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Calibrated cylindrical Mach probe in a plasma wind tunnel
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10.1063/1.3559550
/content/aip/journal/rsi/82/3/10.1063/1.3559550
http://aip.metastore.ingenta.com/content/aip/journal/rsi/82/3/10.1063/1.3559550
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

Mach probe and magnetic probe setup inside the SSX plasma wind tunnel. The dimensions of the tunnel are . Device coordinates are as indicated with the θ-direction pointing into the page and the z along the magnetic probe. The r-direction is radially out from the axis. The plasma originates from the electrode and flows in the positive z-direction (from right to left in the figure).

Image of FIG. 2.
FIG. 2.

Close-up of Mach probe showing orientation of the electrode collector areas and device coordinates. Probes are numbered clock-wise beginning bottom-right (e.g., probes 3 and 6 form the θ pair).

Image of FIG. 3.
FIG. 3.

Typical current measurements for each of the six electrode collectors of the Mach probe with channels labeled. The currents from each probe face have been offset by 0.7 A for clarity.

Image of FIG. 4.
FIG. 4.

T e was determined using VUV spectroscopy and T i with the IDS. Note that T e remained below 15 eV for the duration of the discharge and that T i > T e early in time.

Image of FIG. 5.
FIG. 5.

Using Eq. (3), the sound speed is calculated as a function of time.

Image of FIG. 6.
FIG. 6.

|B| as a function of time for a single discharge. Measurements are displayed for probes 5, 8, and 12 of the linear array, 24.2, 38.6, and 58.0 cm from the first magnetic probe, respectively, beginning with the top trace. Squares indicate the time of detection the leading edge as the plasma approaches each probe. The magnetic field strengths have been offset for clarity.

Image of FIG. 7.
FIG. 7.

The initial plume velocity, , determined using a linear array of magnetic probes. Using the slope of a linear regression of the mean arrival times (squares) for each probe, v d = 55.1 ± 6.4 km/s for data aggregated over 40 discharges.

Image of FIG. 8.
FIG. 8.

Mach number in the (a) z-direction and (b) θ-direction for LH and RH shots aggregated over 20 discharges in each orientation. Peak initial M z flows are observed at approximately 32 μs. Note that very little azimuthal flow is observed in the initial plume.

Image of FIG. 9.
FIG. 9.

Absolute flow velocities in the (a) z-direction and (b) θ-direction. Data included for LH and RH shots aggregated over 20 discharges.

Image of FIG. 10.
FIG. 10.

Simulation plot of z-directed Mach number (using the expression (M 1 + M 2)/2cos 30°) versus the exact input Mach number (defined by v d /v th ). The error bars are smaller than the resolution of the graph. A linear least-squares fit to the data gives an implied calibration constant of K = 2.61 ± 0.01.

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/content/aip/journal/rsi/82/3/10.1063/1.3559550
2011-03-24
2014-04-20
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Calibrated cylindrical Mach probe in a plasma wind tunnel
http://aip.metastore.ingenta.com/content/aip/journal/rsi/82/3/10.1063/1.3559550
10.1063/1.3559550
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