravitational, inertial, reaction, magnetic, electric and friction forces, in particular resulting from the setting in motion of a fluid, for example from the air or is a gravitational force or results from the contact of the drop with a moving body.
    [14" id="c-fr-0014]
    14. Process according to any one of the preceding claims, in which the liquid constituting the droplet is chosen from water, in particular rainwater, a biological liquid, for example an animal or human blood, a suitable liquid. to clean the support, a chemical solution, a fuel and their mixtures.
    [15" id="c-fr-0015]
    A method as claimed in any one of the preceding claims, wherein the support is an optically transparent material.
    [16" id="c-fr-0016]
    16. The method as claimed in any one of the preceding claims, in which the support is chosen from a window of a vehicle, a window of a building, a lens of an optical device, a substrate of a laboratory on a chip, an internal wall of a combustion engine, an element of a turbine, for example a blade, an electric cable, an element of the structure of an aircraft, for example a wing, a fuselage or an empennage, an element of a a medical implant, an element of a heat exchanger, an element of a plumbing installation, an element of a ventilation system, an element of an oil extraction system of a well, an element storing food, for example an inner wall of a refrigerator, a wall exposed to the condensation of a liquid.
    [17" id="c-fr-0017]
    17. The method of any of the preceding claims, wherein the surface temperature of the support is greater than 100 ° C.
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    同族专利:
    公开号 | 公开日
    US11090698B2|2021-08-17|
    JP6921082B2|2021-08-18|
    CA3007721A1|2017-06-15|
    FR3044937B1|2018-01-12|
    CN109153045A|2019-01-04|
    EP3386653B1|2020-01-08|
    US20180369880A1|2018-12-27|
    EP3386653A1|2018-10-17|
    JP2019508301A|2019-03-28|
    WO2017097769A1|2017-06-15|
    ES2780923T3|2020-08-27|
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    EP2663475A1|2011-01-10|2013-11-20|Echovista Systems Limited|Clearing precipitation|
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    GB2518136A|2013-07-22|2015-03-18|Echovista Systems Ltd|Ultrasonically clearing precipitation|FR3100998A1|2019-09-25|2021-03-26|École Centrale De Lille|Device for cleaning a support covered with liquid|JPH0647366B2|1986-04-09|1994-06-22|日産自動車株式会社|Water drop removal device|
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    DE102019006919B3|2019-10-06|2020-10-29|ultraTEC Anlagentechnik Münz GmbH|Method and device for ultrasonic deburring of an object|
    KR102343444B1|2019-11-13|2021-12-27|주식회사 마이크로시스템|Sefl cleaning device and method using electrical oscillation and mechanical oscillation|
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    KR102367531B1|2020-04-16|2022-02-24|명지대학교 산학협력단|Sefl cleaning device and method using removing droplet by using electrical resistance heating and mechanical oscillation|
    法律状态:
    2016-12-29| PLFP| Fee payment|Year of fee payment: 2 |
    2017-06-16| PLSC| Publication of the preliminary search report|Effective date: 20170616 |
    2018-01-02| PLFP| Fee payment|Year of fee payment: 3 |
    2019-12-30| PLFP| Fee payment|Year of fee payment: 5 |
    2020-12-28| PLFP| Fee payment|Year of fee payment: 6 |
    2021-12-30| PLFP| Fee payment|Year of fee payment: 7 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1562067|2015-12-09|
    FR1562067A|FR3044937B1|2015-12-09|2015-12-09|METHOD FOR PROMOTING SLIDING AT LEAST ONE DROP ON A SUPPORT|FR1562067A| FR3044937B1|2015-12-09|2015-12-09|METHOD FOR PROMOTING SLIDING AT LEAST ONE DROP ON A SUPPORT|
    CA3007721A| CA3007721A1|2015-12-09|2016-12-06|Method for increasing the ability of at least one droplet to slide over a medium|
    JP2018530762A| JP6921082B2|2015-12-09|2016-12-06|A method of increasing the slip of one or more droplets on a substrate|
    PCT/EP2016/079902| WO2017097769A1|2015-12-09|2016-12-06|Method for increasing the ability of at least one droplet to slide over a medium|
    ES16808608T| ES2780923T3|2015-12-09|2016-12-06|Procedure to promote the sliding of at least one drop on a support|
    EP16808608.0A| EP3386653B1|2015-12-09|2016-12-06|Method for assisting the sliding of at least one drop on a support|
    CN201680081432.7A| CN109153045B|2015-12-09|2016-12-06|Method for increasing the ability of at least one droplet to slide on a medium|
    US16/060,504| US11090698B2|2015-12-09|2016-12-06|Method for increasing the ability of at least one droplet to slide over a medium|
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