A 'non-local' response of the plasma core triggered by peripheral plasma perturbations other than laser ablation is found in the RTP tokamak. Oblique pellet injection (OPI) has been used to induce fast cooling of the peripheral plasma. In response, an inward cold pulse (T-e drop) and a slightly delayed core T-e rise are observed. A somewhat similar 'non-local' response is observed when the peripheral plasma is heated by modulated electron cyclotron heating or by fast current ramps, i.e. the core temperature drops in response to the peripheral heating. The plasma conditions for the occurrence of the 'non-local' response have been investigated. The core T-e rise following OPI is associated with the formation of a large temperature gradient in the region 1 < q < 2. The T-e rise is largest at low electron density and for large pellet deposition radii. Above a critical density the T-e rise disappears and only the (weaker) drop in core T-e is observed. Time dependent transport simulations show that the propagation of the inward cold pulse is consistent with local transport, while the core T-e rise is a slower phenomenon requiring a large transient drop of chi(e) in the region 1 < q < 2.
`Non-local' response of RTP ohmic plasmas to peripheral perturbations
G Gorini;P Mantica;
1999
Abstract
A 'non-local' response of the plasma core triggered by peripheral plasma perturbations other than laser ablation is found in the RTP tokamak. Oblique pellet injection (OPI) has been used to induce fast cooling of the peripheral plasma. In response, an inward cold pulse (T-e drop) and a slightly delayed core T-e rise are observed. A somewhat similar 'non-local' response is observed when the peripheral plasma is heated by modulated electron cyclotron heating or by fast current ramps, i.e. the core temperature drops in response to the peripheral heating. The plasma conditions for the occurrence of the 'non-local' response have been investigated. The core T-e rise following OPI is associated with the formation of a large temperature gradient in the region 1 < q < 2. The T-e rise is largest at low electron density and for large pellet deposition radii. Above a critical density the T-e rise disappears and only the (weaker) drop in core T-e is observed. Time dependent transport simulations show that the propagation of the inward cold pulse is consistent with local transport, while the core T-e rise is a slower phenomenon requiring a large transient drop of chi(e) in the region 1 < q < 2.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.