In this page, we will define vector field, divergence and
cross product and introduce gradient vector fields and curl
vector fields.
If to each point (x, y, z) of a domain D in the space a vector v =
v(x, y, z) is assigned, then a vector field is said to be given
in D.
Each vector v is regarded as to attach to the corresponding point
(x, y,
z). A good example of vector fields is the gravitational force. It attaches
a vector representing the direction and magnitude of gravity to each point
in
the space.
where
= xi + yj + zk is the vector from origin
to P, r is its magnitude
and k is a universal
constant. See the graph below for the vector field
F.
This is illustrated in the following two graphs around the neighbourhoods
of
(1, 0) and (-1, 0) and can be interpreted as the electric force
field due to two infinite straight wires, perpendicular to the xy plane at
(1, 0) and (-1, 0), homogeneously and oppositely charged with electricity.
Note that the second graph below is the zoom in around (1, 0) of
the first
graph.
For each vector field F = Pi + Qj + Rk in a domain D, if all P, Q, R have first partial derivatives in D, its divergence div F is defined as :
The divergence has a definite physical significance. In fluid dynamics it appeara as a measure of the rate of decease of density at a point. The divergence also play an important part in the theory of electromagnetic fields. It has the following properties:
There are vector fields derived from differentiable functions of multivariable. Let f(x, y, z) be a differentiable function of three variables, then its gradient vector field is defined as
The cross product between vector fields and/or vectors could
produce
vector fields. The definition of cross product is as follows:
Let A = ai + bj + ck and B = di
+ ej
+ fk, then their cross product is defined as
Clearly, their cross product vector k is perpendicular to both A and B. In fact, this is one of the important properties of cross product among the following:
The curl vector field of the vector field F = Pi + Qj + Rk is defined as:
when all P, Q, R have first partial derivatives.
The curl is important in the analysis of the velocity fields of fluid dynamics
and in the analysis of electromagnetic force fields. The curl can be
interpreted as measuring angular motion of a fluid and the condition curl
F = 0 for a velocity field F characterizes what are termed
irrotational flows. The analogous equation curl E = 0
for the
electric force vector E holds when only electrostatic forces are
present. The curl satisfies the basic laws:
If we take G = grad T of Example 4, it is easy to see that curl G = 0. Readers are encouraged to verified the property: curl grad f = 0 for each twice differentiable function f.