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August 16, 2021, 05:50 |
Finite Volume Method
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#1 |
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Mercurial
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Hi guys,
I'm begginer to understand FVM, What is the different between the fluid element and fluid particle; rate and net rate ? Thanks |
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August 16, 2021, 15:33 |
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#2 |
Senior Member
Lucky
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It's called net rate of flow because stuff can flow in and out of a fluid element at the same time in different places. But the overall amount determines whether the phi in the fluid element increases or decreases.
I'm not a fan of this word equation. Fluid element and particle are usually synonymous, they mean the same thing. It's better to just read the math symbols in this case. If you need help understanding the meaning of each term in the equation ask. Otherwise, don't get stuck on trying to grasp this poor presentation. I can't even see the equation but the fluid particle in this context refers to the material volume. |
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August 16, 2021, 15:44 |
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#3 |
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Filippo Maria Denaro
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August 17, 2021, 00:03 |
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#4 |
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Mercurial
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August 17, 2021, 02:15 |
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#5 | |
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Mercurial
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Quote:
For pressure-velocity coupling, why have we 4 equations (1 continuity and 3 momentum) and 4 unknows (1 p, 3 velocity) instead of 6 equations and 6 unknows (3 pressure xyz and 3 velocity uvw)? Thanks. |
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August 17, 2021, 04:13 |
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#6 | |
Senior Member
Lucky
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Quote:
Continuity is a scalar equation, so always it is 1 equation. Energy equation is also a scalar equation in temperature (or internal energy or enthalpy). There isn't a x,y,z component for a scalar. Pressure is also a scalar (1 variable). So for p-v coupling, you will have either 2 equations (continuity & momentum) in 2 unknowns (pressure and your velocity vector) or 4 equations (continuity + 3 momentum equations) in 4 unknowns (pressure, & 3 velocity components). You never have 6, there is no such thing as pressure in x,y,z direction. |
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August 17, 2021, 04:37 |
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#7 | |
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Mercurial
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Quote:
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August 17, 2021, 04:38 |
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#8 |
Senior Member
Filippo Maria Denaro
Join Date: Jul 2010
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Unfortunately, that textbook starts the presentation in a misleading way. They present first the differential equations while I suggest to start from the physical law expressed by the Reynolds theorem. The link between the lagrangian and eulerian representation is in the Eq.(2.40) you should consider as the starting equation for the FVM. Conservation principle, concept of flux and flow rates require the integral formulation. Have a look also to the textbook of Ferziger, Peric, Street. |
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