← 2019 Paper 1

UPSC 2019 Maths Optional Paper 1 Q8c-i — Step-by-Step Solution

15 marks · Section B

Gauss divergence theorem · Vector Analysis · asked 10× in 14 yrs · Read the full method →

Question

State Gauss divergence theorem. Verify this theorem for F⃗=4xi^−2y2j^+z2k^\vec F=4x\hat i-2y^2\hat j+z^2\hat k, taken over the region bounded by x2+y2=4, z=0x^2+y^2=4,\ z=0 and z=3z=3.

Technique

Compute ∇⋅F⃗=4−4y+2z\nabla\cdot\vec F=4-4y+2z and integrate over the cylinder (odd yy-term vanishes by symmetry); compute the flux through the three faces separately and sum.

Solution

Statement (Gauss divergence theorem)

Let VV be a closed bounded region in R3\mathbb R^3 with piecewise-smooth boundary surface SS and outward unit normal n^\hat n. If F⃗\vec F is continuously differentiable on VV, then

∭V(∇⋅F⃗) dV=∬SF⃗⋅n^ dS.\iiint_V (\nabla\cdot\vec F)\,dV=\iint_S \vec F\cdot\hat n\,dS.

Here VV is the solid cylinder x2+y2≤4, 0≤z≤3x^2+y^2\le4,\ 0\le z\le3, and SS is its surface (top disk z=3z=3, bottom disk z=0z=0, lateral surface x2+y2=4x^2+y^2=4). The radius is 22.

Step 1 — Volume integral of the divergence

∇⋅F⃗=∂(4x)∂x+∂(−2y2)∂y+∂(z2)∂z=4−4y+2z.\nabla\cdot\vec F=\frac{\partial(4x)}{\partial x}+\frac{\partial(-2y^2)}{\partial y}+\frac{\partial(z^2)}{\partial z}=4-4y+2z.

In cylindrical coordinates (x=rcos⁡θ, y=rsin⁡θx=r\cos\theta,\ y=r\sin\theta, dV=r dr dθ dzdV=r\,dr\,d\theta\,dz), the −4y-4y term integrates to zero over a full revolution. So

∭V(4−4y+2z) dV=∫03 ⁣ ⁣∫02π ⁣ ⁣∫02(4+2z) r dr dθ dz\iiint_V(4-4y+2z)\,dV=\int_0^3\!\!\int_0^{2\pi}\!\!\int_0^2(4+2z)\,r\,dr\,d\theta\,dz

(the −4y=−4rsin⁡θ-4y=-4r\sin\theta term vanishes on ∫02πsin⁡θ dθ=0\int_0^{2\pi}\sin\theta\,d\theta=0). The remaining integral factorises:

∫02r dr=2,∫02πdθ=2π,∫03(4+2z) dz=12+9=21,\int_0^2 r\,dr=2,\qquad \int_0^{2\pi}d\theta=2\pi,\qquad \int_0^3(4+2z)\,dz=12+9=21,

so

∭V∇⋅F⃗ dV=2⋅2π⋅21=84π.\iiint_V\nabla\cdot\vec F\,dV=2\cdot2\pi\cdot21=84\pi.

Step 2 — Surface integral (three faces)

Top disk z=3z=3, n^=+k^\hat n=+\hat k: F⃗⋅n^=z2=9\vec F\cdot\hat n=z^2=9. Area =π(2)2=4π=\pi(2)^2=4\pi:

∬top=9⋅4π=36π.\iint_{\text{top}}=9\cdot4\pi=36\pi.

Bottom disk z=0z=0, n^=−k^\hat n=-\hat k: F⃗⋅n^=−z2=0\vec F\cdot\hat n=-z^2=0:

∬bottom=0.\iint_{\text{bottom}}=0.

Lateral surface x2+y2=4x^2+y^2=4: outward normal n^=(x,y,0)2=(cos⁡θ,sin⁡θ,0)\hat n=\dfrac{(x,y,0)}{2}=(\cos\theta,\sin\theta,0), with x=2cos⁡θ, y=2sin⁡θx=2\cos\theta,\ y=2\sin\theta, surface element dS=2 dθ dzdS=2\,d\theta\,dz (radius ×dθ×dz\times d\theta\times dz):

F⃗⋅n^=4xcos⁡θ−2y2sin⁡θ=4(2cos⁡θ)cos⁡θ−2(2sin⁡θ)2sin⁡θ=8cos⁡2θ−8sin⁡3θ.\vec F\cdot\hat n=4x\cos\theta-2y^2\sin\theta=4(2\cos\theta)\cos\theta-2(2\sin\theta)^2\sin\theta=8\cos^2\theta-8\sin^3\theta. ∬lat=∫03 ⁣ ⁣∫02π(8cos⁡2θ−8sin⁡3θ)⋅2 dθ dz.\iint_{\text{lat}}=\int_0^3\!\!\int_0^{2\pi}(8\cos^2\theta-8\sin^3\theta)\cdot2\,d\theta\,dz.

Over a full period ∫02πcos⁡2θ dθ=π\int_0^{2\pi}\cos^2\theta\,d\theta=\pi and ∫02πsin⁡3θ dθ=0\int_0^{2\pi}\sin^3\theta\,d\theta=0, so the θ\theta-integral is 8π8\pi. Then

∬lat=∫032⋅8π dz=16π⋅3=48π.\iint_{\text{lat}}=\int_0^3 2\cdot8\pi\,dz=16\pi\cdot3=48\pi.

Total flux:

∬SF⃗⋅n^ dS=36π+0+48π=84π.\iint_S\vec F\cdot\hat n\,dS=36\pi+0+48\pi=84\pi.

Step 3 — Conclusion

Answer

  ∭V∇⋅F⃗ dV=84π=∬SF⃗⋅n^ dS.  \boxed{\;\iiint_V\nabla\cdot\vec F\,dV=84\pi=\iint_S\vec F\cdot\hat n\,dS.\;}
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