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
How to Reset Passwords on Multiple Websites Easily?
Indicator light circuit
calculus parametric curve length
What's the best way to handle refactoring a big file?
How to transpose the 1st and -1th levels of arbitrarily nested array?
What was the first Unix version to run on a microcomputer?
Received an invoice from my ex-employer billing me for training; how to handle?
Return the Closest Prime Number
What benefits would be gained by using human laborers instead of drones in deep sea mining?
What does convergence in distribution "in the Gromov–Hausdorff" sense mean?
Do I need to enable Dev Hub in my PROD Org?
Example of a Mathematician/Physicist whose Other Publications during their PhD eclipsed their PhD Thesis
Would a galaxy be visible from outside, but nearby?
Can I equip Skullclamp on a creature I am sacrificing?
Is there an analogue of projective spaces for proper schemes?
Would this house-rule that treats advantage as a +1 to the roll instead (and disadvantage as -1) and allows them to stack be balanced?
Can you replace a racial trait cantrip when leveling up?
Is it professional to write unrelated content in an almost-empty email?
Unreliable Magic - Is it worth it?
Sending manuscript to multiple publishers
What exact does MIB represent in SNMP? How is it different from OID?
Is it ever safe to open a suspicious html file (e.g. email attachment)?
Elegant way to replace substring in a regex with optional groups in Python?
How does the mv command work with external drives?
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
$begingroup$
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)
taylor-expansion binomial-coefficients physics binomial-theorem electromagnetism
$endgroup$
add a comment |
$begingroup$
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)
taylor-expansion binomial-coefficients physics binomial-theorem electromagnetism
$endgroup$
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
add a comment |
$begingroup$
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)
taylor-expansion binomial-coefficients physics binomial-theorem electromagnetism
$endgroup$
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
taylor-expansion binomial-coefficients physics binomial-theorem electromagnetism
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
add a comment |
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
add a comment |
2 Answers
2
active
oldest
votes
$begingroup$
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:
$$
left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
left( frac516-frac32costhetaright)fraca^3r^3+ cdots
$$
$endgroup$
add a comment |
$begingroup$
$$frac1sqrt1+x sim 1-frac12x, x<<1.$$
So,
$$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$
$endgroup$
add a comment |
Your Answer
StackExchange.ifUsing("editor", function ()
return StackExchange.using("mathjaxEditing", function ()
StackExchange.MarkdownEditor.creationCallbacks.add(function (editor, postfix)
StackExchange.mathjaxEditing.prepareWmdForMathJax(editor, postfix, [["$", "$"], ["\\(","\\)"]]);
);
);
, "mathjax-editing");
StackExchange.ready(function()
var channelOptions =
tags: "".split(" "),
id: "69"
;
initTagRenderer("".split(" "), "".split(" "), channelOptions);
StackExchange.using("externalEditor", function()
// Have to fire editor after snippets, if snippets enabled
if (StackExchange.settings.snippets.snippetsEnabled)
StackExchange.using("snippets", function()
createEditor();
);
else
createEditor();
);
function createEditor()
StackExchange.prepareEditor(
heartbeatType: 'answer',
autoActivateHeartbeat: false,
convertImagesToLinks: true,
noModals: true,
showLowRepImageUploadWarning: true,
reputationToPostImages: 10,
bindNavPrevention: true,
postfix: "",
imageUploader:
brandingHtml: "Powered by u003ca class="icon-imgur-white" href="https://imgur.com/"u003eu003c/au003e",
contentPolicyHtml: "User contributions licensed under u003ca href="https://creativecommons.org/licenses/by-sa/3.0/"u003ecc by-sa 3.0 with attribution requiredu003c/au003e u003ca href="https://stackoverflow.com/legal/content-policy"u003e(content policy)u003c/au003e",
allowUrls: true
,
noCode: true, onDemand: true,
discardSelector: ".discard-answer"
,immediatelyShowMarkdownHelp:true
);
);
Sign up or log in
StackExchange.ready(function ()
StackExchange.helpers.onClickDraftSave('#login-link');
);
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
StackExchange.ready(
function ()
StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f3153220%2fbinomial-series-expansion-of-a-trinomial%23new-answer', 'question_page');
);
Post as a guest
Required, but never shown
2 Answers
2
active
oldest
votes
2 Answers
2
active
oldest
votes
active
oldest
votes
active
oldest
votes
$begingroup$
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:
$$
left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
left( frac516-frac32costhetaright)fraca^3r^3+ cdots
$$
$endgroup$
add a comment |
$begingroup$
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:
$$
left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
left( frac516-frac32costhetaright)fraca^3r^3+ cdots
$$
$endgroup$
add a comment |
$begingroup$
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:
$$
left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
left( frac516-frac32costhetaright)fraca^3r^3+ cdots
$$
$endgroup$
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:
$$
left[ 1+ frac2arcostheta + left(fracar right)^2 right]^-frac12=
1 - fraca2r + left( frac38-costhetaright)fraca^2r^2 -
left( frac516-frac32costhetaright)fraca^3r^3+ cdots
$$
edited Mar 18 at 20:25
answered Mar 18 at 19:56
Mark FischlerMark Fischler
33.8k12552
33.8k12552
add a comment |
add a comment |
$begingroup$
$$frac1sqrt1+x sim 1-frac12x, x<<1.$$
So,
$$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$
$endgroup$
add a comment |
$begingroup$
$$frac1sqrt1+x sim 1-frac12x, x<<1.$$
So,
$$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$
$endgroup$
add a comment |
$begingroup$
$$frac1sqrt1+x sim 1-frac12x, x<<1.$$
So,
$$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$
$endgroup$
$$frac1sqrt1+x sim 1-frac12x, x<<1.$$
So,
$$frac1sqrt1+(a/r)(a/r+2cos(theta)) sim 1-frac12fracar(fracar+2cos(theta)) = 1-cos(theta)fracar-frac12(fracar)^2.$$
edited Mar 18 at 20:01
answered Mar 18 at 19:55
D.B.D.B.
1,34019
1,34019
add a comment |
add a comment |
Thanks for contributing an answer to Mathematics Stack Exchange!
- Please be sure to answer the question. Provide details and share your research!
But avoid …
- Asking for help, clarification, or responding to other answers.
- Making statements based on opinion; back them up with references or personal experience.
Use MathJax to format equations. MathJax reference.
To learn more, see our tips on writing great answers.
Sign up or log in
StackExchange.ready(function ()
StackExchange.helpers.onClickDraftSave('#login-link');
);
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
StackExchange.ready(
function ()
StackExchange.openid.initPostLogin('.new-post-login', 'https%3a%2f%2fmath.stackexchange.com%2fquestions%2f3153220%2fbinomial-series-expansion-of-a-trinomial%23new-answer', 'question_page');
);
Post as a guest
Required, but never shown
Sign up or log in
StackExchange.ready(function ()
StackExchange.helpers.onClickDraftSave('#login-link');
);
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
Sign up or log in
StackExchange.ready(function ()
StackExchange.helpers.onClickDraftSave('#login-link');
);
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
Sign up or log in
StackExchange.ready(function ()
StackExchange.helpers.onClickDraftSave('#login-link');
);
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Sign up using Google
Sign up using Facebook
Sign up using Email and Password
Post as a guest
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
Required, but never shown
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