CUTIE - Revision history

Admin: Updated reference links

2018-04-03T13:26:15Z

Updated reference links

← Older revision		Revision as of 15:26, 3 April 2018
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	CUTIE is a quasi-neutral two-fluid computer model for turbulence in a toroidal plasma.		CUTIE is a quasi-neutral two-fluid computer model for turbulence in a toroidal plasma.
	<ref>~~[http://dx.doi.org/10.1088/0741-3335/42/12B/320~~ A. Thyagaraja, ''Numerical simulations of tokamak plasma turbulence and internal transport barriers'', Plasma Phys. Control. Fusion '''42''' (2000) B255]</ref>		<ref>A. Thyagaraja, ''Numerical simulations of tokamak plasma turbulence and internal transport barriers'', [[doi:10.1088/0741-3335/42/12B/320\|Plasma Phys. Control. Fusion '''42''' (2000) B255]]</ref>
	<ref>~~[http://dx.doi.org/10.1016/j.euromechflu.2003.10.009~~ A. Thyagaraja, P.J. Knight, and N. Loureiro, ''Mesoscale plasma dynamics, transport barriers and zonal flows: simulations and paradigms'', Eur. Journal of Mech. B/Fluids '''23''' (2004) 475]</ref>		<ref>A. Thyagaraja, P.J. Knight, and N. Loureiro, ''Mesoscale plasma dynamics, transport barriers and zonal flows: simulations and paradigms'', [[doi:10.1016/j.euromechflu.2003.10.009\|Eur. Journal of Mech. B/Fluids '''23''' (2004) 475]]</ref>
	<ref>~~[http://link.aps.org/doi/10.1103/PhysRevLett.94.035002~~ M.R. de Baar, A. Thyagaraja, G.M.D. Hogeweij, P.J. Knight, and E. Min, ''Global Plasma Turbulence Simulations of q=3 Sawtoothlike Events in the RTP Tokamak'', Phys. Rev. Lett. '''94''' (2005) 035002]</ref>		<ref>M.R. de Baar, A. Thyagaraja, G.M.D. Hogeweij, P.J. Knight, and E. Min, ''Global Plasma Turbulence Simulations of q=3 Sawtoothlike Events in the RTP Tokamak'', [[doi:10.1103/PhysRevLett.94.035002\|Phys. Rev. Lett. '''94''' (2005) 035002]]</ref>
	<ref name="cutie">~~[http://link.aip.org/link/?PHPAEN/12/090907/1~~ A. Thyagaraja, P.J. Knight, M.R. de Baar, G.M.D. Hogeweij, and E. Min, ''Profile-turbulence interactions, magnetohydrodynamic relaxations, and transport in tokamaks'', Phys. Plasmas '''12''' (2005) 090907]</ref>		<ref name="cutie">A. Thyagaraja, P.J. Knight, M.R. de Baar, G.M.D. Hogeweij, and E. Min, ''Profile-turbulence interactions, magnetohydrodynamic relaxations, and transport in tokamaks'', [[doi:10.1063/1.2034387\|Phys. Plasmas '''12''' (2005) 090907]]</ref>
	The large aspect ratio tokamak ordering is used (''R/a >> 1''), and ''B<sub>p</sub> << B<sub>tor</sub>, β << 1''.		The large aspect ratio tokamak ordering is used (''R/a >> 1''), and ''B<sub>p</sub> << B<sub>tor</sub>, β << 1''.
	The plasma modelled consists of electrons and a single ion species.		The plasma modelled consists of electrons and a single ion species.

Admin at 10:33, 15 August 2012

2012-08-15T10:33:16Z

← Older revision		Revision as of 12:33, 15 August 2012
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	== References ==		== References ==
	<references />		<references />

			[[Category:Software]]

Admin: Reverted edits by 204.45.66.178 (Talk) to last revision by Admin

2011-05-19T05:31:18Z

Reverted edits by 204.45.66.178 (Talk) to last revision by Admin

← Older revision		Revision as of 07:31, 19 May 2011
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	* [[Laboratorio Nacional de Fusión]], [[CIEMAT]], Madrid, Spain		* [[Laboratorio Nacional de Fusión]], [[CIEMAT]], Madrid, Spain

	~~THX that's a great aswner!~~		== References ==
			<references />

204.45.66.178: /* References */

2011-05-19T05:03:11Z

References

← Older revision		Revision as of 07:03, 19 May 2011
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	* [[Laboratorio Nacional de Fusión]], [[CIEMAT]], Madrid, Spain		* [[Laboratorio Nacional de Fusión]], [[CIEMAT]], Madrid, Spain

	~~== References ==~~		THX that's a great aswner!
	~~<references />~~

Admin at 14:31, 30 July 2010

2010-07-30T14:31:27Z

← Older revision		Revision as of 16:31, 30 July 2010
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	electron and ion temperatures (''T<sub>e</sub>, T<sub>i</sub>''), the ion fluid velocty (''v''),		electron and ion temperatures (''T<sub>e</sub>, T<sub>i</sub>''), the ion fluid velocty (''v''),
	the electrostatic potential (Φ) and the parallel vector potential (Ψ).		the electrostatic potential (Φ) and the parallel vector potential (Ψ).
	The poloidal magnetic field (and consequently the safety factor, ''q'') evolves in time.		The poloidal magnetic field (and consequently the [[Rotational transform\|safety factor]], ''q'') evolves in time.
	[[File:CUTIE.jpg\|265px\|thumb\|right\|Density fluctuations in a CUTIE simulation (from <ref name="cutie"/>)]]		[[File:CUTIE.jpg\|265px\|thumb\|right\|Density fluctuations in a CUTIE simulation (from <ref name="cutie"/>)]]

Admin at 08:23, 7 December 2009

2009-12-07T08:23:47Z

← Older revision		Revision as of 10:23, 7 December 2009
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	CUTIE is a quasi-neutral two-fluid computer model for turbulence in a toroidal plasma.		CUTIE is a quasi-neutral two-fluid computer model for turbulence in a toroidal plasma.
	<ref>[http://dx.doi.org/10.1088/0741-3335/42/12B/320 A. Thyagaraja, Plasma Phys. Control. Fusion '''42''' (2000) B255]</ref>		<ref>[http://dx.doi.org/10.1088/0741-3335/42/12B/320 A. Thyagaraja, ''Numerical simulations of tokamak plasma turbulence and internal transport barriers'', Plasma Phys. Control. Fusion '''42''' (2000) B255]</ref>
	<ref>[http://dx.doi.org/10.1016/j.euromechflu.2003.10.009 A. Thyagaraja, P.J. Knight, and N. Loureiro, Eur. Journal of Mech. B/Fluids '''23''' (2004) 475]</ref>		<ref>[http://dx.doi.org/10.1016/j.euromechflu.2003.10.009 A. Thyagaraja, P.J. Knight, and N. Loureiro, ''Mesoscale plasma dynamics, transport barriers and zonal flows: simulations and paradigms'', Eur. Journal of Mech. B/Fluids '''23''' (2004) 475]</ref>
	<ref>[http://link.aps.org/doi/10.1103/PhysRevLett.94.035002 M.R. de Baar, A. Thyagaraja, G.M.D. Hogeweij, P.J. Knight, and E. Min, Phys. Rev. Lett. '''94''' (2005) 035002]</ref>		<ref>[http://link.aps.org/doi/10.1103/PhysRevLett.94.035002 M.R. de Baar, A. Thyagaraja, G.M.D. Hogeweij, P.J. Knight, and E. Min, ''Global Plasma Turbulence Simulations of q=3 Sawtoothlike Events in the RTP Tokamak'', Phys. Rev. Lett. '''94''' (2005) 035002]</ref>
	<ref name="cutie">[http://link.aip.org/link/?PHPAEN/12/090907/1 A. Thyagaraja, P.J. Knight, M.R. de Baar, G.M.D. Hogeweij, and E. Min, Phys. Plasmas '''12''' (2005) 090907]</ref>		<ref name="cutie">[http://link.aip.org/link/?PHPAEN/12/090907/1 A. Thyagaraja, P.J. Knight, M.R. de Baar, G.M.D. Hogeweij, and E. Min, ''Profile-turbulence interactions, magnetohydrodynamic relaxations, and transport in tokamaks'', Phys. Plasmas '''12''' (2005) 090907]</ref>
	The large aspect ratio tokamak ordering is used (''R/a >> 1''), and ''B<sub>p</sub> << B<sub>tor</sub>, β << 1''.		The large aspect ratio tokamak ordering is used (''R/a >> 1''), and ''B<sub>p</sub> << B<sub>tor</sub>, β << 1''.
	The plasma modelled consists of electrons and a single ion species.		The plasma modelled consists of electrons and a single ion species.

Admin at 12:15, 4 December 2009

2009-12-04T12:15:46Z

← Older revision		Revision as of 14:15, 4 December 2009
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	the electrostatic potential (Φ) and the parallel vector potential (Ψ).		the electrostatic potential (Φ) and the parallel vector potential (Ψ).
	The poloidal magnetic field (and consequently the safety factor, ''q'') evolves in time.		The poloidal magnetic field (and consequently the safety factor, ''q'') evolves in time.
	[[File:CUTIE.jpg\|265px\|thumb\|right\|Density ~~fluxtuations~~ in a CUTIE simulation (from <ref name="cutie"/>)]]		[[File:CUTIE.jpg\|265px\|thumb\|right\|Density fluctuations in a CUTIE simulation (from <ref name="cutie"/>)]]

	The code solves the evolution on the meso-scale level (larger than the ion gyroradius), co-evolving the [[Flux surface\|flux surface]] averaged quantities and the turbulence in a self-consistent manner;		The code solves the evolution on the meso-scale level (larger than the ion gyroradius), co-evolving the [[Flux surface\|flux surface]] averaged quantities and the turbulence in a self-consistent manner;

Admin at 12:14, 4 December 2009

2009-12-04T12:14:55Z

← Older revision		Revision as of 14:14, 4 December 2009
Line 1:		Line 1:
	CUTIE is a quasi-neutral two-fluid computer model for turbulence in a toroidal plasma.		CUTIE is a quasi-neutral two-fluid computer model for turbulence in a toroidal plasma.
			<ref>[http://dx.doi.org/10.1088/0741-3335/42/12B/320 A. Thyagaraja, Plasma Phys. Control. Fusion '''42''' (2000) B255]</ref>
			<ref>[http://dx.doi.org/10.1016/j.euromechflu.2003.10.009 A. Thyagaraja, P.J. Knight, and N. Loureiro, Eur. Journal of Mech. B/Fluids '''23''' (2004) 475]</ref>
			<ref>[http://link.aps.org/doi/10.1103/PhysRevLett.94.035002 M.R. de Baar, A. Thyagaraja, G.M.D. Hogeweij, P.J. Knight, and E. Min, Phys. Rev. Lett. '''94''' (2005) 035002]</ref>
			<ref name="cutie">[http://link.aip.org/link/?PHPAEN/12/090907/1 A. Thyagaraja, P.J. Knight, M.R. de Baar, G.M.D. Hogeweij, and E. Min, Phys. Plasmas '''12''' (2005) 090907]</ref>
	The large aspect ratio tokamak ordering is used (''R/a >> 1''), and ''B<sub>p</sub> << B<sub>tor</sub>, β << 1''.		The large aspect ratio tokamak ordering is used (''R/a >> 1''), and ''B<sub>p</sub> << B<sub>tor</sub>, β << 1''.
	The plasma modelled consists of electrons and a single ion species.		The plasma modelled consists of electrons and a single ion species.
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	the electrostatic potential (Φ) and the parallel vector potential (Ψ).		the electrostatic potential (Φ) and the parallel vector potential (Ψ).
	The poloidal magnetic field (and consequently the safety factor, ''q'') evolves in time.		The poloidal magnetic field (and consequently the safety factor, ''q'') evolves in time.
			[[File:CUTIE.jpg\|265px\|thumb\|right\|Density fluxtuations in a CUTIE simulation (from <ref name="cutie"/>)]]

	The code solves the evolution on the meso-scale level (larger than the ion gyroradius), co-evolving the [[Flux surface\|flux surface]] averaged quantities and the turbulence in a self-consistent manner;		The code solves the evolution on the meso-scale level (larger than the ion gyroradius), co-evolving the [[Flux surface\|flux surface]] averaged quantities and the turbulence in a self-consistent manner;
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	linear and non-linear shear Alfvén waves, slow magneto-acoustic modes, drift-tearing modes, ballooning modes (ideal and viscoresistive), and the fluid branch of the ion temperature gradient (ITG) instability.		linear and non-linear shear Alfvén waves, slow magneto-acoustic modes, drift-tearing modes, ballooning modes (ideal and viscoresistive), and the fluid branch of the ion temperature gradient (ITG) instability.
	The code contains sufficient mechanisms for the generation of sheared flow by turbulence and produces a spontaneous confinement transition similar to the [[H-mode\|L-H transition]] in experimental devices.		The code contains sufficient mechanisms for the generation of sheared flow by turbulence and produces a spontaneous confinement transition similar to the [[H-mode\|L-H transition]] in experimental devices.
	~~<ref>[http://dx.doi.org/10.1088/0741-3335/42/12B/320 A. Thyagaraja, Plasma Phys. Control. Fusion '''42''' (2000) B255]</ref>~~
	~~<ref>[http://dx.doi.org/10.1016/j.euromechflu.2003.10.009 A. Thyagaraja, P.J. Knight, and N. Loureiro, Eur. Journal of Mech. B/Fluids '''23''' (2004) 475]</ref>~~
	~~<ref>[http://link.aps.org/doi/10.1103/PhysRevLett.94.035002 M.R. de Baar, A. Thyagaraja, G.M.D. Hogeweij, P.J. Knight, and E. Min, Phys. Rev. Lett. '''94''' (2005) 035002]</ref>~~
	~~<ref>[http://link.aip.org/link/?PHPAEN/12/090907/1 A. Thyagaraja, P.J. Knight, M.R. de Baar, G.M.D. Hogeweij, and E. Min, Phys. Plasmas '''12''' (2005) 090907]</ref>~~

	== Code history ==		== Code history ==

Admin at 12:00, 4 December 2009

2009-12-04T12:00:30Z

← Older revision		Revision as of 14:00, 4 December 2009
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	The code contains sufficient mechanisms for the generation of sheared flow by turbulence and produces a spontaneous confinement transition similar to the [[H-mode\|L-H transition]] in experimental devices.		The code contains sufficient mechanisms for the generation of sheared flow by turbulence and produces a spontaneous confinement transition similar to the [[H-mode\|L-H transition]] in experimental devices.
	<ref>[http://dx.doi.org/10.1088/0741-3335/42/12B/320 A. Thyagaraja, Plasma Phys. Control. Fusion '''42''' (2000) B255]</ref>		<ref>[http://dx.doi.org/10.1088/0741-3335/42/12B/320 A. Thyagaraja, Plasma Phys. Control. Fusion '''42''' (2000) B255]</ref>
	<ref>A. Thyagaraja, P.J. Knight, and N. Loureiro, Eur. Journal of Mech. B/Fluids '''23''' (2004) 475</ref>		<ref>[http://dx.doi.org/10.1016/j.euromechflu.2003.10.009 A. Thyagaraja, P.J. Knight, and N. Loureiro, Eur. Journal of Mech. B/Fluids '''23''' (2004) 475]</ref>
	<ref>[http://link.aps.org/doi/10.1103/PhysRevLett.94.035002 M.R. de Baar, A. Thyagaraja, G.M.D. Hogeweij, P.J. Knight, and E. Min, Phys. Rev. Lett. '''94''' (2005) 035002]</ref>		<ref>[http://link.aps.org/doi/10.1103/PhysRevLett.94.035002 M.R. de Baar, A. Thyagaraja, G.M.D. Hogeweij, P.J. Knight, and E. Min, Phys. Rev. Lett. '''94''' (2005) 035002]</ref>
	<ref>[http://link.aip.org/link/?PHPAEN/12/090907/1 A. Thyagaraja, P.J. Knight, M.R. de Baar, G.M.D. Hogeweij, and E. Min, Phys. Plasmas '''12''' (2005) 090907]</ref>		<ref>[http://link.aip.org/link/?PHPAEN/12/090907/1 A. Thyagaraja, P.J. Knight, M.R. de Baar, G.M.D. Hogeweij, and E. Min, Phys. Plasmas '''12''' (2005) 090907]</ref>

Admin: /* Current installations */

2009-12-04T11:35:52Z

Current installations

← Older revision		Revision as of 13:35, 4 December 2009
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	The code is being used at:		The code is being used at:
	* [[http://www.ccfe.ac.uk/ Culham Centre for Fusion Energy]], Culham, UK (code origin)		* [http://www.ccfe.ac.uk/ Culham Centre for Fusion Energy], Culham, UK (code origin)
	* [[Laboratorio Nacional de Fusión]], [[CIEMAT]], Madrid, Spain		* [[Laboratorio Nacional de Fusión]], [[CIEMAT]], Madrid, Spain

	== References ==		== References ==
	<references />		<references />