FRX-L: A field-reversed configuration plasma injector for magnetized target fusion

We describe the experiment and technology leading to a target plasma for the magnetized target fusion research effort, an approach to fusion wherein a plasma with embedded magnetic fields is formed and subsequently adiabatically compressed to fusion conditions. The target plasmas under consideration, field-reversed configurations (FRCs), have the required closed-field-line topology and are translatable and compressible. Our goal is to form high-density (1017 cm−3) FRCs on the field-reversed experiment-liner (FRX-L) device, inside a 36 cm long, 6.2 cm radius theta coil, with 5 T peak magnetic field and an azimuthal electric field as high as 1 kV/cm. FRCs have been formed with an equilibrium density ne≈(1 to 2)×1016 cm−3, Te+Ti≈250 eV, and excluded flux ≈2 to 3 mWb.

[1]  G. A. Bennett,et al.  The Atlas project-a new pulsed power facility for high energy density physics experiments , 1997 .

[2]  M. Tuszewski,et al.  Field reversed configurations , 1988 .

[3]  J. Slough,et al.  Formation of field-reversed configurations using scalable, low-voltage technology , 1986 .

[4]  T. Intrator,et al.  DIAGNOSTICS FOR A MAGNETIZED TARGET FUSION EXPERIMENT , 2000 .

[5]  T. S. Green,et al.  RADIAL HYDROMAGNETIC OSCILLATIONS , 1959 .

[6]  Ronald C. Kirkpatrick,et al.  Experimental measurements of a converging flux conserver suitable for compressing a field reversed configuration for magnetized target fusion , 2002 .

[7]  T. Intrator,et al.  Magnetic Field Measurements inside a Converging Flux Conserver for Magnetized Target Fusion Applications , 2002 .

[8]  Ronald C. Kirkpatrick,et al.  Magnetized Target Fusion: An Overview , 1995 .

[9]  W. Armstrong,et al.  Review of the Los Alamos FRX-C Experiment , 1986 .

[10]  T. Minato,et al.  Quadrupole Stabilization of the n = 2 Rotational Instability of a Field-Reversed Theta-Pinch Plasma , 1983 .

[11]  R. K. Linford,et al.  Experimental studies of field‐reversed configuration translation , 1986 .

[12]  Harold P. Furth,et al.  Plasma Physics and Controlled Nuclear Fusion Research , 2007 .

[13]  Tadashi Sekiguchi,et al.  Plasma Physics and Controlled Nuclear Fusion Research , 1987 .

[14]  J. Stillerman,et al.  MDSplus data acquisition system , 1997 .

[15]  J. G Mohr,et al.  Controlled Thermonuclear Reactions , 1957, Nature.

[16]  T. S. Green,et al.  Diffusion of Antiparallel Bias Magnetic Field during the Initial Stages of a Theta‐Pinch , 1966 .

[17]  J. Lindl Development of the indirect‐drive approach to inertial confinement fusion and the target physics basis for ignition and gain , 1995 .

[18]  Glen A. Wurden,et al.  Development of a high-current low-inductance crowbar switch for FRX-L , 2002 .

[19]  M. Tuszewski A semiempirical formation model for field-reversed configurations , 1988 .

[20]  T. S. Green An investigation of the theta pinch using magnetic pick-up loops , 1962 .

[21]  Ronald C. Kirkpatrick,et al.  Implosion of solid liner for compression of field reversed configuration , 2001 .

[22]  Andrew G. Glen,et al.  APPL , 2001 .

[23]  W. Grossmann,et al.  Thetapinch experiments with trapped antiparallel magnetic fields , 1971 .

[24]  Mikhailov,et al.  Target Plasma Formation for Magnetic Compression/Magnetized Target Fusion. , 1995, Physical review letters.

[25]  J. Slough,et al.  The large-s field-reversed configuration experiment , 1993 .

[26]  M. Tuszewski Excluded flux analysis of a field reversed plasma , 1980 .

[27]  W. Armstrong,et al.  ϑ‐pinch ionization for field‐reversed configuration formation , 1981 .

[28]  M. Tuszewski,et al.  A zero-dimensional transport model for field-reversed configurations , 1984 .

[29]  C. Fowler,et al.  Megagauss Technology and Pulsed Power Applications , 1987 .