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Journal ArticleDOI

Whistler observations of the interchange of ionization between the ionosphere and the protonosphere

C. G. Park
- 01 Aug 1970 - 
- Vol. 75, Iss: 22, pp 4249-4260
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TLDR
In this article, the electron content in magnetospheric tubes of force in the range 3.5 to 5.5 was measured at Eights, Antarctica, in June 1965, and the observed rate of increase in daytime tube content gives an upward flux of ∼3×108 electrons/cm² sec across the 1000-km level, which is larger than the downward flux necessary to maintain the nocturnal ionosphere.
Abstract
Whistlers recorded at Eights, Antarctica, in June 1965 were used to measure the electron content in magnetospheric tubes of force in the range 3.5<L<5. Under quiet geomagnetic conditions, the observed rate of increase in daytime tube content gives an upward flux of ∼3×108 electrons/cm² sec across the 1000-km level, which is larger than the downward flux necessary to maintain the nocturnal ionosphere. The observed upward flux is primarily due to diffusion of protons through the diffusive barrier, rather than to an increase in the height of the barrier. The downward flux at night under quiet conditions is ∼1.5×108 electrons/cm² sec, an amount that is considered sufficient to maintain the nocturnal ionosphere. The protonosphere is depleted in less than a day during a magnetic storm or polar substorm activities, and subsequent recovery of tube content takes place at a rate of 3-5×1012 electrons/cm² per day. At this rate, an ‘empty’ tube requires about 5 days to reach the monthly median value, and even after 8 days of quiet conditions it continues to fill. The average spacing of geomagnetic disturbances is such that we expect that the protonosphere almost never reaches the saturation level it would attain if it were in equilibrium with the ionosphere.

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Citations
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Journal ArticleDOI

An ISEE/Whistler model of equatorial electron density in the magnetosphere

TL;DR: In this paper, an empirical model of equatorial electron density in the magnetosphere covering the L range 2.25-8.9043 was presented for application to the local time interval 00-15 MLT, and a way to extend the model to the 15-24 MLT period is presented.
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Storms in the ionosphere: Patterns and processes for total electron content

TL;DR: In this paper, the ionosphere's total electron content (TEC) is a parameter widely used in studies of the near-Earth plasma environment, and a comprehensive summary of pre-GPS storm studies is needed to set the base for progress in the GPS era.
Journal ArticleDOI

Recent satellite measurements of the morphology and dynamics of the plasmasphere

TL;DR: The morphology and dynamics of the plasmasphere vary with local time and with geomagnetic conditions as mentioned in this paper, and can be understood in terms of a time-varying convection electric-field model of the magnetosphere.
Journal ArticleDOI

On what ionospheric workers should know about the plasmapause-plasmasphere

TL;DR: A quick reference guide to the plasmasphere can be found in this article, where a series of equatorial density profiles is shown to illustrate the reduction of plasmapause radius during brief periods of increased disturbance and the recovery of the plasosphere by various processes, particularly by filling from the underlying ionosphere.
Journal ArticleDOI

Magnetospheric convection and the high‐latitude F 2 ionosphere

TL;DR: The behavior of the polar ionospheric F layer as it is convected through the cleft, over the polar cap, and through the nightside F layer trough zone is investigated in this paper.
References
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Journal ArticleDOI

Whistler studies of the plasmapause in the magnetosphere: 1. Temporal variations in the position of the knee and some evidence on plasma motions near the knee

TL;DR: The position of the knee in the density of magnetospheric ionization was measured on a high time-resolution basis using whistlers recorded during July and part of August 1963 as discussed by the authors.
Journal ArticleDOI

High-latitude plasma transport: The polar wind

TL;DR: Plasma transport models of polar ionosphere, discussing physical processes involved and effects on electron concentration, ion composition and speeds were discussed in this paper, where the authors also discussed the physical process involved and the effects of electron concentration and ion composition.
Journal ArticleDOI

Whistler studies of the plasmapause in the magnetosphere: 2. Electron density and total tube electron content near the knee in magnetospheric ionization

TL;DR: In this article, a study of electron density and total electron content in tubes of force near the knee in magnetospheric ionization was made, based on whistler observations made at Eights, Antarctica, in July and August 1963, under conditions of steady, moderate geomagnetic agitation (Kp = 2-4).
Journal ArticleDOI

The coupling between the protonosphere and the normal F region

TL;DR: In this paper, it was shown that the proton distribution in the upper portion of the F2 region must follow a chemical equilibrium distribution up to a critical level, hc, which is determined by the condition lambda A = H2, where lambda is the mean free path for the scattering of protons by oxygen ions, A is the charge exchange mean freepath for protons among oxygen atoms, and H is the scale height of atomic oxygen.
Journal ArticleDOI

The maintenance of the night-time F-layer

TL;DR: In this article, a nighttime F layer maintained by hydrogen ions providing source of oxygen ions through charge exchange or by upward drift of ionization is described, where hydrogen ions are replaced by oxygen ions.
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