Suppose I wish to fine the flux of the curl of the vector field F(x,y,z) = vector brackets (-y(x + 1) + z^7cose(z), z, z^21 + zcos(xy)) Through the surface parameterized by: r(t,s) = vector brackets (scos(t), s sin(t), (1 - s)^2) O <= t <= 2pi 0 <= s <= 1 We could do that with the following surface integral: Flux = integral, integral D, curlF * (rt * rs)dA But given the complexity of the vector field andthe surface parameterization this could be very diffcult. If we ca determine the curve which bounds the bottom of the surface (shown in red on the surface) we can determine the flux o the curl of the vector field by a line integral. This is Stokes's Theorem in reverse. Letting s equal O and 1, choose the correct pair for: r(t, O) = ? r(t, 1) = ?

Advanced Engineering Mathematics
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ISBN:9780470458365
Author:Erwin Kreyszig
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Chapter2: Second-order Linear Odes
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Suppose I wish to fine the flux of the curl of the vector field
F(x,y,z)
= vector brackets (-y(x + 1) + z^7cose(z), z, z^21 + zcos(xy))
Through the surface parameterized by:
r(t,s) = vector brackets (scos(t), s sin(t), (1 - s)^2) 0 <= t <= 2pi 0 <= s <= 1
We could do that with the following surface integral:
Flux = integral, integral D, curlF * (rt * rs)dA
%3D
But given the complexity of the vector field andthe surface parameterization this could be very diffcult. If
we ca determine the curve which bounds the bottom of the surface (shown in red on the surface) we can
determine the flux o the curl of the vector field by a line integral. This is Stokes's Theorem in reverse. Letting
s equal O and 1, choose the correct pair for:
r(t, 0) = ?
r(t, 1) = ?
A.) r(t,0) = vector brackets (0, 0, 1) r(t,1) = vector brackets (cos(t), sin(t), 1)
B.) r(t,0) = vector brackets (0, 0, 0) r(t,1) = vector brackets (cos(t), sin(t), O)
C.) r(t,O) = vector brackets (0, 0, -1) r(t,1) = vector brackets (cos(t), sin(t), O)
D.) r(t,0) :
= vector brackets (0, 0, 1) r(t,1) = vector brackets (cos(t), sin(t), O)
E.) r(t,0) = vector brackets (0, 0, 1) r(t,1) = vector brackets (cos(t), sin(t), -1)
Transcribed Image Text:Suppose I wish to fine the flux of the curl of the vector field F(x,y,z) = vector brackets (-y(x + 1) + z^7cose(z), z, z^21 + zcos(xy)) Through the surface parameterized by: r(t,s) = vector brackets (scos(t), s sin(t), (1 - s)^2) 0 <= t <= 2pi 0 <= s <= 1 We could do that with the following surface integral: Flux = integral, integral D, curlF * (rt * rs)dA %3D But given the complexity of the vector field andthe surface parameterization this could be very diffcult. If we ca determine the curve which bounds the bottom of the surface (shown in red on the surface) we can determine the flux o the curl of the vector field by a line integral. This is Stokes's Theorem in reverse. Letting s equal O and 1, choose the correct pair for: r(t, 0) = ? r(t, 1) = ? A.) r(t,0) = vector brackets (0, 0, 1) r(t,1) = vector brackets (cos(t), sin(t), 1) B.) r(t,0) = vector brackets (0, 0, 0) r(t,1) = vector brackets (cos(t), sin(t), O) C.) r(t,O) = vector brackets (0, 0, -1) r(t,1) = vector brackets (cos(t), sin(t), O) D.) r(t,0) : = vector brackets (0, 0, 1) r(t,1) = vector brackets (cos(t), sin(t), O) E.) r(t,0) = vector brackets (0, 0, 1) r(t,1) = vector brackets (cos(t), sin(t), -1)
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