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A more elegant proof of the second uniqueness theorem uses Green's

identity (Prob. 1.61c), with T=U=V3. Supply the details.

Short Answer

Expert verified

Answer

It is proved as second uniqueness of theorem by using greens identity.

Step by step solution

01

Define function

Write the Greens identity.

~NT~N2U+~NU×~NT=T~NU×da…… (1)

Given that T=U=V3,

Therefore, the greens identity is changes as,

~NV3~N2V3+~NV3×~NV3=V3~NV3×da …… (2)

02

Determine proof of Greens identity

Since

2V3=2V1-2V22V1=-ρε02V2=-ρε0

Then,

2V3=-ρε0+ρε0=0

As known to us,

V3=E3

E3=V3as per derivation.

03

Determine proof of Greens identity

Substitute the above values in equation (1)

V30+E32dτ=-V3E3·daE32dτ=-V3E3·da …… (3)

As,

E3=E1-E2 …… (4)

If V is specified as V3=0or E3=0then,

The equation (4) will be,

0=E1-E2E1=E2

Thus, filed is uniquely determined.

And it is proved as this is a second uniqueness theorem.

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Most popular questions from this chapter

A uniform line charge λis placed on an infinite straight wire, a distanced above a grounded conducting plane. (Let's say the wire runs parallel to the x-axis and directly above it, and the conducting plane is the xyplane.)

  1. Find the potential in the region above the plane. [Hint: Refer to Prob. 2.52.]
  2. Find the charge density σ induced on the conducting plane.

In Ex. 3.2 we assumed that the conducting sphere was grounded ( V=0). But with the addition of a second image charge, the same basic modelwill handle the case of a sphere at any potentialV0 (relative, of course, to infinity). What charge should you use, and where should you put it? Find the force of attraction between a point charge q and a neutral conducting sphere.

Prove that the field is uniquely determined when the charge density ρ

is given and either V or the normal derivative a V/n is specified on each boundary surface. Do not assume the boundaries are conductors, or that V is constant over any given surface.

(a) Suppose the potential is a constant V0over the surface of the sphere. Use the results of Ex. 3.6 and Ex. 3.7 to find the potential inside and outside the sphere. (Of course, you know the answers in advance-this is just a consistency check on the method.)

(b) Find the potential inside and outside a spherical shell that carries a uniform surface charge σ0, using the results of Ex. 3.9.

Find the potential in the infinite slot of Ex. 3.3 if the boundary at x = 0 consists of two metal strips: one, from y = 0 to y = a/2, is held at a constant Potential V0, and the other, from y = a/2 to y = a , is at potential V0.

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