ELM frequency feedback control on JET

This paper describes the first development and implementation of a closed loop edge localized mode (ELM) frequency controller using gas injection as the actuator. The controller has been extensively used in recent experiments on JET and it has proved to work well at ELM frequencies in the 15–40 Hz range. The controller responds effectively to a variety of disturbances, generally recovering the requested ELM frequency within approximately 500 ms. Controlling the ELM frequency has become of prime importance in the new JET configuration with all metal walls, where insufficient ELM frequency is associated with excessive tungsten influx. The controller has allowed successful operation near the minimum acceptable ELM frequency where the best plasma confinement can be achieved. Use of the ELM frequency controller in conjunction with pellet injection has enabled investigations of ELM triggering by pellets while maintaining the desired ELM frequency even when pellets fail to trigger ELMs.

[1]  Jet Efda Contributors,et al.  Global and pedestal confinement in JET with a Be/W metallic wall , 2014 .

[2]  A. Loarte,et al.  Progress on the application of ELM control schemes to ITER scenarios from the non-active phase to DT operation , 2014 .

[3]  I. T. Chapman,et al.  Sawtooth control in JET with ITER relevant low field side resonance ion cyclotron resonance heating and ITER-like wall , 2014 .

[4]  Jet Efda Contributors,et al.  Observations on the W-transport in the core plasma of JET and ASDEX Upgrade , 2013 .

[5]  Jet Efda Contributors,et al.  The effect of a metal wall on confinement in JET and ASDEX Upgrade , 2013 .

[6]  Jet Efda Contributors,et al.  Overview of the JET results with the ITER-like wall , 2013 .

[7]  P B Parks,et al.  Reduction of edge-localized mode intensity using high-repetition-rate pellet injection in tokamak H-mode plasmas. , 2013, Physical review letters.

[8]  Jet Efda Contributors,et al.  First operation with the JET International Thermonuclear Experimental Reactor-like wall , 2013 .

[9]  A. Neishtadt,et al.  Quasiadiabatic dynamics of charged particles in a space plasma , 2013 .

[10]  Jet Efda Contributors,et al.  First scenario development with the JET new ITER-like wall , 2013 .

[11]  M. N. A. Beurskens,et al.  JET ITER-like wall—overview and experimental programme , 2011 .

[12]  I. T. Chapman,et al.  Feedback control of the sawtooth period through real time control of the ion cyclotron resonance frequency , 2011 .

[13]  Ronald Wenninger,et al.  ELM pacing investigations at JET with the new pellet launcher , 2011 .

[14]  E. L. Luna ELM mitigation studies in JET and implications for ITER , 2009 .

[15]  R. Neu,et al.  Plasma-wall interaction and plasma behaviour in the non-boronised all tungsten ASDEX Upgrade , 2009 .

[16]  P. C. de Vries,et al.  Recent contribution of JET to the ITER physics , 2009 .

[17]  A. Loarte,et al.  Chapter 3: ELMy H-Mode Operation in JET , 2008 .

[18]  Contributors Jet-Efda,et al.  Synchronous ELM Pacing at JET using the Vertical Stabilisation Controller , 2008 .

[19]  M. Gryaznevich,et al.  Active control of type-I edge localized modes on JET. Invited Paper , 2007 .

[20]  R. Sartori,et al.  Edge localized modes: recent experimental findings and related issues , 2007 .

[21]  Keith H. Burrell,et al.  Edge stability and transport control with resonant magnetic perturbations in collisionless tokamak plasmas , 2006 .

[22]  J. B. Lister,et al.  LETTER TO THE EDITOR: Frequency control of type-I ELMs by magnetic triggering in ASDEX Upgrade , 2004 .

[23]  M E Fenstermacher,et al.  Suppression of large edge-localized modes in high-confinement DIII-D plasmas with a stochastic magnetic boundary. , 2004, Physical review letters.

[24]  L. Horton,et al.  ELM pace making and mitigation by pellet injection in ASDEX Upgrade , 2004 .

[25]  V. Parail,et al.  Characterization of pedestal parameters and edge localized mode energy losses in the Joint European Torus and predictions for the International Thermonuclear Experimental Reactor , 2004 .

[26]  M. Sugihara,et al.  Characteristics of type I ELM energy and particle losses in existing devices and their extrapolation to ITER , 2003 .

[27]  J. B. Lister,et al.  Magnetic triggering of ELMs in TCV , 2003 .

[28]  A. Loarte,et al.  Assessment of erosion of the ITER divertor targets during type I ELMs , 2003 .

[29]  Bogdan Hnat,et al.  Self-organization of internal pedestals in a sandpile , 2003 .

[30]  Filippo Sartori,et al.  Plasma control at JET , 2000 .

[31]  R. L. Miller,et al.  Magnetohydrodynamic stability of tokamak edge plasmas , 1998 .

[32]  A. Loarte,et al.  Influence of active pumping on density and confinement behaviour of JET plasmas , 1997 .

[33]  M. Mori Active control of H-mode , 1996 .

[34]  H. Zohm Edge localized modes (ELMs) , 1996 .

[35]  Geist,et al.  H mode of the W 7-AS stellarator. , 1993, Physical review letters.

[36]  M. Keilhacker,et al.  Confinement Studies in L and H-Type ASDEX Discharges , 1984 .

[37]  J. R. Myra,et al.  Stability optimization in tandem mirrors , 1984 .