Droplet generation method and device

• US 6,659,364 B1
• Filed: 08/14/2001
• Issued: 12/09/2003
• Est. Priority Date: 02/15/1999
• Status: Expired due to Fees

• Current Assignee: The Technology Partnership PLC (TTP Group Ltd.)
• Original Assignee: The Technology Partnership PLC (TTP Group Ltd.)
• Inventors: Blakey, David Mark, Humberstone, Victor Carey
• Primary Examiner(s): HWU, DAVIS D
• Application Number:
  US09/913,406
• Time in Patent Office: 847 Days
• Field of Search: 239/4, 239/102.2, 239/102.1, 239/558, 239/589.1, 239/590.3, 239/145, 239/DIG.12, 239/101, 310/324, 310/331, 310/332, 310/321, 310/328
• US Class Current: 239/4
• CPC Class Codes: B05B 17/0646 Vibrating plates, i.e. plates being directly subjected to the vibrations, e.g. having a piezoelectric transducer attached thereto
• CPC Class Codes: B41J 2202/15 Moving nozzle or nozzle plate

Abstract

A method of and apparatus for generating liquid droplets from an aperture in a membrane are disclosed in which the aperture has a diameter φ at one face which is at most as large as its diameter at the other face, and a liquid is provided to the one face of the membrane adjacent the aperture. The liquid has a surface tension σ and density ρ. A pressure bias is applied such that the pressure of the liquid at the one face of the membrane is lower than the pressure immediately adjacent to the opposing face of the membrane, and while the bias pressure is applied, the membrane is vibrated at a frequency f which is determined by the relationship: $f\le {\left(\frac{5\pi \sigma }{\rho {\phi }^3}\right)}^{1/2}$

in order to generate droplets emerging from the other face.

Claims

1. A method of generating liquid droplets from an aperture in a membrane, the aperture having a diameter φ

at one face at most as large as its diameter at the other face, the method comprising;

providing a liquid to the one face of the membrane adjacent the aperture, the liquid having a surface tension σ and

density ρ

;

applying a pressure bias such that the pressure of the liquid at the one face of the membrane is lower than the pressure immediately adjacent to the opposing face of the membrane; and

while the bias pressure is applied, vibrating the membrane at a frequency f which is determined by the relationship;

$f\le <br><br>{\left(\frac{8<br><br>\text{\hspace{1em}<br><br>}<br><br>\mathrm{\pi <br><br>}<br><br>\text{\hspace{1em}<br><br>}<br><br>\mathrm{\sigma <br><br>}}{27<br><br>\text{\hspace{1em}<br><br>}<br><br>\mathrm{\rho <br><br>}<br><br>\text{\hspace{1em}<br><br>}<br><br>{\mathrm{\phi <br><br>}}^3}\right)}^{1/2}$

in order to generate droplets emergent from the other face.

2. A method according to claim 1, wherein the frequency f is determined by the relationship:

$f\le <br><br>{\left(\frac{2.13\times <br><br>{10}^{-5}·<br><br>\mathrm{\pi <br><br>}}{{\mathrm{\phi <br><br>}}^3}\right)}^{1/2}.$

3. A method according to claim 1, wherein the liquid is brought to the perforate membrane at a pressure equal to that immediately in front of the perforate membrane.

4. A method according to claim 3, wherein, when atomisation into droplets is required, the pressure of the liquid body that contacts those perforations is reduced to below the pressure immediately in front of the perforate membrane.

5. A method according to claim 3, wherein, when atomisation into droplets is required, the pressure of the atmosphere immediately in front of the membrane is increased.

6. A method according to claim 1, wherein the liquid is brought to the perforate membrane at a higher pressure that is insufficient, of itself, to cause the liquid to flow through the perforations.

7. A droplet generator for generating droplets of a liquid having a surface tension σ

and density ρ

, the droplet generator comprising;

a membrane having a first face and a second face, an aperture extending through the membrane from the first face to the second face, the aperture being of a diameter φ

at the first face at most as large as its diameter at the second face;

means for applying a pressure bias such that the pressure of the liquid at the first face of the membrane is lower than the pressure immediately adjacent to the second face of the membrane; and

a vibration generating means for causing the membrane to vibrate at a frequency f which is determined by the relationship;

$f\le <br><br>{\left(\frac{8<br><br>\text{\hspace{1em}<br><br>}<br><br>\mathrm{\pi <br><br>}<br><br>\text{\hspace{1em}<br><br>}<br><br>\mathrm{\sigma <br><br>}}{27<br><br>\text{\hspace{1em}<br><br>}<br><br>\mathrm{\rho <br><br>}<br><br>\text{\hspace{1em}<br><br>}<br><br>{\mathrm{\phi <br><br>}}^3}\right)}^{1/2}$

in order to generate droplets emergent from the other face.

8. A droplet generator according to claim 7, wherein the frequency f is determined by the relationship:

$f\le <br><br>{\left(\frac{2.13\times <br><br>{10}^{-5}·<br><br>\mathrm{\pi <br><br>}}{{\mathrm{\phi <br><br>}}^3}\right)}^{1/2}.$

9. A droplet generator according to claim 7, wherein the atomisation head includes an aerosol generation device.

10. A droplet generator according to claim 7, wherein the atomisation head includes an ink jet device.

11. A droplet generator according to claim 7, wherein the vibration generating means is integrally or intimately formed with the membrane.

12. A liquid atomisation head for a droplet generator for generating droplets of a liquid having a surface tension a and density p, the liquid atomisation head comprising:

a membrane having a first face and a second face, an aperture extending through the membrane from the first face to the second face, the aperture being of a diameter φ

at the first face at most as large as its diameter at the second face; and

a vibration generating means for causing the membrane to vibrate at a frequency f which is determined by the relationship;

$f\le <br><br>{\left(\frac{8<br><br>\text{\hspace{1em}<br><br>}<br><br>\mathrm{\pi <br><br>}<br><br>\text{\hspace{1em}<br><br>}<br><br>\mathrm{\sigma <br><br>}}{27<br><br>\text{\hspace{1em}<br><br>}<br><br>\mathrm{\rho <br><br>}<br><br>\text{\hspace{1em}<br><br>}<br><br>{\mathrm{\phi <br><br>}}^3}\right)}^{1/2}$

in order to generate droplets emergent from the other face.

13. A liquid atomisation head according to claim 12, wherein the frequency f is determined by the relationship:

$f\le <br><br>{\left(\frac{2.13\times <br><br>{10}^{-5}·<br><br>\mathrm{\pi <br><br>}}{{\mathrm{\phi <br><br>}}^3}\right)}^{1/2}.$