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The effect of impurity seeding on edge toroidal rotation in the ADITYA-U tokamak

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Abstract Intrinsic toroidal rotation velocity (Vφ ) has been measured from the Doppler shift of C5+ carbon spectral lines (at 529.05 nm) in the edge region of the ADITYA-U tokamak without any auxiliary torque input in an ohmically heated pure hydrogen (H2) plasma as well as in H2 plasmas seeded with medium-Z (neon and argon) impurities . The toroidal rotation in the edge region is observed to reverse its direction from the counter-current to the co-current direction with an increase in plasma current beyond I p ∼ 145–150 kA. Furthermore, a systematic decrease in the co-current Vφ has been observed with the edge density, which tends to decrease to almost zero velocity with an increase in the edge density. The injection of medium-Z (neon and argon) impurities is observed to influence the edge toroidal rotation significantly. In low I p discharges, argon injection leads to a reversal of edge intrinsic rotation from the counter-current to the co-current direction. In high I p discharges, both neon and argon seeding enhance the co-current rotation by about ∼5–10 km s−1, at a constant I p compared to pure H2 discharges. Simultaneous measurements of the edge radial electric field, E r, shows that the E r × Bθ flow seems to be driving the edge toroidal rotation in ADITYA-U. With impurity injection, the E r also gets modified, leading to an observed increase in the edge toroidal rotation.
Title: The effect of impurity seeding on edge toroidal rotation in the ADITYA-U tokamak
Description:
Abstract Intrinsic toroidal rotation velocity (Vφ ) has been measured from the Doppler shift of C5+ carbon spectral lines (at 529.
05 nm) in the edge region of the ADITYA-U tokamak without any auxiliary torque input in an ohmically heated pure hydrogen (H2) plasma as well as in H2 plasmas seeded with medium-Z (neon and argon) impurities .
The toroidal rotation in the edge region is observed to reverse its direction from the counter-current to the co-current direction with an increase in plasma current beyond I p ∼ 145–150 kA.
Furthermore, a systematic decrease in the co-current Vφ has been observed with the edge density, which tends to decrease to almost zero velocity with an increase in the edge density.
The injection of medium-Z (neon and argon) impurities is observed to influence the edge toroidal rotation significantly.
In low I p discharges, argon injection leads to a reversal of edge intrinsic rotation from the counter-current to the co-current direction.
In high I p discharges, both neon and argon seeding enhance the co-current rotation by about ∼5–10 km s−1, at a constant I p compared to pure H2 discharges.
Simultaneous measurements of the edge radial electric field, E r, shows that the E r × Bθ flow seems to be driving the edge toroidal rotation in ADITYA-U.
With impurity injection, the E r also gets modified, leading to an observed increase in the edge toroidal rotation.

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