The variations of the midday critical frequency of the F2-layer, ƒ0F2, with the phase of the moon are computed for eighteen stations within about ±40° latitude during a period of low sunspot activity. The results show that the phase of the lunar variation of ƒ0F2 is determined by the magnetic and not by the geomagnetic or the geographic latitude. The reversal from the equatorial type of variation with a maximum near 04 lunar hour to the higher latitude type with a maximum near 10 lunar hour occurs at about ±11° magnetic latitude. The variation of amplitude with latitude shows a sharp maximum on the magnetic equator, associated with the equatorial electro-jet, and two broad maxima at about ±20° magneti...
The lunar daily (L) and lunar monthly (M) variations in horizontal magnetic field (H), maximum elect...
The analysis of 20-year long-term semidiurnal lunar tidal variations gave the evidence that the semi...
The analysis of 20-year long-term semidiurnal lunar tidal variations gave the evidence that the semi...
It is well known that the maximum in the lunar tide variation of ƒ0F2 occurs at about 10 lunar ...
The paper describes lunar daily (L) variation at fixed lunar ages and lunar monthly (M) variation at...
It is well known that the maximum in the lunar tide variation of ƒ0F2 occurs at about 10 lunar ...
The paper contains an analysis of the variation of the midday values of foF2, h'F2 and hpF2 with lun...
The lunar semidiurnal variations in the solar diurnal range of the horizontal component of the earth...
The lunar semidiurnal variations in the solar diurnal range of the horizontal component of the earth...
The lunar semi-diurnal oscillations in the midday values of the critical frequency (ƒ0F2) and t...
Lunar tidal variations in the electron density N at fixed heights of the ionosphere for different so...
Lunar tidal variations in the electron density N at fixed heights of the ionosphere for different so...
The dependence of geomagnetic lunar daily variation (L) on lunar distance in different seasons and f...
Chapman’s Phase Rule L = Σ 4n=1Cnsin{nτ+(n-2)υ+αn} shown by him to be true for g...
Ionospheric total electron content (N<SUB>F</SUB>) data obtained from Faraday rotation measurements ...
The lunar daily (L) and lunar monthly (M) variations in horizontal magnetic field (H), maximum elect...
The analysis of 20-year long-term semidiurnal lunar tidal variations gave the evidence that the semi...
The analysis of 20-year long-term semidiurnal lunar tidal variations gave the evidence that the semi...
It is well known that the maximum in the lunar tide variation of ƒ0F2 occurs at about 10 lunar ...
The paper describes lunar daily (L) variation at fixed lunar ages and lunar monthly (M) variation at...
It is well known that the maximum in the lunar tide variation of ƒ0F2 occurs at about 10 lunar ...
The paper contains an analysis of the variation of the midday values of foF2, h'F2 and hpF2 with lun...
The lunar semidiurnal variations in the solar diurnal range of the horizontal component of the earth...
The lunar semidiurnal variations in the solar diurnal range of the horizontal component of the earth...
The lunar semi-diurnal oscillations in the midday values of the critical frequency (ƒ0F2) and t...
Lunar tidal variations in the electron density N at fixed heights of the ionosphere for different so...
Lunar tidal variations in the electron density N at fixed heights of the ionosphere for different so...
The dependence of geomagnetic lunar daily variation (L) on lunar distance in different seasons and f...
Chapman’s Phase Rule L = Σ 4n=1Cnsin{nτ+(n-2)υ+αn} shown by him to be true for g...
Ionospheric total electron content (N<SUB>F</SUB>) data obtained from Faraday rotation measurements ...
The lunar daily (L) and lunar monthly (M) variations in horizontal magnetic field (H), maximum elect...
The analysis of 20-year long-term semidiurnal lunar tidal variations gave the evidence that the semi...
The analysis of 20-year long-term semidiurnal lunar tidal variations gave the evidence that the semi...