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1 - Nuclear Sciences and Applications - IAEA

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674 SIMONEN et al.<br />

MHD modes, observed in ISX-B [16] <strong>and</strong> Doublet III [17] at high 0P. As<br />

shown in Fig. 4, no sawteeth are present in the central soft X-ray emission.<br />

Edge localized modes (ELMs) similar to those observed at lower j3p are<br />

seen on the Ha emission in the divertor region, <strong>and</strong> on the soft X—ray<br />

signals near the edge of the discharge. Despite the large (3p, the moderately<br />

large ratio of toroidal beta to I/aB, <strong>and</strong> the large fast ion population, the<br />

only coherent MHD activity observed on the magnetic probes is associated<br />

with the ELMs. Except during the ELM events, the amplitude of poloidal<br />

magnetic field oscillations measured at the wall is at most 0.1% of the total<br />

poloidal field.<br />

Figure 5 shows EFIT magnetic analysis [18] of measurements from<br />

41 flux loops distributed around the outside <strong>and</strong> 25 magnetic probes distributed<br />

around the inside wall of the DIII-D vacuum vessel. Shownare<br />

the flux surface equilibrium, toroidal current density <strong>and</strong> q profiles at two<br />

times: (a) before beam injection <strong>and</strong> (b) in steady-state when /9p = 3.5.<br />

This analysis is based on a third-degree polynomial for j versus magnetic<br />

flux. The radial current profile exhibits (see Fig. 5b) a 0.2 m outward<br />

Shafranov shift <strong>and</strong> an extreme outward current peaking which, together<br />

with ej3p > 1, are indicators of possible second region stability.<br />

The issue of whether these plasmas entered the second stable regime<br />

revolves around the exact value of the axial safety factor qo. MHD equilibrium<br />

analysis of external magnetic measurements for these elongated<br />

plasmas can determine accurately the plasma shape, edge q (or q at the<br />

95% flux surface, qgs), the poloidal beta /?p, the plasma internal inductance<br />

ti [18], i<strong>and</strong> the magnetic axis shift. Information on q0 is only weakly<br />

1000<br />

-5.0 -2.5 0<br />

PRESSURE GRADIENT P^<br />

1 ST REGIME<br />

RADIUS<br />

NORMALIZED *<br />

PLASMA CENTER<br />

FIG. 6. A stability diagram for shot 57456 with q0 = 3 calculated with the CAMINO code. Here \<br />

is the radial flux coordinate, <strong>and</strong> p^, <strong>and</strong> q^ are the pressure <strong>and</strong> safety factor gradients relative to $<br />

The bold curve indicates that the plasma is at the entrance to the second stability region.

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