For the vector function
in the x-y plane:
The vector function
is obviously well-defined (and infinitely
differentiable) everywhere except the origin.
The distance of the origin (0, 0) from the point (2, 2) is
The only singularity is outside
.
Green’s theorem is therefore valid everywhere on
.
Green’s theorem
everywhere in the domain, including within C .
[The direct evaluation of the line integral is very difficult and should be avoided!]
For the vector field
:
Therefore
is irrotational everywhere and a potential function
exists.
The potential function
is such that
where f (y, z) is an
arbitrary function of integration
where g (z) is another
arbitrary function of integration
The potential function is therefore
where C is an
arbitrary constant of integration.
However, we require that the potential be zero at the
origin:
The potential function is therefore
A sheet is in the shape of that part of the circular
paraboloid
that lies between the circular cylinders
The sheet has a surface density of
Let r2 =
x2 + y2
then the equation of the circular paraboloid becomes
Use the parametric grid (r, q), such
that
The ranges of the parameters are
2 < r < 4 and
0 < q < 2p.
The tangent vectors along the coordinate grid lines are
A normal vector to the surface at every point is
By symmetry,
Taking moments about the x-y plane,
Therefore the centre of mass of the sheet is located at
[Note that the centroid is located exactly half way between the bottom and top of the sheet. As z increases, the decreasing surface area compensates exactly for the increasing surface density.]
An alternative solution, using the projection method, is available from this link.