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九州大学 システム情報科学府 情報理工学専攻・電気電子工学専攻 2024年1月実施 ベクトル解析

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祭音Myyura (assisted by ChatGPT 5.5)

Description

(1) Prove the following relationship between the volume integral and the surface integral:

V{f2g+(f)(g)}dV=S(fg)dS.\iiint_V \left\{ f\nabla^2 g+(\nabla f)\cdot(\nabla g) \right\}\,dV = \iint_S (f\nabla g)\cdot d\mathbf{S}.

(2) Prove the following relationship between the volume integral and the surface integral:

V(f2gg2f)dV=S(fggf)dS.\iiint_V \left(f\nabla^2 g-g\nabla^2 f\right)\,dV = \iint_S \left(f\nabla g-g\nabla f\right)\cdot d\mathbf{S}.

Here,

dS=ndSd\mathbf{S}=\mathbf{n}\,dS

where n\mathbf{n} is the outward unit normal vector to the closed surface SS.

Kai

(1)

We use the divergence theorem:

VFdV=SFdS.\iiint_V \nabla\cdot \mathbf{F}\,dV = \iint_S \mathbf{F}\cdot d\mathbf{S}.

Choose the vector field

F=fg.\mathbf{F}=f\nabla g.

Then

F=(fg).\nabla\cdot \mathbf{F} = \nabla\cdot(f\nabla g).

Using the product rule for divergence,

(fg)=(f)(g)+f(g).\nabla\cdot(f\nabla g) = (\nabla f)\cdot(\nabla g)+f\nabla\cdot(\nabla g).

Since

(g)=2g,\nabla\cdot(\nabla g)=\nabla^2 g,

we have

(fg)=(f)(g)+f2g.\nabla\cdot(f\nabla g) = (\nabla f)\cdot(\nabla g)+f\nabla^2 g.

Therefore,

V(fg)dV=V{f2g+(f)(g)}dV.\iiint_V \nabla\cdot(f\nabla g)\,dV = \iiint_V \left\{ f\nabla^2 g+(\nabla f)\cdot(\nabla g) \right\}\,dV.

By the divergence theorem,

V(fg)dV=S(fg)dS.\iiint_V \nabla\cdot(f\nabla g)\,dV = \iint_S (f\nabla g)\cdot d\mathbf{S}.

Hence,

V{f2g+(f)(g)}dV=S(fg)dS\boxed{ \iiint_V \left\{ f\nabla^2 g+(\nabla f)\cdot(\nabla g) \right\}\,dV = \iint_S (f\nabla g)\cdot d\mathbf{S} }

as required.

(2)

We again use the divergence theorem.

Choose the vector field

F=fggf.\mathbf{F}=f\nabla g-g\nabla f.

Then

F=(fggf).\nabla\cdot \mathbf{F} = \nabla\cdot(f\nabla g-g\nabla f).

Using linearity of divergence,

F=(fg)(gf).\nabla\cdot \mathbf{F} = \nabla\cdot(f\nabla g)-\nabla\cdot(g\nabla f).

From the product rule,

(fg)=(f)(g)+f2g,\nabla\cdot(f\nabla g) = (\nabla f)\cdot(\nabla g)+f\nabla^2 g,

and

(gf)=(g)(f)+g2f.\nabla\cdot(g\nabla f) = (\nabla g)\cdot(\nabla f)+g\nabla^2 f.

Thus,

F={(f)(g)+f2g}{(g)(f)+g2f}.\nabla\cdot \mathbf{F} = \left\{(\nabla f)\cdot(\nabla g)+f\nabla^2 g\right\} - \left\{(\nabla g)\cdot(\nabla f)+g\nabla^2 f\right\}.

Since the dot product is commutative,

(f)(g)=(g)(f),(\nabla f)\cdot(\nabla g) = (\nabla g)\cdot(\nabla f),

these two terms cancel. Therefore,

F=f2gg2f.\nabla\cdot \mathbf{F} = f\nabla^2 g-g\nabla^2 f.

Now applying the divergence theorem,

VFdV=SFdS.\iiint_V \nabla\cdot \mathbf{F}\,dV = \iint_S \mathbf{F}\cdot d\mathbf{S}.

Substituting

F=fggf,\mathbf{F}=f\nabla g-g\nabla f,

we get

V(f2gg2f)dV=S(fggf)dS.\iiint_V \left(f\nabla^2 g-g\nabla^2 f\right)\,dV = \iint_S \left(f\nabla g-g\nabla f\right)\cdot d\mathbf{S}.

Hence,

V(f2gg2f)dV=S(fggf)dS\boxed{ \iiint_V \left(f\nabla^2 g-g\nabla^2 f\right)\,dV = \iint_S \left(f\nabla g-g\nabla f\right)\cdot d\mathbf{S} }

as required.