J. Vaclavik
École Polytechnique
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Featured researches published by J. Vaclavik.
Physics of Fluids | 1984
K. Appert; J. Vaclavik; L. Villard
Reference CRPP-ARTICLE-1983-008View record in Web of Science Record created on 2008-04-16, modified on 2017-05-12
Physics of Fluids | 1977
K. Appert; J. Vaclavik
Keywords: LRP 125 Reference CRPP-REPORT-1977-001 Record created on 2008-04-18, modified on 2017-05-12
Physics of Fluids | 1981
R. W. Means; L. Muschietti; M. Q. Tran; J. Vaclavik
The problem of the linear conversion of a Langmuir wave to a transverse electromagnetic wave in the presence of a density gradient has been solved numerically with appropriate boundary conditions. A reciprocity principle was found, allowing the deduction of solutions of this problem from those obtained from the transverse‐Langmuir conversion. This model has been applied to study the spectrum emitted from an inhomogeneous plasma, including the effect of the antenna radiation pattern. Experiments have been performed in a large unmagnetized dc discharge plasma (ne∼5×1010 cm−3, Te = 1.3 eV, gradient scale length L = 100−1000 cm). The shape of the spectrum observed with a horn antenna agrees with the theoretical one, but the deduced level of Langmuir fluctuations is much higher than the thermal level. This enhancement is due to the presence of primary energetic (E = 60 eV) electrons.
Physics of Fluids | 1981
L. Muschietti; K. Appert; J. Vaclavik
The interplay between the Cerenkov and anomalous Doppler interactions in the relaxation of a warm electron beam is investigated by numerical means. The most important feature in the interplay is found to be a nonelastic isotropization. A simple semianalytical model which allows one to estimate various quantities relevant to the relaxation process is also presented.
Physics of Fluids | 1982
L. Muschietti; K. Appert; J. Vaclavik
The evolution of the turbulence driven by runaway electrons has been followed by means of a computer code based on the quasilinear equations. The evolution is not characterized by periodic relaxations as claimed in previous works but ends in a quasisteady turbulent, yet very persistent state, accessible from different initial conditions. This discrepancy is clarified as being due to the excessive stiffness of the moment equations used to demonstrate the relaxations. Moreover, a theory is developed to interpret the quasisteady state found.
Physics of Fluids | 1980
J. Vaclavik; K. Appert
Reference CRPP-ARTICLE-1980-002doi:10.1063/1.863204View record in Web of Science Record created on 2008-04-16, modified on 2017-05-12
Physics of Fluids | 1986
J. Vaclavik; M.L. Sawley; F. Anderegg
The ponderomotive force acting on a magnetized plasma resulting from a radio‐frequency (rf) electric field is studied both theoretically and experimentally. The fundamental difference between the predictions of the single‐particle and fluid approaches is emphasized and its origin elucidated. An experiment is described that illustrates the collective interaction of a fluid with an rf field. This collective behavior manifests itself in the perpendicular ponderomotive force by the interaction of the rf‐induced magnetization current with the magnetic field.
Physics of Fluids | 1981
E. S. Weibel; J. Vaclavik
The system of quasi‐linear equations is derived without making use of the random phase approximation. The fluctuation quantities are described by the autocorrelation function of the electric field using the techniques of Fourier analysis. The resulting equations possess the necessary conservation properties, but comprise new terms which hitherto have been lost in the conventional derivations.
Physics of Fluids | 1983
F. Yasseen; J. Vaclavik
Reference CRPP-ARTICLE-1983-030View record in Web of Science Record created on 2008-04-16, modified on 2017-05-12
Physics of Fluids | 1979
K. Appert; J. Vaclavik
Saturation of the current‐driven ion‐acoustic instability in a weakly ionized plasma is investigated within the context of a quasi‐linear model that includes the effects of collisions. The turbulent wave energy is calculated under the assumption that the waves are excited within the cone of a small angle. The results obtained compare favorably with the recent experimental observations of Ilic.