It was originally asked here. This was also asked here.
I have faced some difficulties to do the following integral:
I=∫2π0dϕ∫π0dθ sinθ∫∞0dr r23x2y2cos(ursinθcosϕ)cos2θ(y2cosϕ+x2sin2ϕ)sin2θ+x2y2cos2θe−r22,
where x, y, and u are real positive constants. I tried at least two ways to solve this integral:
- First attempt:
I began to solve the r integral first. By using Mathematica, then
I=∫2π0dϕ∫π0dθ sinθ3x2y2(1−u2sin2θcos2ϕ)cos2θ(y2cosϕ+x2sin2ϕ)sin2θ+x2y2cos2θe−u22sin2θcos2ϕ.
After that, I looked for a solution for ϕ integral. My best attempt was:
Iϕ(x,y,u,θ)=2B[B(12)F1(12,1,−;1;ν,−a2)−aB(12)F1(32,1,−;2;ν,−a2)],
where B=x2sin2θ+x2y2cos2θ, a=u2sin2θ, and ν=x2−y2x2+x2y2cot2θ. In this way, the final results it's something like that:
I=∫π0dθ 3x2y2sinθcos2θ Iϕ(x,y,u,θ)..
Eq. (3) cannot be further simplied in general and is the nal result.
- Second attempt:
To avoid the hypergeometric function F1, I tried to start with the ϕ integral. In this case, my initial problem is an integral something like that:
∫2π0dϕcos(Acosϕ)a2cos2ϕ+b2sin2ϕ.
This integral (4) can be solved by series (see Vincent's answer and Jack's answer). However those solutions, at least for me, has not a closed form. This is my final step on this second attempt :(
What is the point? It turns out that someone has managed to solve the integral (1), at least the integral in r and ϕ. The final resuls found by this person was:
IG=12πx y(1−x2)3/2∫√1−x20dkk2exp(−u22x2k2(1−x2)(1−k2))√1−k2√1−k21−y21−x2,
where, I belive, k=√1−x2cosθ. As you can see in this following code performed in Mathematica
IG[x_, y_, u_] :=
Sqrt[Pi/2] NIntegrate[(12 Pi x y)/(1 - x^2)^(3/2)
(v^2 Exp[-(u^2 x^2 v^2)/(2 (1 - x^2) (1 - v^2))])/(Sqrt[1 - v^2] Sqrt[1 - v^2 (1 - y^2)/(1 - x^2)]), {v, 0, Sqrt[1 - x^2]}]
IG[.3, .4, 1]
** 4.53251 **
I[x_, y_, u_] :=
NIntegrate[(r^2 Sin[a] Cos[
u r Sin[a] Cos[b]] 3 x^2 y^2 Cos[a]^2 Exp[-r^2/
2])/((y^2 Cos[b]^2 + x^2 Sin[b]^2) Sin[a]^2 +
x^2 y^2 Cos[a]^2), {r, 0, Infinity}, {a, 0, Pi}, {b, 0, 2 Pi}]
I[.3, .4, 1]
** 4.53251 **
the integrals I and IG are equals. Indeed, since that they emerge from the same physical problem.
So, my question is: what are the steps applied for that integral I gives the integral IG?
Edit
Since my question was not solved yet, I think it is because it is a tough question, I will show a particular case of the integral I, letting u=0. I hope with this help you help me.
In this case, the r integral in (1) is trivial and the integral takes the form:
IP=∫2π0dϕ∫π0dθ sinθ3x2y2cos2θ(y2cosϕ+x2sin2ϕ)sin2θ+x2y2cos2θ.
The ϕ integral can be integrated with the help of Eq. 3.642.1 in Gradstein and Ryzhik's tables of integrals. Thereby, the IP takes the for:
IP=3xy∫π0dθsinθcos2θ√1+(x2−1)cos2θ√1+(y2−1)cos2θ.
Now the change of variable k=√1−x2cosθ bring expression (6) to the form
IP=(const)x y(1−x2)3/2∫√1−x20dkk2√1−k2√1−k21−y21−x2.
Did you notice how IG and IP are similar? Do you think a similar approach can be applied to my original problem? Please, let me know.
Edit 2
The integral (1) is also evaluated in Appendix A.4 of this thesis. However, there he used cylindrical symmetry.
Edit: ended
My bounty ended, and unfortunately, I don't have enough reputation to offer another one. My question was not solved. Perhaps to solve that it is necessary to make some physical consideration. Anyway, I thanks to all who helped me. If I can solve this, I put the solution here.
I've solved this problem applying the Schwinger proper-time substitution: 1q2=∫∞0dξ e−q2ξ
Answer
Here is an outline of the approach I have taken to solve this integral.
First rewrite the integral (1) in Cartesian variables:
I=∫∞−∞d3v 3x2y2v2zy2v2x+x2v2y+x2y2v2zcos(uvx)exp(−v2x2−v2y2−v2z2).
Now use the following substitution
1y2v2x+x2v2y+x2y2v2z=∫∞0dτ e−(y2v2x+x2v2y+x2y2v2z)τ,
such that
I=∫∞0dτ∫∞−∞d3v 3x2y2v2zcos(uvx)e−v2x(τy2+1/2)−v2y(τx2+1/2)−v2z(τx2y2+1/2).
The (vx,vy,vz) integrals can be evaluated with the help of Mathematica. The results gives
∫∞−∞d3v 3x2y2v2zcos(uvx)e−αv2x−βv2y−γv2z=3π3/22x2y2exp(−u24y21τ+1/2y2)(τ+1/2x2y2)3/2(τ+1/2x2)1/2(τ+1/2y2)1/2.
Thereby,
I=−3 constx2y2 const∫∞0dτexp(−u24y21τ+1/2y2)(τ+1/2x2y2)3/2(τ+1/2x2)1/2(τ+1/2y2)1/2.
Now, performing the substitution τ=1−x22x2y2k2−12x2y2 gives us
I=(const) 3x y(1−x2)3/2∫√1−x20dkk2exp(−u22x2k2(1−x2)(1−k2))√1−k2√1−k21−y21−x2,
which is the desired integral unless of a constant. ;)
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