Appendix/Ramblings/51BiPolytropeStability/NoAnalytic

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Do Not Confine Search to Analytic Eigenvector

Overview

STEP01:
Develop an algorithm (for Excel) that numerically integrates the LAWEs from the center to the surface of a (nc,ne)=(5,1) bipolytrope, for an arbitrary specification of the three parameters:   μe/μc,ξi, and σc2.

  • Enforce the proper interface matching condition(s) at the interface location, ξi.
  • Note that in general, for an arbitrarily chosen set of the three parameter values, the resulting surface displacement function will not match the desired boundary condition.

STEP02:
Fix your chosen value of the parameter pair, (μe/μc,ξi), and vary σc2 until the proper surface boundary condition is realized.

  • In an accompanying discussion, we claim to have identified at what point along various μe/μc sequences the fundamental mode of radial oscillation becomes unstable — that is, when σc2=0. For a given choice of μe/μc, it would be wise to begin our eigenvector search at a value of ξi<[ξi]FM, as specified in the following table:
    Marginally Unstable Fundamental Modes
    μeμc [ξi]FM
    1 1.6686460157
    12 2.27925811317
    0.345 2.560146865247
    13 2.582007485476
    0.309 2.6274239687695
    14 2.7357711469398
    See orange-colored triangular markers in the associated Figure 4
  • Keep steadily raising the value of the interface location until you find the 1st overtone mode; a related discussion (with animation) shows the results of this type of search in the context of isolated n = 1 polytropes. Our expectation is that, if this mode is unstable, the model will coincide with the turning point along the equilibrium sequence and its eigenvector will essentially overlap with the eigenvector found using the B-KB74 conjecture. At the same time, the square-of-the-eigenfrequency for the fundamental mode will be very negative.

See Also

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