By L. Marton, C. Marton (Eds.)
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Extra info for Advances in Electronics and Electron Physics, Vol. 54
20. Selected flux tubes in the DIPD. Two rods supply current, which is returned principally along the outer cylindrical oval. The dark figure-eight tube is the separatrix that divides the flux into three regions or cells. Cells 1 and 2 are “parent” cells as they contain the sources (rods). Cell 3 is the “daughter” cell. Flux is transferred from the parent cells to the daughter cell during field line reconnection. The line along which cells 1 and 2 touch (the line of x points) is the separator for the system.
Figure 28 shows parameters at the neutral point, for example, electron density N ; , current densityj,, drift velocity V,,and resistivity q. As estimated by a Hall probe, N i is seen decreasing prior to IFTE and & is rising. The current density decreases at IFTE, while the resistivity abruptly rises. Similar behavior is seen in later data (Fig. 29), where temperatures (T,, T,), and radiation levels are presented as well as the preceding parameters. In these experiments, some parameters have changed quantitatively, but little qualitatively.
Smith (1977) points out that oscillatory solutions can exist. B. Numerical Approaches While analytic approaches are conceptually and sometimesquantitatively helpful, the numerical computer approach seems even more useful. Provided sufficient attention is paid to initial and boundary conditions, quite complex problems become soluble. , the propensity of plasmas to assume anomalous transport coefficients. Therefore, some comparison with experimental evidence is desirable. The reader is referred to the references listed in the following papers for earlier numerical work.