Chapter7
Vector Calculus I
One aspect of vector calculus can be described as taking many of the concepts
from scalar calculus, generalizing these concepts and representing them in a vector
format. These alternative vector representations have many applications in repre-
senting two-dimensional and three-dimensional physical problems. Let us begin by
examining the representation of curves using vectors.
Curves
Atwo-dimensional curve can be defined
(i) Explicitly y=f(x)
(ii) Implicitly F(x, y ) = 0
(iii) Parametrically x=x(t), y =y(t)
(iv ) As a vector r =r (t) = x(t)eˆ 1 +y(t)ˆe 2 or r =r (x) = xˆe 1 +f(x)ˆe 2
Athree-dimensional curve can be defined
(i) Parametrically x=x(t), y =y(t), z =z(t)
(ii) As a vector r =r (t) = x(t)ˆe 1 +y(t)eˆ 2 +z(t)eˆ 3
(iii) A curve in space is sometimes defined as the intersection of two surfaces
F(x, y, z ) = 0 and G(x, y, z ) = 0 and in this special case the curve
is defined by a set of (x, y, z)values which are common to both surfaces.
It is assumed that the functions used to define these curves are continuous single-
valued functions which are everywhere differentiable. Also note that the parametric
and vector representations of a curve are not unique.