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A New Approach to Fusion Energy

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How to lower the fusion threshold? Beam-target fusion. 100 keV D beam into T plasma ... How to make plasma heat engine? Centrifugal well created in rotating plasma ... – PowerPoint PPT presentation

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Title: A New Approach to Fusion Energy


1
A New Approach to Fusion Energy
  • D. C. Barnes
  • coronadocon_at_msn.com
  • FPA Pathways to the Future
  • September 28, 2006

2
Outline
  • Ultimate fusion neutronless
  • Two new ideas (both for rotating plasmas)
  • Use high T to make efficient heat engine
  • Use rotation to make waves from static field
    (Doppler effect)
  • Summary and plans

3
The challenge of aneutronic fusion
  • p-11B is 1000 times more difficult than D-T
  • T is 6 x and 3 electrons/ion ? n is 0. 05 x , and
    yield is 1/2 ? P' is 0.001 ? V is 1000 x
  • Thermonuclear p-11B tokamak wont work (physics
    or economics)
  • What alternatives might exist?
  • Apply to D-T reduced size and field

4
How to lower the fusion threshold?
  • Beam-target fusion
  • 100 keV D beam into T plasma
  • More heat than fusion

16 bar
5
New idea 1 Heat engine power flow
Beam-target fusion gives this Qphys 10-20
Plant engineers see this Qeng 10
6
Plasma Centrifuge Heat Engine for Colliding Beam
Fusion Reactor
Plasma Centrifuge Heat Engine for Continuous Beam
Fusion Reactor
Plasma Centrifuge Heat Engine Beam Fusion
Reactor
Patent Pending, App. No. 60/596567, USPTO
(2005). Patent Pending, App. No. 60/766791,
USPTO (2006). Patent Pending, App. No.
1153471, USPTO (2006).
7
How to make plasma heat engine?
  • Several ways
  • Make potential field force on plasma
  • Plasma does work against field, giving mechanical
    energy to source of field
  • Barnes Nebel POPS (1998)
  • Collisionless plasma can oscillate without
    entropy generation
  • Chacón et al. work (2000)
  • Thermonuclear plasma in equilibrium with low T
    particle replacement
  • Continuous or oscillating
  • Continuous trap (Pastukov 1974)

This result can be understood if one bears in
mind that all the energy of an escaping particle
consists of transverse motion,
If make B ? 0 at outflow, get low T exhaust!
8
How to make plasma heat engine?
  • Centrifugal well created in rotating plasma
  • Make B and r small at ends where particles escape
  • Open field is that outside a field reversed
    configuration (FRC)

9
Supersonic rotating plasmas exist
Maryland Centrifugal eXperiment (MCX) From Ellis,
et al.
PSP-2 ½ MV Experiment at Novosibirsk From
Abdrashitov, et al.
10
P-CHES D-T reactor
1T
1m
  • High-b and beam-target operation implies low B
    operation 33 W/cm3 ? 400 MW

11
P-CHES D-T reactor (cartoon approximation)
  • Beam formed by electrostatic acceleration of
    injected, low-energy particles
  • e.g. Ftrapped 0.45 W ? Vtrapped 200 kV
  • Toroidal current driven by rotating magnetic
    field (RMF) with stationary dipole

12
P-CHES on the path to fusion energy
  • Form supersonically rotating FRC
  • Study Tloss/Tcentral show small and dependencies
    to minimize
  • Raise applied and induced voltage and inject beam
    to get fusion conditions
  • D-T fusion system
  • p-11B fusion system

13
Forming rotating FRC
  • New idea 2 Make and use waves with plasma
    rotation e.g. RMF

From Slough and Miller
From Hoffman, et al.
14
Forming rotating FRC
  • Firing end anodes produces rotating plasma

Rotating plasma sees RMF, producing FRC
15
Summary and future
  • A new paradigm is proposed
  • Beam-target fusion with heat recovered to
    rotation
  • High efficiency of beam formation from rotation
  • Many advantages
  • Very high power density
  • Required T reduced (500 eV for D-T)
  • Required confinement reduced (lt 1 ms for D-T)
  • Static fields, DC operation
  • Extensible to aneutronic systems
  • 2 new ideas suggest a modest experiment
  • Demonstrate formation of rotating FRC
  • Heat engine physics diagnosed if warm FRC
    produced
  • Propose future study
  • Theory and design
  • Small experiment
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