Journal articles: 'Electrostatic turbulence'

1

Garbet, X., L. Laurent, and A. Samain. "Nonlinear electrostatic turbulence." Physics of Plasmas 1, no. 4 (April 1994): 850–62. http://dx.doi.org/10.1063/1.870744.

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2

Connor, J. W. "Tokamak turbulence-electrostatic or magnetic?" Plasma Physics and Controlled Fusion 35, SB (December 1, 1993): B293—B305. http://dx.doi.org/10.1088/0741-3335/35/sb/024.

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3

Riccardi, C., D. Caspani, L. Gamberale, G. Chiodini, and M. Fontanesi. "Turbulence Generated by Electrostatic Fluctuations." Physica Scripta T75, no. 1 (1998): 232. http://dx.doi.org/10.1238/physica.topical.075a00232.

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4

Chen, Deng Feng, Xiao Dong Yang, and Hai Yan Xiao. "Numerical Simulation of Particle Trajectory in Electrostatic Precipitator." Applied Mechanics and Materials 568-570 (June 2014): 1743–48. http://dx.doi.org/10.4028/www.scientific.net/amm.568-570.1743.

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The performance of Electrostatic Precipitator (ESP) is significantly affected by complex flow distribution. Recent years, many numerical models have been developed to model the particle motion in the electrostatic precipitators. The computational fluid dynamics (CFD) code FLUENT is used in description of the turbulent gas flow and the particle motion under electrostatic forces. The gas flow are carried out by solving the Reynolds-averaged Navier-Stokes equations and turbulence is modeled by the k-ε turbulence model. The effect of electric field is described by a series equations, such as the electric field and charge transport equations, the charged particle equation, the charge conservation equation, the mass and momentum equations of gas, the mass and momentum equations of particle and so on. The particle phase is simulated by using Discrete Phase Model (DPM). The simulations showed that the particle trajectory inside the ESP is influenced by both the aerodynamic and electrostatic forces. The simulated results have been validated by the established data.

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5

HELLER, M. V. A. P., I. L. CALDAS, A. A. FERREIRA, E. A. O. SAETTONE, and A. VANNUCCI. "Tokamak turbulence at the scrape-off layer in TCABR with an ergodic magnetic limiter." Journal of Plasma Physics 73, no. 3 (June 2007): 295–306. http://dx.doi.org/10.1017/s0022377806004569.

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AbstractThe influence of an ergodic magnetic limiter (EML) on plasma turbulence is investigated in the Tokamak Chauffage Alfvén Brésilien (TCABR), a tokamak with a peculiar natural superposition of the electrostatic and magnetic fluctuation power spectra. Experimental results show that the EML perturbation can reduce both the magnetic oscillation and the electrostatic plasma turbulence. Whenever this occurs, the turbulence-driven particle transport is also reduced. Moreover, a bispectral analysis shows that the nonlinear coupling between low- and high-frequency electrostatic fluctuations increases significantly with the EML application.

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6

Hamed, M., M. J. Pueschel, J. Citrin, M. Muraglia, X. Garbet, and Y. Camenen. "On the impact of electric field fluctuations on microtearing turbulence." Physics of Plasmas 30, no. 4 (April 2023): 042303. http://dx.doi.org/10.1063/5.0104879.

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The magnetic drift and the electric potential play an important role in microtearing destabilization by increasing the growth rate of this instability in the presence of collisions, while in electrostatic plasma micro-turbulence, zonal electric potentials can have a strong impact on turbulent saturation. A reduced model has been developed, showing that the Rechester–Rosenbluth model is a good model for the prediction of electron heat diffusivity by microtearing turbulence. Here, nonlinear gyrokinetic flux-tube simulations are performed in order to compute the characteristics of microtearing turbulence and the associated heat fluxes in tokamak plasmas and to assess how zonal flows and zonal fields affect saturation. This is consistent with a change in saturation mechanism from temperature corrugations to zonal field- and zonal flow-based energy transfer. It is found that removing the electrostatic potential causes a flux increase, while linearly stabilization is observed.

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7

Zakharov, V. E., and C. V. Meister. "Transport of thermal plasma above the auroral ionosphere in the presence of electrostatic ion-cyclotron turbulence." Annales Geophysicae 17, no. 1 (January 31, 1999): 27–36. http://dx.doi.org/10.1007/s00585-999-0027-3.

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Abstract. The electron component of intensive electric currents flowing along the geomagnetic field lines excites turbulence in the thermal magnetospheric plasma. The protons are then scattered by the excited electromagnetic waves, and as a result the plasma is stable. As the electron and ion temperatures of the background plasma are approximately equal each other, here electrostatic ion-cyclotron (EIC) turbulence is considered. In the nonisothermal plasma the ion-acoustic turbulence may occur additionally. The anomalous resistivity of the plasma causes large-scale differences of the electrostatic potential along the magnetic field lines. The presence of these differences provides heating and acceleration of the thermal and energetic auroral plasma. The investigation of the energy and momentum balance of the plasma and waves in the turbulent region is performed numerically, taking the magnetospheric convection and thermal conductivity of the plasma into account. As shown for the quasi-steady state, EIC turbulence may provide differences of the electric potential of ΔV≈1–10 kV at altitudes of 500 < h < 10 000 km above the Earth's surface. In the turbulent region, the temperatures of the electrons and protons increase only a few times in comparison with the background values.Key words. Magnetospheric physics (electric fields; plasma waves and instabilities)

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8

Tucker, P. G. "Computation of Particle and Scalar Transport for Complex Geometry Turbulent Flows." Journal of Fluids Engineering 123, no. 2 (February 6, 2001): 372–81. http://dx.doi.org/10.1115/1.1365959.

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The prediction of particle and scalar transport in a complex geometry with turbulent flow driven by fans is considered. The effects of using different turbulence models, anisotropy, flow unsteadiness, fan swirl, and electrostatic forces on particle trajectories are shown. The turbulence models explored include k−l, zonal k−ε/k−l, and nonlinear eddy viscosity models. Particle transport is predicted using a stochastic technique. A simple algorithm to compute electrostatic image forces acting on particles, in complex geometries, is presented. Validation cases for the particle transport and fluid flow model are shown. Comparison is made with new smoke flow visualization data and particle deposition data. Turbulence anisotropy, fan swirl, and flow unsteadiness are shown to significantly affect particle paths as does the choice of isotropic turbulence model. For lighter particles, electrostatic forces are found to have less effect. Results suggest, centrifugal forces, arising from regions of strong streamline curvature, play a key particle deposition role. They also indicate that weaknesses in conventional eddy viscosity based turbulence models make the accurate prediction of complex geometry particle deposition a difficult task. Axial fans are found in many fluid systems. The sensitivity of results to their modeling suggests caution should be used when making predictions involving fans and that more numerical characterization studies for them could be carried out (especially when considering particle deposition). Overall, the work suggests that, for many complex-engineering systems, at best (without excessive model calibration time), only qualitative particle deposition information can be gained from numerical predictions.

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9

Angelis, U. de, A. Forlani, A. Litvak, V. N. Tsytovich, R. Bingham, and P. K. Shukla. "Particle acceleration by weak electrostatic turbulence." Physica Scripta T50 (January 1, 1994): 90–97. http://dx.doi.org/10.1088/0031-8949/1994/t50/015.

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10

Neto, C. Rodrigues, Z. O. Guimarães-Filho, I. L. Caldas, I. C. Nascimento, and Yu K. Kuznetsov. "Multifractality in plasma edge electrostatic turbulence." Physics of Plasmas 15, no. 8 (August 2008): 082311. http://dx.doi.org/10.1063/1.2973175.

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11

Basu, Ronni, Thomas Jessen, Volker Naulin, and Jens Juul Rasmussen. "Turbulent flux and the diffusion of passive tracers in electrostatic turbulence." Physics of Plasmas 10, no. 7 (July 2003): 2696–703. http://dx.doi.org/10.1063/1.1578075.

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12

Vasquez, Alberto M., and Daniel O. Gomez. "Electrostatic Decay of Beam‐generated Plasma Turbulence." Astrophysical Journal 607, no. 2 (June 2004): 1024–31. http://dx.doi.org/10.1086/381934.

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13

Terry, R. E. "Electrostatic turbulence in the Z pinch corona." Physics of Plasmas 1, no. 7 (July 1994): 2189–99. http://dx.doi.org/10.1063/1.870618.

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14

Balescu, R., I. Petrisor, and M. Negrea. "Anisotropic electrostatic turbulence and zonal flow generation." Plasma Physics and Controlled Fusion 47, no. 12 (November 1, 2005): 2145–59. http://dx.doi.org/10.1088/0741-3335/47/12/005.

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15

Waelbroeck, F. L., F. Militello, R. Fitzpatrick, and W. Horton. "Effect of electrostatic turbulence on magnetic islands." Plasma Physics and Controlled Fusion 51, no. 1 (December 11, 2008): 015015. http://dx.doi.org/10.1088/0741-3335/51/1/015015.

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16

Shaikh, Dastgeer. "Coherent structures in electrostatic interchange mode turbulence." Physica Scripta 74, no. 6 (November 9, 2006): 646–52. http://dx.doi.org/10.1088/0031-8949/74/6/008.

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17

Numata, Ryusuke, Rowena Ball, and Robert L. Dewar. "Bifurcation in electrostatic resistive drift wave turbulence." Physics of Plasmas 14, no. 10 (October 2007): 102312. http://dx.doi.org/10.1063/1.2796106.

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18

Huld, T., S. Iizuka, H. L. Pecseli, and J. J. Rasmussen. "Experimental investigation of flute-type electrostatic turbulence." Plasma Physics and Controlled Fusion 30, no. 10 (September 1, 1988): 1297–318. http://dx.doi.org/10.1088/0741-3335/30/10/008.

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19

Coghe, Aldo, Michele Mantegna, and Giorgio Sotgia. "Fluid Dynamic Aspects of Electrostatic Precipatators: Turbulence Characteristics in Scale Models." Journal of Fluids Engineering 125, no. 4 (July 1, 2003): 694–700. http://dx.doi.org/10.1115/1.1593704.

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The present work originated in an investigation on fluid dynamic aspects of electrostatic precipitators performed on scale models of an industrial apparatus. The experimental analysis of velocity and turbulence distribution, performed by hot-wire anemometry, confirmed that significant turbulence levels are found inside particle collectors. In fact, components used to spatially smooth the flow and lower its velocity peaks, such as hoods with wide divergence angles, turning vanes, and perforated plates, may also act as sources of turbulence and reduce the efficiency of electrostatic precipitators. These observations prompted a deeper analysis, both analytical and experimental, of the turbulence decay downstream perforated screens. A new simple semi-empirical model of turbulence decay is proposed, which has shown reasonably good agreement with experimental data, even at short downstream distance from the perforated plate, 50 to 250 hydraulic diameters.

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20

RICCARDI, C., C. BEVILACQUA, G. CHIODINI, E. SINDONI, and M. FONTANESI. "Modification of electrostatic fluctuations by externally imposed radial electric fields." Journal of Plasma Physics 64, no. 3 (September 2000): 227–33. http://dx.doi.org/10.1017/s0022377800008539.

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This paper concerns experiments on the turbulence of a toroidal magnetoplasma in the presence of a radial electric field. The possibility of reduction of turbulence through the application of an external biasing potential has been evaluated by measuring the electrostatic fluctuations and main plasma parameters.

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21

Robson, RE. "Anisotropic Dispersion of a Charged Particle Swarm in a Turbulent Gas in an Electrostatic Field." Australian Journal of Physics 46, no. 2 (1993): 261. http://dx.doi.org/10.1071/ph930261.

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This paper generalises an earlier result of Saffman (1960) to account for cross effects between turbulent and molecular diffusion for charged particle swarms in a gas in the presence of an electrostatic field. It is shown that turbulence enhances the anisotropic character of diffusion. The desirability of using a full kinetic theory analysis as against a limited hydrodynamic description of the swarm is discussed, and one possible tractable approach pointed out.

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22

Dyrud, L., B. Krane, M. Oppenheim, H. L. Pécseli, J. Trulsen, and A. W. Wernik. "Structure functions and intermittency in ionospheric plasma turbulence." Nonlinear Processes in Geophysics 15, no. 6 (November 10, 2008): 847–62. http://dx.doi.org/10.5194/npg-15-847-2008.

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Abstract. Low frequency electrostatic turbulence in the ionospheric E-region is studied by means of numerical and experimental methods. We use the structure functions of the electrostatic potential as a diagnostics of the fluctuations. We demonstrate the inherently intermittent nature of the low level turbulence in the collisional ionospheric plasma by using results for the space-time varying electrostatic potential from two dimensional numerical simulations. An instrumented rocket can not directly detect the one-point potential variation, and most measurements rely on records of potential differences between two probes. With reference to the space observations we demonstrate that the results obtained by potential difference measurements can differ significantly from the one-point results. It was found, in particular, that the intermittency signatures become much weaker, when the proper rocket-probe configuration is implemented. We analyze also signals from an actual ionospheric rocket experiment, and find a reasonably good agreement with the appropriate simulation results, demonstrating again that rocket data, obtained as those analyzed here, are unlikely to give an adequate representation of intermittent features of the low frequency ionospheric plasma turbulence for the given conditions.

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23

Dieckmann, M. E., G. Sarri, D. Doria, H. Ahmed, and M. Borghesi. "Evolution of slow electrostatic shock into a plasma shock mediated by electrostatic turbulence." New Journal of Physics 16, no. 7 (July 2, 2014): 073001. http://dx.doi.org/10.1088/1367-2630/16/7/073001.

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24

Yoon, Peter H., and Luiz F. Ziebell. "Electrostatic weak turbulence theory for warm magnetized plasmas." Physics of Plasmas 28, no. 12 (December 2021): 122302. http://dx.doi.org/10.1063/5.0071803.

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25

Pécseli, H. L., and J. Trulsen. "Velocity correlations in two-dimensional electrostatic plasma turbulence." Physica Scripta T50 (January 1, 1994): 28–37. http://dx.doi.org/10.1088/0031-8949/1994/t50/004.

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26

Wang, Lu, Tiliang Wen, and P. H. Diamond. "Nonlinear parallel momentum transport in strong electrostatic turbulence." Physics of Plasmas 22, no. 5 (May 2015): 052302. http://dx.doi.org/10.1063/1.4919622.

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27

Waelbroeck, F. L., P. J. Morrison, and W. Horton. "Hamiltonian formulation and coherent structures in electrostatic turbulence." Plasma Physics and Controlled Fusion 46, no. 9 (July 13, 2004): 1331–50. http://dx.doi.org/10.1088/0741-3335/46/9/001.

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28

Catto, Peter J., Andrei N. Simakov, Felix I. Parra, and Grigory Kagan. "Electrostatic turbulence in tokamaks on transport time scales." Plasma Physics and Controlled Fusion 50, no. 11 (September 29, 2008): 115006. http://dx.doi.org/10.1088/0741-3335/50/11/115006.

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29

Pécseli, H. L., F. Primdahl, and A. Bahnsen. "Low-frequency electrostatic turbulence in the polar capEregion." Journal of Geophysical Research 94, A5 (1989): 5337. http://dx.doi.org/10.1029/ja094ia05p05337.

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30

Naulin, V., J. Nycander, and J. Juul Rasmussen. "Equipartition and Transport in Two-Dimensional Electrostatic Turbulence." Physical Review Letters 81, no. 19 (November 9, 1998): 4148–51. http://dx.doi.org/10.1103/physrevlett.81.4148.

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31

Katou, K. "Early onset of dissipative electrostatic drift-wave turbulence." Journal of Plasma Physics 40, no. 3 (December 1988): 567–78. http://dx.doi.org/10.1017/s0022377800013520.

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The nonlinear dynamics of a low-frequency electrostatic dissipative inhomogeneous plasma in an external magnetic field is studied for conditions above the critical point. The diffusion flux and the saturation level are self-consistently calculated from first principles, i.e. from the Braginskii equation.

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32

Plunk, G. G., M. Barnes, W. Dorland, and G. G. Howes. "Freely decaying turbulence in two-dimensional electrostatic gyrokinetics." Physics of Plasmas 19, no. 12 (December 2012): 122305. http://dx.doi.org/10.1063/1.4769029.

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33

Wang, W. X., P. H. Diamond, T. S. Hahm, S. Ethier, G. Rewoldt, and W. M. Tang. "Nonlinear flow generation by electrostatic turbulence in tokamaks." Physics of Plasmas 17, no. 7 (July 2010): 072511. http://dx.doi.org/10.1063/1.3459096.

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34

Atten, Pierre, Frank M. J. McCluskey, and Ahmed Chakib Lahjomri. "The Electrohydrodynamic Origin of Turbulence in Electrostatic Precipitators." IEEE Transactions on Industry Applications IA-23, no. 4 (July 1987): 705–11. http://dx.doi.org/10.1109/tia.1987.4504969.

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35

Horacek, J., R. A. Pitts, and J. P. Graves. "Overview of edge electrostatic turbulence experiments on TCV." Czechoslovak Journal of Physics 55, no. 3 (March 2005): 271–83. http://dx.doi.org/10.1007/s10582-005-0040-z.

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36

Thejappa, G., and R. J. MacDowall. "Ulysses Observations of Nonlinear Wave-wave Interactions in the Source Regions of Type III Solar Radio Bursts." International Astronomical Union Colloquium 179 (2000): 447–50. http://dx.doi.org/10.1017/s0252921100065003.

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AbstractThe Ulysses Unified Radio and Plasma Wave Experiment (URAP) has observed Langmuir, ion-acoustic and associated solar type III radio emissions in the interplanetary medium. Bursts of 50–300 Hz (in the spacecraft frame) electric field signals, corresponding to long-wavelength ion-acoustic waves are often observed coincident in time with the most intense Langmuir wave spikes, providing evidence for the electrostatic decay instability. Langmuir waves often occur as envelope solitons, suggesting that strong turbulence processes, such as modulational instability and soliton formation, often coexist with weak turbulence processes, such as electrostatic decay, in a few type III burst source regions.

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37

Lotko, William. "Particle Energization in Stochastic Double Layers." Symposium - International Astronomical Union 107 (1985): 125–29. http://dx.doi.org/10.1017/s0074180900075550.

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Electrostatic turbulence develops in current carrying plasmas when the relative electron-ion drift exceeds the critical value for laminar current flow. Recent 2D computer experiments (Barnes, 1982) indicate that many weak ion acoustic double layers form in such turbulence when the plasma is strongly magnetized (ωce ≳ ωpe), the electron/ion temperature ratio is large (≳10), and the relative electron-ion drift is comparable to or less than the electron thermal speed. The double layers emerge from the incoherent spectrum of electrostatic ion cyclotron and ion acoustic waves as intense localized electric field structures propagating subsonically relative to the ion bulk flow. The occurrence of weak ion acoustic double layers, excited by field-aligned currents in the Earth's auroral regions, has also been reported from in situ spacecraft measurements (Temerin et al., 1982). An important question concerns the effect of these coherent electric fields on plasma transport properties such as bulk heating and acceleration. For example, one might expect nonlinear diffusion processes, manifested as distinct nonthermal features in the particle spectra, to accompany the quasilinear diffusion of ions as they traverse turbulent regions in space. This idea motivates the work presented here.

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38

Pottelette, R., R. A. Treumann, and E. Georgescu. "Crossing a narrow-in-altitude turbulent auroral acceleration region." Nonlinear Processes in Geophysics 11, no. 2 (April 14, 2004): 197–204. http://dx.doi.org/10.5194/npg-11-197-2004.

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Abstract. We report on the in situ identification of a narrow electrostatic acceleration layer (electrostatic shock) containing intense plasma turbulence in the upward current region, and its effect on auroral particles. Wave turbulence recorded in the center of the layer differs in character from that recorded above and beneath. It is concluded that the shock is sustained by different nonlinear waves which, at each level, act on the particles in such a way to produce a net upward directed electric field. The main power is in the ion acoustic range. We point out that anomalous resistivities are incapable of locally generating the observed parallel potential drop.

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39

Shivamoggi, Bhimsen K. "Spectral laws for energy and enstrophy cascades in electrostatic turbulence." Journal of Plasma Physics 42, no. 2 (October 1989): 291–97. http://dx.doi.org/10.1017/s0022377800014367.

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In this paper we develop spectral laws for the small- and large-wavenumber regimes of the energy and enstrophy cascades in electrostatic turbulence and discuss how these spectra differ, owing to compressibility effects, from those for two-dimensional hydrodynamic turbulence. We also show that the compressibility effects on the scaling laws can be described as intermittency corrections formulated according to the log-normal model of Obukhov and Kolmogorov.

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40

Sydora, R. D., J. N. Leboeuf, Z. G. An, P. H. Diamond, G. S. Lee, and T. S. Hahm. "Dynamics and fluctuation spectra of electrostatic resistive interchange turbulence." Physics of Fluids 29, no. 9 (September 1986): 2871–80. http://dx.doi.org/10.1063/1.865487.

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41

Vlad, M., F. Spineanu, J. Misguich, and R. Balescu. "Collisional effects on diffusion scaling laws in electrostatic turbulence." Physical Review E 61, no. 3 (March 2000): 3023–32. http://dx.doi.org/10.1103/physreve.61.3023.

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42

Hasegawa, Akira, and Masahiro Wakatani. "Self-organization of electrostatic turbulence in a cylindrical plasma." Physical Review Letters 59, no. 14 (October 5, 1987): 1581–84. http://dx.doi.org/10.1103/physrevlett.59.1581.

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43

Hidalgo, C., M. A. Pedrosa, A. P. Navarro, F. L. Tabarés, E. Ascasébar, and F. Pérez Murano. "Electrostatic and magnetic turbulence in the TJ-I tokamak." Nuclear Fusion 30, no. 4 (April 1, 1990): 717–22. http://dx.doi.org/10.1088/0029-5515/30/4/012.

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44

Negrea, M., I. Petrisor, and B. Weyssow. "Characterization of zonal flow generation in weak electrostatic turbulence." Physica Scripta 77, no. 5 (April 16, 2008): 055502. http://dx.doi.org/10.1088/0031-8949/77/05/055502.

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45

Wang, R., I. Y. Vasko, F. S. Mozer, S. D. Bale, A. V. Artemyev, J. W. Bonnell, R. Ergun, et al. "Electrostatic Turbulence and Debye-scale Structures in Collisionless Shocks." Astrophysical Journal 889, no. 1 (January 20, 2020): L9. http://dx.doi.org/10.3847/2041-8213/ab6582.

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46

Newman, D. E., P. W. Terry, P. H. Diamond, Y. ‐M Liang, G. G. Craddock, A. E. Koniges, and J. A. Crottinger. "The dynamics of long wavelength electrostatic turbulence in tokamaks*." Physics of Plasmas 1, no. 5 (May 1994): 1592–600. http://dx.doi.org/10.1063/1.870935.

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47

Labit, B., A. Diallo, A. Fasoli, I. Furno, D. Iraji, S. H. Müller, G. Plyushchev, et al. "Statistical properties of electrostatic turbulence in toroidal magnetized plasmas." Plasma Physics and Controlled Fusion 49, no. 12B (November 16, 2007): B281—B290. http://dx.doi.org/10.1088/0741-3335/49/12b/s26.

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48

Fasoli, A., B. Labit, M. McGrath, S. H. Müller, G. Plyushchev, M. Podestà, and F. M. Poli. "Electrostatic turbulence and transport in a simple magnetized plasma." Physics of Plasmas 13, no. 5 (May 2006): 055902. http://dx.doi.org/10.1063/1.2178773.

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49

Yamamoto, Takashi, and J. R. Kan. "Interruption of field-aligned current due to electrostatic turbulence." Journal of Geophysical Research 91, A6 (1986): 7119. http://dx.doi.org/10.1029/ja091ia06p07119.

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50

Gordienko, S. N., and É. I. Yurchenko. "Electrostatic plasma turbulence and spitzer longitudinal conductivity in tokamaks." Plasma Physics Reports 26, no. 9 (September 2000): 721–36. http://dx.doi.org/10.1134/1.1309468.

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Journal articles on the topic 'Electrostatic turbulence'

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