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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=ฮผ0nI2ฯ€s.

02

Determine the formula of the energy stored in the toroidal coil

Write the formula ofthe energy stored in the toroidal coil.

W=12ฮผ0โˆซallspaceB2dฯ„ โ€ฆโ€ฆ (1)

Here, ฮผ0 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 ฮผ0nI2ฯ€s for B and localid="1658742313069" hrdฯ•ds for dฯ„ into equation (1).

Here, r = s

Then

W=12ฮผ0โˆซallspaceฮผ0nI2ฯ€s2hrdฯ•ds=12ฮผ0ฮผ02n2I24ฯ€โˆซ1s2hrdฯ•ds=12ฮผ0ฮผ02n2I24ฯ€h2ฯ€โˆซabdss=ฮผ0n2I24ฯ€hlnba

From reference equation as 7.27.

L=ฮผ0n2h2ฯ€lnba

But W=ฮผ0n2I24ฯ€hlnba โ€ฆโ€ฆ (2)

Substitute ฮผ0n2h2ฯ€lnba 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 metal bar of mass m slides frictionlessly on two parallel conducting rails a distance l apart (Fig. 7 .17). A resistor R is connected across the rails, and a uniform magnetic field B, pointing into the page, fills the entire region.


(a) If the bar moves to the right at speed V, what is the current in the resistor? In what direction does it flow?

(b) What is the magnetic force on the bar? In what direction?

(c) If the bar starts out with speedV0at time t=0, and is left to slide, what is its speed at a later time t?

(d) The initial kinetic energy of the bar was, of course,12mv2Check that the energy delivered to the resistor is exactly 12mv2.

A long cylindrical shell of radius Rcarries a uniform surface charge on ฯƒ0the upper half and an opposite charge -ฯƒ0on the lower half (Fig. 3.40). Find the electric potential inside and outside the cylinder.

A long solenoid with radius a and n turns per unit length carries a time-dependent currentl(t) in theฯ•^ direction. Find the electric field (magnitude and direction) at a distance s from the axis (both inside and outside the solenoid), in the quasistatic approximation.

Suppose

E(r,t)=14ฯ€ฮต0qr2ฮธ(rโˆ’ฯ…t)r^; B(r,t)=0

(The theta function is defined in Prob. 1.46b). Show that these fields satisfy all of Maxwell's equations, and determine ฯ and J. Describe the physical situation that gives rise to these fields.

A familiar demonstration of superconductivity (Prob. 7.44) is the levitation of a magnet over a piece of superconducting material. This phenomenon can be analyzed using the method of images. Treat the magnet as a perfect dipole , m a height z above the origin (and constrained to point in the z direction), and pretend that the superconductor occupies the entire half-space below the xy plane. Because of the Meissner effect, B = 0 for Zโ‰ค0, and since B is divergenceless, the normal ( z) component is continuous, so Bz=0just above the surface. This boundary condition is met by the image configuration in which an identical dipole is placed at - z , as a stand-in for the superconductor; the two arrangements therefore produce the same magnetic field in the region z>0.

(a) Which way should the image dipole point (+ z or -z)?

(b) Find the force on the magnet due to the induced currents in the superconductor (which is to say, the force due to the image dipole). Set it equal to Mg (where M is the mass of the magnet) to determine the height h at which the magnet will "float." [Hint: Refer to Prob. 6.3.]

(c) The induced current on the surface of the superconductor ( xy the plane) can be determined from the boundary condition on the tangential component of B (Eq. 5.76): B=ฮผ0(Kร—z^). Using the field you get from the image configuration, show that

K=-3mrh2ฯ€(r2+h2)52ฯ•^

where r is the distance from the origin.

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