If is a vector field and a directed curve, then the two dimensional flux of across is the integral

where is a unit normal vector to the curve , pointing 90 degree clockwise from the tangent vector ()

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Note the orientation convention is arbitrary, and this clockwise convention is also opposite to the one customarily used in Physics, where and form a right-handed coordinate system for motion along . The choice of here is the most natural for applying Green’s theorem to flow problems.

Relation with line Integral

With line integral, if is a vector field and a directed curve, then

We can interpret this as work done by along .

Notice that we are integrating the tangential component of along the curve . In component notation, if , then the above reads

Analogously, we may integrate , the normal component of along the curve .