Divergence Theorem

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Let E be a simple solid region and let S be the boundary surface of E, given with positive (outward) orientation. Let ˉF be a vector field whose component functions have continuous partial derivatives on an open region that contains E. Then,

S¯Fd¯S=Ediv¯FdV.

Thus, the Divergence Theorem states that, under the given conditions, the flux of  ˉF across the boundary surface of E is equal to the triple integral of the divergence of ˉF over E.

 

Example 1. Let S be the circle given by x2+y24 and z=5 and let ¯F=y2¯i+x2¯j+z2¯k. Compute SˉFd¯s.

cylinder

Solution. We use parametric coordinates as follows:

¯r(u,v)=u,v,5,ˉTu=1,0,0,¯Tν=0,1,0,¯N=¯TuׯTv=|¯i¯j¯k100010|=¯k.

We then calculate and obtain

S¯Fd¯s=x2+y24ν2,u2,250,0,1dA=x2+y2425dA=25(16π)=400π.

 

Example 2. Let W be the cylinder given by x2+y24 and 0z5 and let ¯F=xy2¯i+y3¯j+4x2z¯k. Compute the flux of ˉF across the boundary surface of W.

Solution. We begin by calculating the divergence of ˉF

div¯F=xy2x+y3y+4x2zz=y2+3y2+4x2=4y2+4x2.

Then, applying the Divergence Theorem, we obtain

SˉFd¯s=Sxy2,y3,4x2zd¯s=Wdiv¯FdV=W(4y2+4x2)dV=4x2+y24(50(x2+y2)dz)dA=20x2+y24(x2+y2)dA=202π020r2rdrdθ=202π020r3drdθ=202π0[14r4]20dθ=20×2π×4=160π,

where we’ve used the polar coordinates

x=rcosθ,y=rsinθ,r2=x2+y2,dA=rdrdθ.