The ∇operator and integration
16.
∫∫∫
V
∇f dV =
∫∫
S
feˆndS Special case of divergence theorem
17.
∫∫∫
V
∇× A dV =
∫∫
S
ˆen×A dS Special case of divergence theorem
18.
∫
C
©dr ×A=
∫∫
S
(ˆen×∇ )×A dS Special case of Stokes theorem
19.
∫
C
©f dr =
∫∫
S
dS×∇ f Special case of Stokes theorem
Vector Operators in curvilinear coordinates
In this section the concept of curvilinear coordinates is introduced and the rep-
resentation of scalars and vectors in these new coordinates are studied.
If associated with each point (x, y, z)of a rectangular coordinate system there is
a set of variables (u, v, w )such that x, y, z can be expressed in terms of u, v, w by a
set of functional relationships or transformations equations, then (u, v, w )are called
the curvilinear coordinates^2 (x, y, z ).Such transformation equations are expressible
in the form
x=x(u, v, w ), y =y(u, v, w ), z =z(u, v, w ) (8 .68)
and the inverse transformation can be expressed as
u=u(x, y, z ), v =v(x, y, z ) w=w(x, y, z) (8 .69)
It is assumed that the transformation equations (8.68) and (8.69) are single valued
and continuous functions with continuous derivatives. It is also assumed that the
transformation equations (8.68) are such that the inverse transformation (8.69) ex-
ists, because this condition assures us that the correspondence between the variables
(x, y, z )and (u, v, w )is a one-to-one correspondence.
The position vector
r =xˆe 1 +yˆe 2 +zˆe 3 (8 .70)
(^2) Note how coordinates are defined and the order of their representation because there are no standard repre-
sentation of angles or directions. Depending upon how variables are defined and represented, sometime left-hand
coordinates are confused with right-handed coordinates.