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

A square loop of wire (side a) lies on a table, a distance s from a very long straight wire, which carries a current I, as shown in Fig. 7.18.

(a) Find the flux of B through the loop.

(b) If someone now pulls the loop directly away from the wire, at speed, V what emf is generated? In what direction (clockwise or counter clockwise) does the current flow?

(c) What if the loop is pulled to the right at speed V ?

Question: Suppose j(r)is constant in time but ρ(r,t)is not-conditions that

might prevail, for instance, during the charging of a capacitor.

(a) Show that the charge density at any particular point is a linear function of time:

ρ(r,t)=ρ(r,0)+ρ(r,0)t

whereρ(r,0)is the time derivative of at . [Hint: Use the continuity equation.]

This is not an electrostatic or magnetostatic configuration: nevertheless, rather surprisingly, both Coulomb's law (Eq. 2.8) and the Biot-Savart law (Eq. 5.42) hold, as you can confirm by showing that they satisfy Maxwell's equations. In particular:

(b) Show that

B(r)=μ04πJ(r')×r^r2dτ'

obeys Ampere's law with Maxwell's displacement current term.

Imagine a uniform magnetic field, pointing in the zdirection and filling all space (B=B0z). A positive charge is at rest, at the origin. Now somebody turns off the magnetic field, thereby inducing an electric field. In what direction does the charge move?

Refer to Prob. 7.11 (and use the result of Prob. 5.42): How long does is take a falling circular ring (radius a, mass m, resistance R) to cross the bottom of the magnetic field B, at its (changing) terminal velocity?

(a) Referring to Prob. 5.52(a) and Eq. 7.18, show that

E=-At (7.66) for Faraday-induced electric fields. Check this result by taking the divergence and curl of both sides.

(b) A spherical shell of radiusR carries a uniform surface charge σ. It spins about a fixed axis at an angular velocity ω(t)that changes slowly with time. Find the electric field inside and outside the sphere. [Hint: There are two contributions here: the Coulomb field due to the charge, and the Faraday field due to the changing B. Refer to Ex. 5.11.]

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