Split mode traveling wave ring-resonator

Claim 2

A split mode traveling wave ring resonator comprising: A. a ring resonator means including at least one perturbation means in the characteristic impedance around the ring, such that the ring resonator has two standing wave resonant modes; one of these modes shifted around said ring resonator means from the other, and having resonant frequencies of approximately f s +1/2Δf 1 and f s 1/2Δf 2 , where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively; all other standing wave modes of the ring resonator are essentially non-overlapping with f s and B. at least one wave generating means coupled with the ring resonator, said wave generating means all being of about the same phase and positioned around the ring approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the wave generating means constructed to couple wave energy of frequency f s to both modes of the resonator with roughly equal strength.

Claim 3

The split mode traveling wave ring resonator of claim 1 in which said resonator and resonant modes are of the acoustic type, with either a gas, liquid, or solid wave medium.

Claim 4

The split mode traveling wave ring resonator of claim 1 in which said resonator and resonant modes are of the solid surface acoustic wave type.

Claim 5

The split mode traveling wave ring resonator of claim 1 in which said resonator and resonant modes are of the liquid surface wave type.

Claim 6

The split mode traveling wave ring resonator of claim 4 in which said liquid is water.

Claim 7

The split mode traveling wave ring resonator of claim 1 in which said resonator and resonant modes are of the mechanical type.

Claim 8

The split mode traveling wave ring resonator of claim 1 in which said resonator and resonant modes are of the electromagnetic type.

Claim 9

The split mode traveling wave ring resonator of claim 1 in which said resonator is made of discrete elements.

Claim 10

A circular surface wave motor comprising: a circular ring resonator made of solid material, with at least one wave generating means coupled with the surface wave modes of the ring resonator, and a rigid circular rotor in contact with that surface of the ring resonator at the positions of the surface wave crests; the rotor being made to rotate relative to the circular ring resonator by the motion of the traveling surface waves crests, wherein the improvement comprises: A. said circular ring resonator further including at least one perturbation means in the characteristic impedance around the rings, such that the ring resonator has two standing wave resonant modes; one of these modes shifted around said ring resonator from the other, and having resonant frequencies of approximately f s +1/2Δf 1 and f s -1/2Δf 2 , where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively; all other standing wave resonant modes of the ring resonator are essentially non-overlapping with f s and B. said wave generating means furthermore being all of approximately the same phase, positioned around the ring resonator approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the wave generating means constructed to couple wave energy of frequency f s to both modes of the resonator with roughly equal strengths.

Claim 11

A circular surface wave motor comprising: a circular ring resonator made of solid material, with at least one wave generating means coupled with the surface wave modes of the ring resonator, and a rigid circular rotor in contact with that surface of the ring resonator at the positions of the surface wave crests; the rotor being made to rotate relative to the circular ring resonator by the motion of the traveling surface waves crests, wherein the improvement comprises: A. said circular ring resonator further including at least one perturbation means in the characteristic impedance around the rings, such that the ring resonator has two standing wave resonant modes; one of these modes shifted around said ring resonator from the other, and having resonant frequencies of approximately f s +1/2Δf 1 and f s -1/2Δf 2 , where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively; all other standing wave resonant modes of the ring resonator are essentially non-overlapping with f s and B. said wave generating means furthermore being all of approximately the same phase, positioned around the ring resonator approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the wave generating means constructed to couple wave energy of frequency f s to both modes of the resonator with roughly equal strengths.

Claim 12

A traveling wave heat engine/pump comprising: at least one regenerator section with acoustical input and output, and thermal input and output, and an acoustical circuit connected to said acoustical input and output and constructed to feed back some of the acoustical waves from the acoustical output to the acoustical input, the feedback part of the acoustical circuit and the acoustical path between the input and output through the regenerator section comprising an acoustic ring resonator, wherein the improvement comprises: A. said acoustical ring resonator further including at least one perturbation means in the characteristic impedance around the ring, such that the ring resonator has two standing wave resonant modes; one of these modes shifted around said ring resonator from the other, and having resonant frequencies of approximately f s +1/2f 1 and f s -1/2Δf 2 , where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively; all other standing wave modes of the ring resonator are essentially non-overlapping with f s , and B. said regenerator section furthermore being positioned around the ring resonator approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the regenerator section constructed to couple wave energy of frequency f S to both modes of the resonator with approximately equal strength.

Claim 13

A traveling wave heat engine/pump comprising: at least one regenerator section with acoustical input and output, and thermal input and output, and an acoustical circuit connected to said acoustical input and output and constructed to feed back some of the acoustical waves from the acoustical output to the acoustical input, the feedback part of the acoustical circuit and the acoustical path between the input and output through the regenerator section comprising an acoustic ring resonator, wherein the improvement comprises: A. said acoustical ring resonator further including at least one perturbation means in the characteristic impedance around the ring, such that the ring resonator has two standing wave resonant modes; one of these modes shifted around said ring resonator from the other, and having resonant frequencies of approximately f s +1/2f 1 and f s -1/2Δf 2 , where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively; all other standing wave modes of the ring resonator are essentially non-overlapping with f s , and B. said regenerator section furthermore being positioned around the ring resonator approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the regenerator section constructed to couple wave energy of frequency f S to both modes of the resonator with approximately equal strength.

Claim 14

A resonant traveling wave heat engine/pump comprising: a regenerator section with acoustical input and output and thermal input and output, and an acoustical circuit connected to said acoustical input and output and constructed to feed back some of the acoustical waves from the acoustical output to the acoustical input, the feedback part of the acoustical circuit and the acoustical path between the input and output through the regenerator section comprising an acoustic ring resonator, wherein the improvement comprises: A. said acoustic ring resonator further including at least one perturbation means in its characteristic impedance around the ring, such that the ring resonator has two standing wave resonant modes; one of these mode shifted around the ring resonator from the other, and having resonant frequencies of approximately f s +(Δf 1 /2g) and f s -(Δf 2 /2g), where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively, and g is the regenerator impedance enhancement factor which is greater than unity; all other standing wave modes of the ring resonator are essentially non-overlapping with f s , and B. said regenerator section furthermore positioned around the ring approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the regenerator section constructed to couple wave energy of frequency f S to both modes of the resonator with approximately equal strength.

Claim 15

A resonant traveling wave heat engine/pump comprising: a regenerator section with acoustical input and output and thermal input and output, and an acoustical circuit connected to said acoustical input and output and constructed to feed back some of the acoustical waves from the acoustical output to the acoustical input, the feedback part of the acoustical circuit and the acoustical path between the input and output through the regenerator section comprising an acoustic ring resonator, wherein the improvement comprises: A. said acoustic ring resonator further including at least one perturbation means in its characteristic impedance around the ring, such that the ring resonator has two standing wave resonant modes; one of these mode shifted around the ring resonator from the other, and having resonant frequencies of approximately f s +(Δf 1 /2g) and f s -(Δf 2 /2g), where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively, and g is the regenerator impedance enhancement factor which is greater than unity; all other standing wave modes of the ring resonator are essentially non-overlapping with f s , and B. said regenerator section furthermore positioned around the ring approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the regenerator section constructed to couple wave energy of frequency f S to both modes of the resonator with approximately equal strength.

Claim 16

A resonant traveling wave heat engine/pump comprising: two regenerator sections each with acoustical input and output and thermal input and output, and an acoustical circuit connected to the acoustical inputs and outputs of said regenerator sections and constructed to channel some of the acoustical waves from the acoustical output of one regenerator section to the acoustical input of the second regenerator section and some of the acoustical output of tht second regenerator section to the acoustical input of the first regenerator section, said acoustical circuit and the acoustical paths between the inputs and outputs through the regenerator sections comprising an acoustic ring resonator, wherein the improvement comprises: A. said acoustic ring resonator further including at least one perturbation means in its characteristic impedance around the ring, such that said ring resonator has two standing wave resonant modes; one of these modes shifted around the ring resonator from the other, and having resonant frequencies of approximately f s +(Δf 1 /2g) and f s -(Δf 2 /2g), where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively, and g is the regenerator impedance enhancement factor which is greater than unity; all other standing wave modes of the ring resonator being essentially non-overlapping with f s , and B. said regenerator sections furthermore positioned at opposition around the ring and also each approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the regenerator sections constructed to couple wave energy to both modes of the resonator with approximately equal strengths.

Claim 17

A resonant traveling wave heat engine/pump comprising: two regenerator sections each with acoustical input and output and thermal input and output, and an acoustical circuit connected to the acoustical inputs and outputs of said regenerator sections and constructed to channel some of the acoustical waves from the acoustical output of one regenerator section to the acoustical input of the second regenerator section and some of the acoustical output of tht second regenerator section to the acoustical input of the first regenerator section, said acoustical circuit and the acoustical paths between the inputs and outputs through the regenerator sections comprising an acoustic ring resonator, wherein the improvement comprises: A. said acoustic ring resonator further including at least one perturbation means in its characteristic impedance around the ring, such that said ring resonator has two standing wave resonant modes; one of these modes shifted around the ring resonator from the other, and having resonant frequencies of approximately f s +(Δf 1 /2g) and f s -(Δf 2 /2g), where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively, and g is the regenerator impedance enhancement factor which is greater than unity; all other standing wave modes of the ring resonator being essentially non-overlapping with f s , and B. said regenerator sections furthermore positioned at opposition around the ring and also each approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the regenerator sections constructed to couple wave energy to both modes of the resonator with approximately equal strengths.

Claim 18

A split mode rotating wave resonator comprising: A. a simply-connected resonator, approximating an object of revolution including at least one perturbation means in the cylindrical symmetry, such that the resonator has two standing wave resonant modes, with one of these mode rotated around the axis of symmetry from the other, and with resonant frequencies of approximately f s +1/2Δf 1 and f s -1/2Δf 2 , where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively; all other standing wave modes of the resonator being essentially non-overlapping with f s , and B. at least one generating means coupled with the resonator, said wave generating means all being of about the same phase and positioned around the ring approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the wave generating means constructed to couple wave energy of frequency f s to both modes of the resonator with approximately equal strengths.

Claim 19

A split mode rotating wave resonator comprising: A. a simply-connected resonator, approximating an object of revolution including at least one perturbation means in the cylindrical symmetry, such that the resonator has two standing wave resonant modes, with one of these mode rotated around the axis of symmetry from the other, and with resonant frequencies of approximately f s +1/2Δf 1 and f s -1/2Δf 2 , where f s is the operating frequency of the resonator and Δf 1 and Δf 2 are the half power bandwidths of these first and second standing wave modes respectively; all other standing wave modes of the resonator being essentially non-overlapping with f s , and B. at least one generating means coupled with the resonator, said wave generating means all being of about the same phase and positioned around the ring approximately equidistant from two adjacent standing wave maxima, one a maxima of one of the modes and one of the other mode, the wave generating means constructed to couple wave energy of frequency f s to both modes of the resonator with approximately equal strengths.

Claim 20

The split mode rotating wave resonator of claim 13 in which the resonator and resonant modes are of the water wave type.