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Mathematical Methods for Physicists: A concise introduction - Site Map

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VECTOR INTEGRATION AND INTEGRAL THEOREMS<br />

Green's theorem<br />

Green's theorem is an important corollary of the divergence theorem, and it<br />

has many applications in many branches of physics. Recall that the divergence<br />

theorem Eq. (1.78) states that<br />

Z<br />

I<br />

rAdV ˆ A da:<br />

V<br />

Let A ˆ B, where is a scalar function and B a vector function, then rA<br />

becomes<br />

rA ˆr… B† ˆ rB ‡ B r :<br />

Substituting these into the divergence theorem, we have<br />

I<br />

Z<br />

B da ˆ … rB ‡ B r †dV:<br />

S<br />

V<br />

S<br />

…1:84†<br />

If B represents an irrotational vector ®eld, we can express it as a gradient of a<br />

scalar function, say, ':<br />

Then Eq. (1.84) becomes<br />

I<br />

Z<br />

B da ˆ<br />

Now<br />

S<br />

V<br />

B r':<br />

‰ r…r'†‡…r'†…r †ŠdV: …1:85†<br />

B da ˆ…r'†^nda:<br />

The quantity …r'†^n represents the rate of change of in the direction of the<br />

outward normal; it is called the normal derivative and is written as<br />

…r'†^n @'=@n:<br />

Substituting this and the identity r…r'† ˆr 2 ' into Eq. (1.85), we have<br />

I<br />

@'<br />

S @n<br />

ZV<br />

da ˆ ‰ r 2 ' ‡r' r ŠdV: …1:86†<br />

Eq. (1.86) is known as Green's theorem in the ®rst <strong>for</strong>m.<br />

Now let us interchange ' and , then Eq. (1.86) becomes<br />

I<br />

' @<br />

S @n<br />

ZV<br />

da ˆ ‰'r 2 ‡r' r ŠdV:<br />

Subtracting this from Eq. (1.85):<br />

I <br />

@'<br />

@n ' @<br />

@n<br />

S<br />

Z<br />

da ˆ<br />

V<br />

43<br />

<br />

r 2 ' 'r 2 <br />

dV: …1:87†

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