Line Integral
line integral
[′līn ¦int·ə·grəl]Line Integral
an integral taken along some curve in the plane or in space. We distinguish line integrals of the first kind and line integrals of the second kind. A line integral of the first kind arises, for example, in problems involving the calculation of the mass of a curve of variable density and is denoted by
∫Cf (P)ds
where C is the given curve, ds is the differential of its arc, and f(P) is the function of a point on the curve and is the limit of the corresponding integral sums. In the case of a plane curve C given by the equation y = y(x), a line integral of the first kind reduces to an ordinary integral. Specifically,
A line integral of the second kind arises, for example, in connection with the work of a force field. In the case of a plane curve C the integral takes the form
∫CP(x,y)dx + Q(x,y)dy
and is also the limit of the corresponding integral sums. A line integral of the second kind can be expressed as an ordinary integral. Specifically,
wherex = x(t) and y = y(t) for α ≤ t ≤ β, is the parametric equation of the curve C. Its connection with a line integral of the first kind is given by the equality
∫CP(x,y)dx + Q (x,y)dy = ∫C {P cosα + Q sin α} ds
Here, α is the angle between the Ox axis and the tangent to the curve pointing in the direction of the increasing arc length.
A line integral of the second kind in space is defined similarly. (SeeVECTOR CALCULUS for a treatment of line integrals of the second kind from the standpoint of vectors.)
Suppose D is some region and C is its boundary. Under certain conditions, the line integral along the curve C and the double integral over the region D (see) are connected by the relation
Similarly, the line integral and the surface integral are connected by the relation
Line integrals are of great importance in the theory of functions of a complex variable. They are widely used in various branches of mechanics, physics, and engineering.