Within the standard neoclassical theory, we show that, assuming that the mechanical power required to drive the ordered poloidal rotation against the viscous forces is a fraction of the total absorbed power, the poloidal spin up in the L to H transition is predicted as a bifurcation of solutions of the momentum equation.

Neoclassical poloidal flow bifurcation in the H mode transition

E Lazzaro;
1992

Abstract

Within the standard neoclassical theory, we show that, assuming that the mechanical power required to drive the ordered poloidal rotation against the viscous forces is a fraction of the total absorbed power, the poloidal spin up in the L to H transition is predicted as a bifurcation of solutions of the momentum equation.
1992
Istituto di fisica del plasma - IFP - Sede Milano
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/233632
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