Mihály Horányi
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FPDS BASE DESCRIPTION, MULTIPLE YEAR AWARD&INCREMENTAL FUNDING FOR YEARS ONE TO FIVE. THIS PROPOSAL IS ENTITLED, \''INSTITUTE FOR MODELING PLASMA, ATMOSPHERES, AND COSMIC DUST (IMPACT).\'' THIS IS AWARDED IN RESPONSE TO COOPERATIVE AGREEMENT NOTICE (CAN
Open Date: 2014-03-25
Close Date: 2019-02-14
Grant: Close
THE NEAR SURFACE ENVIRONMENT OF AIRLESS BODIES IN THE SOLAR SYSTEM IS A COMPLEX AND DYNAMIC SYSTEM. WITHOUT AN APPRECIABLE ATMOSPHERE, THE SURFACE IS EXPOSED TO A VARIETY OF PLASMA CONDITIONS AND UV RADIATION. THIS IN TURN LEADS TO SURFACE CHARGING,NEAR-S
Open Date: 2012-09-01
Close Date: 2013-08-31
Grant: Close
Proposal entitled ''''NASA Lunar Science Institute Colorado Center for Lunar Dust & Atmospheric Studies' in response to LUNAR CAN #NNH08ZDA008C - NASA responsible: 1. The NLSI Director & NLSI Central will be housed at NASA ARC & will report directly to the
Open Date: 2009-04-09
Close Date: 2013-04-08
Grant: Close
'THE DUSTY PLASMA ENVIRONMENT OF THE MOON' (Andrew Poppe) Due to the lack of an atmosphere, the Moon is exposed to several plasma processes that create a complex environment on the lunar surface. Several observations indicate that micronsized dust grains
Open Date: 2008-09-04
Close Date: 2010-09-03
Grant: Close
'LUNAR DUST TRANSPORT: THEORETICAL MODELS & LABORATORY EXPERIMENTS' The electrostatic liftoff and transport of lunar dust remains an open and controversial issue since the early days of lunar exploration. As function of time and location, the lunar surfac
Open Date: 2008-08-15
Close Date: 2012-08-14
Articles (11)
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2023
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2023
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2023
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2023
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2022
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2022
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2022
Magnetic anomalies on the surface of the Moon interact with the solar wind plasma flow, resulting in both magnetic and electrostatic deflection/reflection of charged particles. Consequently, surface charging in these regions differs from regions without magnetic fields. Using the Colorado Solar Wind Experiment facility, this interaction is investigated with high‐energy flowing plasmas (100–800 eV beam ions) that are incident upon a magnetic dipole embedded beneath an insulating surface. The dipole moment is perpendicular to the surface. The plasma potential distribution is measured above the surface using an emissive probe. In the dipole lobe regions the surface is charged to significantly higher positive potentials by the un‐magnetized ion beam impinging on the surface while the electrons remain excluded by the magnetic field. At low ion beam energies the results agree with these expectations as the surface potential follows the ion beam energy. However, at high beam energies, the surface potentials in the electron‐shielded lobe regions remain significantly lower than the expected magnitude. Surprisingly, electrons are detected in the shielded regions by a Langmuir probe. A test particle simulation indicates that secondary electrons induced by the high energy ion beams impinging on the surface can enter the shielded regions, thus lowering the surface potential.
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2022
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2022
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2022
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2022
Collaborators (7)
J. Deca
University of Colorado Boulder
SASCHA KEMPF
University of Colorado Boulder
Bruce Draine
Professor
Princeton University
Jamey R. Szalay
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XU WANG
University of Colorado Boulder
ZOLTAN STERNOVSKY
University of Colorado Boulder
Lee Fielding
Lecturer in Polymer Chemistry
The University of Manchester
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