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Series expansion of an expression that has productlog function about -1/e



The 2019 Stack Overflow Developer Survey Results Are InSeries Expansion of $frac11-e^int$Taylor / Maclaurin series expansion origin.If I have a holomorphic function on the unit disc, do I know anything about the radius of convergence of its series expansion about zero?Find complex power series expansion for $int e^-w^2 dw$Power series expansion of $f(z)=frac13-z$ about the point $4i$Expansion in power series of $z=0$Laurent series expansion of a given functionPower series expansion questionPower series expansion involving Lambert-W functionFind the power series expansion of $f(x)= frace^x - 1x$










0












$begingroup$


I have this term: $-frac1pW(-fracpe)bigg[logbigg(-frac1pW(-fracpe)bigg)-1bigg]$.



In order to reduce complexity I've taken
$-fracpe=x$ which gives $f(x)=frac1xeW(x)bigg[logbigg(frac1xeW(x)bigg)-1bigg]$.



I need to do a power series expansion for this term at $x=-1/e$.



From the basics of Taylor expansion: $f(x)=f(-1/e)+fracdfdx(-1/e) (x+1/e)^1+fracd^2fdx^2(-1/e)(x+1/e)^2+.....$



The first term $f(-1/e)=-1$ but the second term $fracdfdx=-frac[W(x)]^2bigg[logbigg(fracW(x)xbigg)-1bigg]ex^2[w(x)+1]$ is not defined at $x=-1/e$ since $W(-1/e)=-1$ making the denominator to be $0$ also the numerator is $0$ as well. If the second term is undefined then the Taylor expansion does not work (to my understanding).



I'm not sure where I'm going wrong with this approach or if there's any other way to expand this term as a power series at $x=-1/e$. Any suggestions/help appreciated. Thanks!










share|cite|improve this question











$endgroup$
















    0












    $begingroup$


    I have this term: $-frac1pW(-fracpe)bigg[logbigg(-frac1pW(-fracpe)bigg)-1bigg]$.



    In order to reduce complexity I've taken
    $-fracpe=x$ which gives $f(x)=frac1xeW(x)bigg[logbigg(frac1xeW(x)bigg)-1bigg]$.



    I need to do a power series expansion for this term at $x=-1/e$.



    From the basics of Taylor expansion: $f(x)=f(-1/e)+fracdfdx(-1/e) (x+1/e)^1+fracd^2fdx^2(-1/e)(x+1/e)^2+.....$



    The first term $f(-1/e)=-1$ but the second term $fracdfdx=-frac[W(x)]^2bigg[logbigg(fracW(x)xbigg)-1bigg]ex^2[w(x)+1]$ is not defined at $x=-1/e$ since $W(-1/e)=-1$ making the denominator to be $0$ also the numerator is $0$ as well. If the second term is undefined then the Taylor expansion does not work (to my understanding).



    I'm not sure where I'm going wrong with this approach or if there's any other way to expand this term as a power series at $x=-1/e$. Any suggestions/help appreciated. Thanks!










    share|cite|improve this question











    $endgroup$














      0












      0








      0





      $begingroup$


      I have this term: $-frac1pW(-fracpe)bigg[logbigg(-frac1pW(-fracpe)bigg)-1bigg]$.



      In order to reduce complexity I've taken
      $-fracpe=x$ which gives $f(x)=frac1xeW(x)bigg[logbigg(frac1xeW(x)bigg)-1bigg]$.



      I need to do a power series expansion for this term at $x=-1/e$.



      From the basics of Taylor expansion: $f(x)=f(-1/e)+fracdfdx(-1/e) (x+1/e)^1+fracd^2fdx^2(-1/e)(x+1/e)^2+.....$



      The first term $f(-1/e)=-1$ but the second term $fracdfdx=-frac[W(x)]^2bigg[logbigg(fracW(x)xbigg)-1bigg]ex^2[w(x)+1]$ is not defined at $x=-1/e$ since $W(-1/e)=-1$ making the denominator to be $0$ also the numerator is $0$ as well. If the second term is undefined then the Taylor expansion does not work (to my understanding).



      I'm not sure where I'm going wrong with this approach or if there's any other way to expand this term as a power series at $x=-1/e$. Any suggestions/help appreciated. Thanks!










      share|cite|improve this question











      $endgroup$




      I have this term: $-frac1pW(-fracpe)bigg[logbigg(-frac1pW(-fracpe)bigg)-1bigg]$.



      In order to reduce complexity I've taken
      $-fracpe=x$ which gives $f(x)=frac1xeW(x)bigg[logbigg(frac1xeW(x)bigg)-1bigg]$.



      I need to do a power series expansion for this term at $x=-1/e$.



      From the basics of Taylor expansion: $f(x)=f(-1/e)+fracdfdx(-1/e) (x+1/e)^1+fracd^2fdx^2(-1/e)(x+1/e)^2+.....$



      The first term $f(-1/e)=-1$ but the second term $fracdfdx=-frac[W(x)]^2bigg[logbigg(fracW(x)xbigg)-1bigg]ex^2[w(x)+1]$ is not defined at $x=-1/e$ since $W(-1/e)=-1$ making the denominator to be $0$ also the numerator is $0$ as well. If the second term is undefined then the Taylor expansion does not work (to my understanding).



      I'm not sure where I'm going wrong with this approach or if there's any other way to expand this term as a power series at $x=-1/e$. Any suggestions/help appreciated. Thanks!







      power-series lambert-w






      share|cite|improve this question















      share|cite|improve this question













      share|cite|improve this question




      share|cite|improve this question








      edited Mar 26 at 4:05







      anikfaisal

















      asked Mar 23 at 4:19









      anikfaisalanikfaisal

      266




      266




















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          $begingroup$

          According to R. M. Corless et al. if $p=+sqrt2(ez+1)$ and $mid p mid<sqrt2$ then $W(z)=-1+p-frac13p^2+frac1172p^3+....$



          Also according to the definition of Lambert-W function $We^W=z$, taking logarithm on both sides of this equation yields: $ln W=ln z-W$ gives us a relatively easier way to break down the log term in our function.



          Now getting back to the function we have, $-frac1yW(-fracye)bigg[lnbigg(-frac1yW(-fracye)bigg)-1bigg]$. Let's take $z=-fracye$ and so we get $p=sqrt2(1-y)$. Now we are able to do the power series expansion for our function:



          $W(z)=-1+sqrt2(1-y)^1/2-frac23(1-y)+frac11 times 2^3/272(1-y)^3/2+....$



          Now, using this expansion and after some very tedious multiplication the final expression for the expansion can be derived.






          share|cite|improve this answer









          $endgroup$













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            1 Answer
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            0












            $begingroup$

            According to R. M. Corless et al. if $p=+sqrt2(ez+1)$ and $mid p mid<sqrt2$ then $W(z)=-1+p-frac13p^2+frac1172p^3+....$



            Also according to the definition of Lambert-W function $We^W=z$, taking logarithm on both sides of this equation yields: $ln W=ln z-W$ gives us a relatively easier way to break down the log term in our function.



            Now getting back to the function we have, $-frac1yW(-fracye)bigg[lnbigg(-frac1yW(-fracye)bigg)-1bigg]$. Let's take $z=-fracye$ and so we get $p=sqrt2(1-y)$. Now we are able to do the power series expansion for our function:



            $W(z)=-1+sqrt2(1-y)^1/2-frac23(1-y)+frac11 times 2^3/272(1-y)^3/2+....$



            Now, using this expansion and after some very tedious multiplication the final expression for the expansion can be derived.






            share|cite|improve this answer









            $endgroup$

















              0












              $begingroup$

              According to R. M. Corless et al. if $p=+sqrt2(ez+1)$ and $mid p mid<sqrt2$ then $W(z)=-1+p-frac13p^2+frac1172p^3+....$



              Also according to the definition of Lambert-W function $We^W=z$, taking logarithm on both sides of this equation yields: $ln W=ln z-W$ gives us a relatively easier way to break down the log term in our function.



              Now getting back to the function we have, $-frac1yW(-fracye)bigg[lnbigg(-frac1yW(-fracye)bigg)-1bigg]$. Let's take $z=-fracye$ and so we get $p=sqrt2(1-y)$. Now we are able to do the power series expansion for our function:



              $W(z)=-1+sqrt2(1-y)^1/2-frac23(1-y)+frac11 times 2^3/272(1-y)^3/2+....$



              Now, using this expansion and after some very tedious multiplication the final expression for the expansion can be derived.






              share|cite|improve this answer









              $endgroup$















                0












                0








                0





                $begingroup$

                According to R. M. Corless et al. if $p=+sqrt2(ez+1)$ and $mid p mid<sqrt2$ then $W(z)=-1+p-frac13p^2+frac1172p^3+....$



                Also according to the definition of Lambert-W function $We^W=z$, taking logarithm on both sides of this equation yields: $ln W=ln z-W$ gives us a relatively easier way to break down the log term in our function.



                Now getting back to the function we have, $-frac1yW(-fracye)bigg[lnbigg(-frac1yW(-fracye)bigg)-1bigg]$. Let's take $z=-fracye$ and so we get $p=sqrt2(1-y)$. Now we are able to do the power series expansion for our function:



                $W(z)=-1+sqrt2(1-y)^1/2-frac23(1-y)+frac11 times 2^3/272(1-y)^3/2+....$



                Now, using this expansion and after some very tedious multiplication the final expression for the expansion can be derived.






                share|cite|improve this answer









                $endgroup$



                According to R. M. Corless et al. if $p=+sqrt2(ez+1)$ and $mid p mid<sqrt2$ then $W(z)=-1+p-frac13p^2+frac1172p^3+....$



                Also according to the definition of Lambert-W function $We^W=z$, taking logarithm on both sides of this equation yields: $ln W=ln z-W$ gives us a relatively easier way to break down the log term in our function.



                Now getting back to the function we have, $-frac1yW(-fracye)bigg[lnbigg(-frac1yW(-fracye)bigg)-1bigg]$. Let's take $z=-fracye$ and so we get $p=sqrt2(1-y)$. Now we are able to do the power series expansion for our function:



                $W(z)=-1+sqrt2(1-y)^1/2-frac23(1-y)+frac11 times 2^3/272(1-y)^3/2+....$



                Now, using this expansion and after some very tedious multiplication the final expression for the expansion can be derived.







                share|cite|improve this answer












                share|cite|improve this answer



                share|cite|improve this answer










                answered Mar 26 at 0:09









                anikfaisalanikfaisal

                266




                266



























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