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Calculus · real student question

Evaluate the triple integral of sin of (x squared + y squared + z squared) to the power 3/2, over the region between the cone z = root of 3(x squared + y squared) and the sphere z = root of (1 - x squared - y squared).

Question

Evaluate ∬Dxydx dy∫3(x2+y2)1−x2−y2sin⁡ ⁣((x2+y2+z2)3/2)dz.\iint_{D_{xy}}dx\,dy\int_{\sqrt{3(x^2+y^2)}}^{\sqrt{1-x^2-y^2}}\sin\!\left((x^2+y^2+z^2)^{3/2}\right)dz.

Step-by-step solution

  1. Identify the solid. The lower surface z=3 rz=\sqrt{3}\,r (with r2=x2+y2r^2=x^2+y^2) is a cone, and the upper surface z=1−r2z=\sqrt{1-r^2} is the upper unit hemisphere. They meet where 3 r=1−r2\sqrt3\,r=\sqrt{1-r^2}, i.e. 3r2=1−r23r^2=1-r^2, so r=12r=\tfrac12: the region is the classic 'ice-cream cone' between the cone and the unit sphere, projecting onto the disc r≤12r\le\tfrac12.

  2. Choose spherical coordinates, not cylindrical. The integrand depends only on x2+y2+z2=ρ2x^2+y^2+z^2 = \rho^2, so in spherical coordinates it becomes sin⁡(ρ3)\sin(\rho^3) - a function of one variable. Cylindrical coordinates would leave an inseparable sin⁡ ⁣((r2+z2)3/2)\sin\!\left((r^2+z^2)^{3/2}\right), which is why the conversion has to go all the way to spherical.

  3. Convert the cone into a constant polar angle. On the cone, tan⁡φ=rz=13\tan\varphi = \dfrac{r}{z} = \dfrac{1}{\sqrt3}, so φ=π6\varphi = \dfrac{\pi}{6}. The solid is therefore 0≤ρ≤1,0≤φ≤π6,0≤θ≤2π,0\le\rho\le1,\qquad 0\le\varphi\le\frac{\pi}{6},\qquad 0\le\theta\le2\pi, with volume element dV=ρ2sin⁡φ dρ dφ dθdV=\rho^2\sin\varphi\,d\rho\,d\varphi\,d\theta.

  4. Separate the triple integral into three single ones. I=∫02π ⁣dθ∫0π/6 ⁣sin⁡φ dφ∫01ρ2sin⁡(ρ3) dρ.I = \int_0^{2\pi}\!d\theta\int_0^{\pi/6}\!\sin\varphi\,d\varphi\int_0^{1}\rho^2\sin(\rho^3)\,d\rho. Each factor now involves a single variable.

  5. Evaluate each factor. ∫02πdθ=2π\int_0^{2\pi}d\theta = 2\pi; ∫0π/6sin⁡φ dφ=1−cos⁡π6=1−32\int_0^{\pi/6}\sin\varphi\,d\varphi = 1-\cos\tfrac{\pi}{6} = 1-\tfrac{\sqrt3}{2}; and with u=ρ3u=\rho^3, du=3ρ2dρdu=3\rho^2 d\rho, ∫01ρ2sin⁡(ρ3) dρ=13∫01sin⁡u du=1−cos⁡13.\int_0^1\rho^2\sin(\rho^3)\,d\rho = \frac13\int_0^1\sin u\,du = \frac{1-\cos 1}{3}. The ρ2\rho^2 from the volume element is exactly what makes this substitution work.

  6. Multiply and check. I=2π(1−32)1−cos⁡13≈2π(0.133975)(0.153233)≈0.128989.I = 2\pi\left(1-\frac{\sqrt3}{2}\right)\frac{1-\cos 1}{3} \approx 2\pi(0.133975)(0.153233) \approx 0.128989. Nested numerical quadrature of the original cylindrical form gives 0.12898921380.1289892138, matching to nine decimals.

Answer

2π3(1−32)(1−cos⁡1)≈0.128989\frac{2\pi}{3}\left(1-\frac{\sqrt3}{2}\right)\left(1-\cos 1\right) \approx 0.128989

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