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托卡马克的平衡计算. 李国强 2013.12.18 四室学术报告. Introduction. Decompose the physics problem by the orders (time order and space order) Traditional decomposition of plasma physics (by time order): equilibrium, stability and transport Equilibrium is the basis for other problem
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托卡马克的平衡计算 李国强 2013.12.18 四室学术报告
Introduction • Decompose the physics problem by the orders (time order and space order) • Traditional decomposition of plasma physics (by time order): equilibrium, stability and transport • Equilibrium is the basis for other problem • Here the equilibrium means the state of force equilibrium
Introduction (cont.) • Force balance equation (static momentum equation) • Force balance equation in 2D form → Grad-Shafranov (G-S) equation (For axis symmetric, in (R,z) coordinate): • Then the solution of the G-S equation describes the properties of the equilibrium
Equilibrium and poloidal field coils • Poloidal field coils induct the ohmic plasma current and control the plasma shape • On EAST • PF1-PF6, center solenoid, mainly for the ohmic current • PF7/9, elongation • PF11,PF13, trianglarity • PF5, PF7/9, PF11, divertor control EAST PF coils and plasma configuration
Properties of equilibrium • Plasma configuration • Embedded flux surface • Plasma geometry • Divertor configuration • Profiles (functions of flux surface) • : pressure • : no direct physical meaning, but direct in G-S equation • : safety factor, describe the pitch angle of magnetic field line • : flux surface averaged parallel current • , q and are not independent
Fixed boundary and free boundary equilibrium calculation • Fixed boundary • The plasma boundary is given, only calculate the plasma configuration inside the plasma • Easy to calculate, useful for theory study • Free boundary • To calculate the configuration outside the plasma boundary • The current in the PF coils is given • Complicate but sometimes necessary • A third kind • Prescribe a non-fixed plasma boundary
Coordinate system • Many kinds of coordinate system in tokamak study • Two major coordinate systems: (R,z) coordinate and magnetic surface coordinate • coordinate system • For free boundary calculation • Can handle the X-point z R Mesh in (R,z) coordinate
Coordinate system (cont.) • Flux surface coordinate system • coordinate • Easier, but cannot handle the X-point • can be • Orthogonal • Equal arc length • …… • Some coordinate equivalence • normalized toroidal flux • normalized volume Mesh in flux surface coordinate
Equilibrium construction and reconstruction • Construction • Generate an equilibrium from given profiles, plasma shape or current in PF coils, and other parameters • Basis for tokamak design • Basis for many theory study • Reconstruction • Find the experimental equilibrium from the diagnostic data • Basis for experiments analysis
Equilibrium reconstruction with EFIT • EFIT is the most popular code for equilibrium reconstruction. Maybe the most popular code in tokamak research area • Assume a polynomial or spline profiles of P’ and FF’, then iteratively find the coefficient to minimize the error quality function
Different EFIT reconstruction constraints • At present, EAST only has the magnetic diagnostics and limited kinetic diagnostics • But we can add some constraints to the current profile
Magnetic diagnostic constraints • All kinks of magnetic probe and flux loops Strait (2007)
kinetic profiles on EAST • Te and ne are from Thomson scattering • Ti is from the XCS, but only central region data are available. So Ti is scale from Te and assume Ti=Te at the edge region • First map the data to space, then fit them with tension spline • Assume flat Zeff=2.5 • At present EAST has no NBI, so the fast ion contribution is neglected Data and fitting profiles for 38300.3900
Edge current constraint for H-mode plasma • For H-mode plasma, it is believed that at the edge region, the current is dominated by the bootstrap current • Sauter bootstrap current model is used to calculate the bootstrap current. Bootstrap current calculation relies on the kinetic profiles (Te, Ti, ne, Zeff) • Ohmic current EAST 38300, 3900ms Typical pressure and current profiles of H-mode plasma at edge region Bootstrap current at the edge region
Kinetic equilibrium reconstruction on EAST • With the constrains of magnetic diagnostics, pressure profile, edge current profile, we achieved the kinetic equilibrium • The current/q profiles at the central region are not reliable, though we have the global li constrain 38300, 3900ms Pressure, current profiles and configuration from kinetic EFIT and magnetic EFIT
Equilibrium construction • Lots of codes for equilibrium construction, most of them are fixed boundary codes • EFIT, CORSICA/TEQ, TOQ, ESC, JSOLVER …… • CORSICA • CORSICA has both direct and inverse solver • Inverse solver: coordinate, solve for R, Z, fixed boundary • Direct solver: coordinate, solve for , free boundary • CORSICA can easily change the plasma shape and profiles
Construct self-consistent equilibrium • To construct a self-consistent equilibrium, the self-consistent plasma shape and profiles must be given • Self-consistent profiles: • Bootstrap current dominated edge current • Self-consistent pedestal height and width, EPED model • EPED model (peeling-ballooning model + kinetic ballooning model, ELITE+BALOO) has successfully predict the pedestal height and width • This technic could be useful for EAST and CFETR