Shafranov shift - Revision history

Admin at 10:28, 26 January 2023

2023-01-26T10:28:38Z

← Older revision		Revision as of 12:28, 26 January 2023
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	The Shafranov shift<ref>V.D. Shafranov, Atomnaya Énergiya '''13''' (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated ''Equilibrium of a toroidal pinch in a magnetic field'', At. Energy '''13''', 6 (1963) 1149]</ref> is the outward radial displacement ''Δ(r)'' of the centre of [[Flux surface\|flux surfaces]] with [[Toroidal coordinates\|minor radius]] ''r'', induced by plasma pressure and the hoop force <ref>John Wesson, ''Tokamaks'', Clarendon Press (2004) ISBN 9780198509226</ref>.		The Shafranov shift<ref>V.D. Shafranov, Atomnaya Énergiya '''13''' (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated ''Equilibrium of a toroidal pinch in a magnetic field'', At. Energy '''13''', 6 (1963) 1149]</ref> is the outward radial displacement ''Δ(r)'' of the centre of [[Flux surface\|flux surfaces]] with [[Toroidal coordinates\|minor radius]] ''r'', induced by plasma pressure and the hoop force <ref>John Wesson, ''Tokamaks'', Clarendon Press (2004) {{ISBN\|9780198509226}}</ref>.
	Typically, the shift is linear <ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) ISBN 0521851076</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],		Typically, the shift is linear <ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) {{ISBN\|0521851076}}</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],
	due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.		due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.
	<ref>[http://dx.doi.org/10.1088/0741-3335/48/6/006 T. Kobuchi, K. Ida, H. Yamada, M. Yokoyama, K.Y. Watanabe, S. Sakakibara, M. Yoshinuma and the LHD Experimental Group, ''Magnetic configuration dependence of the shafranov shift in the Large Helical Device'', Plasma Phys. Control. Fusion '''48''' (2006) 789]</ref>		<ref>[http://dx.doi.org/10.1088/0741-3335/48/6/006 T. Kobuchi, K. Ida, H. Yamada, M. Yokoyama, K.Y. Watanabe, S. Sakakibara, M. Yoshinuma and the LHD Experimental Group, ''Magnetic configuration dependence of the shafranov shift in the Large Helical Device'', Plasma Phys. Control. Fusion '''48''' (2006) 789]</ref>

Meritt at 20:10, 15 March 2021

2021-03-15T20:10:31Z

← Older revision		Revision as of 22:10, 15 March 2021
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	The Shafranov shift<ref>V.D. Shafranov, Atomnaya Énergiya '''13''' (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated ''Equilibrium of a toroidal pinch in a magnetic field'', At. Energy '''13''', 6 (1963) 1149]</ref> is the outward radial displacement ''Δ(r)'' of the centre of [[Flux surface\|flux surfaces]] with [[Toroidal coordinates\|minor radius]] ''r'', induced by plasma pressure.		The Shafranov shift<ref>V.D. Shafranov, Atomnaya Énergiya '''13''' (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated ''Equilibrium of a toroidal pinch in a magnetic field'', At. Energy '''13''', 6 (1963) 1149]</ref> is the outward radial displacement ''Δ(r)'' of the centre of [[Flux surface\|flux surfaces]] with [[Toroidal coordinates\|minor radius]] ''r'', induced by plasma pressure and the hoop force <ref>John Wesson, ''Tokamaks'', Clarendon Press (2004) ISBN 9780198509226</ref>.
	Typically, the shift is linear <ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) ISBN 0521851076</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],		Typically, the shift is linear <ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) ISBN 0521851076</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],
	due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.		due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.

Admin at 06:41, 18 August 2010

2010-08-18T06:41:13Z

← Older revision		Revision as of 08:41, 18 August 2010
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	The Shafranov shift<ref>V.D. Shafranov, Atomnaya Énergiya '''13''' (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated ''Equilibrium of a toroidal pinch in a magnetic field'', At. Energy '''13''', 6 (1963) 1149]</ref> is the outward radial displacement ''Δ(r)'' of the centre of [[Flux surface\|flux surfaces]] with [[Toroidal coordinates\|minor radius]] ''r'', induced by plasma pressure.		The Shafranov shift<ref>V.D. Shafranov, Atomnaya Énergiya '''13''' (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated ''Equilibrium of a toroidal pinch in a magnetic field'', At. Energy '''13''', 6 (1963) 1149]</ref> is the outward radial displacement ''Δ(r)'' of the centre of [[Flux surface\|flux surfaces]] with [[Toroidal coordinates\|minor radius]] ''r'', induced by plasma pressure.
	Typically, the shift is linear <ref>K. ~~Miyamoto~~, ''Plasma ~~Physics~~ and ~~Controlled Nuclear Fusion~~'', ~~Springer-Verlag~~ (~~2005~~) ISBN ~~3540242171~~</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],		Typically, the shift is linear <ref>J.P. Freidberg, ''Plasma physics and fusion energy'', Cambridge University Press (2007) ISBN 0521851076</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],
	due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.		due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.
	<ref>[http://dx.doi.org/10.1088/0741-3335/48/6/006 T. Kobuchi, K. Ida, H. Yamada, M. Yokoyama, K.Y. Watanabe, S. Sakakibara, M. Yoshinuma and the LHD Experimental Group, ''Magnetic configuration dependence of the shafranov shift in the Large Helical Device'', Plasma Phys. Control. Fusion '''48''' (2006) 789]</ref>		<ref>[http://dx.doi.org/10.1088/0741-3335/48/6/006 T. Kobuchi, K. Ida, H. Yamada, M. Yokoyama, K.Y. Watanabe, S. Sakakibara, M. Yoshinuma and the LHD Experimental Group, ''Magnetic configuration dependence of the shafranov shift in the Large Helical Device'', Plasma Phys. Control. Fusion '''48''' (2006) 789]</ref>

Admin at 11:38, 17 August 2010

2010-08-17T11:38:51Z

← Older revision		Revision as of 13:38, 17 August 2010
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	The Shafranov shift<ref>V.D. Shafranov, Atomnaya Énergiya '''13''' (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated ''Equilibrium of a toroidal pinch in a magnetic field'', At. Energy '''13''', 6 (1963) 1149]</ref> is the outward radial displacement ''Δ(r)'' of the centre of flux surfaces with minor radius ''r'', induced by plasma pressure.		The Shafranov shift<ref>V.D. Shafranov, Atomnaya Énergiya '''13''' (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated ''Equilibrium of a toroidal pinch in a magnetic field'', At. Energy '''13''', 6 (1963) 1149]</ref> is the outward radial displacement ''Δ(r)'' of the centre of [[Flux surface\|flux surfaces]] with [[Toroidal coordinates\|minor radius]] ''r'', induced by plasma pressure.
	Typically, the shift is linear <ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],		Typically, the shift is linear <ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],
	due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.		due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.

Admin at 11:36, 17 August 2010

2010-08-17T11:36:46Z

← Older revision		Revision as of 13:36, 17 August 2010
Line 1:		Line 1:
	The Shafranov shift<ref>V.D. Shafranov, At. Energy '''13''' (~~1962~~) ~~521~~</ref> is the outward radial displacement ''Δ(r)'' of the centre of flux surfaces with minor radius ''r'', induced by plasma pressure.		The Shafranov shift<ref>V.D. Shafranov, Atomnaya Énergiya '''13''' (1962) 521, [http://dx.doi.org/10.1007/BF01312317 Translated ''Equilibrium of a toroidal pinch in a magnetic field'', At. Energy '''13''', 6 (1963) 1149]</ref> is the outward radial displacement ''Δ(r)'' of the centre of flux surfaces with minor radius ''r'', induced by plasma pressure.
	Typically, the shift is linear <ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],		Typically, the shift is linear <ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],
	due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.		due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.

Admin at 10:49, 17 August 2010

2010-08-17T10:49:15Z

← Older revision		Revision as of 12:49, 17 August 2010
Line 1:		Line 1:
	The Shafranov shift<ref>V.D. Shafranov, At. Energy '''13''' (1962) 521</ref> is the radial displacement ''Δ(r)'' of the centre of flux surfaces with minor radius ''r'', induced by plasma pressure.		The Shafranov shift<ref>V.D. Shafranov, At. Energy '''13''' (1962) 521</ref> is the outward radial displacement ''Δ(r)'' of the centre of flux surfaces with minor radius ''r'', induced by plasma pressure.
	Typically, the shift is linear <ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],		Typically, the shift is linear <ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref> in [[Beta\|beta (β)]], and it tends to be more important for [[Tokamak\|tokamaks]] than [[Stellarator\|stellarators]],
	due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.		due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.

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The Shafranov shift<ref>V.D. Shafranov, At. Energy '''13''' (1962) 521</ref> is the radial displacement ''Δ(r)'' of the centre of flux surfaces with minor radius ''r'', induced by plasma pressure.
Typically, the shift is linear <ref>K. Miyamoto, ''Plasma Physics and Controlled Nuclear Fusion'', Springer-Verlag (2005) ISBN 3540242171</ref> in [[Beta|beta (β)]], and it tends to be more important for [[Tokamak|tokamaks]] than [[Stellarator|stellarators]],
due to the fact that the magnetic configuration is largely or partly imposed externally in the latter case.
<ref>[http://dx.doi.org/10.1088/0741-3335/48/6/006 T. Kobuchi, K. Ida, H. Yamada, M. Yokoyama, K.Y. Watanabe, S. Sakakibara, M. Yoshinuma and the LHD Experimental Group, ''Magnetic configuration dependence of the shafranov shift in the Large Helical Device'', Plasma Phys. Control. Fusion '''48''' (2006) 789]</ref>

== References ==
<references />