Profile consistency: Difference between revisions

Jump to navigation Jump to search
no edit summary
No edit summary
No edit summary
Line 2: Line 2:
<ref>B. Coppi, ''Nonclassical Transport and the "Principle of Profile Consistency"'', Comments Plasma Phys. Cont. Fusion '''5''', 6 (1980) 261-270</ref>
<ref>B. Coppi, ''Nonclassical Transport and the "Principle of Profile Consistency"'', Comments Plasma Phys. Cont. Fusion '''5''', 6 (1980) 261-270</ref>
<ref>Yu.N. Dnestrovsky et al, Sov. J. Plasma Phys. '''16''' (1990) 120</ref>
<ref>Yu.N. Dnestrovsky et al, Sov. J. Plasma Phys. '''16''' (1990) 120</ref>
The resulting profiles are known as ''canonical'' profiles.
The resulting (stiff) profiles are known as ''canonical'' profiles.
<ref>[http://dx.doi.org/10.1134/1.1520282 Yu.N. Dnestrovsky et al, ''Canonical profiles in tokamak plasmas with an arbitrary cross section'', Plasma Physics Reports '''28''', 11 (2002) 887-899]</ref>
<ref>[http://dx.doi.org/10.1134/1.1520282 Yu.N. Dnestrovsky et al, ''Canonical profiles in tokamak plasmas with an arbitrary cross section'', Plasma Physics Reports '''28''', 11 (2002) 887-899]</ref>
This phenomenology is due to plasma [[Self-Organised Criticality|self-organisation]],
This phenomenology is due to plasma [[Self-Organised Criticality|self-organisation]],

Navigation menu