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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 13 yrs · Read the full method →
Question
Evaluate the surface integral ∬ S ∇ × F ⃗ ⋅ n ^ d S \iint_S \nabla\times\vec F\cdot\hat n\,dS ∬ S ∇ × F ⋅ n ^ d S for F ⃗ = y i ^ + ( x − 2 x z ) j ^ − x y k ^ \vec F=y\hat i+(x-2xz)\hat j-xy\hat k F = y i ^ + ( x − 2 x z ) j ^ − x y k ^ and S S S is the surface of the sphere x 2 + y 2 + z 2 = a 2 x^2+y^2+z^2=a^2 x 2 + y 2 + z 2 = a 2 above the x y xy x y -plane.
Technique
Stokes’ theorem replaces the hemisphere flux by the circulation around the bounding circle z = 0 z=0 z = 0 ; the integrand collapses to the exact differential d ( x y ) d(xy) d ( x y ) , hence 0 0 0 . Cross-checked by direct spherical integration and the cap-vs-disk (solenoidal-curl) argument.
Solution
S S S is the upper hemisphere; its boundary ∂ S \partial S ∂ S is the circle x 2 + y 2 = a 2 x^2+y^2=a^2 x 2 + y 2 = a 2 , z = 0 z=0 z = 0 . By Stokes’ theorem the flux of the curl through S S S equals the circulation of F ⃗ \vec F F around ∂ S \partial S ∂ S :
∬ S ( ∇ × F ⃗ ) ⋅ n ^ d S = ∮ ∂ S F ⃗ ⋅ d r ⃗ . \iint_S(\nabla\times\vec F)\cdot\hat n\,dS=\oint_{\partial S}\vec F\cdot d\vec r . ∬ S ( ∇ × F ) ⋅ n ^ d S = ∮ ∂ S F ⋅ d r .
Step 1 — (For reference) the curl
∇ × F ⃗ = ( ∂ y ( − x y ) − ∂ z ( x − 2 x z ) ) i ^ + ( ∂ z ( y ) − ∂ x ( − x y ) ) j ^ + ( ∂ x ( x − 2 x z ) − ∂ 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 ∇ × F = ( ∂ y ( − x y ) − ∂ z ( x − 2 x z ) ) i ^ + ( ∂ z ( y ) − ∂ x ( − x y ) ) j ^ + ( ∂ x ( x − 2 x z ) − ∂ y ( y ) ) k ^
= ( − x − ( − 2 x ) ) i ^ + ( 0 − ( − y ) ) j ^ + ( ( 1 − 2 z ) − 1 ) k ^ = x i ^ + y j ^ − 2 z k ^ . =(-x-(-2x))\hat i+(0-(-y))\hat j+((1-2z)-1)\hat k=x\,\hat i+y\,\hat j-2z\,\hat k . = ( − x − ( − 2 x )) i ^ + ( 0 − ( − y )) j ^ + (( 1 − 2 z ) − 1 ) k ^ = x i ^ + y j ^ − 2 z k ^ .
Step 2 — Reduce to the boundary circle
On ∂ S \partial S ∂ S we have z = 0 z=0 z = 0 , so there F ⃗ = y i ^ + x j ^ − x y k ^ \vec F=y\,\hat i+x\,\hat j-xy\,\hat k F = y i ^ + x j ^ − x y k ^ , and along the curve d z = 0 dz=0 d z = 0 . Hence
F ⃗ ⋅ d r ⃗ = y d x + x d y = d ( x y ) . \vec F\cdot d\vec r=y\,dx+x\,dy=d(xy). F ⋅ d r = y d x + x d y = d ( x y ) .
Since x y xy x y is single-valued and the boundary is a closed curve,
∮ ∂ S F ⃗ ⋅ d r ⃗ = ∮ ∂ S d ( x y ) = 0. \oint_{\partial S}\vec F\cdot d\vec r=\oint_{\partial S}d(xy)=0 . ∮ ∂ S F ⋅ d r = ∮ ∂ S d ( x y ) = 0.
(Explicitly, with x = a cos t , y = a sin t , t : 0 → 2 π x=a\cos t,\ y=a\sin t,\ t:0\to2\pi x = a cos t , y = a sin t , t : 0 → 2 π for the upward-normal orientation: ∫ 0 2 π [ a sin t ( − a sin t ) + a cos t ( a cos t ) ] d t = ∫ 0 2 π a 2 cos 2 t d t = 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 ∫ 0 2 π [ a sin t ( − a sin t ) + a cos t ( a cos t ) ] d t = ∫ 0 2 π a 2 cos 2 t d t = 0 .)
Answer
∬ S ( ∇ × F ⃗ ) ⋅ n ^ d S = 0 \boxed{\,\iint_S(\nabla\times\vec F)\cdot\hat n\,dS=0\,} ∬ S ( ∇ × F ) ⋅ n ^ d S = 0