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Two coils are wrapped around a cylindrical form in such a way that the same flux passes through every turn of both coils. (In practice this is achieved by inserting an iron core through the cylinder; this has the effect of concentrating the flux.) The primary coil hasN1turns and the secondary hasN2(Fig. 7.57). If the current in the primary is changing, show that the emf in the secondary is given by

ε2ε1=N2N1(7.67)

whereε1is the (back) emf of the primary. [This is a primitive transformer-a device for raising or lowering the emf of an alternating current source. By choosing the appropriate number of turns, any desired secondary emf can be obtained. If you think this violates the conservation of energy, study Prob. 7.58.]

Short Answer

Expert verified

The expressionε2ε1=N2N1is verified.

Step by step solution

01

Given information

The number of turns in the primary coils are,N1.

The number of turns in the secondary coils are,N2.

The current passing through the primary coil is,I .

02

Magnetic flux on coils

When the magnitude of the current flowing in the coil varies, a magnetic flux is generated and a certain amount of emf is also induced in the coil.

If the number of turns in the coil are increased then the magnetic flux produced in the coil also increases.

03

Determine the magnetic flux on both coils

When the current passes through a single loop of primary coil, the magnetic field is generated and the change in current value creates the magnetic fluxΦ.

Then, the formula for the magnetic flux on the primary coil is given by,

localid="1658291056948" Φ1=N1Φ

And, the formula for the magnetic flux on the secondary coil is given by,

localid="1658291081661" Φ2=N2Φ

04

Determine emf induced in the primary coil

The formula for the emf induced in the primary coil is given by,

ε1=-dΦ1dtε1=-dN1Φdtε1=-N1dΦdt........(1)

05

Determine emf induced in the secondary coil

The formula for the emf induced in the secondary coil is given by,

ε2=-dΦ2dtε2=-dN2Φdtε2=-N2dΦdt.......(2)

By dividing equation (2) by equation (1),

ε2ε1=-N2dΦdt-N1dΦdtε2ε1=N2N1

Hence proved.

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Most popular questions from this chapter

A certain transmission line is constructed from two thin metal "rib-bons," of width w, a very small distanceh≪w apart. The current travels down one strip and back along the other. In each case, it spreads out uniformly over the surface of the ribbon.

(a) Find the capacitance per unit length, C .

(b) Find the inductance per unit length, L .

(c) What is the product LC , numerically?[ L and C will, of course, vary from one kind of transmission line to another, but their product is a universal constantcheck, for example, the cable in Ex. 7.13-provided the space between the conductors is a vacuum. In the theory of transmission lines, this product is related to the speed with which a pulse propagates down the line: v=1/LC.]

(d) If the strips are insulated from one another by a non-conducting material of permittivity εand permeability εand permeability μ, what then is the product LC ? What is the propagation speed? [Hint: see Ex. 4.6; by what factor does L change when an inductor is immersed in linear material of permeabilityμ?]

A toroidal coil has a rectangular cross section, with inner radius a , outer radius a+w, and height h . It carries a total of N tightly wound turns, and the current is increasing at a constant rate (dl/dt=k). If w and h are both much less than a , find the electric field at a point z above the center of the toroid. [Hint: Exploit the analogy between Faraday fields and magnetostatic fields, and refer to Ex. 5.6.]

An alternating current l=l0cos(wt)flows down a long straight wire, and returns along a coaxial conducting tube of radius a.

(a) In what direction does the induced electric field point (radial, circumferential, or longitudinal)?

(b) Assuming that the field goes to zero as s→∞, findE=(s,t).

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 Z≤0, 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=μ0(K×z^). Using the field you get from the image configuration, show that

K=-3mrh2Ï€(r2+h2)52Ï•^

where r is the distance from the origin.

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

B=μ02πIsϕ^

The electric field inside the wire is uniform:

E=IÒÏÏ€a2z^,

Where ÒÏis 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)=IÒÏzÏ€a2 ; (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 σ(z)on the wire.

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

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