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where <math>B_T</math> is the toroidal magnetic field, <math>q_cyl</math> is the cylindrical safety factor, <math>P_{SOL}</math> is the power flowing into the SOL, and <math>R_{geo}</math> is the geometric major radius of the plasma. | where <math>B_T</math> is the toroidal magnetic field, <math>q_cyl</math> is the cylindrical safety factor, <math>P_{SOL}</math> is the power flowing into the SOL, and <math>R_{geo}</math> is the geometric major radius of the plasma. | ||
There have been other regression fits by different researchers using different subsets of devices and different parameters.<ref>[[doi:10.1016/j.jnucmat.2013.01.028|M.A. Makowski, et al., J. Nucl. Mater. '''438''' (2013) S208-S211]]</ref> | There have been other regression fits by different researchers using different subsets of devices and different parameters.<ref>[[doi:10.1016/j.jnucmat.2013.01.028|M.A. Makowski, et al., J. Nucl. Mater. '''438''' (2013) S208-S211]]</ref><ref>[[doi:10.1088/1741-4326/ab472c|H. Niemann et al 2020 Nucl. Fusion '''60''' (2020) 016014]]</ref> |
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