EUTERPE - Revision history

Sanedi at 07:20, 28 June 2022

2022-06-28T07:20:37Z

← Older revision		Revision as of 09:20, 28 June 2022
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	<ref>V. Kornilov, R. Kleiber, and R. Hatzky, [[doi:10.1088/0029-5515/45/4/003\|Nucl. Fusion '''45''': 238 (2005)]]</ref>		<ref>V. Kornilov, R. Kleiber, and R. Hatzky, [[doi:10.1088/0029-5515/45/4/003\|Nucl. Fusion '''45''': 238 (2005)]]</ref>
	<ref>R. Kleiber, ''Global linear gyrokinetic simulations for stellarator and axisymmetric equilibria'', Joint Varenna-Lausanne International Workshop. [[doi:10.1063/1.2404546\|AIP Conference Proceedings, 871, p. 136, 2006]]</ref>		<ref>R. Kleiber, ''Global linear gyrokinetic simulations for stellarator and axisymmetric equilibria'', Joint Varenna-Lausanne International Workshop. [[doi:10.1063/1.2404546\|AIP Conference Proceedings, 871, p. 136, 2006]]</ref>
	<ref>[[http://fusionsites.ciemat.es/picgklnf/]]</ref>.		<ref>Particle in cell simulations at the Laboratorio Nacional de Fusión[[http://fusionsites.ciemat.es/picgklnf/]]</ref>.
	Afterwards, the code has been heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.		Afterwards, the code has been heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.

Sanedi at 07:19, 28 June 2022

2022-06-28T07:19:32Z

← Older revision		Revision as of 09:19, 28 June 2022
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	<ref>V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. [[doi:10.1063/1.1737393\|Phys. Plasmas '''11''': 3196 (2004)]]</ref>		<ref>V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. [[doi:10.1063/1.1737393\|Phys. Plasmas '''11''': 3196 (2004)]]</ref>
	<ref>V. Kornilov, R. Kleiber, and R. Hatzky, [[doi:10.1088/0029-5515/45/4/003\|Nucl. Fusion '''45''': 238 (2005)]]</ref>		<ref>V. Kornilov, R. Kleiber, and R. Hatzky, [[doi:10.1088/0029-5515/45/4/003\|Nucl. Fusion '''45''': 238 (2005)]]</ref>
	<ref>R. Kleiber, ''Global linear gyrokinetic simulations for stellarator and axisymmetric equilibria'', Joint Varenna-Lausanne International Workshop. [[doi:10.1063/1.2404546\|AIP Conference Proceedings, 871, p. 136, 2006]]</ref>.		<ref>R. Kleiber, ''Global linear gyrokinetic simulations for stellarator and axisymmetric equilibria'', Joint Varenna-Lausanne International Workshop. [[doi:10.1063/1.2404546\|AIP Conference Proceedings, 871, p. 136, 2006]]</ref>
			<ref>[[http://fusionsites.ciemat.es/picgklnf/]]</ref>.
	Afterwards, the code has been heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.		Afterwards, the code has been heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.

Admin at 09:43, 3 April 2018

2018-04-03T09:43:48Z

← Older revision		Revision as of 11:43, 3 April 2018
Line 1:		Line 1:
	The EUTERPE gyrokinetic code was created at the CRPP in Lausanne as a global linear particle in cell code for studying electrostatic plasma instabilities <ref>~~[http://www.ispp.it/Courses_and_Workshops.html~~ G. Jost, T. M. Tran, K. Appert, W. A. Cooper, and L. Villard, in Theory of Fusion Plasmas, International Workshop, Varenna, September 1998 (Editrice Compositori, Società Italiana di Fisica, Bologna, 1999), p. 419.]</ref>. It allows three-dimensional turbulence simulations using a plasma equilibrium calculated with the [[VMEC]] code as a starting point. EUTERPE was further developed at the Max Planck IPP and several linear calculations of ion temperature gradient (ITG) driven turbulence in [[Tokamak\|tokamak]] and [[Stellarator\|stellarator]] geometry have been carried out using it		The EUTERPE gyrokinetic code was created at the CRPP in Lausanne as a global linear particle in cell code for studying electrostatic plasma instabilities <ref>G. Jost, T. M. Tran, K. Appert, W. A. Cooper, and L. Villard, [http://www.ispp.it/Courses_and_Workshops.html in Theory of Fusion Plasmas, International Workshop, Varenna, September 1998 (Editrice Compositori, Società Italiana di Fisica, Bologna, 1999), p. 419.]</ref>. It allows three-dimensional turbulence simulations using a plasma equilibrium calculated with the [[VMEC]] code as a starting point. EUTERPE was further developed at the Max Planck IPP and several linear calculations of ion temperature gradient (ITG) driven turbulence in [[Tokamak\|tokamak]] and [[Stellarator\|stellarator]] geometry have been carried out using it
	<ref>~~[http://pop.aip.org/phpaen/v8/i7/p3321_s1~~ G. Jost, T. M. Tran, W. Cooper, and K. Appert. Phys. Plasmas '''8''': 3321 (2001)]</ref>		<ref>G. Jost, T. M. Tran, W. Cooper, and K. Appert. [[doi:10.1063/1.1374585\|Phys. Plasmas '''8''': 3321 (2001)]]</ref>
	<ref>~~[http://pop.aip.org/phpaen/v11/i6/p3196_s1~~ V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. Phys. Plasmas '''11''': 3196 (2004)]</ref>		<ref>V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. [[doi:10.1063/1.1737393\|Phys. Plasmas '''11''': 3196 (2004)]]</ref>
	<ref>[~~http~~:~~//iopscience.iop~~.~~org~~/0029-5515/45/4/003 ~~V. Kornilov, R. Kleiber, and R. Hatzky,~~ Nucl. Fusion '''45''': 238 (2005)]</ref>		<ref>V. Kornilov, R. Kleiber, and R. Hatzky, [[doi:10.1088/0029-5515/45/4/003\|Nucl. Fusion '''45''': 238 (2005)]]</ref>
	<ref>~~[http://link.aip.org/link/?APCPCS/871/136/1~~ R. Kleiber, ''Global linear gyrokinetic simulations for stellarator and axisymmetric equilibria'', Joint Varenna-Lausanne International Workshop. AIP Conference Proceedings, 871, p. 136, 2006]</ref>.		<ref>R. Kleiber, ''Global linear gyrokinetic simulations for stellarator and axisymmetric equilibria'', Joint Varenna-Lausanne International Workshop. [[doi:10.1063/1.2404546\|AIP Conference Proceedings, 871, p. 136, 2006]]</ref>.
	Afterwards, the code has been heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.		Afterwards, the code has been heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.

Line 30:		Line 30:
	An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program.		An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program.

	EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>~~[http://pop.aip.org/phpaen/v9/i3/p898_s1~~ Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. ~~PHYSICS OF PLASMAS~~, 9- 3,p. ~~912~~,2002.]</ref>.		EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. [[doi:10.1063/1.1449889\|Phys. Plasmas, 9- 3, p. 898, 2002.]]</ref>.

	==References==		==References==

Admin at 10:34, 15 August 2012

2012-08-15T10:34:24Z

← Older revision		Revision as of 12:34, 15 August 2012
Line 34:		Line 34:
	==References==		==References==
	<references />		<references />


			[[Category:Software]]

Admin at 06:40, 4 May 2010

2010-05-04T06:40:35Z

← Older revision		Revision as of 08:40, 4 May 2010
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	<ref>[http://pop.aip.org/phpaen/v8/i7/p3321_s1 G. Jost, T. M. Tran, W. Cooper, and K. Appert. Phys. Plasmas '''8''': 3321 (2001)]</ref>		<ref>[http://pop.aip.org/phpaen/v8/i7/p3321_s1 G. Jost, T. M. Tran, W. Cooper, and K. Appert. Phys. Plasmas '''8''': 3321 (2001)]</ref>
	<ref>[http://pop.aip.org/phpaen/v11/i6/p3196_s1 V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. Phys. Plasmas '''11''': 3196 (2004)]</ref>		<ref>[http://pop.aip.org/phpaen/v11/i6/p3196_s1 V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. Phys. Plasmas '''11''': 3196 (2004)]</ref>
	<ref>[http://iopscience.iop.org/0029-5515/45/4/003 V. Kornilov, R. Kleiber, and R. Hatzky, Nucl. Fusion '''45''': 238 (2005)]</ref><ref>[http://~~scitation~~.aip.org/~~getabs~~/~~servlet~~/~~GetabsServlet?prog=normal&id=APCPCS000871000001000136000001~~ R. Kleiber. Global linear gyrokinetic simulations for stellarator and		<ref>[http://iopscience.iop.org/0029-5515/45/4/003 V. Kornilov, R. Kleiber, and R. Hatzky, Nucl. Fusion '''45''': 238 (2005)]</ref>
	axisymmetric equilibria. Joint Varenna-Lausanne International Workshop.		<ref>[http://link.aip.org/link/?APCPCS/871/136/1 R. Kleiber, ''Global linear gyrokinetic simulations for stellarator and axisymmetric equilibria'', Joint Varenna-Lausanne International Workshop. AIP Conference Proceedings, 871, p. 136, 2006]</ref>.
	AIP Conference Proceedings, 871, p. 136, 2006]</ref>. Afterwards, the code has been heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.		Afterwards, the code has been heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.

	The EUTERPE code solves the gyroaveraged Vlasov equation for the distribution function of ions		The EUTERPE code solves the gyroaveraged Vlasov equation for the distribution function of ions

	<math>		:<math>
	\frac{\partial f}{\partial t} + \frac{\rm{d}v_{\|\|}}{\rm{d}t} \frac{\partial f}{\partial v_{\|\|}} + \frac{\rm{d}\vec{R}}{\rm{d}t} \frac{\partial f}{\partial \vec{R}} = 0		\frac{\partial f}{\partial t} + \frac{\rm{d}v_{\|\|}}{\rm{d}t} \frac{\partial f}{\partial v_{\|\|}} + \frac{\rm{d}\vec{R}}{\rm{d}t} \frac{\partial f}{\partial \vec{R}} = 0
	</math>		</math>
Line 14:		Line 14:
	The code is based on the particle-in-cell (PIC) scheme, where the distribution function is discretized using markers. The δf approximation is used, so that the distribution function is decomposed in an equilibrium part (Maxwellian) and a time-dependent perturbation.		The code is based on the particle-in-cell (PIC) scheme, where the distribution function is discretized using markers. The δf approximation is used, so that the distribution function is decomposed in an equilibrium part (Maxwellian) and a time-dependent perturbation.

	<math>		:<math>
	f(\vec R, v_{\|\|}, \mu, t) = f_{0}(\vec R, v_{\|\|}, v_{\perp})+ \delta f(\vec R, v_{\|\|}, \mu, t)		f(\vec R, v_{\|\|}, \mu, t) = f_{0}(\vec R, v_{\|\|}, v_{\perp})+ \delta f(\vec R, v_{\|\|}, \mu, t)
	</math>		</math>
Line 20:		Line 20:
	Each marker along with its weight is evolved following the particle trayectories and contributes a part to the distribution function, so that		Each marker along with its weight is evolved following the particle trayectories and contributes a part to the distribution function, so that

	<math>		:<math>
	\delta f = \sum_{p=1} ^{N} w_p \delta ^{3}(\vec R - \vec R_p)\delta(v_{\|\|} - v_{\|\|p})\delta(\mu - \mu_p) /(2 \pi B),		\delta f = \sum_{p=1} ^{N} w_p \delta ^{3}(\vec R - \vec R_p)\delta(v_{\|\|} - v_{\|\|p})\delta(\mu - \mu_p) /(2 \pi B),
	</math>		</math>

130.206.40.162 at 08:43, 3 May 2010

2010-05-03T08:43:13Z

← Older revision		Revision as of 10:43, 3 May 2010
Line 4:		Line 4:
	<ref>[http://iopscience.iop.org/0029-5515/45/4/003 V. Kornilov, R. Kleiber, and R. Hatzky, Nucl. Fusion '''45''': 238 (2005)]</ref><ref>[http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=APCPCS000871000001000136000001 R. Kleiber. Global linear gyrokinetic simulations for stellarator and		<ref>[http://iopscience.iop.org/0029-5515/45/4/003 V. Kornilov, R. Kleiber, and R. Hatzky, Nucl. Fusion '''45''': 238 (2005)]</ref><ref>[http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=APCPCS000871000001000136000001 R. Kleiber. Global linear gyrokinetic simulations for stellarator and
	axisymmetric equilibria. Joint Varenna-Lausanne International Workshop.		axisymmetric equilibria. Joint Varenna-Lausanne International Workshop.
	AIP Conference Proceedings, 871, p. 136, 2006]</ref>. Afterwards, the code has been heavily optimized and improved and non-linear dynamics have been included.		AIP Conference Proceedings, 871, p. 136, 2006]</ref>. Afterwards, the code has been heavily optimized and improved. The perturbation to the magnetic field, a third species (in adition to electrons and ions) and the non-linear dynamics have been included.

	The EUTERPE code solves the gyroaveraged Vlasov equation for the distribution function of ions		The EUTERPE code solves the gyroaveraged Vlasov equation for the distribution function of ions

Edi.sanchez at 10:34, 30 April 2010

2010-04-30T10:34:07Z

← Older revision		Revision as of 12:34, 30 April 2010
Line 28:		Line 28:
	The electric potential is represented on a spatial grid, the electric charge being carried by the markers. Two coordinate systems are used in the code: a system of magnetic coordinates (PEST) <math>(s, \theta,\phi )</math> is used for the electrostatic potential and cylindrical coordinates <math>(r, z,\phi )</math> are used for pushing the particles, where <math>s=\Psi / \Psi_0</math> is the normalized toroidal flux. The change between coordinate systems, which is facilitated by the existence of the common coordinate <math>(\phi)</math>, is done in a continuous way. The equation for the field is discretized using finite elements (B-splines) and the PETSc library is used for solving it. The integration of the motion is done using a fourth order Runge-Kutta scheme. In linear simulations a phase factor transformation can be used and the equations can be integrated using a predictor-corrector scheme.		The electric potential is represented on a spatial grid, the electric charge being carried by the markers. Two coordinate systems are used in the code: a system of magnetic coordinates (PEST) <math>(s, \theta,\phi )</math> is used for the electrostatic potential and cylindrical coordinates <math>(r, z,\phi )</math> are used for pushing the particles, where <math>s=\Psi / \Psi_0</math> is the normalized toroidal flux. The change between coordinate systems, which is facilitated by the existence of the common coordinate <math>(\phi)</math>, is done in a continuous way. The equation for the field is discretized using finite elements (B-splines) and the PETSc library is used for solving it. The integration of the motion is done using a fourth order Runge-Kutta scheme. In linear simulations a phase factor transformation can be used and the equations can be integrated using a predictor-corrector scheme.

	An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program. EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>[http://pop.aip.org/phpaen/v9/i3/p898_s1 Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. PHYSICS OF PLASMAS, 9- 3,p. 912,2002.]</ref>.		An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program.

			EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>[http://pop.aip.org/phpaen/v9/i3/p898_s1 Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. PHYSICS OF PLASMAS, 9- 3,p. 912,2002.]</ref>.

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

Edi.sanchez at 10:33, 30 April 2010

2010-04-30T10:33:29Z

← Older revision		Revision as of 12:33, 30 April 2010
Line 26:		Line 26:
	where the <math>w_p</math> are the weights (contribution to the distribution function) associated to each marker.		where the <math>w_p</math> are the weights (contribution to the distribution function) associated to each marker.

	The electric potential is represented on a spatial grid, the electric charge being carried by the markers. Two coordinate systems are used in the code: a system of magnetic coordinates (PEST) <math>(s, \theta,\phi )</math> is used for the electrostatic potential and cylindrical coordinates <math>(r, z,\phi )</math> are used for pushing the particles, where <math>s=\Psi / \Psi_0</math> is the normalized toroidal flux. The change between coordinate systems, which is facilitated by the existence of the common coordinate <math>(\phi)</math>, is done in a continuous way. The equation for the field is discretized using finite elements (B-splines) and the PETSc library is used for solving it. The integration of the motion is done using a fourth order Runge-Kutta scheme. In linear simulations a phase factor transformation can be used and the equations can be integrated using a predictor-corrector scheme~~. These options have not been used in this work~~.		The electric potential is represented on a spatial grid, the electric charge being carried by the markers. Two coordinate systems are used in the code: a system of magnetic coordinates (PEST) <math>(s, \theta,\phi )</math> is used for the electrostatic potential and cylindrical coordinates <math>(r, z,\phi )</math> are used for pushing the particles, where <math>s=\Psi / \Psi_0</math> is the normalized toroidal flux. The change between coordinate systems, which is facilitated by the existence of the common coordinate <math>(\phi)</math>, is done in a continuous way. The equation for the field is discretized using finite elements (B-splines) and the PETSc library is used for solving it. The integration of the motion is done using a fourth order Runge-Kutta scheme. In linear simulations a phase factor transformation can be used and the equations can be integrated using a predictor-corrector scheme.

	An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program. EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>[http://pop.aip.org/phpaen/v9/i3/p898_s1 Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. PHYSICS OF PLASMAS, 9- 3,p. 912,2002.]</ref>.		An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program. EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>[http://pop.aip.org/phpaen/v9/i3/p898_s1 Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. PHYSICS OF PLASMAS, 9- 3,p. 912,2002.]</ref>.

Edi.sanchez at 10:23, 30 April 2010

2010-04-30T10:23:50Z

← Older revision		Revision as of 12:23, 30 April 2010
Line 28:		Line 28:
	The electric potential is represented on a spatial grid, the electric charge being carried by the markers. Two coordinate systems are used in the code: a system of magnetic coordinates (PEST) <math>(s, \theta,\phi )</math> is used for the electrostatic potential and cylindrical coordinates <math>(r, z,\phi )</math> are used for pushing the particles, where <math>s=\Psi / \Psi_0</math> is the normalized toroidal flux. The change between coordinate systems, which is facilitated by the existence of the common coordinate <math>(\phi)</math>, is done in a continuous way. The equation for the field is discretized using finite elements (B-splines) and the PETSc library is used for solving it. The integration of the motion is done using a fourth order Runge-Kutta scheme. In linear simulations a phase factor transformation can be used and the equations can be integrated using a predictor-corrector scheme. These options have not been used in this work.		The electric potential is represented on a spatial grid, the electric charge being carried by the markers. Two coordinate systems are used in the code: a system of magnetic coordinates (PEST) <math>(s, \theta,\phi )</math> is used for the electrostatic potential and cylindrical coordinates <math>(r, z,\phi )</math> are used for pushing the particles, where <math>s=\Psi / \Psi_0</math> is the normalized toroidal flux. The change between coordinate systems, which is facilitated by the existence of the common coordinate <math>(\phi)</math>, is done in a continuous way. The equation for the field is discretized using finite elements (B-splines) and the PETSc library is used for solving it. The integration of the motion is done using a fourth order Runge-Kutta scheme. In linear simulations a phase factor transformation can be used and the equations can be integrated using a predictor-corrector scheme. These options have not been used in this work.

	An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program. EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>[http://pop.aip.org/phpaen/v9/i3/p898_s1 Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. PHYSICS OF PLASMAS, 9- 3,p. 912,2002.]</ref>. ~~More details about the code can be found in the Refs~\cite{EUTERPE:Jost,EUTERPE:Jost2,EUTERPE:Kornilov04,EUTERPE:Kornilov05,EUTERPE:Kleiber06}~~		An equilibrium state calculated with the code VMEC is used as a starting point. The equilibrium quantities computed by VMEC are mapped onto the spatial grid using an intermediate program. EUTERPE features several techniques for the noise control: the filtering of Fourier modes (square and diagonal filters can be used) and the optimized loading <ref>[http://pop.aip.org/phpaen/v9/i3/p898_s1 Hatzky, R Tran, TM Konies, A Kleiber, R Allfrey, SJ .Energy conservation in a nonlinear gyrokinetic particle-in-cell code for ion-temperature-gradient-driven modes in theta-pinch geometry. PHYSICS OF PLASMAS, 9- 3,p. 912,2002.]</ref>.

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

Edi.sanchez at 10:23, 30 April 2010

2010-04-30T10:23:27Z

← Older revision		Revision as of 12:23, 30 April 2010
Line 1:		Line 1:
	The EUTERPE gyrokinetic code was created at the ~~EPFL~~ in Lausanne as a global linear particle in cell code for studying electrostatic plasma instabilities <ref>[http://www.ispp.it/Courses_and_Workshops.html G. Jost, T. M. Tran, K. Appert, W. A. Cooper, and L. Villard, in Theory of Fusion Plasmas, International Workshop, Varenna, September 1998 (Editrice Compositori, Società Italiana di Fisica, Bologna, 1999), p. 419.]</ref>. It allows three-dimensional turbulence simulations using a plasma equilibrium calculated with the [[VMEC]] code as a starting point. EUTERPE was further developed at the Max Planck IPP and several linear calculations of ion temperature gradient (ITG) driven turbulence in [[Tokamak\|tokamak]] and [[Stellarator\|stellarator]] geometry have been carried out using it		The EUTERPE gyrokinetic code was created at the CRPP in Lausanne as a global linear particle in cell code for studying electrostatic plasma instabilities <ref>[http://www.ispp.it/Courses_and_Workshops.html G. Jost, T. M. Tran, K. Appert, W. A. Cooper, and L. Villard, in Theory of Fusion Plasmas, International Workshop, Varenna, September 1998 (Editrice Compositori, Società Italiana di Fisica, Bologna, 1999), p. 419.]</ref>. It allows three-dimensional turbulence simulations using a plasma equilibrium calculated with the [[VMEC]] code as a starting point. EUTERPE was further developed at the Max Planck IPP and several linear calculations of ion temperature gradient (ITG) driven turbulence in [[Tokamak\|tokamak]] and [[Stellarator\|stellarator]] geometry have been carried out using it
	<ref>[http://pop.aip.org/phpaen/v8/i7/p3321_s1 G. Jost, T. M. Tran, W. Cooper, and K. Appert. Phys. Plasmas '''8''': 3321 (2001)]</ref>		<ref>[http://pop.aip.org/phpaen/v8/i7/p3321_s1 G. Jost, T. M. Tran, W. Cooper, and K. Appert. Phys. Plasmas '''8''': 3321 (2001)]</ref>
	<ref>[http://pop.aip.org/phpaen/v11/i6/p3196_s1 V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. Phys. Plasmas '''11''': 3196 (2004)]</ref>		<ref>[http://pop.aip.org/phpaen/v11/i6/p3196_s1 V. Kornilov, R. Kleiber, R. Hatzky, L. Villard, and G. Jost. Phys. Plasmas '''11''': 3196 (2004)]</ref>