2003
DOI: 10.3402/tellusa.v55i3.12097
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Continuity equations as expressions for local balances of masses in cloudy air

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Cited by 15 publications
(15 citation statements)
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“…The use of the full mass‐weighted solution for a system where one wishes to keep a ‘gaseous‐type’ state equation may appear counter‐intuitive. Nevertheless, Wacker and Herbert (2003) make the same recommendation: ‘ In a more detailed framework in which the field balance equations of momentum, energy and entropy of the system are also enclosed, a clear physical preference is seen to exist for the barycentric frame of reference. ’.…”
Section: The Microphysical Schemementioning
confidence: 99%
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“…The use of the full mass‐weighted solution for a system where one wishes to keep a ‘gaseous‐type’ state equation may appear counter‐intuitive. Nevertheless, Wacker and Herbert (2003) make the same recommendation: ‘ In a more detailed framework in which the field balance equations of momentum, energy and entropy of the system are also enclosed, a clear physical preference is seen to exist for the barycentric frame of reference. ’.…”
Section: The Microphysical Schemementioning
confidence: 99%
“…Hence it should be no surprise that the subject of a fully consistent set of multiphase dynamical and thermodynamical equations has recently received substantial attention (e.g. Bannon, 2002; Bryan and Fritsch, 2002; Wacker and Herbert, 2003). This happened although the topic could in fact have been addressed already thirty years ago, following for instance some pioneering work of Hinkelmann (developed and published by Zdunkowski and Bott 2003, in chapter 11 of their textbook).…”
Section: Introductionmentioning
confidence: 99%
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“…Water mass. Wacker and Herbert (2003) and Wacker et al (2006) studied the budget equations for partial densities of a moist atmosphere, particularly incorporating sedimentation fluxes. Following their approach, the budget of any water component x can be formulated as where σ x is the internal production rate, for example, cloud water from a condensation process, and F x is the turbulent mass flux.…”
mentioning
confidence: 99%
“…Taking the impact of water vapour evaporation and precipitation into account, the barycentric velocity is not zero at the surface. Although the Earth surface is impermeable for dry air, the diffusive flux of water vapour J v and the sedimentation flux of the precipitating particles across the Earth surface account for a non‐vanishing barycentric velocity at ground (Wacker and Herbert, 2003): w s = ( J v − P r − P s − P g )/ρ d . Therefore, the turbulent fluxes and precipitation rates of have to be multiplied by a factor of ρ/ρ d , if the lower surface of the CV is equal to the Earth surface.…”
mentioning
confidence: 99%