Convert F from Cartesian coordinates to spherical polar coordinates.
Relative to the coordinate axes, in what direction is F pointing?
The coordinate conversion matrix A for Cartesian coordinates to spherical polar coordinates is
so that Fsph = A Fcart where
![[ F_r ]
F = [ F_theta ] ,
sph [ F_phi ]
F = F_r r^ + F_theta theta^ + F_phi phi^](p4/q2vecsph1.gif)
![[ F_x ]
F = [ F_y ] and
cart [ F_z ]
F = F_x i + F_y j + F_z k](p4/q2veccart1.gif)
Show that the conversion matrix B for the
inverse conversion from spherical polar back to Cartesian coordinates,
such that
B = AT (the transpose of matrix A).
Convert from spherical polar to Cartesian coordinates the vector field
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Find the divergence and curl of each of the following:
For the vector field defined in spherical polar coordinates by
![]()
find
.
Consider the purely radial vector field
F (r, q, f) =
f (r)
, where
is the unit radial vector in the
spherical polar coordinate system and f (r)
is any function of r that is differentiable everywhere
in
(except possibly at the origin).
Of particular interest is the central force law
![]()
Show that the divergence of F vanishes
everywhere in
(except possibly at the origin) if and only if
[Two of the four fundamental forces of nature, electromagnetism and
gravity, both obey this inverse square law.]
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