Capillary fluid switch with asymmetric bubble chamber

• US 6,360,775 B1
• Filed: 12/23/1998
• Issued: 03/26/2002
• Est. Priority Date: 12/23/1998
• Status: Expired due to Fees

• Current Assignee: Avago Technologies General IP PTE Limited (Broadcom, Inc.)
• Original Assignee: Agilent Technologies, Inc.
• Inventors: Field, Leslie A., Donald, David K., Barth, Phillip W.
• Primary Examiner(s): CHAMBERS, A MICHAEL
• Application Number:
  US09/221,655
• Time in Patent Office: 1,189 Days
• Field of Search: 137/803, 137/833, 137/828, 385/17, 385/18
• US Class Current: 137/828
• CPC Class Codes: G02B 26/004 based on a displacement or a deformation of a fluid
• CPC Class Codes: G02B 6/3538 based on displacement or deformation of a liquid controlling the intensity of light by displacement or deformation of a fluid in general G02B26/004; fluid-filled lens of variable focal length G02B3/14
• CPC Class Codes: G02B 6/3544 2D constellations, i.e. with switching elements and switched beams located in a plane
• CPC Class Codes: G02B 6/3576 Temperature or heat actuation thermal forces controlling reflecting elements in general G02B26/0866; thermo-optic devices G02F1/0147
• CPC Class Codes: Y10T 137/206 Flow affected by fluid contact, energy field or coanda effect [e.g., pure fluid device or system]
• CPC Class Codes: Y10T 137/2196 Acoustical or thermal energy
• CPC Class Codes: Y10T 137/2224 Structure of body of device

Abstract

A switching device for controlling fluid motion. The device includes a capillary filled with a first fluid into which a wall-confined bubble of a second fluid is introduced to achieve a first switching event. Capillary geometry and wetting properties provide a pressure-related asymmetric energy potential distribution for controlling the flow of the bubble, and the device is called an asymmetric bubble chamber, or ABC. The bubble is initially trapped in an energy potential well, and upon increase of its volume moves from the well into a region of low energy potential to achieve a second switching event. The first switching event may be blocking of a fluid channel or reflection of an optical beam in an optical crosspoint switch, while the second switching event may be unblocking of a fluid channel or restoration of transmission of an optical beam. The increase in bubble volume between the first and second switching events can act as the stroke of a fluidic piston to pump a volume the first fluid within the capillary. The device can be employed to thermally degas a liquid. The use of large-magnitude geometry-related energy potentials permits rapid cyclical operation of the device in a manner resistant to mechanical shock.

Claims

1. A fluid-control method comprising the steps of:

introducing a wall-confined bubble into a gate region of a capillary fluid channel;

maintaining said bubble in said gate region using a barrier region of higher energy potential with respect to said bubble than said gate region and a source region of higher energy potential than said barrier region; and

increasing the energy of said bubble so that it exits said gate region into a drain region via said barrier region.

2. A fluid-control method as recited in claim 1 wherein, in said increasing step, said bubble extends from said gate region to said drain region before exiting said gate region.

24. The device according to claim 1 wherein the source region is separated from the barrier region and the drain region and acts as a source of the first fluid which refills the gate region as the bubble moves from the gate region.

25. The device according to claim 1 wherein the drain region has proximate to the barrier region a portion wherein the energy potential decreases with increasing distance from the barrier region.

26. The device according to claim 1 wherein the first fluid is a liquid and the second fluid is a gas.

27. The device according to claim 1 further comprising a means for introducing a bubble into the gate region and a means for increasing the energy of the bubble in the capillary.

28. The device according to claim 27 wherein the means for introducing the bubble is separate from the means for increasing the energy of the bubble.

29. The device according to claim 27 wherein the means for introducing the bubble is the same as the means for increasing the energy of the bubble.

30. The device according to claim 27 wherein the means for introducing the bubble is the same as the means for increasing the energy of the bubble and increases the size of the bubble to overcome the difference in energy potentials between the gate region and the barrier region.

31. The device according to claim 27 wherein a gaseous-bubble generator is used for introducing the bubble.

32. The device according to claim 27 wherein the means for introducing the bubble introduces the bubble into the capillary by means selected from the group consisting of thermal, electrical, chemical, electrolytic, pneumatic, hydraulic, optical, inertial, ultrasonic, and microfluidic means.

33. The device according to claim 1 wherein such energy potentials are determined by capillary geometry variations with distance in the capillary, and in which the capillary wetting properties of both the first fluid and the second fluid are substantially constant with distance in the capillary.

34. The device according to claim 1 wherein such energy potentials are determined by variations in capillary wetting properties of the first fluid and the second fluid with distance in the capillary.

35. The device according to claim 1 further comprising multiple source regions.

36. The device according to claim 1 further comprising multiple barrier regions.

37. The device according to claim 36 wherein the energy potential of one of the barrier regions can be changed relative to the other barrier regions thermally.

38. The device according to claim 1 wherein the capillary further comprises an additional set of gate-barrier-drain regions downstream to the gate region, barrier region, and drain region.

39. The device according to claim 1 wherein the first fluid comprises a hydrophilic liquid, the regions having substantially rectangular cross sections and of substantially uniform height but differing widths, the gate region having a gate width, the barrier region having a barrier width less than the gate width, the drain region having a drain width greater than the gate width, the source region having a source width less than the barrier width, the device further comprising an electrical resistor heater adjacent to the gate region, whereby a wall-confined gas phase bubble which substantially fills the volume of the gate region can be created within the liquid by heating, and whereby the volume of the gas phase bubble can be increased to fill both the gate region and the barrier region and to intrude into the drain region, and whereby the volume of the gas phase bubble can be further increased to cause it to be siphoned from the gate region to the drain region.

40. The device according to claim 1 wherein in the capillary, one or more regions are in a different plane than the other regions.

3. A fluid-control device comprising:

a capillary fluid channel for confining a first fluid, having source, gate, barrier, and drain regions such that said gate region is bounded by said source and barrier regions, and said barrier region is bounded by said gate and said drain regions, said regions being ordered as drain, gate, barrier, and source in terms of increasing potential relating to a wall-confined bubble of a second fluid; and

energizer means for increasing the energy of said wall-confined bubble while it is in said gate region.

4. A device as recited in claim 3 wherein said energizer means also introduces said bubble into said gate region.

5. A device as recited in claim 3 wherein, as long as the energy of said bubble is below a first energy level, said source region and said barrier region maintain said bubble in said gate region.

6. A device as recited in claim 5 wherein, when said energizer means increases the energy of said bubble sufficiently said bubble exits from said gate region to said drain region via said barrier region.

7. A device as recited in claim 5 wherein, when said energizer means increases the energy of above a second energy level greater than said first energy level, said bubble extends from said gate region to said drain region.

8. A device as recited in claim 7 wherein, when said energizer means increases the energy of said bubble above a third energy level greater than said second energy level, said bubble exits from said gate region to said drain region via said barrier region.

9. A device for controlling the movement of a fluid, comprising:

(a) a capillary having regions of differing energy potential within the capillary, the energy potential pertaining to the introduction of a wall-confined bubble of a second fluid into the capillary when said capillary is filled with a first fluid immiscible with the second fluid, the regions including a source region, a gate region, a barrier region, and a drain region, which are connected in that spatial sequential order, and wherein the energy potentials are ordered such that

(i) the energy potential of the source region is great than the energy potential of the barrier region;

(ii) the energy potential of the barrier region is greater than the energy potential of the gate region;

(iii) the energy potential of the gate region is greater than the energy potential of the drain region;

(b) a bubble supplier for introducing into the gate region a bubble of the second fluid; and

(c) a power supply for increasing the energy of the bubble to overcome the barrier in energy potential between the gate region and the drain region such that the energy potential difference between the gate region and the drain region will cause the bubble to move from the gate region past the barrier region to the drain region.

10. A method for controlling the movement of a bubble in a channel, comprising:

(a) introducing a bubble of a second fluid into a channel having regions of differing energy potential within the capillary, the energy potential pertaining to the introduction of a wall-confined bubble of a second fluid into the capillary filled with a first fluid immiscible with the second fluid, the regions including a gate region, a barrier region, and a drain region, which are connected in that spatial sequential order, and wherein the energy potentials are ordered such that

(i) the energy potential of the barrier region is greater than the energy potential of the gate region;

(ii) the energy potential of the gate region is greater than the energy potential of the drain region;

(b) subsequently increasing the energy of the bubble to cause the bubble to move downstream from the gate region to the drain region due to the energy potential difference between the gate region and the drain region; and

(c) flowing the first fluid to the gate region from a source region connected to the gate region in the capillary as the bubble moves from the gate region.

11. The method according to claim 10 comprising introducing the bubble in the gate region and increasing the size of the bubble to overcome the barrier in energy potential between the gate region and the drain region.

12. The method according to claim 10 wherein the bubble of the second fluid is moved using no solid mechanical moving part.

13. The method according to claim 10 wherein the bubble of the second fluid is moved solely by differences in fluid pressures arising from energy potential differences within the capillary.

14. The method according to claim 10 wherein the first fluid is a liquid and the second fluid is gaseous.

15. A device for pumping a liquid, comprising:

a capillary having regions of differing energy potential within the capillary, the energy potential pertaining to the introduction of a wall-confined bubble of a fluid (bubble fluid) into the capillary when said capillary is filled with a liquid immiscible with the bubble fluid, the regions including a gate region, a barrier region, and a drain region, which are connected in that spatial sequential order, the regions further including a source region connected to the gate region to provide the liquid to the gate region, wherein the energy potentials are ordered such that

(a) the energy potential of the source region is greater than the energy potential of the barrier region;

(b) the energy potential of the barrier region is greater than the energy potential of the gate region;

(c) the energy potential of the gate region is greater than the energy potential of the drain region; and

wherein a bubble of the bubble fluid can be introduced into the gate region of the capillary filled with the liquid and confined by the gate region capillary wall circumferentially, the energy of the bubble can be increased to cause the bubble to move downstream due to the energy potential difference between the gate region and the drain region, the bubble pushing the liquid from the gate region past the barrier region to the drain region and beyond;

whereupon the gate region is replenished with additional liquid coming from the source region.

16. The device according to claim 15 wherein the liquid is fluiphilic to the capillary walls and the bubble fluid is gaseous, the regions having substantially rectangular cross sections and of substantially uniform height but differing widths, the gate region having a gate width, the barrier region having a barrier width less than the gate width, the drain region having a drain width greater than the gate width, the source region having a source width less than the barrier width, the device further comprising an electrical resistor heater adjacent to the gate region, whereby a wall-confined gas phase bubble which substantially fills the volume of the gate region can be created within the liquid by heating, and whereby the volume of the gas phase bubble can be increased to fill both the gate region and the barrier region and to intrude into the drain region, and whereby the volume of the gas phase bubble can be further increased to cause it to move from the gate region to the drain region.

17. A device for degassing a liquid, comprising:

(a) a gate channel portion in a channel at which the liquid can be heated to obtain from dissolved gas a bubble which is wall-confined in the gate channel portion;

(b) a barrier channel portion in the channel, connected to the gate channel portion downstream thereto;

(c) a drain channel portion in the channel, connected to the barrier channel portion downstream thereto;

wherein the gate channel portion, the barrier channel portion, and the drain channel portion are in fluid communication in that spatial sequential order and having differing energy potentials, the energy potentials pertaining to a wall-confined bubble in the liquid;

the barrier channel portion having an energy potential greater than the energy potential of the gate channel portion, the gate channel portion having an energy potential greater than that of the drain channel portion;

(d) one or more source channel portions connected to the gate channel portion such that liquid can flow from each source channel to the gate channel portion for degassing, each source channel portion having dimensions to effect an energy potential greater than the energy potential of the gate channel portion; and

(e) heater for heating the liquid near the gate channel portion to release gas thereinto;

wherein gas released into the gate channel portion will increase the size of the bubble therein to cause the bubble to move from the gate channel portion to the drain channel portion due to the difference in energy potentials between the gate channel portion and the drain channel portion.

18. The device according to claim 17 wherein the liquid is fluiphilic to the capillary walls, and the gate, the source, barrier, and drain channel portions have substantially rectangular cross sections and of substantially uniform height but differing widths, the gate region having a gate width, the barrier channel portion having a barrier width less than the gate width, the drain channel portion having a drain width greater than the gate width, the source region having a source width less than the barrier width, the device further comprising an electrical resistor heater adjacent to the gate region, whereby a wall-confined gas phase bubble which substantially fills the volume of the gate region can be created within the liquid by heating, and whereby the volume of the gas phase bubble can be increased to fill both the gate region and the barrier region and to intrude into the drain region, and whereby the volume of the gas phase bubble can be further increased to cause it to move from the gate region to the drain region.

19. A liquid-controlling valve, comprising:

(a) a capillary having a source region, gate region, barrier region, and drain region, spatially connected in that sequence, the regions having substantially rectangular cross-sections with substantially uniform height and differing widths, the gate region has a gate width, the barrier region having a barrier width less than the gate width, the drain region having a drain width greater than the gate width, the source region having a source width less than the barrier width; and

(b) electrical resistor heater adjacent to the gate region, whereby when the capillary is filled with a liquid a wall-confined gas phase bubble that substantially fills the volume of the gate region can be created within the liquid by heating, thereby blocking the flow of the liquid between the source region and the drain region, and whereby the volume of the gas phase bubble can be increased to fill both the gate region and the barrier region and to intrude into the drain region, and whereby the volume of the gas phase bubble can be further increased to cause it to move from the gate region to the drain region;

thereby unblocking flow of the liquid from the source region to the drain region.

20. The valve according to claim 19 wherein the width of the drain region increases with distance from the barrier region.

21. The valve according to claim 19 wherein the volume of the bubble decreases while it is within the drain region, thereby unblocking flow of the liquid from the drain region to the source region.

22. The valve according to claim 19 wherein the bubble can separate from contact with one or more walls of the capillary within the drain region, thereby unblocking flow of the liquid from the drain region to the source region.

23. A device for controlling movement of a bubble in a capillary, comprising:

a capillary having regions of differing energy potentials pertaining to the introduction of a wall-confined bubble of a second fluid into the capillary when said capillary is filled with a first fluid immiscible with the second fluid, the regions including a gate region, a barrier region, and a drain region connected in that spatial sequential order, the regions further including a source region connected to the gate region to provide the first fluid to the gate region, wherein the energy potentials are ordered such that

(a) the energy potential of the source region is greater than the energy potential of the barrier region;

(b) the energy potential of the barrier region is greater than the energy potential of the gate region;

(c) the energy potential of the gate region is greater than the energy potential of the drain region; and

wherein a wall-confined bubble of the second fluid can be introduced into the capillary filled with the first fluid and the energy of the bubble can be increased sufficiently to cause the bubble to move from the gate region to the drain region due to the energy potential difference between the gate region and the drain region.