| Autor: |
Lazarus, E.A., Navratil, G.A., Greenfield, C.M., Strait, E.J., Austin, M.E., Burrell, K.H., Casper, T.A., Baker, D.R., DeBoo, J.C., Doyle, E.J., Durst, R.D., Ferron, J.R., Forest, C.B., Gohil, P., Groebner, R.J., Heidbrink, W.W., Hong, R., Howald, A.W., Hsieh, C.-L., Hyatt, A.W., Jackson, G.L., Kim, J., Lao, L.L., Lanier, C.J., Leonard, A.W., Lohr, J.M., Haye, R.J. La, Maingi, R., Miller, R.L., Murakami, M., Osborne, T.H., Perkins, L.J., Petty, C.C., Rettig, C.L., Rhodes, T.L., Rice, B.W., Sabbagh, S.A., Schissel, D.P., Scovill, J.T. |
| Zdroj: |
Nuclear Fusion; January 1, 1997, Vol. 37 Issue: 1 p7-12, 6p |
| Abstrakt: |
Strong shaping, favourable for stability and improved energy confinement, together with a significant expansion of the central region of improved confinement in negative central magnetic shear target plasmas, increased the maximum fusion power produced in DIII-D by a factor of 3. Using deuterium plasmas, the highest fusion power gain, the ratio of fusion power to input power, Q, was 0.0015, corresponding to an equivalent Q of 0.32 in a deuterium-tritium plasma, which is similar to values achieved in tokamaks of larger size and magnetic field. A simple transformation relating Q to the stability parameters is presented |
| Databáze: |
Supplemental Index |
| Externí odkaz: |
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