Two‐dimensional magnetic field evolution measurements and plasma flow speed estimates from the coaxial thruster experiment

1994 ◽  
Vol 1 (9) ◽  
pp. 3115-3131 ◽  
Author(s):  
D. C. Black ◽  
R. M. Mayo ◽  
R. A. Gerwin ◽  
K. F. Schoenberg ◽  
J. T. Scheuer ◽  
...  
1998 ◽  
Vol 5 (3) ◽  
pp. 792-798 ◽  
Author(s):  
R. Shpitalnik ◽  
A. Weingarten ◽  
K. Gomberoff ◽  
Ya. Krasik ◽  
Y. Maron

Entropy ◽  
2018 ◽  
Vol 20 (10) ◽  
pp. 799 ◽  
Author(s):  
George Livadiotis

The paper derives the polytropic indices over the last two solar cycles (years 1995–2017) for the solar wind proton plasma near Earth (~1 AU). We use ~92-s datasets of proton plasma moments (speed, density, and temperature), measured from the Solar Wind Experiment instrument onboard Wind spacecraft, to estimate the moving averages of the polytropic index, as well as their weighted means and standard errors as a function of the solar wind speed and the year of measurements. The derived long-term behavior of the polytropic index agrees with the results of other previous methods. In particular, we find that the polytropic index remains quasi-constant with respect to the plasma flow speed, in agreement with earlier analyses of solar wind plasma. It is shown that most of the fluctuations of the polytropic index appear in the fast solar wind. The polytropic index remains quasi-constant, despite the frequent entropic variations. Therefore, on an annual basis, the polytropic index of the solar wind proton plasma near ~1 AU can be considered independent of the plasma flow speed. The estimated all-year weighted mean and its standard error is γ = 1.86 ± 0.09.


1987 ◽  
Vol 37 (3) ◽  
pp. 335-346
Author(s):  
Satoru Iizuka ◽  
Yasujiroh Minamitani ◽  
Hiroshi Tanaca

Plasma behaviour during magnetic field-line reconnection which is driven by a rapid toroidal current reversal in a tokamak is investigated by calculating plasma flow speed from the magnetohydromatic equations with variables measured in the experiment. A strong plasma acceleration appears in the outside region of the X-type separatrix formed in the poloidal magnetic field lines. The induced electric field inside the plasma is evaluated directly from Ohm's law by using the fact that the toroidal current density vanishes during the current reversal. Then, plasma resistivity is estimated in the cross-section and the resulting value of energy flow is compared with that given by Poynting's theorem. It is found that the input energy is dissipated effectively through anomalous resistivity in the reconnection region.


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