UAH The Spinning Terrella Experiment: Lab Analog for Earth's Magnetosphere Robert Sheldon1, Eric Reynolds2 1National Space Science and Technology Center, 2West Virginia University May 30, 2001
Download ReportTranscript UAH The Spinning Terrella Experiment: Lab Analog for Earth's Magnetosphere Robert Sheldon1, Eric Reynolds2 1National Space Science and Technology Center, 2West Virginia University May 30, 2001
UAH The Spinning Terrella Experiment: Lab Analog for Earth's Magnetosphere Robert Sheldon1, Eric Reynolds2 1National Space Science and Technology Center, 2West Virginia University May 30, 2001 Why do we need global pix? UAH • Chapman & Ferraro [1932] wanted the neutral plasma from the • • sun to produce a "ring current" as it envoloped the Earth. This current was needed to explain Dst. But they didn't know how. Alfven tried electric fields [1952?] and failed. Finally Fred Singer [1957] realized that dipoles trap charged particles which carry a current via the grad-B drift. – If they had taken Birkeland's apparatus [1902] and applied a 400V DC bias, this is what they would have seen: Ring Current in the Lab UAH UAH Spinning Terrella Experiment • Bell jar, oil roughing pump, HV power supply, Nd-B ceramic magnet • Needle valve used to control the pressure from 10-400 mTorr • Langmuir • 2 ports • Webcam • ~$10k The Distorted Dipole -But the Earth is NOT a simple dipole, it is distorted by the Solar Wind. - The SW acts as a "superconductor" which prevents B-normal across the separatrix. -This is equivalent to an "image" dipole from elementary electrostatics. -Chapman 32, and Parker 61 simulated this distortion as an image dipole "reflected" by the magnetopause. UAH UAH The Double Dipole M'sphere • Chapman & Ferraro 1932 • Parker 1961 used the double dipole model to explain geomagnetic storms – Laboratory plasmas can easily be set up which are topologically equivalent to Earth's M'sphere • any space effects are topological, no M microphysical •Global dynamics and imaging is easily accomplished 2 Terrella • Two Nd-B-Fe magnets, on alumina standoffs. • We vary the orientation of the magnets, the aspect ratio of the magnets, and the voltage of the magnets. • Glow discharges at 10-200 mTorr = m.f.p 0.3 - 6 mm • The smallest dimension of the glow is 1-10 mfp UAH Parallel Dipoles @ High P UAH -High latitude minimum, and Shabansky orbits -Bistable distributions - Quadrupolar regions of magnetosphere are important for trapping and feeding dipole. Parallel Dipoles @ Low P -Assymetries are caused by 2-dipoles. -Possibly due to separatrix of grad-B and ExB drifts. -This leads to closed orbits that do not encircle the central magnet, "banana orbits", which only occur at narrow range of Voltages at low pressure -Region between the dipoles has compressed fields & appears brighter UAH Plasma Entry @ Cusps UAH -One magnet grounded, other biassed -Plasma generated by electrons on one magnet, feed into other trapping field due to diffusion though "x-line" -Like northward Bz, this feeding happens at the cusps -The cusps themselves hold the plasma long enough to glow, "Sheldon orbits" Anti-Parallel Merging UAH -Left magnet grounded, right magnet w/ increasing bias -X-line plasma merging -Isotropization at min-B Quadrupoles and Merging UAH -Balanced voltages -Appearance of trapped plasma above and below the null point. - These orbits are quadrupolar trapped (drifting around a minima) -Is there a Earth analog? Conclusions UAH • We show that global topology can be seen in a laboratory without "artist's conception" involved. With an inexpensive bell jar setup, we can visualize: – Ring Current – substorms – reconnection – cusp entry, cusp trapping – Shabansky orbits vs. Sheldon orbits UAH Ring Current instability (storm) UAH Spinning magnet with sparks Stationary magnet w/ sparks UAH Complete field-line spark UAH Arcing in 40s exposure UAH