Consider the vector ficld Co sin 0 A(r,0, ¢) – which (although irrelevant to solving this problem) corresponds to the magnetic vec- tor potential outside of a spherical solid object of uniform charge density spinning at a constant angular velocity and centered at the origin. Calculate the flux of the curl of A upwards through a flat disk of radius so and height zo above the origin (see the figure below).. 0- (a) by computing the surface integral of V × A through the disk directly. (b) by using Stokes' theorem to convert the surface integral into a line integral around the disk boundary, and then solving for that instead.

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Author:Robert L. Boylestad
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Consider the vector ficld
Co sin
A(r,8, 6) –
r2
which (although irrelevant to solving this problem) corresponds to the magnetic vec-
tor potential outside of a spherical solid object of uniform charge density spinning at
a constant angular velocity and centered at the origin. Calculate the flux of the curl
of A upwards through a flat disk of radius so and height zo above the origin (sce the
figure below).
(a) by computing the surface integral of V x A through the disk dircctly.
(b) by using Stokcs' theorem to convert the surface integral into a line integral around the
disk boundary, and then solving for that instead.
N°
Transcribed Image Text:Consider the vector ficld Co sin A(r,8, 6) – r2 which (although irrelevant to solving this problem) corresponds to the magnetic vec- tor potential outside of a spherical solid object of uniform charge density spinning at a constant angular velocity and centered at the origin. Calculate the flux of the curl of A upwards through a flat disk of radius so and height zo above the origin (sce the figure below). (a) by computing the surface integral of V x A through the disk dircctly. (b) by using Stokcs' theorem to convert the surface integral into a line integral around the disk boundary, and then solving for that instead. N°
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