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Journal ArticleDOI

Very low frequency phase perturbations and the soviet high-altitude nuclear bursts of October 22 and 28, 1962: 1. Observations and inferred radiation belts

C. R. Haave, +2 more
- 01 Sep 1965 - 
- Vol. 70, Iss: 17, pp 4191-4206
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TLDR
In this paper, the same types of particles and their energies were the same for both detonations, but differences existed in the spatial extent of the radiation belts producing the VLF phase perturbations, and the trapped particles were electrons with E ≲ 4 Mev and protons in the range 23 to 46 Mev.
Abstract
On October 22 and 28, 1962, nuclear explosions over central Asia produced ionospheric D-layer perturbations as monitored on various VLF paths in the northern hemisphere Delayed VLF effects due to trapped particles averaged 53% of the normal diurnal change for the burst of October 22, and 29% for the burst of October 28 The types of particles and their energies were the same for both detonations, but differences existed in the spatial extent of the radiation belts producing the VLF phase perturbations The trapped particles were electrons with E ≲ 4 Mev and protons in the range 23 to 46 Mev The electron spectrum is composed of fission and neutron-decay β particles, the latter predominating for E < 078 Mev Protons <23 Mev may have also been present, but those with E < 1 Mev cannot penetrate into the D region and are of no direct VLF interest With the dipole field approximation, for the detonation of October 22, fission and neutron-decay β particles were trapped in a region bounded by field lines intersecting the earth's surface in a range extending at least from 365° to 56° geomagnetic (for the real field the shells are 175 ≤ L ≤ 376) For October 28, fission β particles were confined to areas <49°N (L < 232) and probably to field lines around that passing through the burst point (at 365°N and L = 175); this type of confinement also existed for 23- to 46-Mev protons after both nuclear bursts For October 28, effects due to neutron-decay β particles were found at 49°–51°N (232 ≤ L ≤ 279), a region which formed the outer boundary for these trapped particles For the burst of October 22, a prompt effect was observed on the GBR to APL transmission

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Citations
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Journal ArticleDOI

ELF and VLF radio waves

TL;DR: A review of developments in ELF and VLF radio-wave propagation research over the last 50 years of the Journal of Atmospheric and Solar-Terrestrial Physics can be found in this paper.
Journal ArticleDOI

A study of electrons artificially injected into the geomagnetic field in october, 1962

TL;DR: Particle detectors in the Alouette satellite measured the electrons with energy greater than 3.9 MeV which were trapped in the geomagnetic field as the result of three Russian high-altitude nuclear...
Journal ArticleDOI

Very low frequency phase perturbations and the Soviet high-altitude nuclear bursts of October 22 and 28, 1962: 2. Comparison with satellite particle data

TL;DR: In this article, the authors examined the temporal histories of the VLF phase perturbations produced by the two Soviet high-altitude nuclear bursts of October 22 and 28, 1962.
Journal ArticleDOI

VLF phase perturbations produced by the Soviet high‐altitude nuclear explosion of November 1, 1962

Abstract: The Soviet high-altitude nuclear burst of 0912 UT on November 1, 1962, produced delayed perturbations of the VLF transmissions monitored at APL/JHU over five paths remote from the burst region. The burst-related VLF effects varied from 6 to 55% and averaged 32% of the normal diurnal variation. It is suggested that the VLF phase perturbations are produced by particles from the burst that drift to the remote regions and produce an ionization enhancement in the lower ionosphere in their first, and sometimes in their second, global orbit. The temporal histories of the VLF phase perturbations are compatible with a model wherein it is assumed that the trapped particles are electrons from the radio-active decay of neutrons, the artificial belt extending from an outer shell of L ≈ 3.4 to at least L = 1.9. Satellite particle data do not show an artificial belt of electrons from the decay of neutrons, a belt which in this case may have been obscured by the background flux of electrons from the natural Van Allen belt and from the artificial belts from the earlier Soviet explosions. Satellite data do, however, show a narrow belt of fission electrons ≳1 Mev with maximum flux at L ≈ 1.77 and a lower boundary at L = 1.73. These fission electrons did not affect the VLF paths intercepted by these shells. The VLF and satellite data agree that fission electrons ≳1 Mev were not present on shells above L ≈ 1.9.
References
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Journal ArticleDOI

Coordinates for Mapping the Distribution of Magnetically Trapped Particles

TL;DR: In this article, it is shown that a parameter L = f(B,I) can be defined which retains most of the desirable properties of I and has the additional property of organizing measurements along lines of force.
Journal ArticleDOI

Mirror and azimuthal drift frequencies for geomagnetically trapped particles

TL;DR: For charged particles trapped in the geomagnetic field, the frequencies of the mirror oscillations ωm and the azimuthal drift ωd are defined as appropriate averages over the helical motion around the field lines and the mirror motion between reflection points in the two magnetic hemispheres as discussed by the authors.
Journal ArticleDOI

A study of charged particles in the earth's outer radiation zone with explorer 14

TL;DR: In this article, the earths outer radiation zone from explorer xiv satellite has been observed from the Xiv satellite, and charged particles in the outer radiation zones have been detected.
Journal ArticleDOI

The Radiation Belts, Natural and Artificial

TL;DR: About 1 or 2% of the electrons generated by the nuclear detonation of July 9, 1962 were found to be present in the geomagnetic field 125 days later, and a new outer zone of both high- and low-energy electrons was formed by the magnetic storm which began December 18, 1962.
Journal ArticleDOI

Results of the Telstar radiation experiments

TL;DR: In this article, the Telstar data were analyzed to provide maps of the distribution of electrons and protons as measured in three detectors during the period from July through October, 1962, and the connection of these observations to the high-altitude nuclear explosion of July 9, 1962 was discussed.
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