Difference between revisions of "User:Tohline/PGE/Hybrid Scheme"
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==Traditional Eulerian Representation (Review)== | ==Traditional Eulerian Representation (Review)== | ||
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The second term on the left-hand-side of this last expression represents the divergence of the "dyadic product" of the vector momentum density ({{User:Tohline/Math/VAR_Density01}}{{User:Tohline/Math/VAR_VelocityVector01}}) and the velocity vector {{User:Tohline/Math/VAR_VelocityVector01}} and is sometimes written as, <math>\nabla\cdot [(\rho \vec{v}) \otimes \vec{v}]</math>. | The second term on the left-hand-side of this last expression represents the divergence of the "dyadic product" of the vector momentum density ({{User:Tohline/Math/VAR_Density01}}{{User:Tohline/Math/VAR_VelocityVector01}}) and the velocity vector {{User:Tohline/Math/VAR_VelocityVector01}} and is sometimes written as, <math>\nabla\cdot [(\rho \vec{v}) \otimes \vec{v}]</math>. | ||
=Component Forms= | |||
Let's split the vector Euler equation into its three scalar components; various examples are identified in Table 1. | |||
<div align="center"> | |||
<table border="1" cellpadding="5"> | |||
<tr> | |||
<th align="center"> | |||
Example # | |||
</th> | |||
<th align="center"> | |||
Grid Basis | |||
</th> | |||
<th align="center"> | |||
Grid Rotation | |||
</th> | |||
<th align="center"> | |||
Momentum Basis | |||
</th> | |||
<th align="center"> | |||
Momentum Frame | |||
</th> | |||
</tr> | |||
<tr> | |||
<td align="center"> | |||
1 | |||
</td> | |||
<td align="center"> | |||
Cartesian | |||
</td> | |||
<td align="center"> | |||
Nonrotating | |||
</td> | |||
<td align="center"> | |||
Cartesian | |||
</td> | |||
<td align="center"> | |||
Inertial | |||
</td> | |||
</tr> | |||
<tr> | |||
<td align="center"> | |||
2 | |||
</td> | |||
<td align="center"> | |||
Cylindrical | |||
</td> | |||
<td align="center"> | |||
Nonrotating | |||
</td> | |||
<td align="center"> | |||
Cylindrical | |||
</td> | |||
<td align="center"> | |||
Inertial | |||
</td> | |||
</tr> | |||
</table> | |||
</div> | |||
===CartNon & CartNon== | |||
Consider the familiar case of transport of | |||
=Related Discussions= | =Related Discussions= |
Revision as of 00:47, 26 February 2014
Hybrid Scheme
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Traditional Eulerian Representation (Review)
Here we review the traditional Eulerian representation of the Euler Equation, as has been discussed in detail earlier.
in terms of velocity:
The so-called "Eulerian form" of the Euler equation can be straightforwardly derived from the standard Lagrangian representation to obtain,
Eulerian Representation
of the Euler Equation,
<math>~\frac{\partial\vec{v}}{\partial t} + (\vec{v}\cdot \nabla) \vec{v}= - \frac{1}{\rho} \nabla P - \nabla \Phi</math>
in terms of momentum density:
Also, we can multiply this expression through by <math>~\rho</math> and combine it with the continuity equation to derive what is commonly referred to as the,
Conservative Form
of the Euler Equation,
<math>~\frac{\partial(\rho\vec{v})}{\partial t} + \nabla\cdot [(\rho\vec{v})\vec{v}]= - \nabla P - \rho \nabla \Phi</math>
The second term on the left-hand-side of this last expression represents the divergence of the "dyadic product" of the vector momentum density (<math>~\rho</math><math>~\vec{v}</math>) and the velocity vector <math>~\vec{v}</math> and is sometimes written as, <math>\nabla\cdot [(\rho \vec{v}) \otimes \vec{v}]</math>.
Component Forms
Let's split the vector Euler equation into its three scalar components; various examples are identified in Table 1.
Example # |
Grid Basis |
Grid Rotation |
Momentum Basis |
Momentum Frame |
---|---|---|---|---|
1 |
Cartesian |
Nonrotating |
Cartesian |
Inertial |
2 |
Cylindrical |
Nonrotating |
Cylindrical |
Inertial |
=CartNon & CartNon
Consider the familiar case of transport of
Related Discussions
- Euler equation viewed from a rotating frame of reference or Main Page.
- An earlier draft of this "Euler equation" presentation.
© 2014 - 2021 by Joel E. Tohline |