Answers are grounded in this paper and cite their sources.
Turbulent structure of the electrojet is discussed in detail, and a unified interpretation of the electrojet irregularities (type I and type II) is given in terms of nonlinear two-stream and cross field instabilities. It is emphasized that small-scale type II irregularities (3∼15 meters) can be interpreted as resulting from nonlinear decay (collapse) of large-scale irregularities (∼150 meters), which are directly excited by the cross field instability. It is shown that polarization fields associated with the large irregularities modify the straight (horizontal) electron flow substantially; electrons are constrained to make periodic excursions vertically upward and downward in accord with the period of the irregularities. Consequently, the type I irregularities arising from the two-stream instability are excited obliquely and vertically, as well as horizontally. It is also shown that the observed constant phase velocity of the type I irregularities can be explained in terms of the quasilinear stabilization. In addition, it is emphasized that one should not regard the mean Doppler velocity of the type II (3-meter) echoes Vph3II as representing the electron drift velocity when type I echoes coexist, i.e., when Vph3II > Cs, where Cs is the ion sound velocity.
No takes yet. Share an insight, caveat, or question.
Tetsuya Sato (1973) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: