The vertical drift is inferred from the time rate of change of hmF2 and the hmF2 is inferred from the proposed formulae of Shimazaki (1955). hmF2= {1490/M3000}-176.
At mid latitudes, the much larger effect is observed in the component parallel to the magnetic field of the O+ and H+ velocities, see Measurements of the topside ionosphere over Arecibo during the total solar eclipse of February 26, 1998
B. MacPherson, S. A. González, M. P. Sulzer, G. J. Bailey, F. Djuth, P. Rodriguez, Journal of Geophysical Research (Impact Factor: 3.17). 10/2000; 105(A10):23055-23068. DOI:10.1029/2000JA000145
ABSTRACT The Arecibo incoherent scatter radar facility was operated on February 26, 1998, and was used to observe the total solar eclipse that occurred over the Caribbean. A maximum of 87% obscuration was observed over Arecibo at 1430 LT (1830 UT). The radar was operated using an
experimental technique, which uses a 300 μs single/multi-frequency
pulse, to gather data from the altitude range 146-2412 km. The Sheffield
University plasmasphere ionosphere model was used to interpret the
measurements. The electron temperature was found to have decreased by
600 K at 400 km altitude, but the magnitude of the decrease becomes
smaller with increasing altitude. This is shown to be the result of the
lesser degree of obscuration of the solar disk at latitudes north of
Arecibo. Conjugate point photo-electron heating effects are also shown to
play a significant role in the electron energy balance during the
eclipse. The H+ ion temperature exhibited a response to the
eclipse, with temperatures being around 200 K lower than expected at the
time of maximum obscuration. There was relatively little variation
observed in the O+ temperature. The response of the topside
ionosphere is characterized by a downward motion arising from the
contraction of the plasma due to reduced plasma temperatures. This is
most clearly seen in the O+-H+ transition altitude
which falls by 200 km. The transition altitude fully recovers within 2
hours after the eclipse. The location of the transition altitude acts to
mitigate the effects of the eclipse on the topside electron densities.
An edited version of this paper was published by AGU. Copyright 2000 American Geophysical Union. To view the published open abstract, go to http://dx.doi.org and enter the DOI.
Why is Shimazaki fomula is not suitable for the time of eclipse? Have you ever compared a real measurement of peak height with the one inferred from Shimazaki? What are your Justification.