Abstract:Complete one cycle and 1.5 cycle ac operations are performed in the STOR-M tokamak with the plasma current of ∼20 kA using newly developed feedback control and Ohmic heating circuits. Bias voltage adjustment is installed in the plasma position circuit to optimize the plasma position in the second negative plasma current phase for multicycle ac operation. The key to successful, reproducible multicycle ac tokamak operations on STOR-M is to control both the total vertical field by the feedback control system and … Show more
“…While maintaining the toroidal field in the CCW direction (top view), the toroidal plasma current direction can be easily reversed by changing the current direction in the primary windings. The horizontal position feedback control system was already designed for alternating current operation in STOR-M and is able to handle the normal (CCW) and reversed (CW) tokamak discharge current directions in STOR-M without any further modifications [15].…”
In the Saskatchewan torus-modified (STOR-M) tokamak, tangential compact torus injection (CTI) experiments have been performed with normal (counter-clockwise, CCW, top view) and reversed (clockwise, CW, top view) plasma current directions while the compact torus (CT) injection direction remains in the CCW direction. The intrinsic toroidal flow direction reverses when the discharge current is reversed. However, the change in the toroidal flow direction is always toward the CTI direction (CCW). It has been determined that the momentum in high density and high velocity CT is more than ten times larger than the intrinsic toroidal rotation momentum in the typical STOR-M plasma. Therefore, the modification of the plasma toroidal rotation velocity is attributed to momentum transfer from CT to the tokamak discharge.
“…While maintaining the toroidal field in the CCW direction (top view), the toroidal plasma current direction can be easily reversed by changing the current direction in the primary windings. The horizontal position feedback control system was already designed for alternating current operation in STOR-M and is able to handle the normal (CCW) and reversed (CW) tokamak discharge current directions in STOR-M without any further modifications [15].…”
In the Saskatchewan torus-modified (STOR-M) tokamak, tangential compact torus injection (CTI) experiments have been performed with normal (counter-clockwise, CCW, top view) and reversed (clockwise, CW, top view) plasma current directions while the compact torus (CT) injection direction remains in the CCW direction. The intrinsic toroidal flow direction reverses when the discharge current is reversed. However, the change in the toroidal flow direction is always toward the CTI direction (CCW). It has been determined that the momentum in high density and high velocity CT is more than ten times larger than the intrinsic toroidal rotation momentum in the typical STOR-M plasma. Therefore, the modification of the plasma toroidal rotation velocity is attributed to momentum transfer from CT to the tokamak discharge.
“…AC operation was first demonstrated on a STOR-1M tokamak with a plasma current of 4 kA [1]. Plasma properties when the plasma current crosses zero and some key technologies have been introduced in several papers [2][3][4][5]. JET has demonstrated a full cycle of ac operation with a reactorrelevant plasma current of 2 MA, but with a dwell time between two half-cycles from 50 ms to 6 s, which means the ionization was lost when the plasma current crosses zero [6].…”
A quasi-steady-state alternating current operation assisted by lower hybrid wave (LHW) was achieved on a HT-7 superconducting tokamak with plasma current of I
p = 125 kA, line-averaged density of 1.5 × 1019 m−3, electron temperature of T
e = 500 eV and 30–50 s plasma duration. Plasma current was sustained and smoothly transferred from one direction to the other without loss of ionization. Plasma position control, LHW assistance, strong gas puffing and good wall condition are the key issues to have a smooth transition of plasma current. Our modelling results show that current reversal equilibrium configuration with two oppositely flowing currents in the high-field-side and the low-field-side during current reversal exists. This is in agreement with experimental measurements.
“…To mitigate this problem, several square voltage pulses, marked as dist in Fig. 1, from a set of signal generators were added to the ∆H signal during the current crossing phases based on our best guess of the polarity of the ∆H signal saturation and the required current in the feedback windings [21]. This improved feedback position control system, combined with careful control of gas puffing pulses, significantly reduced the adjusting time required when the operation circuit is converted from the normal mode to the AC mode of operation as compared with the previous AC operation campaigns on STOR-M.…”
An experiment to investigate the source of plasma equilibrium of the residual plasma at zero cross over of plasma current is presented. The role of limiter in providing this equilibrium by short circuiting the electric field developed due to the toroidal drifts is examined by measuring the current flowing through the limiter. The role of a fast poloidal rotation observed by a set of Mach probes, during zero cross over is also examined in providing the equilibrium.
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