Download presentation
Presentation is loading. Please wait.
1
SCHOOL OF PHYSICS Space Weather in the Equatorial Ionosphere Robert Stening School of Physics, University of New South Wales Acknowledge help from Dr J Du, IPS Radio and Space Services
2
SCHOOL OF PHYSICS
3
Variability Source Atmospheric Tidal Winds Driving Ionospheric Dynamo Equatorial Electrojet Electric Field E Magnetic Variations H Vertical Ion Drifts Plasma Bubbles Scintillation GPS Problems Equatorial Anomaly Ion Density Gradients Communication Problems
4
SCHOOL OF PHYSICS
6
3m radar signal/noise (original Wes Swartz- Cornell)
7
SCHOOL OF PHYSICS Vert. Drift velocities, Heights of max. backscattered power, Spread F layers. Equinox, solar maximum From Fejer et al, 1999
8
SCHOOL OF PHYSICS 1988 1999 Scintillation Occurrence at Indonesian Station (crest). Monitor results Model From Cervera et al Radio Sci 2001
9
SCHOOL OF PHYSICS WAAS (Wide Area Augmentation System)
10
SCHOOL OF PHYSICS
11
What conditions are necessary for bubble formation? Most often occurs at equinox and solar maximum. Often inhibited by magnetic disturbance More likely if both end of field line pass into darkness at the same time Lasts longer into night if electric field reversal is weak
12
SCHOOL OF PHYSICS Low Kp High Kp Low solar flux Medium solar flux High solar flux Peru. Radar echo occurrence Hysell & Burcham Clemson University
13
SCHOOL OF PHYSICS From Tsunoda (1985) Scintillation maximises when sunset at same time at each end of field line.
14
SCHOOL OF PHYSICS Modelled spread F growth rates (Du et al)
15
SCHOOL OF PHYSICS What measurable parameters might help forecast bubble formation? Vertical drifts are the main factor but not always measured Ground-based magnetic fields as a proxy? Need model and measure drift – H relationship C/NOFS satellite
16
SCHOOL OF PHYSICS Modelling problems Is equatorial electrojet controlled locally or is it part of the worldwide current system?
17
SCHOOL OF PHYSICS Modelling problems Is equatorial electrojet controlled locally or is it part of the worldwide current system? Or a bit of both?
18
SCHOOL OF PHYSICS Modelling problems Is equatorial electrojet controlled locally or is it part of the worldwide current system? Or a bit of both? ►Are the day-to-day changes due to tidal changes or local wind changes?
19
SCHOOL OF PHYSICS Modelling problems Is equatorial electrojet controlled locally or is it part of the worldwide current system? Or a bit of both? ►Are the day-to-day changes due to tidal changes or local wind changes? Why does latitude profile not model correctly?
20
SCHOOL OF PHYSICS Trivandrum H 70 120
21
SCHOOL OF PHYSICS HH Vertical Drift Vel. Comparison of Drift velocities with H for 11 days (10-13 LT) from Anderson et al
22
SCHOOL OF PHYSICS Vertical field Northward field Points – observed Curve -simulation 86 nT added to X simulation
23
SCHOOL OF PHYSICS HH ZZ African chain latitude profiles
24
SCHOOL OF PHYSICS Fambitakoye et al (1976) – African data “Total” electrojet current Worldwide component Data Model
25
SCHOOL OF PHYSICS Communication/Navigation Outage Forecasting System Launch 2003
26
SCHOOL OF PHYSICS ZZ YY X added 86 nT Points – data Curves -simulation
27
SCHOOL OF PHYSICS
Similar presentations
© 2025 SlidePlayer.com. Inc.
All rights reserved.