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Study of electromagnetic fluctuations in high beta plasma of a large linear device
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10.1063/1.3376302
/content/aip/journal/pop/17/4/10.1063/1.3376302
http://aip.metastore.ingenta.com/content/aip/journal/pop/17/4/10.1063/1.3376302
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

A schematic diagram of the experimental setup. Both the anode plate and the end plate have multicusped magnetic mirrors mounted on them and they are electrically grounded along with the vacuum vessel. The side view (looking from narrow source end) shows the poloidal ion and electron drift directions along with a cross-sectional view of electric and magnetic probes.

Image of FIG. 2.
FIG. 2.

(a) A typical probe characteristics of Langmuir probe obtained in the LVPD plasma at a location, , , and , (b) electron current after subtracting the ion current from the total probe current, and (c) the selected region of the bias voltage that gives straight line fit for determining electron temperature, .

Image of FIG. 3.
FIG. 3.

Three traces each of: (a) discharge currents, , (b) ion saturation currents, , and (c) floating potential, , when the LVPD is operated with the narrow source. The negative during turn off is an artifact of droop characteristics of the CT and it does not indicate any plasma feedback. The ion saturation current exhibits fluctuation for plasma density exceeding . The traces in (b) and (c) are obtained at the location , , and .

Image of FIG. 4.
FIG. 4.

The induced voltage, when pickup coil is rotated from to 360° with respect to the direction of . Here, represents the angle between the coil-normal and the magnetic field.

Image of FIG. 5.
FIG. 5.

(a) The ensemble average of 100 discharges (smooth) and a single discharge (with fluctuations) data for (a) ion saturation current and (b) the diamagnetic loop pickup voltage. (c) The magnetic field in presence of plasma was obtained from the ensemble-averaged signal of (b). All measurements were at .

Image of FIG. 6.
FIG. 6.

Evolution of plasma density profile during discharge pulse. The evolution is broadly divided into three parts, i.e., the formation, the steady state, and the decay phases. The steady state phase is attained during 6–9 ms in the discharge.

Image of FIG. 7.
FIG. 7.

Evolution of floating potential profile during the discharge. The profile shows absence of electric field in the core region during the steady state phase.

Image of FIG. 8.
FIG. 8.

Radial profiles of plasma parameters obtained at and during steady state. (a) Plasma electron density, , (b) electron temperature, , (c) plasma potential, , and (d) net magnetic field after diamagnetic expulsion when the LVPD is operated with the narrow source.(e)–(h) represents similar measurements for the broad source.

Image of FIG. 9.
FIG. 9.

Radial profiles of fluctuations measured at a location and . (a) Axial magnetic field, and (b) ion saturation current, . The data for the narrow source are represented by the bullets (with large error bars) and by the open circles when the LVPD is operated at 6 and 11 G, respectively. The data for the broad source (at 6 G) are represented by “” symbols. The dashed line in (a) represents capacitive noise of the pickup coils. A significant suppression of fluctuations is observed for the broad source.

Image of FIG. 10.
FIG. 10.

Normalized density and magnetic field fluctuations measured at a location, , , and for different applied axial magnetic field. Since plasma density and electron temperature do not change significantly, the -axis can be converted into plasma beta, .

Image of FIG. 11.
FIG. 11.

(a) Time series of simultaneously measured from the probe array and (b) cross-correlation functions between various Langmuir probe pairs (with increasing separation). The estimated poloidal phase velocity (between probe 1 and 5) , (c) cross power spectrum, and (d) coherency spectrum of fluctuations signifies the existence of low frequency mode.

Image of FIG. 12.
FIG. 12.

Radial profile of azimuthal phase velocity, , of fluctuation (bullets) and the drift velocity as determined from the fitted form of the measured plasma potential. The corrected azimuthal phase velocity, , is shown by cross symbol.

Image of FIG. 13.
FIG. 13.

(a) Power spectra for ion current fluctuation at a location , , and , (b) radial profile of electron temperature shows a gradient region in the core plasma, and (c) contour plot of autopower with frequency and radial distance. The spectral power is concentrated in the core region and exhibits broad peak.

Image of FIG. 14.
FIG. 14.

Contour plot of joint wave number-frequency spectrum, for (a) and . The spectrum also indicates that fluctuations in both propagate in electron diamagnetic drift direction.

Image of FIG. 15.
FIG. 15.

[(a), (b), (d), and (e)] Time series of different fluctuation data from the same plasma discharge, (c) cross-correlation function of and data, and (f) cross-correlation function of and data. The data presented here are for probe location, , , and .

Image of FIG. 16.
FIG. 16.

The axial variation in (a) fluctuations, three regions are demarcated as A, B, and C. They represent the cusp region, cathode region and the uniform plasma region, (b) fluctuations. Fluctuations are maximizing much away from the cusp region. Observation rules out the origin of instability near the mirrors or near the filaments.

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/content/aip/journal/pop/17/4/10.1063/1.3376302
2010-04-20
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Study of electromagnetic fluctuations in high beta plasma of a large linear device
http://aip.metastore.ingenta.com/content/aip/journal/pop/17/4/10.1063/1.3376302
10.1063/1.3376302
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