Fluidic oscillator

• US 7,908,855 B2
• Filed: 06/09/2005
• Issued: 03/22/2011
• Est. Priority Date: 06/10/2004
• Status: Active Grant

• Current Assignee: Thermofluidics Limited
• Original Assignee: Thermofluidics Limited
• Inventors: Smith, Thomas Charles Brannam
• Primary Examiner(s): Nguyen; Hoang M
• Application Number:
  US11/629,253
• Publication Number:
  US 20080156373A1
• Time in Patent Office: 2,112 Days
• Field of Search: 60516-526
• US Class Current: 60/516
• CPC Class Codes: F04F 1/04 generated by vaporising and condensing
• CPC Class Codes: Y10T 137/0396 Involving pressure control
• CPC Class Codes: Y10T 137/206 Flow affected by fluid contact, energy field or coanda effect [e.g., pure fluid device or system]

Abstract

The invention relates to fluidic oscillators including compressed gas driven pumps and liquid piston and thermoacoustic heat engines and heat pumps in which the intention is to generate large amplitude oscillations by eliminating the dependence of the oscillations on inertia. According to the principle embodiment represented by circuit 200 pressure or temperature variations 27′ drive pressure variations in vessel 11′ causing a flow of further working fluid between vessel 11′ and load 12′ wherein useful work is consumed. Said flow varies out of phase with said pressure variations in vessel 11′ by a first phase angle determined by inter alia the dissipative load 12′ and the capacity of vessel 11′. Oscillations are sustained due to a second phase angle determined by inter alia subcircuit 13′ comprising dissipative processes 260, 262 and capacitive processes 261, 263 wherein each said dissipative process comprises any one, or combination of the following: viscous drag, thermal resistance or mechanical friction and each capacitive process comprises any one, or combination of the following: hydrostatic pressure change due to a flow, fluid compressibility, thermal capacitance, or elasticity; and wherein, the magnitude of the pressure changes in the working fluid increases or remains constant with time due to at least one mechanism giving rise to a gain.

Claims

1. A fluidic oscillator comprising:

at least one vessel arranged to contain a working fluid;

a pressuring means for pressurising said working fluid;

a de-pressurising means for de-pressurising said working fluid;

wherein said pressurising and de-pressurising causes said working fluid to move in and out of said at least one vessel;

at least two time delay mechanisms associated with said working fluid to cause a phase shift between changes in mass and pressure of working fluid in said at least one vessel; and

including a gain mechanism that gives rise to a gain;

wherein each said time delay mechanism comprises a dissipative process and a capacitive process, and wherein said gain is sufficient that in normal operation the magnitude of said pressure changes in said working fluid increases or remains constant with time to permit steady oscillations independent of the inertia of the working fluid; and

further comprising a plurality of heat exchangers for giving rise to a flow of heat into and from said at least one vessel, and

wherein said fluidic oscillator is configured such that, in operation, a total phase shift between a flow of heat through said heat exchangers and a saturation temperature of said working fluid in said at least one vessel is close to a value required to give a maximum difference between mean heat addition and heat rejection temperatures for the pressure amplitude within said working fluid during said operation; and

wherein each said time delay mechanism is dominated by said dissipative process and said capacitive process or wherein said fluidic oscillator further comprises two said working vessels coupled by saturator means and a conduit, said fluidic oscillator being coupled to a load, and said load has inertance with reactive impedance with a magnitude substantially equal to that of a compliance contained within said saturator and said conduit at a frequency of oscillation of the fluidic oscillator.

2. A fluidic oscillator as claimed in claim 1 configured as a heat engine which, when coupled to a load, has a load phase shift between displacement and pressure of working fluid in said load which in said normal operation matches said phase shift between changes mass and pressure of working fluid in said at least one vessel.

3. A fluidic oscillator as claimed in claim 1 configured as a heat engine and further comprising high and low pressure working fluid reservoirs for supplying and removing working fluid respectively to and from said at least one vessel.

4. A fluidic oscillator as claimed in claim 1 configured as a heat engine and further comprising a second vessel from which working fluid is coupled to a load, wherein said working fluid has a passive gas component mainly occupying said second vessel, the fluidic oscillator further comprising a diffusion column or separation chamber to separate said passive component of said working fluid from an active component of said working fluid giving rise to said pressure changes in said working fluid.

5. A fluidic oscillator as claimed in claim 1 configured as a heat engine and further comprising a second vessel from which working fluid is coupled to a load, wherein said working fluid is part vapour and part liquid, said first and second vessels being coupled by a conduit for said vapour and through a restriction for said liquid, for controlling said phase shift between changes mass and pressure of working fluid in said at least one vessel.

6. A pump comprising the fluidic oscillator of claim 1.

13. A fluidic oscillator as claimed in claim 1 comprising first and second said vessels, and wherein said first vessel has a cross-section which is larger at each end than between the ends of said first vessel.

7. A method of operating a fluidic oscillator, the fluidic oscillator comprising:

at least one vessel arranged to contain a working fluid;

a pressuring means for pressurising said working fluid;

a de-pressurising means for de-pressurising said working fluid;

wherein said pressurising and de-pressurising causes said working fluid to move in and out of said at least one vessel;

at least two time delay mechanisms associated with said working fluid to cause a phase shift between changes in mass and pressure of working fluid in said at least one vessel;

a gain mechanism that gives rise to a gain; and

a plurality of heat exchangers for giving rise to a flow of heat into and from said at least one vessel;

the method comprising configuring said fluidic oscillator such that said time delay mechanisms each comprise a dissipative process and a capacitive process to thereby permit steady oscillations independently of the inertia of said working fluid; and

wherein, in operation, a total phase shift between a flow of heat through said heat exchangers and a saturation temperature of said working fluid in said at least one vessel is close to a value required to give a maximum difference between mean heat addition and heat rejection temperatures for the pressure amplitude within said working fluid during said operation; and

wherein each said time delay mechanism is dominated by said dissipative process and said capacitive process or wherein said fluidic oscillator further comprises two said working vessels coupled by saturator means and a conduit, said fluidic oscillator being coupled to a load, and said load has inertance with reactive impedance with a magnitude substantially equal to that of a compliance contained within said saturator and said conduit at a frequency of oscillation of the fluidic oscillator.

12. A method as claimed in claim 7 wherein said heat exchangers are configured to alternately evaporate and condense said working fluid, and wherein, in operation, said oscillator has a load phase shift and a feedback phase shift each of substantially 90 degrees and a thermal phase angle of substantially 0 degrees.

8. A fluidic oscillator comprising:

a. first and second vessels arranged to contain a working fluid, the cross sectional area of said second vessel being minimised within limits set by surface tension and the cross sectional area of the first vessel being less than two times greater than the cross sectional area of the second vessel;

b. a first coupling conjoining the first and second vessels so as to subject said two vessels to a common pressure;

c. a second coupling to communicate a volume of working fluid contained within the first vessel to the second vessel;

d. drive mechanism to provide pressure changes in the working fluid, located substantially within the second vessel;

e. a load comprising dissipative and reactive components giving rise to a load phase angle between the mass of working fluid contained within the first vessel and the pressure changes therein due to said load;

f. a third coupling to couple the working fluid in the first vessel to said load such that changes in the volume of the working fluid contained in said first and second vessels give rise to transfer of work between the first vessel and the load;

g. a gain mechanism configured to provide viscous drag, hydrostatic pressure changes due to a flow, and thermal resistance;

h. the compliance of said working fluid and the reactive component of said load being arranged to resonate at frequency of oscillation, determined by said dissipative and reactive components and said gain.

10. A fluidic oscillator according to claim 8, in which said working fluid is part liquid and part gas or vapour within the vessels, said fluidic oscillator further comprising a coupling to permit a flow of liquid between the first vessel and the second vessel driven by the hydrostatic pressure difference at a lower portion of each said vessel due to the liquid therein, and wherein said coupling to permit said flow of liquid is further configured to provide a viscous drag to give rise to a phase shift between the liquid levels in said first and second vessels.

11. A fluidic oscillator according to claim 8, said fluidic oscillator further comprising a coupling to connect said vessels to reservoirs of high or low pressure, located substantially within the second vessel, and pressure sources having a pressure difference there between coupled to said pressure reservoirs.

14. A fluidic oscillator as claimed in claim 8 wherein said first vessel has a waist in a central region of first vessel.

9. A fluidic oscillator comprising:

a. first and second vessels arranged to contain a working fluid;

b. a first coupling conjoining the first and second vessels so as to subject said two vessels to a common pressure;

c. a second coupling to communicate a volume of working fluid contained within the first vessel to the second vessel;

d. a drive mechanism provide pressure changes in the working fluid, located substantially within the second vessel;

e. a load comprising dissipative and reactive components giving rise to a load phase angle between the mass of working fluid contained within the first vessel and the pressure changes therein due to said load;

f. a third coupling to couple the working fluid in the first vessel to said load such that changes in the volume of the working fluid contained in said first and second vessels give rise to transfer of work between the first vessel and the load;

g. a gain mechanism configured to provide viscous drag, hydrostatic pressure changes due to a flow, and thermal resistance;

h. the compliance of said working fluid and the reactive component of said load being arranged to resonate at the frequency of the oscillations, determined by said dissipative and reactive components and said gain.

15. A fluidic oscillator as claimed in claim 9 wherein said first vessel has a waist in a central region of first vessel.