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=Appendix B: Elliptic Integrals= ==Summary Table== If the default argument of a [[Appendix/EquationTemplates#Complete_Elliptic_Integrals|complete elliptic integral function]] is the parameter, <math>~k</math>, then we should also appreciate that the following additional arguments may be useful: <table border="1" cellpadding="8" align="center"> <tr> <td align="center" rowspan="2" width="10%">parameter</td> <td align="center" colspan="4">In terms of …</td> </tr> <tr> <td align="center" width="20%"><math>~k</math><br /> <font size="-1">([http://dlmf.nist.gov/22.7.i Descending Landen Transformation])</font> </td> <td align="center" width="20%"><math>~k_1</math><br /> <font size="-1">([http://dlmf.nist.gov/22.7.ii Ascending Landen Transformation])</font> </td> <td align="center" width="20%><math>~\frac{R}{R_1} = e^{-\eta}</math></td> <td align="center"><math>~\eta \equiv \ln\biggl(\frac{R_1}{R}\biggr)</math></td> </tr> <tr> <td align="center"><math>~k</math></td> <td align="center"><math>~k</math></td> <td align="center"><math>~\frac{2\sqrt{k_1}}{1+k_1}</math></td> <td align="center"><math>~\biggl[1 - \biggl( \frac{R}{R_1}\biggr)^2 \biggr]^{1 / 2}</math></td> <td align="center"><math>~\biggl[ \frac{2}{\coth\eta + 1} \biggr]^{1 / 2}= \biggl[ 1 - e^{-2\eta} \biggr]^{1 / 2}</math></td> </tr> <tr> <td align="center"><math>~k^{\prime}</math></td> <td align="center"><math>~\sqrt{1 - k^2}</math></td> <td align="center"><math>~\frac{1-k_1}{1+k_1}</math></td> <td align="center"><math>~\frac{R}{R_1}</math></td> <td align="center"><math>~\frac{1}{\cosh\eta + \sinh\eta} = e^{-\eta}</math></td> </tr> <tr> <td align="center"><math>~k_1 = \frac{1-k^{\prime}}{1+k^{\prime}}</math></td> <td align="center"><math>~\frac{1-\sqrt{1 - k^2}}{1+\sqrt{1 - k^2}}</math></td> <td align="center"><math>~k_1</math></td> <td align="center"><math>~\frac{R_1 - R}{R_1 +R}</math></td> <td align="center"><math>~\tanh\biggl(\frac{\eta}{2}\biggr) = \frac{1 - e^{-\eta}}{1 + e^{-\eta}}</math></td> </tr> </table> <span id="GandR65">As published, for example,</span> in §8.126 of [http://www.mathtable.com/gr/ Gradshteyn & Ryzhik (1965)], the following mappings are valid: <table border="1" cellpadding="8" width="85%" align="center"> <tr> <th> Explicitly Published in §8.126 of [http://www.mathtable.com/gr/ G & R (1965)] </th> <th> Additional Implications </th> </tr> <tr> <td> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~ K\biggl( \frac{1-k^\prime}{1+k^\prime} \biggr) = K(k_1)</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\frac{1}{2} (1+k^{\prime}) K(k)</math> </td> </tr> <tr> <td align="right"> <math>~ E\biggl( \frac{1-k^\prime}{1+k^\prime} \biggr) = E(k_1)</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\frac{1}{1+k^\prime} \biggl[E(k) + k^\prime K(k) \biggr]</math> </td> </tr> </table> </td> <td> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~ \frac{4K(k_1)}{R_1 + R} </math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\frac{2K(k)}{R_1}</math> </td> </tr> <tr> <td align="right"> <math>~E(k)</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~(1+k^\prime)E(k_1) - k^\prime K(k)</math> </td> </tr> <tr> <td align="center" colspan="3">[http://dlmf.nist.gov/19.8.E12 DLMS §19.8.12]</td> </tr> </table> </td> </tr> <tr> <td> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~ K\biggl( \frac{2\sqrt{k}}{1+k} \biggr) </math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~(1+k)K(k)</math> </td> </tr> <tr> <td align="right"> <math>~ E\biggl( \frac{2\sqrt{k}}{1+k} \biggr) </math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\frac{1}{1+k} \biggl[2E(k) - (k^\prime)^2 K(k) \biggr]</math> </td> </tr> </table> </td> <td> <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~ K( k ) </math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~(1+k_1)K(k_1)</math> </td> </tr> <tr> <td align="center" colspan="3">[http://dlmf.nist.gov/19.8.E12 DLMS §19.8.12]</td> </tr> <tr> <td align="right"> <math>~ E\biggl( \frac{2\sqrt{k_1}}{1+k_1} \biggr) = E(k) </math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\frac{1}{1+k_1} \biggl[2E(k_1) - (1-k_1^2) K(k_1) \biggr]</math> </td> </tr> </table> </td> </tr> </table> ==One Set of Details== Following advice that we have received from Howard Cohl (private communication), we can demonstrate this most efficiently by employing the [https://dlmf.nist.gov/19.8#ii ''Descending Landen Transformation'' for the complete elliptic integral of the first kind], that is, <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~K(k)</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ (1 + k_1)K(k_1) \, , </math> </td> <td align="center"> where, </td> <td align="right"> <math>~k_1</math> </td> <td align="center"> <math>~\equiv</math> </td> <td align="left"> <math>~ \frac{1-\sqrt{1-k^2}}{1+\sqrt{1-k^2}} \, . </math> </td> </tr> </table> Given our just-stated definition of the parameter, <math>~k</math>, we have, <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~\sqrt{1-k^2}</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \biggl[ 1 - \frac{2}{\coth\eta + 1} \biggr]^{1 / 2} = \biggl[ \frac{\coth\eta - 1 }{\coth\eta + 1} \biggr]^{1 / 2} </math> </td> </tr> <tr> <td align="right"> <math>~\Rightarrow ~~~ 1 \pm \sqrt{1-k^2}</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ 1 \pm \biggl[ \frac{\coth\eta - 1 }{\coth\eta + 1} \biggr]^{1 / 2} = \frac{ [\coth\eta + 1]^{1 / 2} \pm [\coth\eta - 1]^{1 / 2} }{ [\coth\eta + 1]^{1 / 2} } </math> </td> </tr> <tr> <td align="right"> <math>~\Rightarrow ~~~k_1 \equiv \frac{1 - \sqrt{1-k^2}}{1 + \sqrt{1-k^2}}</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \frac{ [\coth\eta + 1]^{1 / 2} - [\coth\eta - 1]^{1 / 2} }{ [\coth\eta + 1]^{1 / 2} + [\coth\eta - 1]^{1 / 2} } </math> </td> </tr> <tr> <td align="right"> <math>~\Rightarrow ~~~k_1^2 </math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \frac{ [\coth\eta + 1] -2[\coth\eta + 1]^{1 / 2}[\coth\eta - 1]^{1 / 2} + [\coth\eta - 1] }{ [\coth\eta + 1] + 2[\coth\eta + 1]^{1 / 2}[\coth\eta - 1]^{1 / 2} + [\coth\eta - 1] } </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \frac{ 2\coth\eta -2[\coth\eta + 1]^{1 / 2}[\coth\eta - 1]^{1 / 2} }{ 2\coth\eta + 2[\coth\eta + 1]^{1 / 2}[\coth\eta - 1]^{1 / 2} } </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \frac{ \coth\eta - [\coth^2\eta - 1]^{1 / 2} }{ \coth\eta + [\coth^2\eta - 1]^{1 / 2} } </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \frac{ \coth\eta/[\coth^2\eta - 1]^{1 / 2} - 1 }{ \coth\eta/[\coth^2\eta - 1]^{1 / 2} + 1 } </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\frac{\cosh\eta - 1}{\cosh\eta + 1}</math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~\tanh^2\biggl(\frac{\eta}{2}\biggr) \, .</math> </td> </tr> </table> Note as well that, <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~1 + k_1</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~1+ \frac{1 - \sqrt{1-k^2}}{1 + \sqrt{1-k^2}} = \frac{2}{1 + \sqrt{1-k^2}} \, .</math> </td> </tr> </table> Hence, the "second attempt" expression for <math>~P_{1 / 2}(z)</math> becomes, <table border="0" cellpadding="5" align="center"> <tr> <td align="right"> <math>~P_{-1 / 2}(\cosh\eta)</math> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \frac{\sqrt{2}}{\pi}~ (\sinh\eta)^{-1 / 2} \biggl[ \frac{2k}{1 + \sqrt{1-k^2}} \biggr] K\biggl(\tanh \frac{\eta}{2} \biggr) </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \frac{2^{2}}{\pi}~ (\sinh\eta)^{-1 / 2} \biggl[ \frac{1}{\coth\eta + 1}\biggr]^{1 / 2} \biggl\{ \frac{ [\coth\eta + 1]^{1 / 2} }{ [\coth\eta + 1]^{1 / 2} + [\coth\eta - 1]^{1 / 2} } \biggr\}K\biggl(\tanh \frac{\eta}{2} \biggr) </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \frac{2^{2}}{\pi}~ \biggl[ ( \cosh\eta + \sinh\eta )^{1 / 2} + (\cosh\eta - \sinh\eta)^{1 / 2} \biggr]^{-1} K\biggl(\tanh \frac{\eta}{2} \biggr) </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \frac{2^{2}}{\pi}~ \biggl[ e^{\eta/2} + e^{-\eta/2} \biggr]^{-1} K\biggl(\tanh \frac{\eta}{2} \biggr) </math> </td> </tr> <tr> <td align="right"> </td> <td align="center"> <math>~=</math> </td> <td align="left"> <math>~ \biggl[ \frac{\pi}{2} \cdot \cosh\frac{\eta}{2} \biggr]^{-1} K\biggl(\tanh \frac{\eta}{2} \biggr) \, . </math> </td> </tr> </table> This is, indeed, identical to the "Attempt #1" expression for <math>~P_{-1 / 2}(z)</math> that was used by Wong. '''Q.E.D.''' ==Series Expansions== From our [[Appendix/EquationTemplates#Complete_Elliptic_Integrals|accompanying set of Key mathematical relations]] we find the following series expansions for complete elliptic integrals of, respectively, the first and second kind: <div align="center"> {{ Math/EQ_EllipticIntegral01 }}<br /> {{ Math/EQ_EllipticIntegral02 }} </div> If you don't know how to handle a ''double factorial'' — also referred to as a ''semifactorial'' — see, for example, [https://en.wikipedia.org/wiki/Double_factorial this wikipedia page].
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