Magnetic confinement: Difference between revisions
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Charged particles can be confined in a volume by means of the [[:Wikipedia:Lorentz Force|Lorentz Force]]. | Charged particles can be confined in a spatial volume by means of the [[:Wikipedia:Lorentz Force|Lorentz Force]]. | ||
In order to minimize the interaction between the confined particles and the surrounding material structures, the required magnetic fields typically have a [[Flux surface|toroidal topology]] | In order to minimize the interaction between the confined particles and the surrounding material structures, the required magnetic fields typically have a [[Flux surface|toroidal topology]] | ||
(see [[MHD equilibrium]]). | (see [[MHD equilibrium]]). | ||
In order to achieve [[Nuclear fusion|fusion]], the parameters of the confined plasma must satisfy the [[:Wikipedia:Lawson criterion|Lawson criterion]]. | |||
== | == Toroidal magnetic confinement devices == | ||
* [[Tokamak]] | * [[Tokamak]]; [[Spheromak]] | ||
* [[Stellarator]] | * [[Stellarator]] | ||
* [[Reversed Field Pinch]] | * [[Reversed Field Pinch]] | ||
== See also == | |||
* [[:Wikipedia:Magnetic confinement fusion|Magnetic confinement fusion]] | |||
Latest revision as of 09:42, 26 October 2009
Charged particles can be confined in a spatial volume by means of the Lorentz Force. In order to minimize the interaction between the confined particles and the surrounding material structures, the required magnetic fields typically have a toroidal topology (see MHD equilibrium). In order to achieve fusion, the parameters of the confined plasma must satisfy the Lawson criterion.