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Anomalous transport: Difference between revisions
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<ref name="Freidberg" /> | <ref name="Freidberg" /> | ||
the cited [[Scaling law|scaling laws]] can be rewritten in terms of the temperature dependence (eliminating the heating power dependence). | the cited [[Scaling law|scaling laws]] can be rewritten in terms of the temperature dependence (eliminating the heating power dependence). | ||
Then, classical and neoclassical estimates would predict that the confinement increases with ''T'' (namely: ''τ<sub>E</sub>'' ∝ ''T<sup>0.5</sup>'', associated with collisionality). | Then, classical and neoclassical estimates would predict that the confinement increases with ''T'' (namely: ''τ<sub>E</sub>'' ∝ ''T<sup>0.5</sup>'', associated with [[Collisionality|collisionality]]). | ||
However, the experimental scalings give a ''decrease'' with ''T'' | However, the experimental scalings give a ''decrease'' with ''T'' | ||
(namely: ''τ<sub>E</sub>'' ∝ ''T<sup>α</sup>'' with '' α'' < -1). | (namely: ''τ<sub>E</sub>'' ∝ ''T<sup>α</sup>'' with '' α'' < -1). | ||