Note: You need the
Symbol
font (68 kB)
in order to display various symbols correctly, such as
(otherwise they appear as
p, r, q and f ).
Find the Fourier series expansion on the interval (–1, 1) of the function
The function f (x) is odd
(using the symmetry property for integrals of odd functions)
Therefore the Fourier series for f (x)
on (–1, 1) is
The plot below illustrates how good an approximation the Fourier series is, even after the partial sum of only the first two terms:
The vector field
is defined by
.
Show that
everywhere in
3.
Hence evaluate
,
where S is the surface of the sphere
of radius 1 and centre at
[You may express your answer in terms of p.]
By Gauss’ divergence theorem,
where V is the volume enclosed by
S .
But the volume of a sphere of radius 1 is
.
Therefore the flux through the sphere is
In spherical polar coordinates (r, q,
f), a scalar function V is
defined on the domain
W = { all of
3
except the z-axis } by
V(r, q, f) = ln (r sin q )
Find
in spherical polar coordinates.
Therefore, in spherical polar coordinates,
Express V as a function of the Cartesian coordinates (x, y, z) only.
Use your answer to part (b) to find
in Cartesian coordinates.
Show that your answers to parts (a) and (c) are equivalent by using the appropriate coordinate conversion matrix.
Either
First note that
Converting the answer to part (c) into spherical polar
coordinates,
which matches the answer to part (a)
or
Converting the answer to part (a) into Cartesian
coordinates,
which matches the answer to part (c)
Find the Laplacian
in one of the two coordinate systems.
Either in spherical polar coordinates
(except possibly on the z-axis, where
r sin q = 0).
Therefore on W
or in Cartesian coordinates
Is V harmonic on any domain that excludes the z axis?
YES |
---|
For the partial differential equation
Classify this partial differential equation (as one of hyperbolic, parabolic or elliptic).
Therefore the PDE is
hyperbolic |
---|
Find the general solution u(x, y).
The complementary function is
(where f and g
are arbitrary functions).
The right side is a zero order polynomial (a constant)
For the particular solution, try second order polynomials,
without the lower order terms:
Substitute this trial particular solution into the PDE:
There is only one constraint on three unknowns, leaving two
free choices.
Choose a = b = 0, then c = 1.
[Other choices are valid, but this is the easiest.]
The particular solution is
uP = y2 and the
general solution is
The choice b = 0 , a = c
leads to the alternative form
Using the additional information
Find the complete solution u(x, y).
Following the choice made in part (b),
[The choice 2(B) + (C)
to find f(x) first is
also valid.]
Substituting g(–2x)
back into equation (A):
[Note that the arbitrary constants of integration for
the two functions f(x)
and g(x) cancel each other
out.]
The general solution becomes the complete solution
The complete solution is therefore
[It is easy to verify that this solution does satisfy the PDE and both conditions.]
Find the equations of the line of force for the vector field
that passes through the point
Therefore the family of lines of force is
[The solution
is part of this general solution.]
The required line of force passes through (1, 1, 1).
Therefore the required line of force is
A vector
is defined in the cylindrical polar coordinate system by
.
Find the derivative
in terms of
.
Therefore
Show whether or not a potential function exists for
and, if it does exist, on what domain.
Therefore
a potential function does not exist
anywhere in ![]() |
Find the value of the line integral
where C is the arc of the parabola
y = x2 between
Check for any potential function:
A potential function therefore exists and the value of the
line integral is simply the potential difference between
the two endpoints.
Therefore
OR
The line integral can be evaluated directly.
Along the parabolic path the natural parameters are
Note that the inverse of y = x2
is
along the right half of the path (x=0 to x=1),
but is
along the left half of the path (x=–1 to x=0).
Another direct evaluation of the line integral is therefore
A shell is in the shape of that part of the ellipsoid
that is above the x-y plane (z > 0).
Its surface density is
Find the mass m of this shell.
Note: For the upper half of the general ellipsoid
,
a parametric net is (q, f),
such that
.
For the projection method, start with
.
If necessary, you may quote
.
Either method (parametric net or projection) may be used in
this question.
Parametric Net Method:
For this ellipsoid,
a = 3, b = 2, c = 1
The outward normal vector at every point on the ellipsoid is
Converting the density function to the new coordinate system:
The mass of the shell is
Therefore the mass of the shell is
OR
Projection Method:
A normal vector to the surface is
The mass of the shell is then
where A is the area of the shadow of
the ellipsoid on the x-y plane, that is,
the area of an ellipse of semi-major axis
a = 3 and semi-minor axis
b = 2.
Therefore the mass of the shell is
In the event that the formula for the area of an ellipse
is not immediately available, the area can be calculated
in Cartesian coordinates as follows.
The area of the entire ellipse is four times the area of that
part of the ellipse in the first quadrant.
Using the integration identity in the question,
.
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Created 2008 04 27 and most recently modified 2008 04 29 by Dr. G.H. George