Difference between revisions of "User:Tohline/PGE/Hybrid Scheme"

From VistrailsWiki
Jump to navigation Jump to search
(Begin new page to present Jay Call's hybrid scheme)
 
(Begin page that discusses hybrid scheme)
Line 1: Line 1:
=Euler Equation=
=Hybrid Scheme=
{{LSU_HBook_header}}
{{LSU_HBook_header}}
==Traditional Eulerian Representation (Review)==
==Traditional Eulerian Representation (Review)==
Line 28: Line 28:
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 &amp; CartNon==
Consider the familiar case of transport of


=Related Discussions=
=Related Discussions=

Revision as of 00:47, 26 February 2014

Hybrid Scheme

Whitworth's (1981) Isothermal Free-Energy Surface
|   Tiled Menu   |   Tables of Content   |  Banner Video   |  Tohline Home Page   |

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


Whitworth's (1981) Isothermal Free-Energy Surface

© 2014 - 2021 by Joel E. Tohline
|   H_Book Home   |   YouTube   |
Appendices: | Equations | Variables | References | Ramblings | Images | myphys.lsu | ADS |
Recommended citation:   Tohline, Joel E. (2021), The Structure, Stability, & Dynamics of Self-Gravitating Fluids, a (MediaWiki-based) Vistrails.org publication, https://www.vistrails.org/index.php/User:Tohline/citation