Technical Readiness Level For Plasma Control

Similar documents
The use of technical readiness levels in planning the fusion energy development

Technology readiness evaluations for fusion materials science & technology

System Upgrades to the DIII-D Facility

The Application of Technology Readiness Levels in Planning the Fusion Energy Sciences Program. M. S. Tillack. ARIES Project Meeting 4 5 September2008

The Role of a Long Pulse, High Heat Flux, Hot Walls Experiment in the Study of Plasma Wall Interactions for CTF & Demo

Active Control for Stabilization of Neoclassical Tearing Modes

C-Mod ICRF Research Program

Realization of Fusion Energy: How? When?

Technology readiness applied to materials for fusion applications

Helicon Wave Current Drive in KSTAR Plasmas

ICRF Physics in KSTAR Steady State

Contributions of Advanced Design Activities to Fusion Research

Advanced Tokamak Program and Lower Hybrid Experiment. Ron Parker MIT Plasma Science and Fusion Center

A Modular Commercial Tokamak Reactor with Day Long Pulses

RF Heating and Current Drive in the JT-60U Tokamak

Real-time Systems in Tokamak Devices. A case study: the JET Tokamak May 25, 2010

Research Thrust for Reliable Plasma Heating and Current Drive using ICRF

Compact Torus Injection for Fuelling* C. Xiao, A. Hirose, STOR-M team Plasma Physics Laboratory University of Saskatchewan

Improvements in the fast vertical control systems in KSTAR, EAST, NSTX and NSTX-U

A roadmap to the realization of fusion energy

Importance of edge physics in optimizing ICRF performance

Observation of Toroidal Flow on LHD

Study of Plasma Equilibrium during the AC Current Reversal Phase on the STOR-M Tokamak

Toroidal Rotation and Ion Temperature Validations in KSTAR Plasmas

RF Physics: Status and Plans

Profile Scan Studies on the Levitated Dipole Experiment

Investigation of ion toroidal rotation induced by Lower Hybrid waves in Alcator C-Mod * using integrated numerical codes

DEMO work in future. Association Euratom-Tekes. Leena Aho-Mantila VTT Technical Research Centre of Finland. Euratom-TEKES Annual Seminar 2013

Particle Simulation of Lower Hybrid Waves in Tokamak Plasmas

GA A25836 PRE-IONIZATION EXPERIMENTS IN THE DIII-D TOKAMAK USING X-MODE SECOND HARMONIC ELECTRON CYCLOTRON HEATING

GA A24030 ECE RADIOMETER UPGRADE ON THE DIII D TOKAMAK

Fusion Simulation Project (FSP) Workshop Report

Effect of Resonant and Non-resonant Magnetic Braking on Error Field Tolerance in High Beta Plasmas

GA A26495 PHYSICS OPERATIONS WITH THE DIII-D PLASMA CONTROL SYSTEM

Magnetic Reconnection and Ion Flows During Point Source Helicity Injection on the Pegasus Toroidal Experiment

Investigating High Frequency Magnetic Activity During Local Helicity Injection on the PEGASUS Toroidal Experiment

Sensitivity study for the optimization of the viewing chord arrangement of the ITER poloidal polarimeter

Real time control of the sawtooth period using EC launchers

Improved core transport triggered by off-axis ECRH switch-off on the HL-2A tokamak

Overview and Initial Results of the ETE Spherical Tokamak

Overview of ICRF Experiments on Alcator C-Mod*

GA A27238 MEASUREMENT OF DEUTERIUM ION TOROIDAL ROTATION AND COMPARISON TO NEOCLASSICAL THEORY IN THE DIII-D TOKAMAK

Korean Fusion Energy Development Strategy*

US ITER Electron Cyclotron System White Paper

Abstract. PEGASUS Toroidal Experiment University of Wisconsin-Madison

Whistlers, Helicons, Lower Hybrid Waves: the Physics of RF Wave Absorption for Current Drive Without Cyclotron Resonances

High Performance Computing for Plasma Control

Presented by Rob La Haye. on behalf of Francesco Volpe. at the 4 th IAEA-TM on ECRH for ITER

FESAC Panel on Priorities

Observation of Electron Bernstein Wave Heating in the RFP

Advanced Density Profile Reflectometry; the State-of-the-Art and Measurement Prospects for ITER

PLASMA BUILD-UP and CONFINEMENT IN URAGAN-2M DEVICE

Foundations for Knowledge Management Practices for the Nuclear Fusion Sector

Magnetics and Power System Upgrades for the Pegasus-U Experiment

Recent Results on RFX-mod control experiments in RFP and tokamak configuration

Implementing Agreement for Co operation in Development of the Stellarator Heliotron Concept (SH IA) Strategic Plan

Sustainment and Additional Heating of High-Beta Field-Reversed Configuration Plasmas

EX/P9-5. Comprehensive Control of Resistive Wall Modes in DIII-D Advanced Tokamak Plasmas

3D modeling of toroidal asymmetry due to localized divertor nitrogen puffing on Alcator C-Mod

Local Helicity Injection Startup and Edge Stability Studies in the Pegasus Toroidal Experiment

Mid Term Exam SES 405 Exploration Systems Engineering 3 March Your Name

Fusion Nuclear Science and T e T chnology Progr ogr m Issues and Strategy for Fusion Nuclear Science Facility (FNSF)

GA A22338 A HYBRID DIGITAL-ANALOG LONG PULSE INTEGRATOR

INITIAL RESULTS FROM THE MULTI-MEGAWATT 110 GHz ECH SYSTEM FOR THE DIII D TOKAMAK

Plasma Confinement by Pressure of Rotating Magnetic Field in Toroidal Device

Detection and application of Doppler and motional Stark features in the DNB emission spectrum in the high magnetic field of the Alcator C-Mod tokamak

Interdependence of Magnetic Islands, Halo Current and Runaway Electrons in T-10 Tokamak

Feedback control of ECRH for MHD mode stabilization on TEXTOR

Simulation Studies of Field-Reversed Configurations with Rotating Magnetic Field Current Drive

Structural Analysis of High-field-Side RF antennas during a disruption on the Advanced Divertor experiment (ADX)

Error Fields Expected in ITER and their Correction

ICRF-Edge and Surface Interactions

GA A26865 PEDESTAL TURBULENCE DYNAMICS IN ELMING AND ELM-FREE H-MODE PLASMAS

Varying Electron Cyclotron Resonance Heating to Modify Confinement on the Levitated Dipole Experiment

CXRS-edge Diagnostic in the Harsh ITER Environment

Active beam-based diagnostics in KSTAR

Lower Hybrid. Ron Parker Alcator C-Mod PAC Meeting January January 2006 Alcator C-Mod PAC Meeting 1

Increased Stable Beta in DIII D by Suppression of a Neoclassical Tearing Mode Using Electron Cyclotron Current Drive and Active Feedback

Gyung-Su Lee National Fusion R & D Center Korea Basic Science Institute

High Performance Engineering

GENERATION OF RF DRIVEN CUR RENTS BY LOWER-IIYBRID WAVE INJECTION IN THE VERSATOR II TOKAMAK

Pedestal Turbulence Dynamics in ELMing and ELM-free H-mode Plasmas

ICRF-Edge and Surface Interactions

DEVELOPMENT OF MULTIVARIABLE CONTROL TECHNIQUES FOR USE WITH THE DIII D PLASMA CONTROL SYSTEM

Technology Readiness Levels for Partitioning and Transmutation of Minor Actinides in Japan

Locked-mode avoidance and recovery without external momentum input using Ion Cyclotron Resonance Heating

Evaluation of a Field Aligned ICRF Antenna in Alcator C-Mod

Abstract. G.D. Garstka 47 th APS-DPP Denver October 27, Pegasus Toroidal Experiment University of Wisconsin-Madison

Pedestal Turbulence Dynamics in ELMing and ELM-free H-mode Plasmas

ICRF Mode Conversion Flow Drive Studies with Improved Wave Measurement by Phase Contrast Imaging

Task on the evaluation of the plasma response to the ITER ELM stabilization coils in ITER H- mode operational scenarios. Technical Specifications

Outline of optical design and viewing geometry for divertor Thomson scattering on MAST

SUMMARY OF THE EXPERIMENTAL SESSION EC-10 WORKSHOP

Neoclassical Tearing Mode Control with ECCD and Magnetic Island Evolution in JT-60U

Study of Ion Cyclotron Emissions due to DD Fusion Product Ions on JT-60U

C-Mod ICRF Program. Alcator C-Mod PAC Meeting January 25-27, 2006 MIT Cambridge MA. Presented by S.J. Wukitch

II. PHASE I: TECHNOLOGY DEVELOPMENT Phase I has five tasks that are to be carried out in parallel.

EXW/10-2Ra. Avoidance of Disruptions at High β N in ASDEX Upgrade with Off-Axis ECRH

Particle Simulation of Radio Frequency Waves in Fusion Plasmas

Dynamics of energetic particle driven modes and MHD modes in wall-stabilized high beta plasmas on JT-60U and DIII-D

Transcription:

Technical Readiness Level For Plasma Control PERSISTENT SURVEILLANCE FOR PIPELINE PROTECTION AND THREAT INTERDICTION A.D. Turnbull, General Atomics ARIES Team Meeting University of Wisconsin, Madison, WI May 28-29 2008

Control Of Plasma Shape And Profiles Requires Four Steps: Essentially Measuring A Quantity And Modifying It Identification of the required parameter value and acceptable range: This is defined by the design process and performance requirements Diagnosis of the current state: Diagnostic measurement How are the parameters measured? Actuator to modify the profile: How are they modified - what is the input controller? Algorithm to translate required change in profile to actuator signal: What is the algorithm for translating the required change in parameters to the needed change in controller? Ultimately the diagnostic and actuator technologies need to survive in a BPX environment

Technology Readiness Level: Concept Development TRL Generic Definition Issue-Specific Definition 1 Co nc ept Basic principles observed and formulated. Development of basic concepts for diagnostics and actuators for controlling plasma shape and profiles. 2 Co nc ept Technology concepts and/or applications formulated. +Design of systems and hardware to diagnose profiles and systems to modify profiles in open loop in a moderate β plasma. Development of robust algorithms for translating diagnostic measurements to actuator signals. 3 Co nc ept Analytical and experimental demonstration of critical function and/or proof of concept. +Demonstration of techniques for controlled plasma shape and profiles within approximate limits in closed loop in a moderate β laboratory plasma. + This can be performed in either a dedicated laboratory plasma physics experiment or one of the current national facilities

Technology Readiness Level: Proof Of Principle TRL 5 6 P o P P o P P o P Generic Definition Component and/or bench-scale validation in a laboratory environment. Component and/or breadboard validation in a relevant environment. System/subsystem model or prototype demonstration in relevant environment. Issue-Specific Definition #Demonstration of controlled plasma shape and profiles within approximate limits in closed loop in a current high temperature plasma confinement experiment. #Self-consistent integration of multiple techniques to control each of the required plasma parameters in closed loop in a current high temperature plasma confinement experiment. Scale-up of diagnostic and actuator technologies to realistic fusion conditions. Demonstration that excursions from transient phenomena can be kept to a tolerable level. # This should be performed in one of the current national facilities This step should be performed in a dedicated planned experiment such as KSTAR

Technology Readiness Level: Proof Of Performance TRL Generic Definition Issue-Specific Definition 7 Pe rfo rm an ce System prototype demonstration in an operational environment Demonstration of the integrated plasma shape and profile control system with control of excursions from transient phenomena in a high performance reactor grade plasma in long pulse, essentially steady state operation. 8 Pe rfo rm an ce Actual system completed and qualified through test and demonstration Demonstration of the integrated plasma shape and profile control system in a steady state burning plasma configuration. 9 Pe rfo rm an ce Actual system proven through successful mission operations Demonstration of the integrated plasma shape and profile control system in a steady state burning plasma configuration for lifetime conditions. This step can be performed in KSTAR or in ITER running in high power mode. ITER might be able to satisfactorily complete this step but it may require a burning plasma experiment. This may be a dedicated experiment or DEMO.

Plasma Parameters Requiring Diagnostics And Control Can Be Broken Down Into Seven Categories Global parameters: Fusion power Plasma beta Plasma shape: Elongation Triangularity Power handling control Confinement quality Heat and radiation loads Higher order shaping Plasma kinetic profiles: Pressure Temperature Density Plasma current density profile: Current density Safety factor Plasma rotation profile Plasma composition profiles: D-T ratios Impurities

Control Of Global Parameters: Fusion Power, Beta Confinement, And Power Loads Is Well Understood Required values and range set by fusion power requirements and POPCON calculations Measurements using: Equilibrium reconstruction Neutron rates and power flows to material surfaces Parameters modified by: Fueling, D-T ratios Control of transport barriers Translation algorithm requires: Time dependent 1 1/2 D transport calculations Overall, control of global parameters is unlikely to be an obstacle: Modest extrapolation scenario: Current TRL = Advanced concept scenario: Current TRL = Very high confidence that the techniques currently available will scale if applied in a BPX

Control Of Plasma Shape Is Also Well Advanced Required values and range set by ARIES-AT design Measurements using: External magnetic loop measurements Equilibrium reconstruction Parameters modified by external poloidal field coils Translation algorithms are well established: Routinely applied in all major tokamaks Elongations up to 3 to 1 and triangularity ~ 1 Overall control of plasma shape rates a moderate TRL: Modest extrapolation scenario: Current TRL = Advanced concept scenario: Current TRL = 3 High confidence techniques currently available will scale to a BPX: Divertor requirements may limit the higher triangularities needed for the most advanced scenarios

Control Of Pressure, Density, And Temperature Profiles Is A Key Feature Of All Advanced Scenarios Required profiles and ranges set by ARIES-AT design: T i ~ T e and n e from fusion cross section requirements Range from sensitivity calculations Profile measurements using Thomson scattering and Charge Exchange Recombination (CER) diagnostics Profiles modified by: Pellet injection, gas puffing, and Neutral Beam input RF wave heating Divertor pumping Translation of desired profiles to fueling input requires: Deposition calculations for pellets, RF, beams, and gas Alpha particle slowing down and heating calculations Equilibrium reconstruction Control of kinetic profiles is still an active area of current research: Modest extrapolation scenario: Current TRL = Advanced concept scenario: Current TRL = 3

Current Profile Control Techniques Are Less Developed But Present Experiments Are Moving To Closed Loop Required current profile and allowable range set by ARIES-AT design and sensitivity calculations Profile measurements using Motional Stark Effect (MSE): Requires at least a diagnostic Neutral Beam Equilibrium reconstruction from magnetic field pitch angle Current profile modified by noninductive current drive: ECCD, Lower Hybrid, and ICRF Translation of desired current profile to input current drive requires: Ray tracing and current drive deposition calculations Current research is actively focused on current profile control: Modest extrapolation scenario: Current TRL = Advanced concept scenario: Current TRL = 3 MSE diagnostic scales to higher fields but current drive techniques have scaling issues: Density limitations Efficiency scales with T but required driven current also increases

Plasma Rotation Profile Control Is A Key Issue For Advanced But Not For Modest Extrapolation Scenarios Required rotation values and profile set by resistive wall mode (RWM) stability and possibly confinement requirements: Minimum generally needs to be satisfied only Low momentum input a reactor is unlikely to rotate too fast Rotation profile measurements using: CER for impurity rotation Main ion rotation is not well diagnosed Rotation profile modified by: Momentum input from Neutral Beams Possibly external rotating nonaxisymmetric fields Translation of desired rotation to beam input requires: Beam deposition, angular momentum transport, particle loss, and magnetic drag calculations Rotation profile can be diagnosed but few methods to modify it exist: Modest extrapolation scenario (limited need):current TRL = Advanced concept scenario: Current TRL < 2

D-T Ratio Is Relatively Easily Controlled By Fuelling Required values set by fusion yield calculations: Allowable range needs to be adjustable during operation D-T mix diagnostics: Global measurements from neutron rates and fusion power No known method for obtaining D-T ratio profile measurements Global mix and profile modified by: Tritium neutral beam input Pellet fuelling Control of isotopic differential transport rates Translation of desired D-T ratios to fueling input requires: Deposition calculations for beams Alpha particle slowing down and heating calculations Neutron rates and fusion power easily diagnosed: Empirically determine needed adjustments in D-T fuelling Modest extrapolation scenario: Current TRL = Advanced concept scenario: Current TRL = High confidence current techniques will scale in a BPX

Impurity And Alpha Ash Not Easily Controlled: Requires Control Over Relative Particle And Heat Transport Rates Required values and allowable range set by fusion yield Impurity profile measurements using CER Impurity profile modified by: Altering balance between particle and energy confinement MHD fluctuations from Sawteeth and ELMs Translation of desired ash and impurity concentration to MHD fluctuation size and frequencies requires: Impurity transport calculations ELM and sawtooth frequency and size control Some techniques exist for selectively transporting impurities but are not yet reactor relevant: Temperature and density transport barriers Some ELM-free regimes hold some promise Modest extrapolation scenario: Current TRL = 3 Advanced concept scenario: Current TRL = 2

Key Issues For Advanced Scenario Are Scale Up Of Rotation Control And Impurity Control Technologies Issue Modest Extrapolation Scenario TRL Advanced Extrapolation Scenario TRL Scale up Confidence Level Global parameters Very High Plasma Shape 3 High Kinetic Profiles 3 Moderate Current Profile 3 Moderate Plasma Rotation 2 Low D-T Ratio High Impurities 3 2 Low-moderate