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Question:Calculate the energy stored in the toroidal coil of Ex. 7.11, by applying Eq. 7.35. Use the answer to check Eq. 7.28.

Short Answer

Expert verified

Answer

The value of the energy stored in the toroidal coil is W=12LI2.

Step by step solution

01

Write the given data from the question

Consider the magnetic field inside the toroid is B=0nI2s.

02

Determine the formula of the energy stored in the toroidal coil

Write the formula ofthe energy stored in the toroidal coil.

W=120allspaceB2d 鈥︹ (1)

Here, 0 is permeability and B is magnetic field inside the toroid

03

(a) Determine the value of the energy stored in the toroidal coil

Determine theenergy stored in the toroidal coil.

Substitute 0nI2s for B and localid="1658742313069" hrdds for d into equation (1).

Here, r = s

Then

W=120allspace0nI2s2hrdds=12002n2I241s2hrdds=12002n2I24h2abdss=0n2I24hlnba

From reference equation as 7.27.

L=0n2h2lnba

But W=0n2I24hlnba 鈥︹ (2)

Substitute 0n2h2lnba for L into above equation (2).

W=12LI2

Therefore, thevalue ofthe energy stored in the toroidal coil is W=12LI2.

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Most popular questions from this chapter

Two long, straight copper pipes, each of radius a, are held a distance 2d apart (see Fig. 7.50). One is at potential V0, the other at -V0. The space surrounding the pipes is filled with weakly conducting material of conductivity . Find the current per unit length that flows from one pipe to the other. [Hint: Refer to Prob. 3.12.]

Find the self-inductance per unit length of a long solenoid, of radius R , carrying n turns per unit length.

(a) Show that Maxwell's equations with magnetic charge (Eq. 7.44) are invariant under the duality transformation

E'=Ecos+cBsin,cB'=cBcos-Esin,cq'e=cqecos+qmsin,q'm=qmcos-cqesin,

Where c1/00and is an arbitrary rotation angle in 鈥淓/B-space.鈥 Charge and current densities transform in the same way as qeand qm. [This means, in particular, that if you know the fields produced by a configuration of electric charge, you can immediately (using =90) write down the fields produced by the corresponding arrangement of magnetic charge.]

(b) Show that the force law (Prob. 7.38)

F=qe(E+VB)+qm(B-1c2VE)

is also invariant under the duality transformation.

The magnetic field outside a long straight wire carrying a steady current I is

B=02Is^

The electric field inside the wire is uniform:

E=Ia2z^,

Where is the resistivity and a is the radius (see Exs. 7.1 and 7 .3). Question: What is the electric field outside the wire? 29 The answer depends on how you complete the circuit. Suppose the current returns along a perfectly conducting grounded coaxial cylinder of radius b (Fig. 7.52). In the region a < s < b, the potential V (s, z) satisfies Laplace's equation, with the boundary conditions

(i) V(a,z)=Iza2 ; (ii) V(b,z)=0

Figure 7.52

This does not suffice to determine the answer-we still need to specify boundary conditions at the two ends (though for a long wire it shouldn't matter much). In the literature, it is customary to sweep this ambiguity under the rug by simply stipulating that V (s,z) is proportional to V (s,z) = zf (s) . On this assumption:

(a) Determine (s).

(b) E (s,z).

(c) Calculate the surface charge density (z)on the wire.

[Answer: V=(-Iz/a2) This is a peculiar result, since Es and (z)are not independent of localid="1658816847863" zas one would certainly expect for a truly infinite wire.]

A square loop, side a , resistance R , lies a distance from an infinite straight wire that carries current l (Fig. 7.29). Now someone cuts the wire, so l drops to zero. In what direction does the induced current in the square loop flow, and what total charge passes a given point in the loop during the time this current flows? If you don't like the scissors model, turn the current down gradually:

I(t)={(1-t)I0for0t1/afort>/a

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