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Observation of a nonaxisymmetric magnetohydrodynamic self-organized statea)
a)Paper XI3 6, Bull. Am. Phys. Soc. 54, 345 (2009).
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10.1063/1.3327214
/content/aip/journal/pop/17/5/10.1063/1.3327214
http://aip.metastore.ingenta.com/content/aip/journal/pop/17/5/10.1063/1.3327214
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Sketch of the SSX device. Numbers indicate the following: (1) the cylindrical conducting boundary with ; (2) one of 12 linear magnetic probe arrays inserted radially into the device; and for one of the two plasma guns on each end of the device, the (3) inner and (4) outer coaxial electrodes linked by (5) magnetic flux from (6) an external coil (the ignitron switched capacitor banks are also indicated schematically). Each magnetic probe array makes eight measurements with radial spacing of 2.5 cm. The full set of twelve probes determines three right circular cross sections of the cylindrical plasma volume at , , and , each with four probes equally spaced azimuthally (i.e., at , 135°, 225°, and 315°), in addition to two planes of data. Only one plane of data is shown in this figure since at this early time (, where initiation of the discharge defines ) the two right-handed spheromaks have not interacted much and are largely axisymmetric.

Image of FIG. 2.
FIG. 2.

The measured magnetic structure of the relaxed state at , following the completion of the cohelicity merging process. The mostly axisymmetric initial state containing two spheromaks is shown in Fig. 1. Both planes of data are shown since this state is inherently nonaxisymmetric.

Image of FIG. 3.
FIG. 3.

Time dependence of average , electron density , and carbon (impurity) ion temperature . Once the relaxed state forms the plasma has symmetry and self-similarly decays with about a -folding time in and .

Image of FIG. 4.
FIG. 4.

Measured magnetic structure for single plasma gun discharge. The initial spheromak state (a) is mostly axisymmetric, but the final state (b) is the same (except for an arbitrary global azimuthal rotation) as the nonaxisymmetric relaxed state seen in Fig. 2 for cohelicity merging.

Image of FIG. 5.
FIG. 5.

(a) The determinant of Eq. (4) evaluated for and . (b) dependence of the values of for and solutions. The minimum energy state (smallest ) is axisymmetric for and nonaxisymmetric for ). (c) The normalized axial wavenumber spectrum for the coefficients in the numerical solution [Eq. (3)] for show a narrowing peak around the value with increasing , indicating that the helical structure approaches that of the Taylor double helix solution. The peak value of each spectrum is normalized to one.

Image of FIG. 6.
FIG. 6.

isosurfaces for the Taylor state (top) and two orthogonal views (middle and bottom) of a field line to illustrate the helical character of the structure and the simplified description of the structure as a twisted closed loop of flux. The dotted line is the cylindrical axis; the perpendicular line segments on the end walls (circles) indicate the rotation between the two views of the field lines.

Image of FIG. 7.
FIG. 7.

(a) isosurfaces for the Taylor state and two orthogonal views of a field line to illustrate the helical character of the structure. (b) Field lines drawn through the final state of an MHD simulation using the HiFi (Refs. 23) code initialized with the Bessel function double-spheromak state. The final state is consistent with the Taylor state structure. The cylindrical boundary is not shown in (b) but is in roughly the same horizontal orientation as the figures in (a).

Image of FIG. 8.
FIG. 8.

Measurements of for the cohelicity merging experiment [(a) and (c)] and for the single plasma gun discharge (single spheromak) experiment [(b) and (d)]. The radial profiles of [(a) and (b)] are consistent with the Taylor state value (lower dotted line at ); the next larger value giving an state (see Fig. 5) is indicated by the upper dotted line. The radial average of (excluding the two values at smallest ) stays very near the Taylor state value throughout the decay of the nonaxisymmetric self-organized state [(c) and (d)]. Figure adapted from Ref. 12.

Image of FIG. 9.
FIG. 9.

Contour plots of , , and determined experimentally (corresponding to the data of Fig. 2). Isosurfaces are separated by 150 G. Red/yellow colors (solid lines) are positive values; blue/green (dotted lines) are negative values. Figure adapted from Ref. 12.

Image of FIG. 10.
FIG. 10.

Contour plots of , , and for the calculated Taylor state with . The only free parameter is the total helicity, which was adjusted to give best agreement with the experimental results. Isosurfaces are separated by 150 G. Red/yellow colors (solid lines) are positive values; blue/green (dotted lines) are negative values. Figure adapted from Ref. 12.

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2010-03-30
2014-04-23
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Observation of a nonaxisymmetric magnetohydrodynamic self-organized statea)
http://aip.metastore.ingenta.com/content/aip/journal/pop/17/5/10.1063/1.3327214
10.1063/1.3327214
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