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These data are all applicable to low heliographic latitudes, i.e. to the slow solar wind.
The spatial distribution of E at different latitudes i.e. by different magnetic field orientation is modeled.
Two of these models will be spherical harmonic descriptions of the ionospheric magnetic field at mid-to-low latitudes, i.e., below 55? dipole latitude.
Under quiet conditions, however, the ionosphere at high latitudes will behave as at other latitudes, i.e. only determined by the solar zenith angle and solar activity.
At high latitudes, i.e. outside the ±55° magnetic latitudes interval, the three component vector magnetic satellite data are used in North, East, Center (NEC) system of coordinates.
The dashed curves represent the ±15° latitudes, i.e., the approximate positions of the crest regions of the equatorial ionization anomaly.
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The modelled dispersal route suggests that H. erectus remained preferentially associated with low/middle latitude (i.e., comparatively warm) sites throughout its colonization history.
It is possible to see that for the same time interval near midnight, the westward auroral electrojet was located at the latitude near the 62° geographic latitude, i.e., near the 60° geomagnetic latitude.
For upland SOC there was a six-fold non-linear increase in SOC with latitude (i.e., temperature) where SOC was lowest in the Intermontane Boreal compared to the Arctic Tundra and Coastal Rainforest.
Therefore, to examine the effect of the other dominant mechanism at the low latitude, i.e., electrojet, the variation of hourly NmF2 with maximum electrojet strength over Dibrugarh and Okinawa was investigated for the period of August 2010 till December 2012.
The prevalence rates of a number of diseases increase with increasing latitude, i.e., prevalence rates tended to be very low near the equator and to increase as one moved toward the poles.
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