V. A. Soukhanovskii 1 Acknowledgement s: R. Maingi 2, D. A. Gates 3, J. Menard 3, R. Raman 4, R. E. Bell 3, C. E. Bush 2, R. Kaita 3, H. W. Kugel 3, B.

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V. A. Soukhanovskii 1 Acknowledgement s: R. Maingi 2, D. A. Gates 3, J. Menard 3, R. Raman 4, R. E. Bell 3, C. E. Bush 2, R. Kaita 3, H. W. Kugel 3, B. P. LeBlanc 3, S. F. Paul 3, A. L. Roquemore 3, and the NSTX Team 1 Lawrence Livermore National Laboratory, Livermore, CA 2 Oak Ridge National Laboratory, Oak Ridge, TN 3 Princeton Plasma Physics Laboratory, Princeton, NJ 4 University of Washington, Seattle, WA NSTX Results Review 23 July 2007 Princeton, NJ Heat flux amelioration in highly shaped plasmas in NSTX Supported by Office of Science

V. A. Soukhanovskii, NSTX Results Review, 23 July 2007, Princeton, NJ 2 of 10 Goal: develop steady-state divertor heat load mitigation scenarios in a large Spherical Torus Divertor heat flux mitigation solutions: – Poloidal flux expansion at outer strike point – Strike point sweeping – Radiative divertor: outer SOL in high-recycling regime with enhanced radiation at divertor plate – Dissipative divertor (detachment)  Goal - study divertor heat flux reduction and detachment – in lower single null  = ,  = configuration with divertor D 2 injection – in lower single null  = ,  = configuration by flux expansion – in lower single null  = ,  = configuration with divertor D 2 injection

V. A. Soukhanovskii, NSTX Results Review, 23 July 2007, Princeton, NJ 3 of 10 XP 708 summary  Steady-state divertor heat flux amelioration in low aspect ratio geometry is studied in MA 4-6 MW NBI highly shaped H-mode plasmas in NSTX  Significant (x 2-3) reduction in divertor peak heat flux is achieved by using high flux expansion divertor (in comparison with low  lower single null configuration)  Divertor peak heat flux is reduced further by x 2-3 using partially detached divertor regime with divertor D 2 injection in low  shape in high  shape Partial Detachment in high  shape

V. A. Soukhanovskii, NSTX Results Review, 23 July 2007, Princeton, NJ 4 of 10 Proper diagnostic configuration and rtEFIT shape control were essential for success of experiment rtEFIT control was used for drsep, R OSP, and gap control

V. A. Soukhanovskii, NSTX Results Review, 23 July 2007, Princeton, NJ 5 of 10 Partial strike point detachment is obtained using divertor D 2 injection D 2 injected for 200 ms Peak heat flux reduced x 2-3 Core confinement and performance were not affected Core carbon concentration reduced x 1.5 Clear signs of divertor radiated power increase and neutral pressure increase No signs of X-point MARFE (?) Volume recombination in outer divertor Same PDD picture in 1 MA, 4 MW; 1 MA, 6 MW; 1.2 MA, 6 MW cases

V. A. Soukhanovskii, NSTX Results Review, 23 July 2007, Princeton, NJ 6 of 10 Divertor peak heat flux significantly reduced during partial detachment phase Peak heat flux reduced by 2-3 Profile  q changes from 5-10 to cm PDD zone is cm ( in   ) 1 MA, 6 MW 1 MA, 4 MW

V. A. Soukhanovskii, NSTX Results Review, 23 July 2007, Princeton, NJ 7 of 10 Divertor D  profiles are indicative of partial detachment Camera signal saturated during PDD (indication of X-point MARFE ?) Increase consistent with low T e, high n e plasmas Outside of PDD zone - high-recycling SOL PDD zone is cm ( in   )

V. A. Soukhanovskii, NSTX Results Review, 23 July 2007, Princeton, NJ 8 of 10 Significant volume recombination is observed at outer strike point during detachment Balmer series lines 2-6…11 Sign of strong volume recombination Stark broadening yields n e Intensities determined by Saha- Boltzman level population distribution n e ~ 2-3 x m -3 in inner divertor (bottom panel) n e ~ 4-6 x m -3 at outer strike point (top panel) T e < 1.5 eV Interim calibration used Soukhanovskii et. al., Rev. Sci. Instrum. 77, 10F127 (2006)

V. A. Soukhanovskii, NSTX Results Review, 23 July 2007, Princeton, NJ 9 of 10 Study radiative divertor and detachment in highly shaped plasmas Highly shaped plasmas mean high performance » higher bootstrap current fraction at higher  » small ELM regimes at higher  Highly shaped plasmas have high flux expansion divertor » Reduced peak heat flux - favorable for detachment threshold » Higher neutral penetration (?) » Higher “plasma plugging” (?) - Important in open divertor » Higher isothermal radiating volume (?) » Sputtering yield (?) » Parallel and poloidal connection lengths are shortest

V. A. Soukhanovskii, NSTX Results Review, 23 July 2007, Princeton, NJ 10 of 10 Magnetic field line length and radial gradient are different in high  and low  shape Figure courtesy of Dr M. Bell (PPPL) low  shape high  shape Different power and momentum losses Different sensitivity to MARFE onset high  shape