# US 9,949,355 B2 · Plasma flow interaction simulator

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- Number: US 9,949,355 B2
- Document ID: US9949355B2
- Status: Granted
- Kind: B2
- Application number: 15/343,024
- Filed: 2016-11-03
- Published: 2017-03-16
- Granted: 2018-04-17
- Earliest claimed: 2007-10-24
- Assignees: Torus Tech LLC
- Applicants: Torus Tech, Inc.
- Inventors: Nassim Haramein
- Web page: https://patentgrep.com/patent/US9949355B2

## CPC

- H05H 1/12: wherein the containment vessel forms a closed or nearly closed loop {(G21B1/05 takes precedence)}
- G06F 30/20: Design optimisation, verification or simulation (optimisation, verification or simulation of circuit designs G06F30/30)
- G06F 30/28: using fluid dynamics, e.g. using Navier-Stokes equations or computational fluid dynamics [CFD]
- G09B 23/06: for physics
- G09B 23/12: of liquids or gases
- H02K 44/06: Induction pumps
- H02K 44/085: {with conducting liquids}
- H05H 1/0006: {Investigating plasma, e.g. measuring the degree of ionisation or the electron temperature}
- H05H 1/03: using electrostatic fields
- H05H 1/04: using magnetic fields substantially generated by the discharge in the plasma
- G06F 2111/10: Numerical modelling
- H05H: PLASMA TECHNIQUE (apparatus or processes specially adapted for producing X-rays H05G2/00); PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
- G06F: ELECTRIC DIGITAL DATA PROCESSING (computer systems based on specific computational models G06N)
- G09B: EDUCATIONAL OR DEMONSTRATION APPLIANCES; APPLIANCES FOR TEACHING, OR COMMUNICATING WITH, THE BLIND, DEAF OR MUTE; MODELS; PLANETARIA; GLOBES; MAPS; DIAGRAMS (devices for psychotechnics or for testing reaction times A61B5/16; games, sports, amusements A63; projectors, projector screens G03B)
- H02K: DYNAMO-ELECTRIC MACHINES (dynamo-electric relays H01H53/00; conversion of DC or AC input power into surge output power {H03K3/53})

## Abstract

A plasma interaction simulator is presented. The simulator magnetically induces multiple distinct flows of plasma within a physical plasma vessel. The plasma flows collide with each other at flow interaction boundaries where discontinuities arising due to differences between the flows give rise to interactions. Sensors can be incorporated into the plasma simulator to observe and collect data about the plasma flow interactions.

## Claims

### Claim 1

A method of simulating a plasma flow interaction, comprising:
placing a plasma vessel in a gas chamber;
at least partially filling the gas chamber with a gas mixture at a first pressure;
sealing the plasma vessel to thereby enclose at least a portion of the gas mixture;
removing the plasma vessel from the gas chamber;
positioning the plasma vessel within a simulator having a set of ribs, a set of coils, and an ionization source; and
ionizing the enclosed gas mixture in the plasma vessel using the ionization source; and
generating, after ionizing the gas mixture, a rib magnetic field and a coil magnetic field via the set of ribs and the set of coils, respectively, wherein the ionized gas mixture and the rib and coil magnetic fields cooperate to create first and second ionized gas mixture flows that interact at an interaction boundary.

### Claim 2 (depends on 1)

The method of claim 1, wherein the plasma vessel is made from crystal.

### Claim 3 (depends on 1)

The method of claim 1, wherein the first and second flows are counter rotating.

### Claim 4 (depends on 1)

The method of claim 1, wherein the plasma vessel is spherical, and wherein the interaction boundary includes at least one of a counter-flow interaction, an opposed-flow interaction, and an aligned-flow interaction.

### Claim 5 (depends on 1)

The method of claim 1, wherein generating the rib magnetic field and the coil magnetic field comprises generating substantially orthogonal magnetic fields.

### Claim 6 (depends on 1)

The method of claim 1, wherein the set of ribs includes a first rib loop that includes a gap and a first electrical connection on a first side of the gap, and wherein positioning the plasma vessel within the simulator comprises positioning the plasma vessel within the simulator such that the first rib loop is positioned adjacent to and extends radially from the plasma vessel.

### Claim 7 (depends on 6)

The method of claim 6, wherein the set of coils includes a first coil, and wherein positioning the plasma vessel within the simulator further comprises positioning the plasma vessel within the simulator such that the first coil is wound about the plasma vessel, and orthogonally through the first rib loop.

### Claim 8 (depends on 1)

The method of claim 1, wherein the first ionized gas mixture flow is a rotating toroidal flow.

### Claim 9 (depends on 1)

The method of claim 1, further comprising controlling a pattern of the first and second ionized gas mixture flows.

### Claim 10 (depends on 1)

The method of claim 1, wherein the simulator further comprises a second set of coils, and wherein positioning the plasma vessel within the simulator comprises positioning the plasma vessel such that the second set of coils is wound around the plasma vessel, and wherein generating the rib magnetic field and the coil magnetic field via the set of ribs and the set of coils further comprises generating a second coil magnetic field, wherein the ionized gas mixture the rib magnetic field, the coil magnetic field, and the second coil magnetic field cooperate to create first and second ionized gas mixture flows that interact at the interaction boundary.

### Claim 11

A plasma interaction simulator, comprising:
a plasma container configured to contain a gas mixture;
a set of rib conducting loops including a first rib loop, wherein each rib conducting loop in the set of rib conduction loops (i) comprises a front end disposed adjacent to the plasma container, and (ii) extends from the front end to a distal end radially away from the plasma container;
a set of coil conducting loops including a first coil loop;
wherein the first coil loop traverses through the first rib loop;
an ionization source configured to ionize the gas mixture to generate plasma; and
wherein the set of rib conducting loops and the set of coil conducting loops are configured to yield first and second magnetic fields, respectively, that magnetically induce first and second plasma flows that interact at an interaction boundary.

### Claim 12 (depends on 11)

The simulator of claim 11, wherein the set of rib conducting loops comprises a plurality of duos including a first duo, and wherein the first duo includes the first rib loop and a second rib loop, and wherein the first and second rib loops are substantially coplanar rib loops.

### Claim 13 (depends on 11)

The simulator of claim 11, wherein the set of rib conducting loops comprises a quartet of four substantially coplanar rib loops including the first rib loop.

### Claim 14 (depends on 11)

The simulator of claim 11, further comprising a circuit coupled to the set of coil conducting loops via an electrical connection and configured to provide current pulses to the set of coil conducting loops to generate the second magnetic field.

### Claim 15 (depends on 14)

The simulator of claim 14, wherein the set of coil conducting loops further comprises a second coil loop, and wherein the circuit is configured to pulse the first coil loop and the second coil loop in sequence.

### Claim 16 (depends on 11)

The simulator of claim 11, wherein each of the first and second plasma flows that interact at the interaction boundary are toroidal.

### Claim 17 (depends on 11)

The simulator of claim 11, wherein the interaction boundary comprises at least one of a counter-flow interaction, an opposed-flow interaction, and an aligned-flow interaction.

### Claim 18 (depends on 11)

The simulator of claim 11, wherein the plasma container comprises crystal.

### Claim 19 (depends on 11)

The simulator of claim 11, further comprising at least one sensor configured to capture data associated with the plasma while under flow.

### Claim 20 (depends on 11)

The simulator of claim 11, wherein a speed of the first plasma flow is different from a speed of the second plasma flow.