1992
DOI: 10.1109/74.163808
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Finite-difference time-domain solution of Maxwell's equations for the dispersive ionosphere

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Cited by 75 publications
(50 citation statements)
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“…Thus, a negative space charge forms ahead of the shock and a positive space charge forms behind it as in Figure 1. Although Adamovich et al [2] found that the kinetic energy inherent in an EDL effect was insufficient to create the observed effects, Saeks and Kunhardt [16] point out that their analysis didn't account for the Coulomb forces in the EDL. Accounting for the Coulomb forces may explain the observed shock standoff distance increase.…”
Section: Edl Modellmentioning
confidence: 99%
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“…Thus, a negative space charge forms ahead of the shock and a positive space charge forms behind it as in Figure 1. Although Adamovich et al [2] found that the kinetic energy inherent in an EDL effect was insufficient to create the observed effects, Saeks and Kunhardt [16] point out that their analysis didn't account for the Coulomb forces in the EDL. Accounting for the Coulomb forces may explain the observed shock standoff distance increase.…”
Section: Edl Modellmentioning
confidence: 99%
“…Saeks and Kunhardt [16] posit the existence of an EDL at the shock surface itself. They cite experimental work by Mishin [15] that shows an increase in electron density and conductivity ahead of the shock front and a similar decrease behind the shock front.…”
Section: Edl Modellmentioning
confidence: 99%
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“…The medium of concern here is the structured ionospheric plasma. Because this plasma is a frequency-dependent (dispersive) dielectric medium, it is necessary to extend the usual FDTD methodology, and this was done by Nickisch and Franke [1992]. The method has been Copyright 2001 by the American Geophysical Union.…”
Section: Introductionmentioning
confidence: 99%