TJ-II: Pellet induced Enhanced Confinement: the role of Er and turbulence: Difference between revisions

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== Description of the activity ==
== Description of the activity ==
Enter description here <ref>A. Einstein, Journal of Exceptional Results (2017)</ref>, including motivation/objectives and experience of the proponent (typically one-two pages)


Pellet-induced Enhanced Confinement (PiEC) has been recently reported [1] in discharges made in the stellarator TJ-II after a cryogenic fuel pellet is injected into its neutral beam injection (NBI) heated phase. In addition to increased particle density in the plasma core after pellet injection (PI), these plasmas show diamagnetic energy content up to 40% higher to the reference shot without PI. Moreover, the energy confinement time, as determined using a diamagnetic loop, is enhanced when compared to predictions obtained using the International Stellarator Scaling law (H. Yamada et al., Nucl. Fusion 45 (2005) 1684). In general, the PiEC in TJ-II is characterized by increased density gradients, by enhanced negative radial electric fields that extend from the plasma edge region to the core, as observed by HIBP and Doppler reflectometer systems, as well as by reductions in density, plasma potential and magnetic fluctuations in the plasma core.
A Pellet-induced Enhanced Confinement (PiEC) regime has been recently reported <ref>I. García-Cortés et al. submitted for publication in Nucl. Fusion</ref> in discharges made in the TJ-II after a cryogenic fuel pellet is injected into its neutral beam injection (NBI) heated phase. In addition to increased particle density in the plasma core after pellet injection (PI), these plasmas show diamagnetic energy content up to 40% higher to in reference shots without PI. Moreover, the energy confinement time, as determined using a diamagnetic loop, is enhanced when compared to predictions obtained using the International Stellarator Scaling law <ref>H. Yamada et al., Nucl. Fusion 45 (2005) 1684</ref>. In general, the PiEC in TJ-II is characterized by increased density gradients, by enhanced negative radial electric fields that extend from the plasma edge region to the core, as observed by HIBP and Doppler reflectometer systems, as well as by reductions in density, plasma potential and magnetic fluctuations in the plasma core.
However, the underlying physics that can induce this regime is still unclear in TJ-II. Taking into account that the Er and turbulence seems to play un key role in similar phenomena in W7-X (enhanced confinement after pellet injection), we propose series of shots with controlled density and with different NBI heating power (from low, only one NBI to high power, both NBI) in order to study at the same time the evolution of profiles like Er (by HIBP and DR) and density and its flucutations (HIBP and DR).
 
However, the underlying physics that can induce this regime is still unclear in TJ-II. Taking into account that Er and turbulence seems to play a key role in similar phenomena observed in the W7-X (enhanced confinement after pellet injection)<ref>T. Estrada et al., Nucl. Fusion 61 (2021) 046008</ref>, we propose series of PIs into plasmas with controlled density and different NBI heating powers (from low power, with 1 NBI working, to high power, with both NBI working) in order to study simultaneously the evolution of plasma potential and Er profiles (HIBPs and DR) as well as of the plasma density and its fluctations (HIBPs and DR).


== International or National funding project or entity ==
== International or National funding project or entity ==


Cryogenic and impurity pellet studies in the stellarators TJ-II and W7-X
Studies of fuelling and impurity control in the stellarators TJ-II and W7-X through the use of cryogenic and TESPEl pellets (Estudios de abastacimiento y control de impurezas en los stellarators mediante el uso de perdigones criogenicos y TESPEL",
Ref: PID2020-116599RB-I00
Ref: PID2020-116599RB-I00


== Description of required resources ==
== Description of required resources ==
Required resources:
Required resources:
* Number of plasma discharges or days of operation: 2 days (if possible to make scan in NBI power and magnetic configuration)
* Number of plasma discharges or days of operation: 2 days (scan in NBI power and magnetic configuration)  
* Essential diagnostic systems: TS, HIBP, Doppler Reflectometer, He-Beam.
* Essential diagnostic systems: TS, HIBP, Doppler Reflectometer, He-Beam, Pellet injection
* Type of plasmas (heating configuration): NBI#1, NIB#2 and NBI#1+2
* Type of plasmas (heating configuration): ECRH, NBI
* Specific requirements on wall conditioning if any:
* Specific requirements on wall conditioning if any: Good control of NBI heated plasmas
* External users: need a local computer account for data access: yes/no
* External users: need a local computer account for data access: no
* Any external equipment to be integrated? Provide description and integration needs:
* Any external equipment to be integrated? No:


== Preferred dates and degree of flexibility ==
== Preferred dates and degree of flexibility ==
Preferred dates: (format dd-mm-yyyy)
Preferred dates: 26-10-2021 to 30-11-2021 when HIBPs available


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[[Category:TJ-II internal documents]]
[[Category:TJ-II internal documents]]
[[Category:TJ-II experimental proposals Autumn 2021]]
[[Category:TJ-II experimental proposals Autumn 2021]]
<hr>

Latest revision as of 10:52, 23 September 2021

Experimental campaign

Autumn 2021

Proposal title

Pellet induced Enhanced Confinement regime in NBI plasmas: the role of Er and turbulence in PiEC phase

Name and affiliation of proponent

I. García-Cortés, K. McCarthy, Nerea Panadero, Macarena Liniers, Teresa Estrada, Daniel Carralero and HIBP group

Laboratorio Nacional de Fusión, CIEMAT

Details of contact person at LNF

If applicable, enter contact person here or write N/A

Description of the activity

A Pellet-induced Enhanced Confinement (PiEC) regime has been recently reported [1] in discharges made in the TJ-II after a cryogenic fuel pellet is injected into its neutral beam injection (NBI) heated phase. In addition to increased particle density in the plasma core after pellet injection (PI), these plasmas show diamagnetic energy content up to 40% higher to in reference shots without PI. Moreover, the energy confinement time, as determined using a diamagnetic loop, is enhanced when compared to predictions obtained using the International Stellarator Scaling law [2]. In general, the PiEC in TJ-II is characterized by increased density gradients, by enhanced negative radial electric fields that extend from the plasma edge region to the core, as observed by HIBP and Doppler reflectometer systems, as well as by reductions in density, plasma potential and magnetic fluctuations in the plasma core.

However, the underlying physics that can induce this regime is still unclear in TJ-II. Taking into account that Er and turbulence seems to play a key role in similar phenomena observed in the W7-X (enhanced confinement after pellet injection)[3], we propose series of PIs into plasmas with controlled density and different NBI heating powers (from low power, with 1 NBI working, to high power, with both NBI working) in order to study simultaneously the evolution of plasma potential and Er profiles (HIBPs and DR) as well as of the plasma density and its fluctations (HIBPs and DR).

International or National funding project or entity

Studies of fuelling and impurity control in the stellarators TJ-II and W7-X through the use of cryogenic and TESPEl pellets (Estudios de abastacimiento y control de impurezas en los stellarators mediante el uso de perdigones criogenicos y TESPEL", Ref: PID2020-116599RB-I00

Description of required resources

Required resources:

  • Number of plasma discharges or days of operation: 2 days (scan in NBI power and magnetic configuration)
  • Essential diagnostic systems: TS, HIBP, Doppler Reflectometer, He-Beam, Pellet injection
  • Type of plasmas (heating configuration): ECRH, NBI
  • Specific requirements on wall conditioning if any: Good control of NBI heated plasmas
  • External users: need a local computer account for data access: no
  • Any external equipment to be integrated? No:

Preferred dates and degree of flexibility

Preferred dates: 26-10-2021 to 30-11-2021 when HIBPs available


References

  1. I. García-Cortés et al. submitted for publication in Nucl. Fusion
  2. H. Yamada et al., Nucl. Fusion 45 (2005) 1684
  3. T. Estrada et al., Nucl. Fusion 61 (2021) 046008

Back to list of experimental proposals