Analysis of Runaway Beam Suppression Experiments in FTU
Creators
- 1. Università di Tor Vergata, 00173 Rome (Italy)
- 2. ENEA C. R. Frascati, Dipartimento FSN, Frascati (Italy)
- 3. Universidad Carlos III de Madrid, Madrid (Spain)
Description
Full text: The challenging task for a disruption mitigation system (DMS) is the implementation of reliable strategies in order to mitigate thermal, mechanical and electromagnetic loads at disruptions. Furthermore, the DMS has to cope with control and suppression of runaway electron beams, which are possibly generated during major disruptions, in order to avoid localized high-energy deposition causing deep melting of the structures. Strategies for runaway electron (RE) suppression are massive gas injection (MGI) or shattered pellet injection (SPI) although alternative or simultaneous strategies based on RE current dissipation via the central solenoid (ohmic coil) have been proposed. In ITER a preemptive strategy exploiting the central solenoid to deal with current quenches (CQ), yielding RE beam onset with current drop less than 5 MA, has been proposed. In the case the position control of the RE beam is not lost during the CQ, the maximum RE beam current decay rate has to remain below 0.5 MA/s, a limit that increases up to 1 MA/s for initial RE current of 12 MA. In FTU a large database (650 pulses) of highly energetic post disruption RE beams, produced spontaneously or with high-Z gas injection, have been analyzed. The study reveals that the decay rate during RE beam current ramp-down is an important parameter for runaway energy suppression. We have proposed a possible performance index to define suitable characteristics of the RE beam controller. Analysis of experimental data indicates that the reduction of the runaway current is possible when associated to small decay rate (longer confinement) of about 1 MA/s and a dedicated RE beam controller. Other important factors of RE beam premature final loss have been found to be: the large radial shift of the RE beam that potentially causes impacts on the low field side of the vessel during the plateau phase, MHD instabilities induced by large electrical field, VDE (elongated beams). The hysteretic behaviour of the runaway dynamics has been highlighted and experimentally quantified. Such nonlinearity affects runaway dynamics leading to increased density thresholds for runaway suppression once they have been previously formed. (author)
Additional details
Identifiers
Publishing Information
- Imprint Title
- 26. IAEA Fusion Energy Conference. Programme, Abstracts and Conference Material
- Imprint Pagination
- 935 p.
- Journal Page Range
- p. 433
- Report number
- IAEA-CN--234
Conference
- Title
- 26. IAEA Fusion Energy Conference
- Acronym
- FEC 2016
- Dates
- 17-22 Oct 2016
- Place
- Kyoto (Japan)
INIS
- Country of Publication
- International Atomic Energy Agency (IAEA)
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 49093311
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Resource subtype / Literary indicator
- Conference, Numerical Data
- Descriptors DEI
- BEAM CURRENTS; COEFFICIENT OF PERFORMANCE; CONTAINERS; CONTROL; ELECTRIC FIELDS; ELECTRON BEAMS; ENERGY LOSSES; EXPERIMENTAL DATA; FT TOKAMAK; GAS INJECTION; INSTABILITY; ITER TOKAMAK; MAGNETOHYDRODYNAMICS; MELTING; PELLET INJECTION; RUNAWAY ELECTRONS; SOLENOIDS
- Descriptors DEC
- BEAMS; CLOSED PLASMA DEVICES; CURRENTS; DATA; ELECTRIC COILS; ELECTRICAL EQUIPMENT; ELECTRONS; ELEMENTARY PARTICLES; EQUIPMENT; FERMIONS; FLUID INJECTION; FLUID MECHANICS; HYDRODYNAMICS; INFORMATION; LEPTON BEAMS; LEPTONS; LOSSES; MECHANICS; NUMERICAL DATA; PARTICLE BEAMS; PHASE TRANSFORMATIONS; THERMONUCLEAR DEVICES; THERMONUCLEAR REACTORS; TOKAMAK DEVICES; TOKAMAK TYPE REACTORS
Optional Information
- Notes
- Abstract only
- Secondary number(s)
- IAEA-CN--234-0527