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Use Stokes' Theorem to evaluate the double integral of the curl of F

F(x, y, z) = e^(xy) cos(z)i + x^2 zj + xyk,

S is the hemisphere
x = radical 49 − y^2 − z^2
oriented in the direction of the positive x-axis.

User Abbood
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Stokes' theorem relates the surface integral of the curl of
\vec F across
S to the line integral of
\vec F along the boundary of
S.

The boundary of
S is a circle with radius 7 centered at the origin in the
x,y-plane. Parameterize this path by


\vec r(t) = 7\cos(t)\,\vec\imath + 7\sin(t)\,\vec\jmath

with
0\le t\le2\pi. Observe that
z=0, so
\cos(z) = 1 and the
\vec\jmath-component of
\vec F contributes nothing. The double integral then reduces to


\displaystyle \iint_S (\\abla*\vec F)\cdot d\vec S = \int_0^(2\pi) \vec F(\vec r(t)) \cdot (d\vec r)/(dt) \, dt \\\\ ~~~~~~~~ = \int_0^(2\pi) \left(e^(49\cos(t)\sin(t))\,\vec\imath + 49\cos(t)\sin(t)\,\vec\jmath\right) \cdot \left(-7\sin(t)\,\vec\imath + 7\cos(t)\,\vec\jmath\right) \, dt \\\\ ~~~~~~~~ = -7 \int_0^(2\pi) e^(49\cos(t)\sin(t)) \sin(t) \, dt

Observe that by substituting
t=u+\pi, we have


\sin(t) = \sin(u+\pi) = \sin(u)\cos(\pi) + \cos(u)\sin(\pi) = -\sin(u)

so that the integral over
[\pi,2\pi] can be expressed in terms of the integral over
[0,\pi] as


\displaystyle \int_\pi^(2\pi) e^(49\cos(t)\sin(t)) \sin(t) \, dt = \int_0^\pi -e^(49\cos(t)\sin(t)) \sin(t) \, dt

Then the integrals over
[0,\pi] and
[\pi,2\pi] cancel each other and integral of the curl of
\vec F is


\displaystyle -7 \int_0^(2\pi) e^(49\cos(t)\sin(t)) \sin(t) \, dt = -7 \int_0^\pi 0 \, dt = \boxed{0}

User Get
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