Editing Appendix/Ramblings/ForOuShangli (section)

=Catalog of Local 3D Model Files <font size="-1">(cannot be downloaded)</font>=
==3Dviewers==
===AutoRiemann===

<ul>
  <li>
Trial.Ou_b28c256<br />
''Generally speaking ...'' Translucent surface; one Lagrangian (red surface arrow) fluid element; no axis arrow; NO WALL LABELs.
  <ul>
    <li>
<font color="maroon">Ou_b28c256.Dir.Inertial.dae</font> (12/01/2019)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">Ou_b28c256.Dir.Rot.dae</font> (12/01/2019)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">Ou_b28c256.Adj.Inertial.dae</font> (12/01/2019)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">Ou_b28c256.Adj.Rot.dae</font> (12/01/2019)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>

<ul>
  <li>
Cylinder<br />
''Generally speaking ...'' Translucent surface; one Lagrangian (red surface arrow) fluid element; no axis arrow; PROBLEM RESETING CLOCK. 
  <ul>
    <li>
<font color="maroon">Dir.Inertial_b28c256.labeled.dae</font> (12/22/2019)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">Dir.Rot_b28c256.labeled.dae</font> (12/22/2019)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>

<ul>
  <li>
BESTmodels<br />
''Generally speaking ...'' Translucent surface; six Lagrangian (red arrow markers) fluid elements. 
  <ul>
    <li>
<font color="maroon">b28c256/b28c256.DI.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">b28c256/b28c256.DRot.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">b28c256/b28c256.AI.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">b28c256/b28c256.ARot.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
&nbsp;
<hr>
&nbsp;
    <li>
<font color="maroon">b41c385/b41c385.DI.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.41~~~~~c/a = 0.385</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">b41c385/b41c385.DRot.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.41 ~~~~~c/a = 0.385</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">b41c385/b41c385.AI.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.41 ~~~~~c/a = 0.385</math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon">b41c385/b41c385.ARot.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.41 ~~~~~c/a = 0.385</math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
&nbsp;
<hr>
&nbsp;
    <li>
<font color="maroon">b74c692/b74c692.DI.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.74~~~~~c/a = 0.692</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon"> b74c692/b74c692.DRot.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.74 ~~~~~c/a = 0.692 </math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon"> b74c692/b74c692.AI.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.74 ~~~~~c/a = 0.692 </math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon"> b74c692/b74c692.ARot.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.74 ~~~~~c/a = 0.692 </math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
&nbsp;
<hr>
&nbsp;
    <li>
<font color="maroon">b90c333/b90c333.DI.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.90~~~~~c/a = 0.333</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon"> b90c333/b90c333.DRot.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.90 ~~~~~c/a = 0.333 </math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon"> b90c333/b90c333.AI.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.90 ~~~~~c/a = 0.333 </math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
    <li>
<font color="maroon"> b90c333/b90c333.ARot.dae</font> (01/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.90 ~~~~~c/a = 0.333 </math><br />'''<font color="red">ADJOINT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>

<ul>
  <li>
TypeI<br />
Translucent surface; just '''Type I tilted''' figure motion (no Lagrangian fluid elements). 
  <ul>
    <li>
<font color="maroon">TypeIa10.GREAT.dae</font> (01/04/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 1.25~~~~~c/a = 0.470</math><br />'''<font color="red">DIRECT figure</font>''' (only) motion - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>

<ul>
  <li>
TypeI/Lagrange<br />
Depicts motion of (3) Lagrangian fluid elements across an opaque surface; no figure motion; three separate, tilted fluid orbits are identified by small yellow markers. 
  <ul>
    <li>
<font color="maroon">TL15.lagrange.dae</font> (01/26/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 1.25~~~~~c/a = 0.470</math><br />'''<font color="red">LAGRANGIAN element</font>''' (only) motion - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>

==Lenovo==

===KhronosGroup's COLLADA_to_gltf/COLLADA2GLTF-v2===

<ul>
  <li>
ModelsB41C385<br />
Fundamentally this model is identical to the one developed earlier (and [[#b41c385|presented above]]) that shows how the ''DIRECT'' flow version of model "b41c385" appears when viewed from either the inertial or rotating reference frame: The ellipsoidal surface is purple [either translucent or opaque, as indicated]; the equatorial plane is identified by a series of small yellow markers; and 9 red markers depict the (slow, retrograde) Lagrangian motion of fluid elements that lie in the equatorial plane.  
  <ul>
    <li>
<font color="maroon">MultiFluidElements/MultiLagrange26.dae</font> [translucent purple] (05/28/2020) and <font color="orange">/output/MultiLagrange26.glb</font> (06/04/2020) &#8212; both files also copied (01/31/2021) to LSU physics website with filename &hellip; COLLADA/b41c385DirRotating.
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.41~~~~~c/a = 0.385</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  <ul>
    <li>
<font color="maroon">InertialFrame/Inertial34.dae</font> [opaque purple] (05/29/2020) and <font color="orange">/output/Inertial34.glb</font> (06/04/2020) &#8212; both files also copied (01/31/2021) to LSU physics website with filename &hellip; COLLADA/b41c385DirInertial.
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.41~~~~~c/a = 0.385</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>

<ul>
  <li>
ModelsB90C333<br />
Fundamentally this model is identical to the one developed earlier (and [[#b90c333|presented above]]) that shows how the ''DIRECT'' flow version of model "b90c333" appears when viewed from either the inertial or a rotating reference frame:  The ellipsoidal surface is purple [either translucent or opaque, as indicated]; the equatorial plane is identified by a series of small yellow markers; and 9 red markers depict the (slow, prograde) Lagrangian motion of fluid elements that lie in the equatorial plane.  
  <ul>
    <li>
<font color="maroon">FastRot79.dae</font>  [translucent purple] (06/03/2020) and <font color="orange">/output/FastRot79.glb</font> (06/04/2020) &#8212; both files also copied (01/31/2021) to LSU physics website with filename &hellip; COLLADA/b90c333DirRotating.
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.90~~~~~c/a = 0.333</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  <ul>
    <li>
<font color="maroon">FastInertial80.dae</font> [opaque purple] (06/03/2020) &#8212; Also available is <font color="orange">../output/FastInertial80.glb</font> (06/04/2020)  &#8212; both files also copied (01/31/2021) to LSU physics website with filename &hellip; COLLADA/b90c333DirInertial.
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.90~~~~~c/a = 0.333</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>

<ul>
  <li>
ModelsB74C692<br />
Fundamentally this model is identical to the one developed earlier (and [[#b74c692|presented above]]) that shows how the ''DIRECT'' flow version of model "b74c692" appears when viewed from the rotating reference frame: The ellipsoidal surface is translucent (purple); the equatorial plane is identified by a series of small yellow markers; and 9 red markers depict the (slow, retrograde) Lagrangian motion of fluid elements that lie in the equatorial plane.  
  <ul>
    <li>
<font color="maroon">TestMulti74.dae</font> (06/03/2020) &#8212; Also available is <font color="orange">../output/TestMulti74.glb</font> (06/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.74~~~~~c/a = 0.692</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  <ul>
    <li>
<font color="maroon">InertialB74C692aa.dae</font> [opaque purple] (06/02/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.74~~~~~c/a = 0.692</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>

<ul>
  <li>
(no subdirectory)<br />
Fundamentally this model is identical to the one developed earlier (and [[#b28c256|presented above]]) that shows how the ''DIRECT'' flow version of model "b28c256" appears when viewed from the inertial reference frame: The ellipsoidal surface is purple [either translucent or opaque, as indicated]; the equatorial plane is identified by a series of small yellow markers; and 9 red markers depict the (very slow, retrograde) Lagrangian motion of fluid elements that lie in the equatorial plane.  
  <ul>
    <li>
<font color="maroon">Pencil94.dae</font> [translucent purple surface] (06/04/2020) and <font color="orange">/output/Pencil94.glb</font> (06/04/2020) &#8212; both files also copied (01/30/2021) to LSU physics website with filename &hellip; COLLADA/b28c256DirRotating.
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">ROTATING</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  <ul>
    <li>
<font color="maroon">PencilInertial96.dae</font> [opaque purple surface] (06/04/2020) and <font color="orange">/output/PencilInertial95.glb</font> (06/04/2020) &#8212; both files also copied (01/30/2021) to LSU physics website with filename &hellip; COLLADA/b28c256DirInertial.
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.28~~~~~c/a = 0.256</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>

==Workfolder==
===Wiki_edits===

<ul>
  <li>
CoordinateSystems<br />
Fundamentally this model is identical to the one developed earlier (and [[#b41c385|presented above]]) that shows how the ''DIRECT'' flow version of model "b41c385" appears when viewed from the inertial reference frame: The ellipsoidal surface is translucent (purple); the equatorial plane is identified by a series of small yellow markers; and a single, red marker depicts the (slow, retrograde) Lagrangian motion of one fluid element that lies in the equatorial plane.  

But here, in addition across the "northern" hemisphere of the ellipsoid, a sequence of small yellow markers is used to identify the location of one <math>~\lambda_3</math> coordinate curve as defined within our so-called [[Appendix/Ramblings/ConcentricEllipsoidalT8Coordinates|"T8" coordinate system]]. 
  <ul>
    <li>
<font color="maroon">Lambda3Curve03.dae</font> (12/26/2020)
<table border="1" cellpadding="8" align="center" width="50%"><tr><td align="left">
<div align="center"><math>~b/a = 0.41~~~~~c/a = 0.385</math><br />'''<font color="red">DIRECT</font>''' flow - as viewed from '''<font color="red">INERTIAL</font>''' frame</div>
</td></tr></table>
    </li>
  </ul>
  </li>
</ul>