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1 - Nuclear Sciences and Applications - IAEA

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416 MAUELetal.<br />

Small tokamak plasmas illustrating high beta instabilities with m ~ 4 have<br />

also been made in the CDX device at Princeton Plasma Physics Laboratory. The<br />

plasma parameters of CDX are R = 0.59 m, a = 0.04 m, Bt = 0.4 T, 5 < qa < 10,<br />

~ 2 x 10 19 m- 3 , <strong>and</strong> EJ3p < 1 [3]. These plasmas are formed <strong>and</strong><br />

maintained solely by a low energy (~ 400 V), high current (~ 125 A) electron<br />

beam which provides substantial heating power to the plasma [4],<br />

2. High-/} <strong>and</strong> low-? instabilities in the HBT pulsed tokamak<br />

The HBT diagnostic set includes several arrays of internal <strong>and</strong> external<br />

magnetic probes, a CO2 interferometer, a 16-channel IR tomography array, a 10point<br />

Thomson scattering system, a tunable monochromator for visible line<br />

emission detection <strong>and</strong> several Rogowski coils to measure the plasma current<br />

<strong>and</strong> various external coil currents. The poloidal beta, f3p, the cylindrical safety<br />

factor (q* = 2Tta 2 Bt/fjQRIp), <strong>and</strong> the central safety factor (jqeff(P) =BtAr/RABo)<br />

are measured magnetically throughout the shot [1]. The average beta is<br />

determined from the equilibrium relationship <strong>and</strong> is presented here normalized to<br />

the Troyon-Sykes critical beta (fic = 3.5 x 10~ 8 IlaBt) [5,6], The value of <br />

determined from the equilibrium relationship for a circular cross-section plasma<br />

is found to be in close agreement with Thomson scattering profile measurements<br />

<strong>and</strong> free boundary equilibrium calculations described in Section 3.<br />

Figure 1 illustrates the evolution of an ohmically sustained discharge (<br />

~ 10 eV, ~ 1.5 x 10 14 cm~^) in which the plasma current is steadily<br />

increased as the toroidal field decays (Figs, la <strong>and</strong> lb). The plasma is observed<br />

to become unstable as q* approaches 2 <strong>and</strong> //Jc exceeds 1.0 (Figs, lc <strong>and</strong><br />

le). The instability is characterized by the rapid onset of toroidally nonaxisymmetric<br />

fluctuations of the internal magnetic field <strong>and</strong> a gross inward<br />

motion of the plasma column as measured by two multi-channel magnetic probes<br />

(Figs, li <strong>and</strong> Id). The two internal probes, toroidally separated by A

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