Difference between revisions of "User:Tohline/Appendix/Ramblings/RiemannB28C256"

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The subscript "EFE" on &Omega; and &lambda; means that the relevant frequency is given in units that have been adopted in [<b>[[User:Tohline/Appendix/References#EFE|<font color="red">EFE</font>]]</b>], that is, in units of <math>~[\pi G\rho]^{1 / 2}</math>.  In Figure 1a, the solid purple circular marker (where the pair of purple lines cross) identifies the location of this model in the "c/a versus b/a" diagram that appears as Figure 2 on p. 902 of [http://adsabs.harvard.edu/abs/1965ApJ...142..890C S. Chandrasekhar (1965)]; essentially the same diagram appears in &sect;49 (p. 147) of [<b>[[User:Tohline/Appendix/References#EFE|<font color="red">EFE</font>]]</b>].
The subscript "EFE" on &Omega; and &lambda; means that the relevant frequency is given in units that have been adopted in [<b>[[User:Tohline/Appendix/References#EFE|<font color="red">EFE</font>]]</b>], that is, in units of <math>~[\pi G\rho]^{1 / 2}</math>.  In Figure 1a, the solid purple circular marker (where the pair of purple lines cross) identifies the location of this model in the "c/a versus b/a" diagram that appears as Figure 2 on p. 902 of [http://adsabs.harvard.edu/abs/1965ApJ...142..890C S. Chandrasekhar (1965)]; essentially the same diagram appears in &sect;49 (p. 147) of [<b>[[User:Tohline/Appendix/References#EFE|<font color="red">EFE</font>]]</b>].
==Coding Steps==
Here we begin with a working model of [[User:Tohline/Appendix/Ramblings/RiemannB74C692#Another_S-type_Example_b74c692|b74c692]] and use incremental changes in the COLLADA-based code to construct a working model of b90c333.
<ul>
  <li>This pair of starting models has been copied from the successful modeling of Riemann S-type ellipsoids that have (b/a, c/a) = (0.74, 0.692)</li>
  <ul>
  <li>Inertial Frame:  <font color="lightgreen">[KEEP]</font> InertialB74C692aa.dae [02 May 2020]</li>
  <li>Rotating Frame:  <font color="lightgreen">[KEEP]</font> TestMulti74.dae [02 June 2020]</li>
  </ul>
  <li><font color="darkgreen"><b>FastRot75.dae</b></font>
<br />Identical to <b>TestMulti74.dae</b> except wall-mounted labeling has been changed to reflect new values of b/a and c/a.
  </li>
  <li><font color="darkgreen"><b>FastRot76.dae</b></font>
<br />Inserted correct surface geometry of this rapidly rotating Riemann ellipsoid.  <font color="red">This works in both visualization venues</font>.
  </li>
  <li><font color="darkgreen"><b>FastRot78.dae</b></font>
<br />All the animation elements have been inserted and debugged, but as if internal fluid motion is regrograde (clockwise).  Need to flip the fluid motion so that it is prograde (counter-clockwise) even in the rotating frame of reference.
  </li>
  <li><font color="darkgreen"><b>FastRot79.dae</b></font>
<br />All the animation elements have been inserted and debugged, with internal fluid correctly moving prograde (counter-clockwise) even in the rotating frame of reference.  <font color="red">This works in both visualization venues</font>.
  </li>
  <li><font color="darkgreen"><b>FastInertial80.dae</b></font>
<br />Test.
  </li>
</ul>
===Best b90c333 Models===
The example models created for display in the Oculus Rift S are the following:
<ol>
  <li>Inertial Frame:  <font color="lightgreen">[KEEP]</font> FastInertial80.dae [04 June 2020]  </li>
  <li>Rotating Frame:  <font color="lightgreen">[KEEP]</font> FastRot79.dae [04 June 2020] </li>
</ol>
==COLLADA Model Files==
===''Direct'' Configurations===
<div align="center" id="Scroll1">
<b>b90c333DI.dae</b> [''Direct'' Inertial Frame]&nbsp; &nbsp; &hellip; &nbsp; &nbsp; a COLLADA code containing 9198 lines of <xml>-formatted ASCII text
<br />Original filename used above: FastInertial80.dae
</div>
<div style="height: 250px; width: 100%; overflow: scroll;">
<pre>
<?xml version="1.0" encoding="UTF-8" standalone="no" ?>
</pre>
</div>


=See Also=
=See Also=

Revision as of 22:16, 4 June 2020

Another S-type Example b28c256

This chapter is an extension of the chapter we have titled, "Riemann Meets COLLADA & Oculus Rift S." In that chapter we used as our first example of a Riemann S-type ellipsoid the model with parameters, (b/a, c/a) = (0.41, 0.385). Here we construct a model with parameters, (b/a, c/a) = (0.28, 0.256). Other closely related chapters are listed below under the heading, "See Also".

Whitworth's (1981) Isothermal Free-Energy Surface
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Key Physical Parameters

The model that we have chosen to use in our second successful construction of a COLLADA-based, 3D and interactive animation has the following properties; this model has been selected from Table 2 of our accompanying discussion of Riemann S-type ellipsoids:

Figure 1a
EFE Parameter Space

 

<math>~\frac{b}{a} = 0.28</math>

 

Figure 1b
EFE Model b28c256

<math>~\frac{c}{a} = 0.256</math>

Direct

 

Adjoint

<math>~\Omega_\mathrm{EFE} = 0.456676</math>

<math>~\Omega_\mathrm{EFE} = - 0.020692</math>

<math>~\lambda_\mathrm{EFE} = 0.020692</math>

<math>~\lambda_\mathrm{EFE} = - 0.456676</math>

The subscript "EFE" on Ω and λ means that the relevant frequency is given in units that have been adopted in [EFE], that is, in units of <math>~[\pi G\rho]^{1 / 2}</math>. In Figure 1a, the solid purple circular marker (where the pair of purple lines cross) identifies the location of this model in the "c/a versus b/a" diagram that appears as Figure 2 on p. 902 of S. Chandrasekhar (1965); essentially the same diagram appears in §49 (p. 147) of [EFE].

Coding Steps

Here we begin with a working model of b74c692 and use incremental changes in the COLLADA-based code to construct a working model of b90c333.

  • This pair of starting models has been copied from the successful modeling of Riemann S-type ellipsoids that have (b/a, c/a) = (0.74, 0.692)
    • Inertial Frame: [KEEP] InertialB74C692aa.dae [02 May 2020]
    • Rotating Frame: [KEEP] TestMulti74.dae [02 June 2020]
  • FastRot75.dae
    Identical to TestMulti74.dae except wall-mounted labeling has been changed to reflect new values of b/a and c/a.
  • FastRot76.dae
    Inserted correct surface geometry of this rapidly rotating Riemann ellipsoid. This works in both visualization venues.
  • FastRot78.dae
    All the animation elements have been inserted and debugged, but as if internal fluid motion is regrograde (clockwise). Need to flip the fluid motion so that it is prograde (counter-clockwise) even in the rotating frame of reference.
  • FastRot79.dae
    All the animation elements have been inserted and debugged, with internal fluid correctly moving prograde (counter-clockwise) even in the rotating frame of reference. This works in both visualization venues.
  • FastInertial80.dae
    Test.

Best b90c333 Models

The example models created for display in the Oculus Rift S are the following:

  1. Inertial Frame: [KEEP] FastInertial80.dae [04 June 2020]
  2. Rotating Frame: [KEEP] FastRot79.dae [04 June 2020]


COLLADA Model Files

Direct Configurations

b90c333DI.dae [Direct Inertial Frame]    …     a COLLADA code containing 9198 lines of <xml>-formatted ASCII text
Original filename used above: FastInertial80.dae

<?xml version="1.0" encoding="UTF-8" standalone="no" ?>


See Also


Whitworth's (1981) Isothermal Free-Energy Surface

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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