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==Self-Adjoint Sequences== <table border="1" align="center" width="80%" cellpadding="10"><tr><td align="left"> In an email dated 26 January 2022, Howard asked, "Do you have analytic curves for the lower and upper self-adjoint sequences? Otherwise, do you have very accurate data for the lower and upper self-adjoint sequences?" </td></tr></table> On the same day, I sent the following response to Howard: I have added a subsection to my online chapter discussion of {{ LL96 }} in which I derive an expression whose solution/root should map out the **upper** boundary (x = -1) of the horned-shape region. [[ThreeDimensionalConfigurations/Stability/RiemannEllipsoids#Upper_Boundary|Click here]] to see the entire derivation; this derivation ends with the following recommended strategy: <table border="1" align="center" width="80%" cellpadding="8"><tr><td align="left"> <font color="red">STRATEGY</font> for finding the locus of points that define the upper boundary of the horned-shape region … Set <math>a = 1</math>, and pick a value for <math>0 < b < 1</math>; then, using an iterative technique, vary <math>c</math> until the following expression is satisfied: <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math> \biggl[c^2(a+b)+ ab^2 \biggr] \biggl[ \frac{(b/a) \sin\theta - (c/a)E(\theta,k)}{(1-k^2) \sin^3\theta} \biggr] </math> </td> <td align="center"> <math>=</math> </td> <td align="left"> <math> a^2b + bc(a - b) \biggl[ \frac{F(\theta,k) - E(\theta,k)}{k^2 \sin^3\theta} \biggr] \, .</math> </td> </tr> </table> Choose another value of <math>0 < b < 1</math>, then iterate again to find the value of <math>c</math> that corresponds to this new, chosen value of <math>b</math>. Repeat! </td></tr></table> Related remarks: <ol> <li>I have not actually plugged in numbers -- that is, (b,c) pairs -- to see if it works, but I am pretty confident in the result because the derivation was pretty straightforward. Would you mind trying it out for me, since you have working elliptic integral routines?</li> <li>It would be wise to start by trying to duplicate -- then improve upon -- the set of (b, c) coordinate-pairs that were derived by Chandrasekhar and presented in EFE Table VI (section 48, p. 142).</li> <li>Shortly, I will derive the complementary expression that maps out the "lower" boundary (x = +1).</li> </ol> <!-- <table border="1" align="center" cellpadding="10"><tr><td align="left"> <div align="center"><b>Upper Self-Adjoint</b><br />(Howard's email on 1/27/2022)</div> <div align="center"> [[File:EmailFromHowardJan27Yr2022.png|650px|FromHowardJan27Yr2022]] </div> </td></tr></table> --> On 27 January 2022, Joel added a subsection to the online chapter discussion of {{ LL96 }} in which he derives an expression whose solution/root should map out the **lower** boundary (x = +1) of the horned-shape region. [[ThreeDimensionalConfigurations/Stability/RiemannEllipsoids#Lower_Boundary|Click here]] to see the entire derivation; this derivation ends with the following recommended strategy: <table border="1" align="center" width="80%" cellpadding="8"><tr><td align="left"> <font color="red">STRATEGY</font> for finding the locus of points that define the lower boundary of the horned-shape region … Set <math>a = 1</math>, and pick a value for <math>0 < b < 1</math>; then, using an iterative technique, vary <math>c</math> until the following expression is satisfied: <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math> \biggl[ c^2(a-b)+ ab^2 \biggr] \biggl[ \frac{(b/a) \sin\theta - (c/a)E(\theta,k)}{(1-k^2) \sin^3\theta} \biggr] </math> </td> <td align="center"> <math>=</math> </td> <td align="left"> <math>a^2 b - bc(b + a) \biggl[ \frac{F(\theta,k) - E(\theta,k)}{k^2 \sin^3\theta} \biggr] \, . </math> </td> </tr> </table> Choose another value of <math>0 < b < 1</math>, then iterate again to find the value of <math>c</math> that corresponds to this new, chosen value of <math>b</math>. Repeat! </td></tr> <!-- <tr><td align="center"> <div align="center"><b>Lower Self-Adjoint</b><br />(Howard's derivation 1/28/2022)</div> <div align="center"> [[File:EmailFromHowardJan28Yr2022.png|650px|Lower Self-Adjoint Definition]] </div> </td></tr> --> </table> <br /> <div id="HowardHighResolution"> <table border="1" align="center" cellpadding="10" width="80%"> <tr><td align="center"> <div align="center"><b>Upper (USA) and Lower (LSA) Self-Adjoint</b><br />(Howard's Compact Expressions Plus Plot 1/28/2022)</div> <div align="center"> [[File:SelfAdjointDefinitions.png|650px|Self Adjoint Definitions]]<br />[[ThreeDimensionalConfigurations/RiemannStype#SAdata|(tabulated data here)]] </div> </td></tr> <tr><td align="center" bgcolor="black"> [[File:SelfAdjointPlot.png|600px|USA and LSA Plot]] </td></tr> </table> </div>
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