HR: 1340h
AN: SA33B-1322 [Abstracts]
TI: Model Simulation of the Equatorial Electrojet in the Peruvian and Philippine Sectors
AU: * Fang, T
EM: twfang@ucar.edu
AF: High Altitude Observatory, National Center for Atmospheric Research, P.O. Box 3000,
Boulder, CO 80307, United States
AU: * Fang, T
EM: twfang@ucar.edu
AF: Institute of Space Science, National Central University, No.300, Joongda Rd, Jhongli City,
32001, Taiwan
AU: Richmond, A
EM: richmond@ucar.edu
AF: High Altitude Observatory, National Center for Atmospheric Research, P.O. Box 3000,
Boulder, CO 80307, United States
AU: Liu, J
EM: jyliu@jupiter.ss.ncu.edu.tw
AF: Institute of Space Science, National Central University, No.300, Joongda Rd, Jhongli City,
32001, Taiwan
AU: Maute, A
EM: maute@ucar.edu
AF: High Altitude Observatory, National Center for Atmospheric Research, P.O. Box 3000,
Boulder, CO 80307, United States
AU: Lin, C
EM: clin@nspo.org.tw
AF: National Space Organization, 8F, 9 Prosperity 1st Road, Hsinchu Science Park, HsinChu,
300, Taiwan
AU: Chen, C
EM: koichi0925@gmail.com
AF: Institute of Space Science, National Central University, No.300, Joongda Rd, Jhongli City,
32001, Taiwan
AU: Harper, B
EM: bret.harper@gmail.com
AF: Energy and Resources Group, University of California, Berkeley, 310 Barrows Hall,
University of California, Berkeley, CA 94720, United States
AB:
Between 100 and 120 km above the Earth's magnetic equator, the equatorial electrojet (EEJ) flows as an
enhanced eastward current in the daytime E region ionosphere which can induce a magnetic perturbation on the
ground. Calculating the difference between the horizontal components of magnetic perturbation at
magnetometers near the equator and about 6-9 degrees away from equator, ¡µH, provides us information about
the strength of the EEJ. The NCAR Thermosphere-Ionosphere-Electrodynamics General Circulation Model (TIE-
GCM) is capable of simulating the EEJ current and its magnetic perturbation on the ground. The simulated
diurnal, seasonal (March equinox, June solstice, December solstice), and solar activity (F10.7 = 80, 140 and 200)
variations of ¡µH in the Peruvian (75¢XW) and Philippine (120¢XE) sectors, and the relation of ¡µH to the
ionospheric vertical drift velocity, are presented in this paper. Agreement between simulated and observed
magnitudes of ¡µH is improved by modifying the standard daytime E region photochemistry in the TIE-GCM in
order to better simulate observed E region electron densities.
DE: 6999 General or miscellaneous
DE: 7959 Models
SC: SPA-Aeronomy [SA]
MN: 2007 Fall Meeting