The RFX machine stabilizing shell was originally provided with two toroidal insulating gaps and with two poloidal gaps. After short-circuiting one equatorial gap and one poloidal gap, the current distribution through the short-circuited gaps and the distribution of the radial magnetic field along the gaps have been measured during plasma pulses. The experimental data, which give a direct measurement of the shell reaction to the plasma magnetic perturbations, have been analysed and compared with the results of the analytical model of the shell
A method for the calculation of the currents in the poloidal field coils of a toroidal magnetic conf...
This paper presents an overview of recent experimental results obtained on the RFX device. We succee...
The RFP configuration is maintained by an intrinsic dynamo mechanism associated to resistive MHD tea...
The paper describes a method for the identification of the plasma shape in a toroidal device for the...
The experiments proposed with active MHD mode control in RFX require the installation of new saddle ...
The physics results obtained from RFP experiments at high current (0.8\u20131 MA) indicate the need ...
In the modified RFX experiment (RFX-mod) external magnetic field coils and a close fitting thin cond...
The magnetic measurement system of RFX includes a large number of local field probes. A re-calibrati...
The Reversed Field Pinch experiment RFX (R0=2m, a=0.46m) is presently run at approximately 500 kA of...
The experimental determination of the radial electric field Er and the associated E 7 B drift veloc...
The paper presents the application and the first results of a plasma shape identification code used ...
The RFX reversed field pinch experiment has been modified (RFX-mod) to address specific issues of ac...
The reversed field pinch (RFP) magnetic confinement requires both toroidal and poloidal components f...
The paper describes a method for the identification of the plasma shape in a toroidal device for fus...
The edge of the RFX-mod (R=2m, a=0.46m) Reversed Field Pinch device is characterized by weak magneti...
A method for the calculation of the currents in the poloidal field coils of a toroidal magnetic conf...
This paper presents an overview of recent experimental results obtained on the RFX device. We succee...
The RFP configuration is maintained by an intrinsic dynamo mechanism associated to resistive MHD tea...
The paper describes a method for the identification of the plasma shape in a toroidal device for the...
The experiments proposed with active MHD mode control in RFX require the installation of new saddle ...
The physics results obtained from RFP experiments at high current (0.8\u20131 MA) indicate the need ...
In the modified RFX experiment (RFX-mod) external magnetic field coils and a close fitting thin cond...
The magnetic measurement system of RFX includes a large number of local field probes. A re-calibrati...
The Reversed Field Pinch experiment RFX (R0=2m, a=0.46m) is presently run at approximately 500 kA of...
The experimental determination of the radial electric field Er and the associated E 7 B drift veloc...
The paper presents the application and the first results of a plasma shape identification code used ...
The RFX reversed field pinch experiment has been modified (RFX-mod) to address specific issues of ac...
The reversed field pinch (RFP) magnetic confinement requires both toroidal and poloidal components f...
The paper describes a method for the identification of the plasma shape in a toroidal device for fus...
The edge of the RFX-mod (R=2m, a=0.46m) Reversed Field Pinch device is characterized by weak magneti...
A method for the calculation of the currents in the poloidal field coils of a toroidal magnetic conf...
This paper presents an overview of recent experimental results obtained on the RFX device. We succee...
The RFP configuration is maintained by an intrinsic dynamo mechanism associated to resistive MHD tea...