Abstract:In this paper, laboratory work dealing with the frequency characteristic of the plasma impedance of spherical and cylindrical electrode systems is reported. The influence of the ion sheath on various features of the impedance characteristic is considered as the main point of interest throughout this work. Those features are the series and parallel resonance as well as additional resonances due to the excitation of electroacoustic and cyclotron harmonic waves. The dependence of the series and parallel resonance… Show more
“…The three matrices in (15) are: the identity matrix I, the collision matrix T S , and the Vlasov matrix T V . e is the explicitly expanded excitation vector.…”
Section: Explicit Expansion Of the Inner Admittancementioning
confidence: 99%
“…k T 00 1 2 Since all matrices and the excitation vector in equation (15) are defined, the explicit expansion of the admittance can be calculated to compute different spectra of the sIP.…”
Section: Explicit Expansion Of the Inner Admittancementioning
confidence: 99%
“…In subsequent years, the RP was intensively investigated both experimentally and theoretically. Many researchers have attempted this task, especially the RP with a spherical electrode [4][5][6][7][8][9][10][11][12][13][14][15]. The theoretical works of the cited papers share a common feature in that the underlying models are based on an electrostatic approximation, but the plasma description is of a different complexity.…”
The impedance probe is a measurement device to measure plasma parameter like electron density.It consists of one electrode connected to a network analyzer via a coaxial cable and is immersed into a plasma. A bias potential superposed with an alternating potential is applied to the electrode and the response of the plasma is measured. Its dynamical interaction with the plasma in electrostatic, kinetic description can be modeled in an abstract notation based on functional analytic methods.These methods provide the opportunity to derive a general solution, which is given as the response function of the probe-plasma system. It is defined by the matrix elements of the resolvent of an appropriate dynamical operator. Based on the general solution a residual damping for vanishing pressure can be predicted and can only be explained by kinetic effects. Within this manuscript an explicit response function of the spherical impedance probe is derived. Therefore, the resolvent is determined by its algebraic representation based on an expansion in orthogonal basis functions. This allows to compute an approximated response function and its corresponding spectra. These spectra show additional damping due to kinetic effects and are in good agreement with former kinetically determined spectra.
“…The three matrices in (15) are: the identity matrix I, the collision matrix T S , and the Vlasov matrix T V . e is the explicitly expanded excitation vector.…”
Section: Explicit Expansion Of the Inner Admittancementioning
confidence: 99%
“…k T 00 1 2 Since all matrices and the excitation vector in equation (15) are defined, the explicit expansion of the admittance can be calculated to compute different spectra of the sIP.…”
Section: Explicit Expansion Of the Inner Admittancementioning
confidence: 99%
“…In subsequent years, the RP was intensively investigated both experimentally and theoretically. Many researchers have attempted this task, especially the RP with a spherical electrode [4][5][6][7][8][9][10][11][12][13][14][15]. The theoretical works of the cited papers share a common feature in that the underlying models are based on an electrostatic approximation, but the plasma description is of a different complexity.…”
The impedance probe is a measurement device to measure plasma parameter like electron density.It consists of one electrode connected to a network analyzer via a coaxial cable and is immersed into a plasma. A bias potential superposed with an alternating potential is applied to the electrode and the response of the plasma is measured. Its dynamical interaction with the plasma in electrostatic, kinetic description can be modeled in an abstract notation based on functional analytic methods.These methods provide the opportunity to derive a general solution, which is given as the response function of the probe-plasma system. It is defined by the matrix elements of the resolvent of an appropriate dynamical operator. Based on the general solution a residual damping for vanishing pressure can be predicted and can only be explained by kinetic effects. Within this manuscript an explicit response function of the spherical impedance probe is derived. Therefore, the resolvent is determined by its algebraic representation based on an expansion in orthogonal basis functions. This allows to compute an approximated response function and its corresponding spectra. These spectra show additional damping due to kinetic effects and are in good agreement with former kinetically determined spectra.
“…The consequences of this effect for current collection and impedance of an antenna in the ionosphere were discussed by Lafrarnboise et al [1975]. Positive floating potentials on an RF probe were observed in the laboratory by Kist [1977] at frequencies above the plasma frequency. Below plasma frequency, rectification dominated and the floating potential was driven more negative.…”
We present results generated using a computer code which has been developed to model an isotropic inhomogeneous Vlasov plasma surrounding a dc‐biased spherical or infinite cylindrical electrode to which a radio frequency potential is applied. The initial Maxwellian velocity distribution of the plasma is approximated by a multiple water bag distribution. The instantaneous response of the plasma to a sinusoidal potential applied to the electrode is calculated in the electrostatic approximation. Transient and nonlinear effects can be modeled in this way. Ions are usually treated as fixed, but some runs include ion dynamics with an ion/electron mass ratio of 16. Data produced by the code include the instantaneous particle flux and electric field at the electrode surface, from which the RF admittance is calculated. Results are presented for spheres in the frequency range 0.1 ωpe to 3 ωpe, RF amplitudes of 1–9 kT/el, and antenna radii of 1 and 10 λD. Here ωpe is the electron plasma frequency and λD is the Debye shielding distance. The code reproduces the admittance behavior expected near the antenna‐plasma series resonance. Some evidence for RF modification of the sheath is seen well above the frequency of the series resonance.
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