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  • 1
    Monograph available for loan
    Monograph available for loan
    Amsterdam : Gordon and Breach
    Call number: M 98.0417
    Type of Medium: Monograph available for loan
    Pages: xviii, 625 S.
    ISBN: 9056990691
    Classification:
    Geomagnetism, Geoelectromagnetism
    Language: English
    Location: Upper compact magazine
    Branch Library: GFZ Library
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  • 2
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 108 (1992), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: Some 25 rocket profiles of the current density of the eastward ionospheric lower current layer close to the magnetic dip equator, one profile of the reverse westward lower current layer at about 5° dip latitude and five profiles of the eastward upper current layer within 0° to about 8° dip latitude have been modelled giving the following results. The parameters of the eastward lower current layer within 0° to 2° dip latitude around local noon are; peak current density normalized to dip equator 10.4 ± 6 A km-2, peak current intensity normalized to dip equator 145 ± 86 A km-2, and half thickness at half of the peak current density 5.7 ± 1 km. The differences in these parameters between the equatorial electrojet in India and Peru are negligible. The parameters of the ionospheric eastward upper current layer around local noon are; peak current density normalized to the dip equator 2.37 ± 0.5 A km-2, peak current intensity normalized to the dip equator 22.1 ± 7 A km-2, and half thickness at half of the peak current density 4.1 ± 2 km. The parameters of the model fitting the rocket profiles extremely well have been provided. The suggestion that the lower eastward and the lower westward current layers constitute the equatorial electrojet, while the upper eastward current layer is the global part of the Sq currents, has been substantiated. This leads to results consistent with spherical harmonic analysis of geomagnetic Sq variations. The first contours of the ionospheric eastward upper current layer density have been presented and they are consistent with the features of the worldwide Sq.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 108 (1992), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: The study of rocket measurements suggests the following conclusions, (i) Ionospheric currents are basically in two layers, (ii) The upper current layer with a steady altitude extent of 18 ± 3 km is global and should be regarded as the worldwide part of the Sq current system, (iii) The intense eastward lower current layer at the magnetic dip equator that terminates in a focus within 2° to 4° dip latitude, together with the reverse westward lower current layer that peaks around 5.3 ± 0.7° dip latitude, should be regarded as the equatorial electrojet (EEJ). (iv) The EEJ and the worldwide part of the Sq current system are coupled, sometimes overlapping in varying degrees, especially within 0° to 0.5° dip latitude where the overlap often leads to a hybrid current system, (v) The lunar geomagnetic variations result from the modulations of the above current layers and not from a separate current layer. An interesting latitudinal profile of the vertical cross-section of ionospheric currents from the dip equator to about 60° latitude has been presented. Seven of the nine altitude structure parameters of the current layers equatorward of the EEJ current focus differ by 10 to 30 km from their values beyond the EEJ current focus. Six of these altitude parameters tend to recover after their minima at the EEJ current focus and the Sq current focus. The lower current layer is thicker, the upper current layer is higher, and the entire current system is thicker equatorward of the EEJ current focus than beyond it. The half thickness at half of the peak current density of the eastward EEJ is about 2.9 times that of the reverse westward lower current layer, and about 34.3 ± 0.7 per cent greater than that of the worldwide part of the Sq current layer equatorward of the Sq current focus. The continuous distribution of current density model has elucidated the latitudinal variations of ΔF, ΔH and their ratio in the vicinity of the dip equator. It thus explains some observations of Davis, Burrows & Stolarik (1967) and some discrepancies that accompanied the detection of the meridional currents of the equatorial electrojet.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 108 (1992), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: Some 76 results of rocket measurements of ionospheric currents worldwide from 1948 to 1973, have been collected and arranged into seven groups suggested by the characteristics of geomagnetic variations which they cause. Their organization and planned study in five parts are outlined. This first part also presents the study of the group of rocket measurements of night-time ionospheric currents. The finding from nine rocket flight results is that the attempts to detect night-time ionospheric currents with rocket-borne instruments in the low and mid-latitudes have not found distinctly clear indication of such currents. The remnant E-region electron density at night measured aboard two rockets led to calculated currents so small that they support the above finding. Discussion of the rocket and other relevant studies led to the conclusion that nocturnal ionospheric currents do not seem to exist at any part of the solar cycle.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 108 (1992), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: This second part of the series has studied ionospheric currents outside the dip equatorial zone in the three groups of: high-latitude currents beyond 70° latitude (Group 6), daytime currents within 35° to 70° dip latitude (Group 5), and daytime currents within 7° to 35° dip latitude (Group 4). Ionospheric currents have been found and measured with rockets in all three groups, and their directions are in conformity with expectations from geomagnetic variations: eastwards equatorward of the Sq focus (Group 4), westwards between the Sq focus and high latitudes (Group 5), and complex in the higher and polar latitudes (Group 6). Of great interest is the discovery that the currents occur in the two eastward layers in Group 4 but only in one layer in Groups 5 and 6. The altitude of peak current is 105 ± 8 km and 123 ± 8 km for the two layers of Group 4 respectively, 112 ± 3 km in Group 5 and about 120 km in Group 6. The peak current density is about 1.5 A km-2 and 1 A km-2 for layers 1 and 2 respectively in Group 4 and difficult to determine in Groups 5 and 6. The altitude extent of the current layers decreases towards the Sq focus. On average the altitude extent is 19 ± 7 km and 15 ± 8 km for layers 1 and 2 of Group 4 respectively, 17 ± 3 km in Group 5 and is difficult to determine in Group 6. The two peaks of current density in Group 4 did not appear to correlate with peaks of electron density measured with the same rocket. However, the upper current peak occurred near the peak of Pedersen conductivity.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 108 (1992), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: The 31 daytime rocket flight results within 0° or 2° dip latitude provide a good study of several issues leading to the following findings. In this zone, 60 per cent or more of ionospheric current systems have two layers. The lower layer has a peak density of 7 ± 4 A km-2 at an altitude of 106 ± 2 km, a half thickness at half peak of 5.7 ± 0.7 km and an altitude extent of 34 ± 9 km. The upper layer has a peak density of about 1 A km-2 at an altitude of 136 ± 8 km and an altitude extent of 19 ± 5 km. In some altitude structures, the single layer system is like a hybrid of the lower and the upper layers. The thickness of the equatorial electrojet decreases as its peak current density increases. From this and earlier findings, the electrojet contracts vertically and latitudinally as its peak current density increases. From the sample examined, there is not much difference between the intensities of the lower layers over India and Peru. However, the intensity of the upper layer over India is only about half of its intensity over Peru. The decrease of the electrojet current density in the afternoon is related more to the decrease in the east-west electrostatic field than to electron density or conductivity. AC electric field fluctuations caused by the cross-field instability have been observed in situ in the east-west direction only, in the frequency range of 5 to 120 Hz at altitudes of 85 to 105 km. It is shown that the geometrical and current density structures of the electrojet substantially influence the ratios of its internal to external magnetic field components, all of which initially increase in magnitude with dip distance. Within 0° to 2° dip latitude the ratios are 0.28 ± 0.08 for the northward component X, -0.17 ± 0.2 for the vertical component Z, and 0.23 ± 0.02 for the total field F. A proposed simple measure of day-to-day variability shows promise.
    Type of Medium: Electronic Resource
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  • 7
    Publication Date: 1992-01-01
    Print ISSN: 0022-1392
    Topics: Geosciences
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  • 8
    Publication Date: 1992-02-01
    Print ISSN: 0956-540X
    Electronic ISSN: 1365-246X
    Topics: Geosciences
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  • 9
    Publication Date: 1992-02-01
    Print ISSN: 0956-540X
    Electronic ISSN: 1365-246X
    Topics: Geosciences
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  • 10
    Publication Date: 1992-02-01
    Print ISSN: 0956-540X
    Electronic ISSN: 1365-246X
    Topics: Geosciences
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