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Because this form of Green’s theorem contains unit normal vector N , it is sometimes referred to as the normal form of Green’s theorem .
Recall that Let and By the circulation form of Green’s theorem,
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Let C be a circle of radius r centered at the origin ( [link] ) and let Calculate the flux across C .
Let D be the disk enclosed by C. The flux across C is We could evaluate this integral using tools we have learned, but Green’s theorem makes the calculation much more simple. Let and so that Note that and therefore By Green’s theorem,
Since is the area of the circle, Therefore, the flux across C is
Let S be the triangle with vertices and oriented clockwise ( [link] ). Calculate the flux of across S .
To calculate the flux without Green’s theorem, we would need to break the flux integral into three line integrals, one integral for each side of the triangle. Using Green’s theorem to translate the flux line integral into a single double integral is much more simple.
Let D be the region enclosed by S . Note that and therefore, Green’s theorem applies only to simple closed curves oriented counterclockwise, but we can still apply the theorem because and is oriented counterclockwise. By Green’s theorem, the flux is
Notice that the top edge of the triangle is the line Therefore, in the iterated double integral, the y -values run from to and we have
Calculate the flux of across a unit circle oriented counterclockwise.
Water flows from a spring located at the origin. The velocity of the water is modeled by vector field m/sec. Find the amount of water per second that flows across the rectangle with vertices oriented counterclockwise ( [link] ).
Let C represent the given rectangle and let D be the rectangular region enclosed by C . To find the amount of water flowing across C , we calculate flux Let and so that Then, and By Green’s theorem,
Therefore, the water flux is 80 m 2 /sec.
Recall that if vector field F is conservative, then F does no work around closed curves—that is, the circulation of F around a closed curve is zero. In fact, if the domain of F is simply connected, then F is conservative if and only if the circulation of F around any closed curve is zero. If we replace “circulation of F ” with “flux of F, ” then we get a definition of a source-free vector field. The following statements are all equivalent ways of defining a source-free field on a simply connected domain (note the similarities with properties of conservative vector fields):
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