# User:Tohline/Appendix/Ramblings/RiemannB74C692

(Difference between revisions)
 Revision as of 13:30, 29 May 2020 (view source)Tohline (Talk | contribs)← Older edit Revision as of 19:10, 29 May 2020 (view source)Tohline (Talk | contribs) (→Another S-type Example b74c692)Newer edit → Line 70: Line 70: The subscript "EFE" on Ω and λ means that the relevant frequency is given in units that have been adopted in [[[User:Tohline/Appendix/References#EFE|EFE]]], that is, in units of $~[\pi G\rho]^{1 / 2}$.  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 §49 (p. 147) of [[[User:Tohline/Appendix/References#EFE|EFE]]]. The subscript "EFE" on Ω and λ means that the relevant frequency is given in units that have been adopted in [[[User:Tohline/Appendix/References#EFE|EFE]]], that is, in units of $~[\pi G\rho]^{1 / 2}$.  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 §49 (p. 147) of [[[User:Tohline/Appendix/References#EFE|EFE]]]. + + ==Coding Steps== + Here we begin with a working model of [[User:Tohline/Appendix/Ramblings/RiemannMeetsOculus#S-Type_Ellipsoid_b41c385|b41c385]] and use incremental changes in the COLLADA-based code to construct a working model of b74c692. + +
+
• Pulling from the earlier modeling subsection titled, [[User:Tohline/Appendix/Ramblings/RiemannMeetsOculus#Final_Touches|Final Touches]] … +
+
• + Final17.dae   TERRIFIC  !: +
Both hands of the clock now continue to cycle smoothly (through 9.126 "hours" = 9h 8m) while the laboratory frame completes 5.0 full spin periods — which will be 5.0 full spins of the ellipsoid as viewed from the inertial frame.  This works in both visualization venues. +
• +
• + Inertial17.dae: +
This is identical to "Final17.dae" except that the system is viewed from the inertial frame of reference.  This works in both visualization venues. +
• +
+
• + +
• Pulling from a different earlier subsection titled, [[User:Tohline/Appendix/Ramblings/RiemannMeetsOculus#Multiple_Lagrangian_Fluid_Elements|Multiple Lagrangian Fluid Elements]] … +
+
• + MultiLagrange23.dae: +
This model shows the motion of nine (small, red cube) Lagrange particles whose motion is confined to the equatorial plane of the Riemann ellipsoid. This nicely illustrates that the volume occupied by a region of fluid remains unchanged as the fluid moves around the ellipsoid.    This works in both visualization venues! +
• +
• + MultiLagrange24.dae: +
This model shows the motion of '''eight''' (small, red cube) Lagrange particles whose motion is confined to the equatorial plane of the Riemann ellipsoid. This actually does a ''worse'' job of illustrating volume conservation than does the 9-particle (MultiLagrange23) model. +
• +
• + MultiLagrange26.dae: +
Here, we set the "nudging" angle of the MidPlane to 1°, and moved the "nudging" angle of the ellipsoid from 5° to 0°.  This appears to work in both visualization venues. +
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+
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# Another S-type Example b74c692

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) = (0.74, 0.692). Other closely related chapters are listed below under the heading, "See Also".

## 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 $~\frac{b}{a} = 0.74$ Figure 1b $~\frac{c}{a} = 0.692$ Direct Adjoint $~\Omega_\mathrm{EFE} = 0.638747$ $~\Omega_\mathrm{EFE} = - 0.217773$ $~\lambda_\mathrm{EFE} = 0.217773$ $~\lambda_\mathrm{EFE} = - 0.638747$

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 $~[\pi G\rho]^{1 / 2}$. 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 b41c385 and use incremental changes in the COLLADA-based code to construct a working model of b74c692.

• Pulling from the earlier modeling subsection titled, Final Touches
• Final17.dae   TERRIFIC  !:
Both hands of the clock now continue to cycle smoothly (through 9.126 "hours" = 9h 8m) while the laboratory frame completes 5.0 full spin periods — which will be 5.0 full spins of the ellipsoid as viewed from the inertial frame. This works in both visualization venues.
• Inertial17.dae:
This is identical to "Final17.dae" except that the system is viewed from the inertial frame of reference. This works in both visualization venues.
• Pulling from a different earlier subsection titled, Multiple Lagrangian Fluid Elements
• MultiLagrange23.dae:
This model shows the motion of nine (small, red cube) Lagrange particles whose motion is confined to the equatorial plane of the Riemann ellipsoid. This nicely illustrates that the volume occupied by a region of fluid remains unchanged as the fluid moves around the ellipsoid.   This works in both visualization venues!
• MultiLagrange24.dae:
This model shows the motion of eight (small, red cube) Lagrange particles whose motion is confined to the equatorial plane of the Riemann ellipsoid. This actually does a worse job of illustrating volume conservation than does the 9-particle (MultiLagrange23) model.
• MultiLagrange26.dae:
Here, we set the "nudging" angle of the MidPlane to 1°, and moved the "nudging" angle of the ellipsoid from 5° to 0°. This appears to work in both visualization venues.

b74c692DI.dae [Direct Inertial Frame]    …     a COLLADA code containing nnnn lines of <xml>-formatted ASCII text

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


b74c692DRot.dae [Direct Rotating Frame]    …     a COLLADA code containing nnnn lines of <xml>-formatted ASCII text

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


b74c692AI.dae [Adjunct Inertial Frame]    …     a COLLADA code containing nnnn lines of <xml>-formatted ASCII text

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


b74c692ARot.dae [Adjunct Rotating Frame]    …     a COLLADA code containing nnnn lines of <xml>-formatted ASCII text

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