= The Plasmasphere = || {{ attachment:plasmasphere.png }} || Most of the mass of particles in server sky orbits is [[ http://www.johnstonsarchive.net/physics/RBtutorial.pdf | cold (<1eV) plasma ]], in the upper fringes of the atmosphere. The total mass of these particles is small. This plot shows density versus distance. <
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> This plot is modified from http://plasmasphere.nasa.gov/media/meridianswing.html || || orbit || Radius || L,,min,, || L,,max,, || Dens,,min,, || Dens,,max,, || Volume || Mass || || m288 || 12789 km || 1.93 || 2.14 || 4500/cm^3^ || 7000/cm^3^ || 1.8e12 km^3^ || 17000 kg || || m360 || 14441 km || 2.19 || 2.42 || 2500/cm^3^ || 4000/cm^3^ || 2.6e12 km^3^ || 14000 kg || || m480 || 16756 km || 2.55 || 2.79 || 1200/cm^3^ || 2500/cm^3^ || 3.5e12 km^3^ || 11000 kg || ||<-6> Earth || 1.1e12 km^3^ || 6e24 kg || ||<-6> Troposphere || 8e9 km^3^ || 5e18 kg || A few thousand tons of thinsats will vastly increase the number of coulomb scattering centers. MoreLater == The magnetosphere == The dipole field at the equator is 31000nT. A geomagnetic storm changes this by depositing a westward ring of electric current, which induces a negative change in the field: || -30nT to -50nT || weak storm || || -50nT to -100nT || moderate storm || || > -100nT || intense || || > -300nT || "a few times per solar cycle || . Shrivjer and Siscoe "Heliophysics" pp265 Cambridge 2010 . Also see www.nerc.com/files/GMD_Workshop_Report_April_2011.pdf (chair Don Watkins BPA)