1963
DOI: 10.21236/ad0408261
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The Electrical, Structural and Topographical Characteristics of Arctic Sea Ice. Volume 1

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Cited by 1 publication
(2 citation statements)
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“…The electrical properties of sea ice are best understood by considering first the pure ice matrix and then the influence of impurities. Due to the permanent dipole moment of the water molecules, chemically pure ice is a lossy dielectric (Mathews and Clarke, 1963) or a partially conducting medium. The dielectric relaxation behaviour of pure ice can be described by a Debye dispersion with a single relaxation time which varies with temperature (Addison, 1969).…”
Section: Electricalmentioning
confidence: 99%
See 1 more Smart Citation
“…The electrical properties of sea ice are best understood by considering first the pure ice matrix and then the influence of impurities. Due to the permanent dipole moment of the water molecules, chemically pure ice is a lossy dielectric (Mathews and Clarke, 1963) or a partially conducting medium. The dielectric relaxation behaviour of pure ice can be described by a Debye dispersion with a single relaxation time which varies with temperature (Addison, 1969).…”
Section: Electricalmentioning
confidence: 99%
“…In addition to these observed temperature effects, the brine inclusions can migrate vertically, under the influence of changing thermal gradients, to regions of higher temperature (to the bottom of the ice cover in winter and the top in summer) (Mathews and Clarke, 1963). Because of diffusion the salinity of brine within an inclusion will be uniform.…”
Section: Evolutionmentioning
confidence: 99%