On Supplementary Heating of Fusion Plasmas By Means of Alfven Waves

Cover On Supplementary Heating of Fusion Plasmas By Means of Alfven Waves
On Supplementary Heating of Fusion Plasmas By Means of Alfven Waves
J a Tataronis
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From Figure 9 an indication can be obtained as to the position where the iraximum absorption for the Alfven waves occur . This is true since the power absorbed is directly proportional to 2 | (u) A (r) ) ' | at the resonance point as shown by eq. (104) .
From Figure 9 it can be seen that strong absorption should only occur at radial positions greater than at least 60% of the plasma radius. This will be shown to actually be the case as borne out by the numerical results. Figure 13 presents the r
...esults of the numerical computations of the real part of the coil impedance, Z, versus the frequency f. Both Z and f are given in dimensional form, ohms and cycles per second respec- tively. The first noticeable result is the fact that the cusp impedance values are very small, typically less than about 0. 02 ohms over the cusp frequency range. For this reason they are not shown plotted in the figure. The Alfve'n resistance however is plotted. The values for the, admittedly very ideal case, are -59- impressively large.

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