Evaluation of Facility Effects on Ion Migration in a Hall Thruster Plume

5torr. The effects of background facility neutrals were characterized and isolated, which enabled precise and accurate estimation of thruster ion beam current and plume divergence. A set of guidelinesarerecommendedforFaradayprobedesign,experimentalmethodology,anddataanalysisthatareaimed at minimizing uncertainty of far-field Faraday probe measurements. These guidelines were shown to reduce the experimentally derived ion beam current by 10–20%, compared with conventional analysis techniques, and to reduce measurement uncertainty to approximately 3%. The reductions in measurement uncertainty and the increased capability to approximate the onorbit plume expansion from ground-based measurements are significant improvements that can be used for validation of numerical simulations and investigations of Hall thruster performance loss mechanisms. Nomenclature AC = cross-sectional geometric area of Faraday probe collector A0;1;2 = second-order polynomial coefficients G0;1;2;3;4 = Gaussian function coefficients

[1]  E. Ahedo,et al.  A two-dimensional hybrid model of the Hall thruster discharge , 2006 .

[2]  Kunning G. Xu,et al.  Plume Characterization of an Ion Focusing Hall Thruster , 2011 .

[3]  R. Spicer Validation of the DRACO Particle-in-Cell Code using Busek 200W Hall Thruster Experimental Data , 2007 .

[4]  Alec D Gallimore,et al.  Evaluation of ion collection area in Faraday probes. , 2010, The Review of scientific instruments.

[5]  William A. Hargus,et al.  Background Pressure Eects on Internal and Near-eld Ion Velocity Distribution of the BHT-600 Hall Thruster , 2008 .

[6]  Yassir Azziz,et al.  Experimental and theoretical characterization of a Hall thruster plume , 2007 .

[8]  Jeremiah J. Boerner,et al.  Computational simulation of Faraday probe measurements , 2008 .

[9]  Joseph Wang,et al.  Development of the DRACO Code for Modeling Electric Propulsion Plume Interactions , 2004 .

[10]  David Kirtley,et al.  The Development of A Flexible, Usable Plasma Interaction Modeling System , 2002 .

[11]  Robert S. Jankovsky,et al.  Hall Thruster Plume Measurements On-Board the Russian Express Satellites , 2001 .

[12]  Alec D. Gallimore,et al.  Neutral density map of Hall thruster plume expansion in a vacuum chamber , 2005 .

[13]  Alec D. Gallimore,et al.  Magnetically filtered Faraday probe for measuring the ion current density profile of a Hall thruster , 2006 .

[14]  N. T. Peacock,et al.  Comparison of hot cathode and cold cathode ionization gauges , 1991 .

[15]  B. M. Reid,et al.  The Influence of Neutral Flow Rate in the Operation of Hall Thrusters. , 2009 .

[16]  Daniel L. Brown,et al.  Investigation of low discharge voltage Hall thruster characteristics and evaluation of loss mechanisms , 2009 .

[17]  Alec D. Gallimore,et al.  A Comparison of Nude and Collimated Faraday Probes for Use with Hall Thrusters , 2001 .

[18]  I. Mikellides,et al.  Efficacy of Electron Mobility Models in Hybrid-PIC Hall Thruster Simulations , 2008 .

[19]  Alec D. Gallimore,et al.  Effect of Backpressure on Ion Current Density Measurements in Hall Thruster Plumes , 2005 .

[20]  Charles K. Birdsall,et al.  Particle-in-cell charged-particle simulations, plus Monte Carlo collisions with neutral atoms, PIC-MCC , 1991 .

[21]  Brian E. Beal,et al.  Methodology and Historical Perspective of a Hall Thruster Efficiency Analysis , 2009 .

[22]  P. Redhead Instabilities in crossed-field discharges at low pressures , 1988 .

[23]  John M. Sankovic,et al.  Hall thruster ion beam characterization , 1995 .

[24]  Matthew Gibbons,et al.  Flexible Three-Dimensional Modeling of Electric Thrusters in Vacuum Chambers , 2003 .

[25]  M. Walker,et al.  Ion Collection in Hall Thruster Plumes , 2006 .

[26]  Randy Aadland,et al.  BPT Hall thruster plume characteristics , 1999 .

[27]  Iain D. Boyd,et al.  Far field modeling of the plasma plume of a Hall thruster , 2002 .

[28]  C. Birdsall,et al.  Plasma Physics via Computer Simulation , 2018 .