Structure of the n = 1 mode responsible for relaxation and current drive during sustainment of the SPHEX spheromak
暂无分享,去创建一个
[1] M. G. Rusbridge,et al. The design and operation of the SPHEX spheromak , 1997 .
[2] Hattori,et al. Effect of collisionality and diamagnetism on the plasma dynamo. , 1995, Physical review letters.
[3] K. Gibson,et al. Ion energy measurements in the SPHEX spheromak , 1995 .
[4] Prager,et al. Time-resolved observation of discrete and continuous magnetohydrodynamic dynamo in the reversed-field pinch edge. , 1994, Physical review letters.
[5] Thomas R. Jarboe,et al. Review of spheromak research , 1994 .
[6] Naito,et al. Relaxation oscillations and toroidal-current regeneration in a helicity-driven spheromak. , 1993, Physical review letters.
[7] Cunningham,et al. Observations of the magnetohydrodynamic dynamo effect in a spheromak plasma. , 1993, Physical review letters.
[8] M. G. Rusbridge,et al. The direct determination of the current density and mu profiles of a spheromak , 1993 .
[9] Cunningham,et al. Power flow in a gun-injected spheromak plasma. , 1992, Physical review letters.
[10] M. G. Rusbridge,et al. The relationship between the 'tangled discharge' and 'dynamo' models of the magnetic relaxation process , 1991 .
[11] G. Craddock,et al. Nonlinear dynamics of field maintenance and quasiperiodic relaxation in reversed-field pinches , 1991 .
[12] M. Katsurai,et al. Three-dimensional numerical simulation of the multi-helicity magnetohydrodynamic relaxation process in low-q spheromaks , 1991 .
[13] Thomas R. Jarboe,et al. The impedance and energy efficiency of a coaxial magnetized plasma source used for spheromak formation and sustainment , 1990 .
[14] A. Mirin,et al. The evolution of a decaying spheromak , 1987 .
[15] C. Barnes,et al. Experimental determination of the conservation of magnetic helicity from the balance between source and spheromak , 1986 .
[16] A. Janos. Magnetic flux conversion and relaxation toward a minimum‐energy state in spheromak plasmas , 1986 .
[17] J B Taylor,et al. Relaxation and magnetic reconnection in plasmas , 1986 .
[18] M. Katsurai,et al. Three-dimensional numerical simulations of the relaxation process in spheromak plasmas , 1986 .
[19] Wright,et al. Observations of spheromak equilibria which differ from the minimum-energy state and have internal kink distortions. , 1986, Physical review letters.
[20] A. Jacobson,et al. The 'boxcar' method for the analysis of non-Gaussian random signals , 1985 .
[21] J́anos,et al. Relaxation of spheromak plasmas toward a minimum-energy state and global magnetic fluctuations. , 1985, Physical review letters.
[22] Takaya Hayashi,et al. Simulation studies on line-tying stabilization of spheromak tilting instability , 1984 .
[23] R. Gruber,et al. Free-boundary MHD stability of pressureless oblate spheromaks – Dependence on aspect ratio and elongation , 1983 .
[24] J. Hammer,et al. Investigations of the magnetic structure and the decay of a plasma‐gun‐generated compact torus , 1983 .
[25] M. G. Rusbridge. Conditions for the attainment of the minimum-energy state of a diffuse pinch discharge , 1982 .
[26] S. Jardin. Ideal magnetohydrodynamic stability of the spheromak configuration , 1982 .
[27] A. Reiman,et al. Tilt and shift mode stability in spheromaks with line tying , 1982 .
[28] E. Priest,et al. Critical conditions for magnetic instabilities in force-free coronal loops , 1981 .
[29] J. Edenstrasser. Unified treatment of symmetric MHD equilibria , 1980, Journal of Plasma Physics.
[30] A. A. Newton,et al. Reversed-field-pinch research , 1980 .
[31] I. Jones,et al. Compact Torus Configuration Generated by a Rotating Magnetic Field: The Rotamak , 1980 .
[32] A. Todd,et al. A numerical study of MHD equilibrium and stability of the spheromak , 1980 .
[33] M. G. Rusbridge. A model of field reversal in the diffuse pinch , 1977 .
[34] M. G. Rusbridge,et al. Structure of Turbulence in the Zeta Plasma , 1971 .