HIGH ION ENERGY, HIGH POWER ION BEAM SYSTEM FOR SOLAR WIND SIMULATION

Dr. John D. Williams

Introduction

Robert Winglee of the University of Washington has proposed a novel plasma propulsion concept that has received a great deal of attention at NASA’s Marshall Space Flight Center (MSFC). The propulsion concept has been designated as Mini-Magnetospheric Plasma Propulsion (M2P2), and numerical studies and scaling from small vacuum chamber experiments have shown that the M2P2 system will provide high thrust levels (I to 3 N) at very low power and propellant flow rates.

The M2P2 concept generates thrust through the forced expansion of a dipole magnetic field that intercepts and deflects the solar wind analogous to the way in which a more straightforward (albeit more complicated and massive) magsail would operate. The next stage in the development of the M2P2 concept will be experimental testing in a very large vacuum test facility at MSFC. To simulate the solar wind, MSFC plans on procuring several broad beam ion sources that will be mounted at one end of the facility to be used to generate a uniform current density argon ion beam across the entire cross‑section of the cylindrical vacuum chamber.

The need of MSFC for a solar wind simulator offers a unique, multi‑faceted opportunity for the Plasma Engineering Group at Colorado State University. One facet of this opportunity concerns the chance to apply results from the high‑energy ion thruster research program to design a large diameter ion optics system. Another facet concerns the opportunity to become involved in space plasma simulation activities in a large vacuum test facility at NASA. Another facet has to do with optimizing a large diameter discharge chamber so that a very uniform plasma profile is produced across the end of the chamber where the ion optics system is to be mounted. A non‑uniform or peaked ion density profile causes the ion optics system to be overdriven near the maximum ion density region and under‑driven near regions of lower ion density. This problem has recently plagued both NASA and commercial entities that utilize ion propulsion systems, and its solution (i.e., a flatter ion density profile) will significantly increase the total impulse that is available from an ion propulsion system.

Objective and Procedure

 The objective of this project is to design an entire solar wind simulator that could meet the needs of NASA’s Marshall Space Flight Center for testing of advanced solar wind propulsion technologies. Specifically this effort involves (1) the design of an advanced ion optics system that would be capable of forming a 30‑cm diameter argon ion beam with an energy range between 5 keV and 20 keV over a current density range of 1 mA/cm2 to 5 mA/cm2, (2) the adaptation and optimization of a 30‑cm diameter discharge chamber capable of providing a uniform plasma ion flux to the ion optics system, and (3) the development of an advanced ion beam neutralization system capable of servicing a cluster of up to 4 solar wind simulation sources. The Plasma Engineering Group at CSU has developed all of the models and software codes needed to design a solar wind simulator, which will be utilized by the graduate and undergraduate students chosen to work on the project. The approach will include the following steps:

1. Optimization of the ion optics systems. This will be accomplished using the IGX code to simulate ion beamlet properties under various beamlet geometries, potential biases, and ion currents. Operational points will be identified to enable operation of the system over a wide range of ion current densities and voltages.

2. Generate mechanical drawings of grids to be used in the ion optics system and design the optics mounting hardware suitable for withstanding up to 20 kV operation.

3. Optimization of the discharge chamber. This will be accomplished using the HAG and PLASMA codes to design the proper magnetic field confinement scheme and primary electron injection point that will result in the most uniform plasma density profile over the widest possible discharge power and flow rate range.

4. Generate mechanical drawings of the discharge chamber, cathode mount, and expellant injection ports. Also prepare drawings of the ground screen to be placed around the discharge chamber to prevent plasma leakage and the mounting system to be used to attach the ground screen structure to a vacuum test facility. Finally, prepare electrical wiring schematics and layout drawings.

5. Definition of the neutralization system. Model the plasma production requirements needed to provide an electron flux sufficient to neutralize four solar wind simulators. Provide the design of an ionization stage equipped plasma contactor capable of providing the necessary plasma production requirements at the lowest possible flow rates.

6.      Generate mechanical drawings of the neutralization system.

7. Collection of the work conducted under Steps 1 through 6. Generate a preliminary design document and prepare it for submission as part of a proposal to MSFC.

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