(a) Prove the identity
∇(F⋅G)=(F⋅∇)G+(G⋅∇)F+F×(∇×G)+G×(∇×F)
(b) If E is an irrotational vector field (∇×E=0 everywhere ), prove that there exists a scalar potential ϕ(x) such that E=−∇ϕ.
Show that
(2xy2ze−x2z,−2ye−x2z,x2y2e−x2z)
is irrotational, and determine the corresponding potential ϕ.