1 / 1

The toroidal current is consistent with numerical estimates of bootstrap current

Measurement of the Pfirsch-Schlüter and Bootstrap Currents in HSX. J.C. Schmitt, J.N. Talmadge, P.H. Probert, S.F. Knowlton*, D.T. Anderson HSX Plasma Laboratory, Univ. of Wisconsin – Madison, WI USA *Physics Department, Auburn Univ. – Auburn, AL USA. HSX Magnetics and Computational Modeling.

amiel
Download Presentation

The toroidal current is consistent with numerical estimates of bootstrap current

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Measurement of the Pfirsch-Schlüter and Bootstrap Currents in HSX J.C. Schmitt, J.N. Talmadge, P.H. Probert, S.F. Knowlton*, D.T. Anderson HSX Plasma Laboratory, Univ. of Wisconsin – Madison, WI USA *Physics Department, Auburn Univ. – Auburn, AL USA HSX Magnetics and Computational Modeling Operating Parameters & Diagnostics Bootstrap Current Pfirsch-Schlüter Current • Majority of HSX plasmas are in long mean free path (LMFP) regime • Magnetic diffusivity varies across the confinement volume • The Pfirsch-Schlüter current exhibits dipole behavior and rotates with the |B| contours 1/6 FP • B0 = 1 Tesla • 50 kW ECR Heating (1st Harmonic) • 10-chord Thomson Scattering • Te(ρ) and ne(ρ)profiles • Rogowski coil – External • Toroidal current • Low-frequency response • dB/dt triplet array – External • MHD and bootstrap currents • Low-frequency response • Poloidal and toroidal measurements • The Helically Symmetric eXperiment has • Quasi-Helically Symmetric axis: (n,m)=(4,1) • No toroidal curvature • The Pfirsch-Schlüter current • Rotates with toroidal angle • Is reduced by a factor of compared to a conventional stellarator • The bootstrap current • Is in opposite direction than that of a tokamak • Reduces the rotational transform in HSX • VMEC • Calculates free-boundary MHD Equilibrium • Inputs are measured Te & ne profiles and assumed Ti & ni (Zeff≈ 1) • BOOTSJ • Calculates bootstrap current profile from VMEC results. Results may be input back into VMEC as toroidal current profile. • V3FIT • Computes response function for diagnostic coils • Expected magnetic signals are computed from response functions and VMEC output 50 kW ECRH heated plasma JPS 1/6 FP 16 Profiles obtained during resonance heating location scan Poloidal Station # Poloidal Rotation of Null Point in Bθ 1 1/2 FP 16 1/2 FP 2 1 2 Offset in measured Bθ due to toroidal bootstrap current Temporal Evolution of Currents in HSX HSX Vacuum Vessel and Diagnostic Coils VMEC equilibrium, JBS=JBOOTSJ BOOTSJ: 478 A Numerical Model and Measurement • BOOTSJ calculates the bootstrap current; Assumes LMFP regime • BOOTSJ provides an upper limit to the bootstrap current • The toroidal current rises throughout the majority of the shot • Steady state reached only in coldest plasmas • Decaying exponential growth is observed in many cases: projections are based this model • Special thanks to Steve Knowlton and the V3FIT team 1/2 FP 1/6 FP Summary + Future Directions Near-axis ECRH • The toroidal current is consistent with numerical estimates of bootstrap current • The measured magnetic diagnostic signals match predictions of V3FIT • Comparisons with and without toroidal bootstrap current show agreement • Helical nature of Pfirsch-Schlüter current in HSX has been confirmed • Future modeling and measurement • Temporal evolution of toroidal current will be studied – Poloidal flux diffusion • Effects of toroidal current on rotational transform will be studied • Configuration Flexibility: HSX can alter the magnetic spectrum with a set of auxiliary coils • Mirror: The helical symmetry is spoiled by introducing (n,m) = (4,0) component (and harmonics) into the magnetic spectrum, affecting the equilibrium and bootstrap currents • Well/Hill: Rotational transform profile may be raised/lowered, adjusting the location of the = 1 resonant surface Off-axis ECRH • Diagnostic signals and toroidal current evolution • t = 10. ms: MHD equilibrium established, bootstrap current still small • t = 50. ms: ECH turn-off, bootstrap current has grown to 450 A • The diagnostic signals agree well with the V3FIT numerical results • Toroidal current is still evolving – Radial profile information is not yet known • The bootstrap current is the upper limit for the measurements to date • Projected steady state values exceed bootstrap current estimate • Decaying exponential growth is not appropriate for most cases – may overestimate steady state value 49th Annual Meeting of the Division of Plasma Physics, November 12-16, 2007, Orlando, Florida

More Related