# Computer the flux of $\nabla \ln \sqrt{x^2 + y^2 + z^2}$ across an icosahedron centered at the origin

Let $$S$$ be the surface of an icosahedron centered at origin) and let $$f(x,y,z)=\ln \sqrt{x^2+y^2+z^2} .$$ Calculate the flux $$\iint_S (\nabla f \cdot n) d\sigma,$$ where $$n$$ is the outward unit normal vector on $$S$$.

[My attempt]

I tried to use divergence theorem. $$\iint (\nabla f \cdot n) d\sigma = \iiint (\nabla \cdot \nabla f ) dV ,$$ where $$(\nabla \cdot \nabla f ) = \frac{1}{x^2 + y^2+z^2}$$. However, I can't find a parametrization of the icosahedron to find the triple integral. How to find this value?

• Does the Divergence Theorem apply? Aug 17, 2019 at 2:51
• Yes, i did but i can solve this problem yet.
– hew
Aug 17, 2019 at 2:59
• Review the hypotheses. Aug 17, 2019 at 3:01
• is there problem in hypotheses? could you explain in detail? I cant understand..
– hew
Aug 17, 2019 at 3:13
• I suspect this problem may not be written as intended, since there doesn't seem to be a better way than just parameterizing a face $F$ of the icosahedron $I$ and using symmetry to compute $$\iint_I \nabla f \cdot {\bf n} \,d\sigma = 20 \iint_F \nabla f \cdot {\bf n} \,d\sigma .$$ On the other hand, if $f := (x^2 + y^2 + z^2)^{-1 / 2}$, there is a much cleaner method for computing the integral. (In 2 dimensions the radial function with this property is $\log \sqrt{x^2 + y^2}$.) Aug 17, 2019 at 3:45

As I wrote in the comments, I suspect that this question might have been prepared incorrectly: I don't see a method better than exploiting symmetry and integrating directly, and the resulting integral doesn't appear to have a closed form in terms of elementary functions, though it does have an unpleasant expression in terms of dilogarithms.

Since the integrand $$\nabla f \cdot {\bf n}$$ is invariant under symmetries of the icosahedron $$S$$, we need only integrate over a suitable triangle $$T$$ contained in a face $$F$$: $$\iint_S \nabla f \cdot {\bf n} \,d\sigma = 20 \iint_F \nabla f \cdot {\bf n} \,d\sigma = 120 \iint_T \nabla f \cdot {\bf n} \,d\sigma .$$

Now, using the fact that the central angle between two adjacent vertices of $$S$$ is $$\arccos \frac{1}{\sqrt 5}$$ gives that the distance between the center $$U$$ of $$F$$ and a corner of $$F$$ is $$\lambda R$$, where $$R$$ is the radius of the sphere inscribed in $$S$$, and $$\lambda := 3 - \sqrt{5} \approx 0.76393\!\ldots$$.

In spherical coordinates centered at the center of $$S$$, $$\nabla f = \rho^{-1} {\bf \hat \rho}$$, so at a point $$x$$ on $$F$$ at a distance $$r$$ from $$U$$, $$(\nabla f)(x) = \frac{1}{\sqrt{R^2 + r^2}} \hat\rho ,$$ and then some straightforward trigonometery shows that $$\nabla f \cdot {\bf n} = \frac{R}{R^2 + r^2} .$$ Thus, in polar coordinates $$(r, \theta)$$ on $$F$$ centered at $$U$$, we have $$\iint_E \nabla f \cdot {\bf n} \,d\sigma = \int_0^{\frac{\pi}{3}} \int_0^{\frac{1}{2} R \lambda \sec \theta} \underbrace{\frac{R}{R^2 + r^2}}_{\nabla f \cdot {\bf n}} \underbrace{r \,dr \,d\theta}_{d\sigma}.$$ Computing the inner integral gives $$\frac{1}{2} R \int_0^{\frac{\pi}{3}} \log\left(\frac{1}{4} \lambda^2 \sec^2 \theta + 1\right) \,d\theta .$$ This integral, however, does not appear to have a closed form in terms of elementary functions. It does have an explicit formula in terms of dilogarithms, but it's too complicated to be worth reproducing here. I would anyway be pleased to see a more tractable expression for this quantity.

Edit I made some progress on this integral---replacing $$\frac{1}{2} \lambda$$ with $$\alpha$$ and applying Feynman's trick we can reduce computing this integral to understanding $$\frac{\arctan \beta \,d\beta}{\beta^2 - 3}$$. Maple gives a slightly nicer expression, but it still involves dilogarithms. I didn't push the (rather ugly) computation to its end, but the form of the expression suggests that the integral can be written in terms of elementary functions and three instances of Legendre's chi function. It's not clear whether one can improve on this.

At any rate, the flux of $$\nabla f$$ across $$S$$ is thus $$\iint_S \nabla f \cdot {\bf n} \,d\sigma = 60 \left[\int_0^{\frac{\pi}{3}} \log\left(\frac{1}{4} \lambda^2 \sec^2 \theta + 1\right) \,d\theta\right] R .$$ Integrating numerically gives that the quantity in brackets (just as well, the flux across the icosahedron with $$R = 1$$) is $$13.35031\!\ldots$$.

Since $$\nabla \cdot \nabla f > 0$$ everywhere, the Divergence Theorem gives that the flux across $$S$$ is between the fluxes of the spheres inscribing and circumscribing $$S$$, giving the cheap bounds $$4 \pi R < \iint_S \nabla f \cdot {\bf n} \,d\sigma < 4 \pi \sqrt{R^2 + \lambda^2} .$$

Remark Another reason to suspect that the question is not what the preparer intended is that the analogous problem in dimension $$2$$---computing the flux of the vector field $$\nabla \log\sqrt{x^2 + y^2}$$ across a regular polygon in $$\Bbb R^2$$ with the origin on its interior---does admit an efficient solution that uses the Divergence Theorem and the fact that $$\nabla \cdot \nabla \log\sqrt{x^2 + y^2} = 0$$. A vector field in $$\Bbb R^3 \setminus \{0\}$$ with this behavior is $$g(x, y, z) = (x^2 + y^2 + z^2)^{-1 / 2}$$.