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=μ0nI2πs.

02

Determine the formula of the energy stored in the toroidal coil

Write the formula ofthe energy stored in the toroidal coil.

W=12μ0allspaceB2dτ …… (1)

Here, μ0 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 μ0nI2πs for B and localid="1658742313069" hrdϕds for dτ into equation (1).

Here, r = s

Then

W=12μ0allspaceμ0nI2πs2hrdϕds=12μ0μ02n2I24π1s2hrdϕds=12μ0μ02n2I24πh2πabdss=μ0n2I24πhlnba

From reference equation as 7.27.

L=μ0n2h2πlnba

But W=μ0n2I24πhlnba …… (2)

Substitute μ0n2h2πlnba 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

The current in a long solenoid is increasing linearly with time, so the flux is proportional t:.ϕ=αtTwo voltmeters are connected to diametrically opposite points (A and B), together with resistors ( R1and R2), as shown in Fig. 7.55. What is the reading on each voltmeter? Assume that these are ideal voltmeters that draw negligible current (they have huge internal resistance), and that a voltmeter register --abE×dlbetween the terminals and through the meter. [Answer: V1=αR1/(R1+R2). Notice that V1V2, even though they are connected to the same points]

Refer to Prob. 7.16, to which the correct answer was

E(s,t)=μ0I0ω2ττsin(ωt)In(as)z^

(a) Find the displacement current density Jd·

(b) Integrate it to get the total displacement current,

Id=Jd.da

Compare Id and I. (What's their ratio?) If the outer cylinder were, say, 2 mm in diameter, how high would the frequency have to be, forId to be 1% of I ? [This problem is designed to indicate why Faraday never discovered displacement currents, and why it is ordinarily safe to ignore them unless the frequency is extremely high.]

A square loop of wire, with sides of length a , lies in the first quadrant of the xy plane, with one comer at the origin. In this region, there is a nonuniform time-dependent magnetic field B(y,t)=ky3t2z^ (where k is a constant). Find the emf induced in the loop.

A square loop (side a) is mounted on a vertical shaft and rotated at angular velocity ω (Fig. 7.19). A uniform magnetic field B points to the right. Find theεtfor this alternating current generator.

An alternating current I(t)=I0cos(ωt) (amplitude 0.5 A, frequency ) flows down a straight wire, which runs along the axis of a toroidal coil with rectangular cross section (inner radius 1cm , outer radius 2 cm , height 1 cm, 1000 turns). The coil is connected to a 500Ω resistor.

(a) In the quasistatic approximation, what emf is induced in the toroid? Find the current, IR(t), in the resistor.

(b) Calculate the back emf in the coil, due to the current IR(t) . What is the ratio of the amplitudes of this back emf and the "direct" emf in (a)?

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