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Murakami density limit in tokamaks and reversed-field pinches

Journal Article · · Phys. Fluids; (United States)
DOI:https://doi.org/10.1063/1.864927· OSTI ID:5816772
A theoretical upper limit for the density in an Ohmically heated tokamak discharge follows from the requirement that the Ohmic heating power deposited in the current-carrying channel exceed the impurity radiative cooling in this critical region. A compact summary of our results gives this limit n/sub M/ for the central density as n/sub M/ = (Z/sub e/ / (Z/sub e/-1))/sup 1//sup ///sup 2/ n/sub e/0 (B/sub T/ /1T) (1m/R), where n/sub e/0 depends strongly on the impurity species and is remarkably independent of the central electron temperature T/sub e/(0). For T/sub e/(0) approx.1 keV, n/sub e/0 = 1.5 x 10/sup 14/ cm/sup -3/ for beryllium, n/sub e/0 = 5.5 x 10/sup 13/ cm/sup -3/ for oxygen, n/sub e/0 = 1.0 x 10/sup 13/ cm/sup -3/ for iron and, n/sub e/0 = 0.5 x 10/sup 13/ cm/sup -3/ for tungsten. The results agree quantitatively with Murakami's original observations. A similar density limit, known as the I/N limit, exists for reversed-field pinch devices and this limit has also been evaluated for a variety of impurity species.
Research Organization:
Plasma Physics Laboratory, Princeton University, Princeton, New Jersey 08544
DOE Contract Number:
AC02-76CH03073
OSTI ID:
5816772
Journal Information:
Phys. Fluids; (United States), Journal Name: Phys. Fluids; (United States) Vol. 28:6; ISSN PFLDA
Country of Publication:
United States
Language:
English