Line Integral: The integration of a vector along a curve is called its line integral. As shown in Figure 7.11, let MN is a curve drawn between two points M and N in vector field. Let dl is an element of length along the curve MN at O. Suppose A is the vector at 0, making an angle e with the direction of dl.
A .dl = A dl cosθ
Dl = (A cosθ)
Equation (1) shows that the value of A.dl at any point of the curve is equal to the product of small element dl and the component (A cos 8) of A along the direction of dl. The value of A.dl for the complete curve MN can be obtained by integrating Equation (1). Hence
ʃNMA.dl = ʃNM dl (A cos θ).
Integral ʃNMA.dl is defined as the line integral of A along the curve MN.
(i) If A represents the force acting on a particle moving along the curve from M to N, then the line integral ʃNMA.dl represents t1he total workdone by the force during the motion of the particle over its entire path from M to N.
(ii) If A denotes the electric field intensity at any point, then the line integral represents the potential difference between M and N.
Consider a simple surfaceS in a vector field bounded by a curve as shown in Figure 7.12.
Let dS be an infinitesimal element of the surface. The surface element of area can be
represented by area vector dS. If ii be a unit positive vector (drawn outward the surface) in the· direction of dS, then
Ds =n dS
“Let A be a vector at middle of the element d S ID. In the direction making an angle θ with . n .
Now the scalar product
A.ds = A. n ds =Ads cos θ
is called the flux of vector field A across the area element dS. The total flux of the vector
field across the entire surface S is given by
ʃʃS A .DS = ʃ ʃsA. n dS = ʃ ʃS A cos θ ds
This is defined as surface integral.
Consider a closed surface in space enclosing the volume V. If A be a vector point function ata point in a small element of volume dV, then the integral
ʃʃʃ A dV
is called the volume integral of vector A over the surface.