Difference between revisions of "User:Tohline/PGE/ConservingMass"
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=Continuity Equation= | |||
==Various Forms== | |||
Among the [http://www.vistrails.org/index.php/User:Tohline/PGE principal governing equations] we have included the | Among the [http://www.vistrails.org/index.php/User:Tohline/PGE principal governing equations] we have included the | ||
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By replacing the Lagrangian time derivative <math>d\rho/dt</math> in the first expression by its Eulerian counterpart (see the linked [http://en.wikipedia.org/wiki/Material_derivative Wikipedia discussion], and references therein, to understand how the | By replacing the so-called Lagrangian (or "material") time derivative <math>d\rho/dt</math> in the first expression by its Eulerian counterpart (see the linked [http://en.wikipedia.org/wiki/Material_derivative Wikipedia discussion], and references therein, to understand how the Lagrangian and Eulerian descriptions of fluid motion differ from one another conceptually as well as how to mathematically transform from one description to the other), we directly obtain what is commonly referred to as the | ||
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<span id="ConservingMass: | <span id="ConservingMass:Eulerian"><font color="#770000">'''Eulerian Representation'''</font></span><br /> | ||
or<br /> | |||
<span id="ConservingMass:Conservative"><font color="#770000">'''Conservative Form'''</font></span><br /> | |||
of the Continuity Equation, | of the Continuity Equation, | ||
{{User:Tohline/Math/EQ_Continuity02}} | {{User:Tohline/Math/EQ_Continuity02}} | ||
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==Time-independent Behavior== | |||
===Lagrangian Frame of Reference=== | |||
If you are riding along with a fluid element — viewing the system from a ''Lagrangian'' frame of reference — the mass density {{User:Tohline/Math/VAR_Density01}} of your fluid element will, by definition, remain unchanged over time if, | |||
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<math>\frac{d\rho}{dt} = 0</math> . | |||
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From the above "Standard Lagrangian Representation" of the continuity equation, this condition also implies that, | |||
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<math>\nabla\cdot \vec{v} = 0</math> . | |||
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Looking at it a different way, if while riding along with a fluid element you move through a region of space where <math>\nabla\cdot \vec{v} = 0</math>, your mass density will remain unchanged as you move through this region. | |||
===Eulerian Frame of Reference=== | |||
On the other hand, if you are standing at a fixed location in your coordinate frame watching the fluid flow past you — viewing the system from an ''Eulerian'' frame of reference — the mass density of the fluid at your location in space will, by definition, always be the same if, | |||
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<math>\frac{\partial\rho}{\partial t} = 0</math> . | |||
</div> | |||
From the above "Eulerian Representation" of the continuity equation, this condition also implies that, | |||
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<math>\nabla\cdot (\rho \vec{v}) = 0</math> . | |||
</div> | </div> | ||
{{LSU_HBook_footer}} | {{LSU_HBook_footer}} | ||
Revision as of 18:18, 31 January 2010
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Continuity Equation
Various Forms
Among the principal governing equations we have included the
Standard Lagrangian Representation
of the Continuity Equation,
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<math>\frac{d\rho}{dt} + \rho \nabla \cdot \vec{v} = 0</math> |
Note that this equation also may be written in the form,
<math> \frac{d \ln \rho}{dt} = - \nabla\cdot \vec{v} \, . </math>
By replacing the so-called Lagrangian (or "material") time derivative <math>d\rho/dt</math> in the first expression by its Eulerian counterpart (see the linked Wikipedia discussion, and references therein, to understand how the Lagrangian and Eulerian descriptions of fluid motion differ from one another conceptually as well as how to mathematically transform from one description to the other), we directly obtain what is commonly referred to as the
Eulerian Representation
or
Conservative Form
of the Continuity Equation,
<math>~\frac{\partial\rho}{\partial t} + \nabla \cdot (\rho \vec{v}) = 0</math>
Time-independent Behavior
Lagrangian Frame of Reference
If you are riding along with a fluid element — viewing the system from a Lagrangian frame of reference — the mass density <math>~\rho</math> of your fluid element will, by definition, remain unchanged over time if,
<math>\frac{d\rho}{dt} = 0</math> .
From the above "Standard Lagrangian Representation" of the continuity equation, this condition also implies that,
<math>\nabla\cdot \vec{v} = 0</math> .
Looking at it a different way, if while riding along with a fluid element you move through a region of space where <math>\nabla\cdot \vec{v} = 0</math>, your mass density will remain unchanged as you move through this region.
Eulerian Frame of Reference
On the other hand, if you are standing at a fixed location in your coordinate frame watching the fluid flow past you — viewing the system from an Eulerian frame of reference — the mass density of the fluid at your location in space will, by definition, always be the same if,
<math>\frac{\partial\rho}{\partial t} = 0</math> .
From the above "Eulerian Representation" of the continuity equation, this condition also implies that,
<math>\nabla\cdot (\rho \vec{v}) = 0</math> .
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