Natural space plasmas occur almost everywhere in the universe: examples for plasmas are the hot interior of the sun and other stars, their atmospheres, most of the interstellar medium, the solar wind and the Earth's ionosphere. In fact, most of the matter in the universe is in the plasma state. The plasma in the near-Earth space is of special interest, as it interacts with artificial satellites used for communications and research. The near-Earth plasma also interacts with low-altitude rockets used for ionospheric research.
Space plasma environments in near-Earth space can be roughly divided
into two categories: those at low altitudes (100km - 1000km, also called
"low-Earth orbit" for satellites) and those at high altitudes, i.e. around
geosynchronous orbit (6.6 Earth radii or 35000km altitude). The first range
of altitudes is roughly the altitude range of the Earth's ionosphere where
the plasma is dense, cool and fairly steady with the maximum density around
300 km. Here collective effects dominate and the plasma is anisotropic
due to the Earth's magnetic field. At geosynchronous orbit however the
plasma is hot and tenuous and highly variable, depending strongly on solar
activity.
The objectives of our research are theoretical modeling of sheath waves,
experimental studies of sheath waves in magnetized and isotropic laboratory
plasmas as well as data analysis from the OEDIPUS-A
and OEDIPUS-C
experiments.
Morin, G.A. and K.G. Balmain, `Plasma sheath and presheath waves: Theory and experiment', Radio Sci., 151-167, 1993.
Balmain, K.G., D.A. Baker, and C.C. Bantin, `Sheath wave propagation in a magnetoplasma', Proc. Workshop Phys. Charged Bodies in Space Plasmas, Eds. M. Dobrowolny and E. Sindoni, Varenna, Italy, 1991, 223-230.
Morin, G.A. and K.G. Balmain, `Hydrodynamic radio-frequency model of an ion sheath near a conductor in a plasma, Radio Sci., 26(2), 459-467, 1991.
Laurin, J.-J., Morin, and K.G. Balmain, `Sheath wave propagation in
a magnetoplasma', Radio Sci., 24(3), 289-300, 1989.
The charging phenomena are divided into two categories: surface charging which occurs in exposed surface dielectrics such as thermal blankets and internal charging which affects insulating material inside the satallite such as circuit boards. Discharges interfere with control signals and in the worst case can destroy circuits. Consequences of discharges range from temporary operational anomalies to permanent failure of entire satellites. It is believed that the recent failure of the ANIK E1 satellite was caused by unusually high rates of high-energy electrons during the week preceding the problem. ANIK E1 and E2 previously experienced operational difficulties during a similar situation in January 1994.
The objective of our research is the laboratory simulation of surface
and internal charging of spacecraft dielectrics in two specially designed
vacuum chambers using an electron gun for electron energies up to 25 keV
and a Sr90 source for electron energies up to 2 MeV.
K.G. Balmain, `Surface arc discharges on spacecraft dielectrics', IEEE Trans. Elect. Insulation, 21(3), 427-430, 1986.
K.G. Balmain, M. Gossland, and K. Karia, `Spacecraft fiberglass strut charging/discharging and EMI', IEEE Trans. Nucl. Sci., 32(6), 4438-4440, 1985.
K.G. Balmain, A. Battagin, and G.R. Dubois, `Thickness scaling for arc discharges on electron-beam-charged dielectrics', IEEE Trans. Nucl. Sci., 32(6), 4073-4078, 1985.
G. McKeil and K.G. Balmain, `Analysis of the ion spot phenomenon on
beam-charged dielectrics', IEEE Trans. Nucl. Sci., 33(6), 1396-1401,
1986.