ThreeDimensionalConfigurations/DescriptionOfRiemannTypeI: Difference between revisions

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As a consequence &#8212; see [[ThreeDimensionalConfigurations/RiemannTypeI#Try_Again|an accompanying discussion]] for details &#8212; the values of other parameters are &hellip;
As a consequence &#8212; see [[ThreeDimensionalConfigurations/RiemannTypeI#Try_Again|an accompanying discussion]] (alternatively, [[ThreeDimensionalConfigurations/ChallengesPt6#Are_Orbits_Exact_Circles|ChallengesPt6]]) for details &#8212; the values of other parameters are &hellip;


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<math>
<math>
\biggl[ \frac{a^2}{a^2 + c^2} \biggr] \frac{\zeta_2}{\Lambda}  
\biggl[ \frac{a^2}{a^2 + c^2} \biggr] \frac{\zeta_2}{\Lambda}  
=
- \frac{b^2 \sin\theta}{(c^2\cos^2\theta + b^2\sin^2\theta)}
</math>
</math>
   </td>
   </td>

Revision as of 18:58, 16 February 2022


Description of Riemann Type I Ellipsoids

Type I
Riemann
Ellipsoids

Example Equilibrium Model

This particular set of seven key parameters has been drawn from [EFE] Chapter 7, Table XIII (p. 170). The tabular layout presented here, also appears in a related discussion labeled, Challenges Pt. 2.

a=a1=1
b=a2=1.25
c=a3=0.4703
Ω2=0.3639
Ω3=0.6633
ζ2=−2.2794
ζ3=−1.9637

As a consequence — see an accompanying discussion (alternatively, ChallengesPt6) for details — the values of other parameters are …

    Example Values

tan⁡θ

=

−ζ2ζ3[a2+b2a2+c2]c2b2=−0.344793

       

θ=

−19.0238∘

Λ

≡

[a2a2+b2]ζ3cos⁡θ−[a2a2+c2]ζ2sin⁡θ

       

Λ=

−1.332892

y0z0

=

[a2a2+c2]ζ2Λ=−b2sin⁡θ(c2cos2θ+b2sin2θ)

       

y0z0=

+1.400377

xmaxymax

=

{Λ[a2+b2b2]cos⁡θζ3}1/2

       

    xmaxymax=

+1.025854

φ˙

=

{Λ[b2a2+b2]ζ3cos⁡θ}1/2

       

φ˙=

+1.299300

See Also

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