1969
DOI: 10.1007/bf01376219
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Homomorphisms of some function lattices

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Cited by 5 publications
(5 citation statements)
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“…The fluid pressurep must therefore be somewhat smaller inside the tube (where B =+ 0) than just outside, the same is therefore true of the density, and the tube tends to rise, This mechanism of 'magnetic buoyancy' was pointed out by Parker (1955) and Jensen (1955)) and has subsequently been much discussed in connexion with the dynamics of the upper layers of the sun (see, for example, Parker 1976). Note that our assumption here of infinitely fast diffusion of heat has filtered out conventional buoyancy forces that would otherwise arise owing to the vertical entropy gradient.…”
Section: Introductionmentioning
confidence: 97%
“…The fluid pressurep must therefore be somewhat smaller inside the tube (where B =+ 0) than just outside, the same is therefore true of the density, and the tube tends to rise, This mechanism of 'magnetic buoyancy' was pointed out by Parker (1955) and Jensen (1955)) and has subsequently been much discussed in connexion with the dynamics of the upper layers of the sun (see, for example, Parker 1976). Note that our assumption here of infinitely fast diffusion of heat has filtered out conventional buoyancy forces that would otherwise arise owing to the vertical entropy gradient.…”
Section: Introductionmentioning
confidence: 97%
“…Cowling (1946) envisaged flux tubes running as girdles around the Sun and suggested that loops were carried upwards by convection to emerge as sunspot pairs. Soon after, the idea of magnetic buoyancy was put forward as the mechanism by which flux tubes journey from the base of the convection zone to the photosphere (Parker 1955;Jensen 1955). Parker demonstrated that an isolated magnetic flux tube in a stratified plasma under gravity must be buoyant, provided that it is close to thermal equilibrium with its surroundings.…”
Section: Introductionmentioning
confidence: 99%
“…The preceding Proposition is a reformulation of Theorem 3.1 from [8] (see also Lemma 1.1 in [12]) stated for semi-affine lattices. Its proof is the same as that in [9] (Proposition 2.7)-unlike the proof in [8] no ultrafilters are used.…”
Section: Proposition 3 the Functors C And X Are Adjointmentioning
confidence: 92%