Question #275799

[SADT3] For scalar functions u and v, show that



B=( nabla u)*( nabla v)



is solenoidal and that



A= 1 2 (u nabla v-v nabla u)



is a vector potential for B, i.e. B= nabla* A

Expert's answer

B=(∇u)×(∇v)B=( \nabla u)\times( \nabla v)

A=12(u∇v−v∇u)A= \frac{1}{2} (u \nabla v-v \nabla u)

B=∇×AB= \nabla\times A


for solenoidal vector field:

∇⋅B=0\nabla \cdot B=0


∇u=∂u∂xi+∂u∂yj+∂u∂zk\nabla u=\frac{\partial u}{\partial x}i+\frac{\partial u}{\partial y}j+\frac{\partial u}{\partial z}k


∇v=∂v∂xi+∂v∂yj+∂v∂zk\nabla v=\frac{\partial v}{\partial x}i+\frac{\partial v}{\partial y}j+\frac{\partial v}{\partial z}k


B=(∇u)×(∇v)=∣ijk∂u∂x∂u∂y∂u∂z∂v∂x∂v∂y∂v∂z∣=B=( \nabla u)\times( \nabla v)=\begin{vmatrix} i & j&k \\ \frac{\partial u}{\partial x}&\frac{\partial u}{\partial y}&\frac{\partial u}{\partial z}\\ \frac{\partial v}{\partial x}&\frac{\partial v}{\partial y}&\frac{\partial v}{\partial z}\\ \end{vmatrix}=


=(∂u∂y∂v∂z−∂v∂y∂u∂z)i−(∂u∂x∂v∂z−∂u∂z∂v∂x)j+(∂u∂x∂v∂y−∂u∂y∂v∂x)k=0=(\frac{\partial u}{\partial y}\frac{\partial v}{\partial z}-\frac{\partial v}{\partial y}\frac{\partial u}{\partial z})i-(\frac{\partial u}{\partial x}\frac{\partial v}{\partial z}-\frac{\partial u}{\partial z}\frac{\partial v}{\partial x})j+(\frac{\partial u}{\partial x}\frac{\partial v}{\partial y}-\frac{\partial u}{\partial y}\frac{\partial v}{\partial x})k=0


so, ∇⋅B=0\nabla \cdot B=0



A=12(u∇v−v∇u)=12(u∂v∂xi+u∂v∂yj+u∂v∂zk−v∂u∂xi−v∂u∂yj−v∂u∂zk)A= \frac{1}{2} (u \nabla v-v \nabla u)=\frac{1}{2} (u\frac{\partial v}{\partial x}i+u\frac{\partial v}{\partial y}j+u\frac{\partial v}{\partial z}k-v\frac{\partial u}{\partial x}i-v\frac{\partial u}{\partial y}j-v\frac{\partial u}{\partial z}k)


∇×A=[∂∂y(u∂v∂z−v∂u∂z)−∂∂z(u∂v∂y−v∂u∂y)]i+[∂∂z(u∂v∂z−v∂u∂z)−∂∂x(u∂v∂z−v∂u∂z)]j+\nabla\times A=[\frac{\partial}{\partial y}(u\frac{\partial v}{\partial z}-v\frac{\partial u}{\partial z})-\frac{\partial}{\partial z}(u\frac{\partial v}{\partial y}-v\frac{\partial u}{\partial y})]i+[\frac{\partial}{\partial z}(u\frac{\partial v}{\partial z}-v\frac{\partial u}{\partial z})-\frac{\partial}{\partial x}(u\frac{\partial v}{\partial z}-v\frac{\partial u}{\partial z})]j+


+[∂∂x(u∂v∂y−v∂u∂y)−∂∂y(u∂v∂x−v∂u∂x)]k=B+[\frac{\partial}{\partial x}(u\frac{\partial v}{\partial y}-v\frac{\partial u}{\partial y})-\frac{\partial}{\partial y}(u\frac{\partial v}{\partial x}-v\frac{\partial u}{\partial x})]k=B


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