Question #197816

 Verify Stokes’ theorem for 𝐴 = 2𝑥 − 𝑦 𝑖 − 𝑦𝑧2 𝑗 − 𝑦2𝑧𝑘, where S is the upper half of the sphere 𝑥2+ 𝑦2 + 𝑧2 = 1 and C is its boundary.


Expert's answer

∫CF⃗⋅dr⃗=∫∫ScurlF⃗⋅n^dS  (Stoke′s Theorem)\int_C\vec F\cdot \vec{dr}=\int\int_S curl \vec F\cdot \hat ndS\ \ (Stoke's\ Theorem)


where C is the circle: x2+y2=1, z=0  (xy−plane)x^2+y^2=1,\ z=0\ \ (xy-plane)


i.e. x=cost, y=sint, z=0x=cost,\ y=sint,\ z=0

r=xi⃗+yj⃗ where  0≤θ≤2πdr⃗=dxi⃗+dyj⃗r=x\vec i+y\vec j\ where\ \ 0\leq \theta\leq 2\pi\\\vec{dr}=dx\vec i+dy\vec j


where,

F⃗=(2x−y)i⃗−yz2j⃗−y2zk⃗∴F⃗⋅dr⃗=(2x−y)dx (since z=0)\vec F=(2x-y)\vec i-yz^2\vec j-y^2z\vec k\\\therefore\vec F\cdot \vec{dr}=(2x-y)dx\ (since\ z=0 )


LHS =∫CF⃗⋅dr⃗=∫C(2x−y)dx= \int_C \vec F\cdot \vec{dr}=\int_C(2x-y)dx


=∫02π(2cost−sint)(−sint)dt =∫02π(sin2t−2costsint)dt =∫02π{12(1−cos2t)−sin2t}dt =[t2−sin2t4−cos2t2]o2π =(12−12)+(π−0) =π=\int_0^{2\pi}(2cost-sint)(-sint)dt\\\ \\=\int_0^{2\pi}(sin^2t-2costsint)dt\\\ \\=\int_0^{2\pi}\{\frac{1}{2}(1-cos2t)-sin2t\}dt\\\ \\=[\dfrac{t}{2}-\dfrac{sin2t}{4}-\dfrac{cos2t}{2}]_o^{2\pi}\\\ \\=(\dfrac{1}{2}-\dfrac{1}{2})+(\pi-0)\\\ \\=\pi


Hence, F⃗⋅dr⃗=π   .....(1)\vec F\cdot \vec{dr}=\pi\ \ \ .....(1)


Also,

curl  F⃗=▽×F⃗curl \ \ \vec F=\triangledown \times \vec F

=∣i⃗j⃗k⃗δδxδδyδδz2x−y−yz2−y2z∣ =i⃗(−2yz+2yz)−j⃗(0)+k⃗(0+1)=k⃗= \begin{vmatrix} \vec i & \vec j&\vec k \\ \frac{\delta}{\delta x} & \frac{\delta}{\delta y}&\frac{\delta}{\delta z}\\ 2x-y&-yz^2&-y^2z \end{vmatrix}\\\ \\=\vec i(-2yz+2yz)-\vec j (0)+\vec k (0+1)\\=\vec k


∴dS⃗=n^dS=dydz i+dzdx j+dxdy k\therefore \vec {dS}=\hat n dS\\=dydz\ i+dzdx\ j+dxdy\ k


Hence,

RHS = ∫∫S curl F⃗⋅n^dS=∫∫dxdy=π  .....(2)RHS\ =\ \int\int_S\ curl\ \vec F\cdot \hat {n}dS=\int\int dxdy=\pi\ \ .....(2)


Since,  ∫∫dxdySince,\ \ \int\int dxdy represent the area of the circle x2+y2=1x^2+y^2=1 which is π\pi


Thus, from (1) and (2) we conclude that the theorem is verified.


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