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
Author
祭音Myyura (assisted by ChatGPT 5.5)
Description
(1) Prove the following relationship between the volume integral and the surface integral:
∭V{f∇2g+(∇f)⋅(∇g)}dV=∬S(f∇g)⋅dS.
(2) Prove the following relationship between the volume integral and the surface integral:
∭V(f∇2g−g∇2f)dV=∬S(f∇g−g∇f)⋅dS.
Here,
dS=ndS
where n is the outward unit normal vector to the closed surface S.
Kai
(1)
We use the divergence theorem:
∭V∇⋅FdV=∬SF⋅dS.
Choose the vector field
F=f∇g.
Then
∇⋅F=∇⋅(f∇g).
Using the product rule for divergence,
∇⋅(f∇g)=(∇f)⋅(∇g)+f∇⋅(∇g).
Since
∇⋅(∇g)=∇2g,
we have
∇⋅(f∇g)=(∇f)⋅(∇g)+f∇2g.
Therefore,
∭V∇⋅(f∇g)dV=∭V{f∇2g+(∇f)⋅(∇g)}dV.
By the divergence theorem,
∭V∇⋅(f∇g)dV=∬S(f∇g)⋅dS.
Hence,
∭V{f∇2g+(∇f)⋅(∇g)}dV=∬S(f∇g)⋅dS
as required.
(2)
We again use the divergence theorem.
Choose the vector field
F=f∇g−g∇f.
Then
∇⋅F=∇⋅(f∇g−g∇f).
Using linearity of divergence,
∇⋅F=∇⋅(f∇g)−∇⋅(g∇f).
From the product rule,
∇⋅(f∇g)=(∇f)⋅(∇g)+f∇2g,
and
∇⋅(g∇f)=(∇g)⋅(∇f)+g∇2f.
Thus,
∇⋅F={(∇f)⋅(∇g)+f∇2g}−{(∇g)⋅(∇f)+g∇2f}.
Since the dot product is commutative,
(∇f)⋅(∇g)=(∇g)⋅(∇f),
these two terms cancel. Therefore,
∇⋅F=f∇2g−g∇2f.
Now applying the divergence theorem,
∭V∇⋅FdV=∬SF⋅dS.
Substituting
F=f∇g−g∇f,
we get
∭V(f∇2g−g∇2f)dV=∬S(f∇g−g∇f)⋅dS.
Hence,
∭V(f∇2g−g∇2f)dV=∬S(f∇g−g∇f)⋅dS
as required.