Abstract

Quasi‐sinusoidal density waves were frequently observed during the end of the Pioneer Venus Orbiter (PVO) mission when the orbiter was at low periapsis [Brace, this issue]. These waves occur at altitudes ∼145–155 km and have wavelengths ∼1 km. It is suggested that a radial, ambipolar electric field E0, directed downward, is established in the Venus ionosphere during electron pressure enhancements above ∼160 km. This field generates an electron E × B drift VE; the ions move radially and do not E × B drift because they are unmagnetized (i.e., νin » Ωi). This drift is shown to drive a collisional drift wave instability for sufficiently large values of VE, nominally, VE > υi where υi is the ion thermal velocity. For parameters typical of the nightside Venus ionosphere, this instability generates plasma fluctuations with wavelengths ∼1 km, consistent with observations.

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