1997
DOI: 10.1080/10407799708914996
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An Equal-Order Velocity-Pressure Algorithm for Incompressible Thermal Flows, Part 1: Formulation

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Cited by 38 publications
(35 citation statements)
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“…and u 0 , u being subject to the restriction u 0 ·n = u (0, x)·n on (9) From the continuity equation and the divergence theorem, it follows the condition of global mass…”
Section: The Governing Equationsmentioning
confidence: 98%
“…and u 0 , u being subject to the restriction u 0 ·n = u (0, x)·n on (9) From the continuity equation and the divergence theorem, it follows the condition of global mass…”
Section: The Governing Equationsmentioning
confidence: 98%
“…When droplets cover a large part of the surface coalescence or fusion will occur, but since coalescence preserves volume a release of free surface follows, allowing for new nucleation. This leads to self similarity in the droplet pattern, with a stabilization of the value of the surface coverage close to the one corresponding 16 to close packing of small droplets. Assuming such self similar droplets distribution on the interface, the area ratios in Eq.…”
Section: Droplet Condensationmentioning
confidence: 99%
“…(1)) are solved by an in-house finite element code [16], which allows for the solution of the mass transfer equation (2) as well [6,7]. The solid domain conduction problem (Eq.…”
Section: Methodsmentioning
confidence: 99%
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“…The reason for this is due to the error involved in the application of boundary conditions for pressure. Nonino & Comini (1997) developed an algorithm to solve transient Stokes equations which got rid of the error associated with pressure boundary conditions. Based on the algorithm for transient Stokes equations, Codina & Blasco (1997) developed a fractionalstep algorithm to solve steady Stokes equations.…”
Section: Stage 1: Suspension Phase Equationsmentioning
confidence: 99%