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Binomial series expansion of a trinomial?



The Next CEO of Stack OverflowSolving an equation arising from method of image chargesElectrostatic Potential Energy integral in spherical coordinatesBinomial Expansion without inifinty seriesOver an integral arising from Kepler's problem [also: generally useful integral, NOT DUPLICATE!]Integral of solid angle of closed surface from the exteriorBinomial Series Expansionlimit of integration is a vector, but I can rewrite the integrand as a scalar. What do I do?Need help understanding a particular proof regarding integration to find the net electric fieldExpansion question involving Taylor or Binomial series?Analytical solutions to integrals










0












$begingroup$


In electrostatics, the potential of a charge $q$ placed on the $z$-axis at $z=a$ is



beginequation
phi=frac14pi epsilon_0fracqr_1
endequation



where $r_1$ is the distance from the observation point to the charge.



Using law of cosines we get



beginequation
phi=fracq4pi epsilon_0 (r^2+a^2-2artext textcostheta)^-frac12
endequation



That will be Eq.(12.2).



Arkfen's Mathematical Methods for Physicist$^1$ states:




Consider the case of $r > a$ or, more precisely, $r^2 > |a^2 − 2artext cos θ|$. The radical in
Eq. (12.2) may be expanded in a binomial series and then rearranged in powers of ($a/r$).




The expression is a trinomial: $((fracar)^2+1-frac2artextcostheta)^-frac12$.



How can it be expanded through a binomial series? I can't find any source making this expansion explicitly, instead jumping directly into Legendre polynomials.



[1] George Arkfen and Hans Weber. Mathematical Methods for Physicist (6th ed. pp. 742)










share|cite|improve this question











$endgroup$







  • 1




    $begingroup$
    Treat the $1$ and the $(a/r)^2+2(a/r)cos(theta)$ as the two terms in the binomial. You can always expand out the polynomial you get.
    $endgroup$
    – D.B.
    Mar 18 at 19:51















0












$begingroup$


In electrostatics, the potential of a charge $q$ placed on the $z$-axis at $z=a$ is



beginequation
phi=frac14pi epsilon_0fracqr_1
endequation



where $r_1$ is the distance from the observation point to the charge.



Using law of cosines we get



beginequation
phi=fracq4pi epsilon_0 (r^2+a^2-2artext textcostheta)^-frac12
endequation



That will be Eq.(12.2).



Arkfen's Mathematical Methods for Physicist$^1$ states:




Consider the case of $r > a$ or, more precisely, $r^2 > |a^2 − 2artext cos θ|$. The radical in
Eq. (12.2) may be expanded in a binomial series and then rearranged in powers of ($a/r$).




The expression is a trinomial: $((fracar)^2+1-frac2artextcostheta)^-frac12$.



How can it be expanded through a binomial series? I can't find any source making this expansion explicitly, instead jumping directly into Legendre polynomials.



[1] George Arkfen and Hans Weber. Mathematical Methods for Physicist (6th ed. pp. 742)










share|cite|improve this question











$endgroup$







  • 1




    $begingroup$
    Treat the $1$ and the $(a/r)^2+2(a/r)cos(theta)$ as the two terms in the binomial. You can always expand out the polynomial you get.
    $endgroup$
    – D.B.
    Mar 18 at 19:51













0












0








0





$begingroup$


In electrostatics, the potential of a charge $q$ placed on the $z$-axis at $z=a$ is



beginequation
phi=frac14pi epsilon_0fracqr_1
endequation



where $r_1$ is the distance from the observation point to the charge.



Using law of cosines we get



beginequation
phi=fracq4pi epsilon_0 (r^2+a^2-2artext textcostheta)^-frac12
endequation



That will be Eq.(12.2).



Arkfen's Mathematical Methods for Physicist$^1$ states:




Consider the case of $r > a$ or, more precisely, $r^2 > |a^2 − 2artext cos θ|$. The radical in
Eq. (12.2) may be expanded in a binomial series and then rearranged in powers of ($a/r$).




The expression is a trinomial: $((fracar)^2+1-frac2artextcostheta)^-frac12$.



How can it be expanded through a binomial series? I can't find any source making this expansion explicitly, instead jumping directly into Legendre polynomials.



[1] George Arkfen and Hans Weber. Mathematical Methods for Physicist (6th ed. pp. 742)










share|cite|improve this question











$endgroup$




In electrostatics, the potential of a charge $q$ placed on the $z$-axis at $z=a$ is



beginequation
phi=frac14pi epsilon_0fracqr_1
endequation



where $r_1$ is the distance from the observation point to the charge.



Using law of cosines we get



beginequation
phi=fracq4pi epsilon_0 (r^2+a^2-2artext textcostheta)^-frac12
endequation



That will be Eq.(12.2).



Arkfen's Mathematical Methods for Physicist$^1$ states:




Consider the case of $r > a$ or, more precisely, $r^2 > |a^2 − 2artext cos θ|$. The radical in
Eq. (12.2) may be expanded in a binomial series and then rearranged in powers of ($a/r$).




The expression is a trinomial: $((fracar)^2+1-frac2artextcostheta)^-frac12$.



How can it be expanded through a binomial series? I can't find any source making this expansion explicitly, instead jumping directly into Legendre polynomials.



[1] George Arkfen and Hans Weber. Mathematical Methods for Physicist (6th ed. pp. 742)







taylor-expansion binomial-coefficients physics binomial-theorem electromagnetism






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Mar 20 at 2:09









Andrews

1,2812422




1,2812422










asked Mar 18 at 19:41









IchVerlorenIchVerloren

21310




21310







  • 1




    $begingroup$
    Treat the $1$ and the $(a/r)^2+2(a/r)cos(theta)$ as the two terms in the binomial. You can always expand out the polynomial you get.
    $endgroup$
    – D.B.
    Mar 18 at 19:51












  • 1




    $begingroup$
    Treat the $1$ and the $(a/r)^2+2(a/r)cos(theta)$ as the two terms in the binomial. You can always expand out the polynomial you get.
    $endgroup$
    – D.B.
    Mar 18 at 19:51







1




1




$begingroup$
Treat the $1$ and the $(a/r)^2+2(a/r)cos(theta)$ as the two terms in the binomial. You can always expand out the polynomial you get.
$endgroup$
– D.B.
Mar 18 at 19:51




$begingroup$
Treat the $1$ and the $(a/r)^2+2(a/r)cos(theta)$ as the two terms in the binomial. You can always expand out the polynomial you get.
$endgroup$
– D.B.
Mar 18 at 19:51










2 Answers
2






active

oldest

votes


















1












$begingroup$

The multinomial theorem, for the case $n=3$, says that
$$(x_1 + x_2 + x_3)^n =
sum_k_1+k_2+k_3 = n fracn!k_1!k_2!k_3! x_1^k_1 x_2^k_2 x_3^k_3
$$

This generalizes to possibly non-integer real exponents $r$ by writing $r! = Gamma(r+1)$ and
$$
sum_k_1,k_2,k_3 in Bbb Z fracr!k_1!k_2!k_3!(r-k_1-k_2-k_3)! x_1^k_1 x_2^k_2 x_3^k_3
$$



(Notice that in the case of positive integer $r$ this series ends because a $(-1)!$ starts appearing in the denominator, and that is infinite leading to the terms being zero.)



In this case, $(-frac12)! = Gamma(frac12)$ is $sqrtpi$ and the factors of $sqrtpi$ will cancel.



For the expression at hand, the lowest order terms in an expansion for $a << r$ are:
$$
left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
left( frac516-frac32costhetaright)fraca^3r^3+ cdots
$$






share|cite|improve this answer











$endgroup$




















    0












    $begingroup$

    $$frac1sqrt1+x sim 1-frac12x, x<<1.$$
    So,
    $$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$






    share|cite|improve this answer











    $endgroup$













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      2 Answers
      2






      active

      oldest

      votes








      2 Answers
      2






      active

      oldest

      votes









      active

      oldest

      votes






      active

      oldest

      votes









      1












      $begingroup$

      The multinomial theorem, for the case $n=3$, says that
      $$(x_1 + x_2 + x_3)^n =
      sum_k_1+k_2+k_3 = n fracn!k_1!k_2!k_3! x_1^k_1 x_2^k_2 x_3^k_3
      $$

      This generalizes to possibly non-integer real exponents $r$ by writing $r! = Gamma(r+1)$ and
      $$
      sum_k_1,k_2,k_3 in Bbb Z fracr!k_1!k_2!k_3!(r-k_1-k_2-k_3)! x_1^k_1 x_2^k_2 x_3^k_3
      $$



      (Notice that in the case of positive integer $r$ this series ends because a $(-1)!$ starts appearing in the denominator, and that is infinite leading to the terms being zero.)



      In this case, $(-frac12)! = Gamma(frac12)$ is $sqrtpi$ and the factors of $sqrtpi$ will cancel.



      For the expression at hand, the lowest order terms in an expansion for $a << r$ are:
      $$
      left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
      1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
      left( frac516-frac32costhetaright)fraca^3r^3+ cdots
      $$






      share|cite|improve this answer











      $endgroup$

















        1












        $begingroup$

        The multinomial theorem, for the case $n=3$, says that
        $$(x_1 + x_2 + x_3)^n =
        sum_k_1+k_2+k_3 = n fracn!k_1!k_2!k_3! x_1^k_1 x_2^k_2 x_3^k_3
        $$

        This generalizes to possibly non-integer real exponents $r$ by writing $r! = Gamma(r+1)$ and
        $$
        sum_k_1,k_2,k_3 in Bbb Z fracr!k_1!k_2!k_3!(r-k_1-k_2-k_3)! x_1^k_1 x_2^k_2 x_3^k_3
        $$



        (Notice that in the case of positive integer $r$ this series ends because a $(-1)!$ starts appearing in the denominator, and that is infinite leading to the terms being zero.)



        In this case, $(-frac12)! = Gamma(frac12)$ is $sqrtpi$ and the factors of $sqrtpi$ will cancel.



        For the expression at hand, the lowest order terms in an expansion for $a << r$ are:
        $$
        left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
        1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
        left( frac516-frac32costhetaright)fraca^3r^3+ cdots
        $$






        share|cite|improve this answer











        $endgroup$















          1












          1








          1





          $begingroup$

          The multinomial theorem, for the case $n=3$, says that
          $$(x_1 + x_2 + x_3)^n =
          sum_k_1+k_2+k_3 = n fracn!k_1!k_2!k_3! x_1^k_1 x_2^k_2 x_3^k_3
          $$

          This generalizes to possibly non-integer real exponents $r$ by writing $r! = Gamma(r+1)$ and
          $$
          sum_k_1,k_2,k_3 in Bbb Z fracr!k_1!k_2!k_3!(r-k_1-k_2-k_3)! x_1^k_1 x_2^k_2 x_3^k_3
          $$



          (Notice that in the case of positive integer $r$ this series ends because a $(-1)!$ starts appearing in the denominator, and that is infinite leading to the terms being zero.)



          In this case, $(-frac12)! = Gamma(frac12)$ is $sqrtpi$ and the factors of $sqrtpi$ will cancel.



          For the expression at hand, the lowest order terms in an expansion for $a << r$ are:
          $$
          left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
          1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
          left( frac516-frac32costhetaright)fraca^3r^3+ cdots
          $$






          share|cite|improve this answer











          $endgroup$



          The multinomial theorem, for the case $n=3$, says that
          $$(x_1 + x_2 + x_3)^n =
          sum_k_1+k_2+k_3 = n fracn!k_1!k_2!k_3! x_1^k_1 x_2^k_2 x_3^k_3
          $$

          This generalizes to possibly non-integer real exponents $r$ by writing $r! = Gamma(r+1)$ and
          $$
          sum_k_1,k_2,k_3 in Bbb Z fracr!k_1!k_2!k_3!(r-k_1-k_2-k_3)! x_1^k_1 x_2^k_2 x_3^k_3
          $$



          (Notice that in the case of positive integer $r$ this series ends because a $(-1)!$ starts appearing in the denominator, and that is infinite leading to the terms being zero.)



          In this case, $(-frac12)! = Gamma(frac12)$ is $sqrtpi$ and the factors of $sqrtpi$ will cancel.



          For the expression at hand, the lowest order terms in an expansion for $a << r$ are:
          $$
          left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
          1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
          left( frac516-frac32costhetaright)fraca^3r^3+ cdots
          $$







          share|cite|improve this answer














          share|cite|improve this answer



          share|cite|improve this answer








          edited Mar 18 at 20:25

























          answered Mar 18 at 19:56









          Mark FischlerMark Fischler

          33.8k12552




          33.8k12552





















              0












              $begingroup$

              $$frac1sqrt1+x sim 1-frac12x, x<<1.$$
              So,
              $$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$






              share|cite|improve this answer











              $endgroup$

















                0












                $begingroup$

                $$frac1sqrt1+x sim 1-frac12x, x<<1.$$
                So,
                $$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$






                share|cite|improve this answer











                $endgroup$















                  0












                  0








                  0





                  $begingroup$

                  $$frac1sqrt1+x sim 1-frac12x, x<<1.$$
                  So,
                  $$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$






                  share|cite|improve this answer











                  $endgroup$



                  $$frac1sqrt1+x sim 1-frac12x, x<<1.$$
                  So,
                  $$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$







                  share|cite|improve this answer














                  share|cite|improve this answer



                  share|cite|improve this answer








                  edited Mar 18 at 20:01

























                  answered Mar 18 at 19:55









                  D.B.D.B.

                  1,34019




                  1,34019



























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