Calc 3 Lecture Notes Section 14.7 Page 1 of 4 Section 14.7: The Divergence Theorem Big idea: The Divergence Theorem (or Gauss’s Theorem) is like Green’s Theorem in that it relates an integral of a vector field over the boundary of a geometric object to an integral of the divergence of the vector field over the interior of the geometric object. Big skill: You should be able to use Green’s Theorem to go between surface integrals over the boundary of a closed surface and volume integrals of the divergence of the field. Recall Green’s Theorem from section 14.4: N M R Mdx Ndy R x y dA For a vector field F x, y M x, y , N x, y , 0 with curl F 0, 0, N x M y and path parameterized by r x t , y t , 0 so that dr dx, dy,0 Tds (Where T x ', y ', 0 r' is the unit tangent vector to the curve), Green’s theorem can be re-written as: F dr F Tds F kdA R R R But what happens if we take the dot product of F with the unit normal vector as we perform the line integral around the closed curve? Well, we can show F Nds FdA (given that R N y ', x ', 0 r' ): R Calc 3 Lecture Notes Section 14.7 Page 2 of 4 Theorem 7.1: The Divergence Theorem: If F is a vector field whose components have continuous first partial derivatives over some region Q 3 bounded by the closed surface Q with an exterior unit normal vector N, then F NdS FdV Q Q Calc 3 Lecture Notes Section 14.7 Page 3 of 4 Practice: 1. Show that the divergence theorem holds true for the hemispherical solid of radius 1 in the vector field F 0,0,1 (this is the last example from section 14.6’s notes) Calc 3 Lecture Notes Section 14.7 Page 4 of 4 2. Show that the divergence theorem holds true for the hemispherical solid of radius 1 in the vector field F x, y, z . Interpret the non-zero answer in terms of a source for the field lines.
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