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UPSC 2020 Maths Optional Paper 1 Q8b — Step-by-Step Solution

15 marks · Section B

Stokes' theorem · Vector Analysis · asked 10× in 14 yrs · Read the full method →

Question

Evaluate the surface integral ∬S∇×F⃗⋅n^ dS\iint_S \nabla\times\vec F\cdot\hat n\,dS for F⃗=yi^+(x−2xz)j^−xyk^\vec F=y\hat i+(x-2xz)\hat j-xy\hat k and SS is the surface of the sphere x2+y2+z2=a2x^2+y^2+z^2=a^2 above the xyxy-plane.

Technique

Stokes’ theorem replaces the hemisphere flux by the circulation around the bounding circle z=0z=0; the integrand collapses to the exact differential d(xy)d(xy), hence 00. Cross-checked by direct spherical integration and the cap-vs-disk (solenoidal-curl) argument.

Solution

SS is the upper hemisphere; its boundary ∂S\partial S is the circle x2+y2=a2x^2+y^2=a^2, z=0z=0. By Stokes’ theorem the flux of the curl through SS equals the circulation of F⃗\vec F around ∂S\partial S:

∬S(∇×F⃗)⋅n^ dS=∮∂SF⃗⋅dr⃗.\iint_S(\nabla\times\vec F)\cdot\hat n\,dS=\oint_{\partial S}\vec F\cdot d\vec r .

Step 1 — (For reference) the curl

∇×F⃗=(∂y(−xy)−∂z(x−2xz))i^+(∂z(y)−∂x(−xy))j^+(∂x(x−2xz)−∂y(y))k^\nabla\times\vec F=\Big(\partial_y(-xy)-\partial_z(x-2xz)\Big)\hat i+\Big(\partial_z(y)-\partial_x(-xy)\Big)\hat j+\Big(\partial_x(x-2xz)-\partial_y(y)\Big)\hat k =(−x−(−2x))i^+(0−(−y))j^+((1−2z)−1)k^=x i^+y j^−2z k^.=(-x-(-2x))\hat i+(0-(-y))\hat j+((1-2z)-1)\hat k=x\,\hat i+y\,\hat j-2z\,\hat k .

Step 2 — Reduce to the boundary circle

On ∂S\partial S we have z=0z=0, so there F⃗=y i^+x j^−xy k^\vec F=y\,\hat i+x\,\hat j-xy\,\hat k, and along the curve dz=0dz=0. Hence

F⃗⋅dr⃗=y dx+x dy=d(xy).\vec F\cdot d\vec r=y\,dx+x\,dy=d(xy).

Since xyxy is single-valued and the boundary is a closed curve,

∮∂SF⃗⋅dr⃗=∮∂Sd(xy)=0.\oint_{\partial S}\vec F\cdot d\vec r=\oint_{\partial S}d(xy)=0 .

(Explicitly, with x=acos⁡t, y=asin⁡t, t:0→2πx=a\cos t,\ y=a\sin t,\ t:0\to2\pi for the upward-normal orientation: ∫02π[asin⁡t(−asin⁡t)+acos⁡t(acos⁡t)]dt=∫02πa2cos⁡2t dt=0\int_0^{2\pi}\big[a\sin t(-a\sin t)+a\cos t(a\cos t)\big]dt=\int_0^{2\pi}a^2\cos 2t\,dt=0.)

Answer

 ∬S(∇×F⃗)⋅n^ dS=0 \boxed{\,\iint_S(\nabla\times\vec F)\cdot\hat n\,dS=0\,}
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