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Question: (a) Find the density ρof mobile charges in a piece of copper, assuming each atom contributes one free electron. [Look up the necessary physical constants.]

(b) Calculate the average electron velocity in a copper wire 1 mm in diameter, carrying a current of 1 A. [Note:This is literally a snail'space. How, then, can you carry on a long distance telephone conversation?]

(c) What is the force of attraction between two such wires, 1 em apart?

(d) If you could somehow remove the stationary positive charges, what would the electrical repulsion force be? How many times greater than the magnetic force is it?

Short Answer

Expert verified

Answer

  1. The charge density is1.4×104C/cm3 .
  2. The drift velocity is9.1×10-3.
  3. The force of the magnetic field is2×10-7N/cm.

The magnitude of the electric field is2×10-18N/cm

Step by step solution

01

Determine the formulas:

Write the expression for charge density.

ρ=ChargeVolume=(ChargeAtom)(AtomMole)(MoleGram)(GramVolume)=eN(1M)d……. (1)

Here, is the charge of electron, is the Avogadro number, is the atomic mass copper and is the density of copper.

02

Determine the density in the mobile charges. 

a)

Calculate the charge density of mobile charge in piece of copper.

Substitute 1.6×10-19Cfor charge of electron6.0×1023mol, for Avogadro number, for atomic mass of copper and for density of copper in the equation (1)

Therefore,

03

Determine the average electron velocity 

b)

Write the expression for diameter of the copper wire.

d=1mm=1mm1m103mm=10-3m

Write the expression for the radius of the copper wire.

r=d2=10-3m2=5×10-4m

Write the expression for area of the wire.

A=πr2 …… (2)

Substitute for in equation (2)

A=πr2=π5×10-4m2=7.85×10-7m2

Write the formula for current density.

localid="1657976633620" J=IA ……. (3)

Here, is current through the wire and is area.

Substitute 1.0 for I and for in equation (3).

Write the relation between current density and drift velocity .

J=IA=1.0A7.85×10-7m2=1.2738×106A/m2

Rearrange the above equation,

υ=Jρ …… (4)

Substitute for and for in equation (4)

υ=Jρ=1.2738×1061m2104cm21.4×104=9.1×10-3

Hence, the drift velocity is 9.1×10-3cm/s.

04

Determine the force of attraction between the two wires

c)

Calculate the separation between the two wires.

d=1.0cm=1.0cm1m100cm=0.01m

Write the formula for the force per unit length between two parallel wires.

Fmaglength=μ02πI1I2d …… (5)

Substitute for4π×10-7, for current carrying two wires and for separation between the wires .

Fmaglength=μ02πI1I2d=4π×10-72π1.0A1.0A1.0cm=2×10-7

Hence, the force of the magnetic field is 2×10-7.

05

Determine the electrical repulsion force and its intensity compared to the magnetic force

d)

Using Gauss Law,

Write the expression for electric field of symmetrically cylindrical change distribution.

E=12πε0λd …… (6)

Write the expression for the force of electric filed between the two wires.

Fe=12πε0λ1λ2d …… (7)

Here, is the linear charge density.

Using the relation,

λ=Iυ

Here, current is constant and is the drift velocity.

λ1=λ2=Iυ

Here, .I1=I2

Then equation (7) is reduced as,

Fe=1υ212πε0I1I2d …… (8)

Here,

c2=1μ0ε01ε0=μ0c2\

Hence, the equation (8) is reduced as,

Fe=1υ2μ0c22πI1I2d …… (9)

Now, Divide equation Fe=1υ2μ0c22πI1I2dwith Fmag=μ02πI1I2d

FeFmag=1υ2μ0c22πI1I2dμ02πI1I2dfelefmag=c2υ2

localid="1657980326651" FeFmag=1υ2μ0c22πI1I2dμ02πI1I2dfelefmag=c2υ2FeFmag=1υ2μ0c22πI1I2dμ02πI1I2dfelefmag=c2υ2 …… (10)

Thus, the ratio of forces of electric and magnetic field is 1.1 x 1025.

felefmag=1.1×1025=1.1×1025fmag=1.1×1025(2×10-7N/cm)=2×1018N/cm

Thus, the magnitude of the electric field is 2 X 1018.

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Most popular questions from this chapter

(a) Complete the proof of Theorem 2, Sect. 1.6.2. That is, show that any divergenceless vector field F can be written as the curl of a vector potential . What you have to do is find Ax,Ayand Azsuch that (i) Az/y-Ay/z=Fx; (ii) Ax/z-Az/x=Fy; and (iii) Ay/x-Ax/y=Fz. Here's one way to do it: Pick Ax=0, and solve (ii) and (iii) for Ayand Az. Note that the "constants of integration" are themselves functions of y and z -they're constant only with respect to x. Now plug these expressions into (i), and use the fact that F=0to obtain

Ay=0xFz(x',y,z)dx';Az=0yFx(0,y',z)dy'-0yFy(x',y,z)dx'

(b) By direct differentiation, check that the you obtained in part (a) satisfies ×A=F. Is divergenceless? [This was a very asymmetrical construction, and it would be surprising if it were-although we know that there exists a vector whose curl is F and whose divergence is zero.]

(c) As an example, let F=yx^+zy^+xz^. Calculate , and confirm that ×A=F. (For further discussion, see Prob. 5.53.)

Use the Biot-Savart law (most conveniently in the form of Eq. 5.42 appropriate to surface currents) to find the field inside and outside an infinitely long solenoid of radiusR, with n turns per unit length, carrying a steady current I.

A circularly symmetrical magnetic field ( B depends only on the distance from the axis), pointing perpendicular to the page, occupies the shaded region in Fig. 5.58. If the total flux (B.da) is zero, show that a charged particle that starts out at the center will emerge from the field region on a radial path (provided it escapes at all). On the reverse trajectory, a particle fired at the center from outside will hit its target (if it has sufficient energy), though it may follow a weird route getting there. [Hint: Calculate the total angular momentum acquired by the particle, using the Lorentz force law.]

Question: Suppose you want to define a magnetic scalar potential U(Eq. 5.67)

in the vicinity of a current-carrying wire. First of all, you must stay away from the

wire itself (there ×B0); but that's not enough. Show, by applying Ampere's

law to a path that starts at a and circles the wire, returning to b (Fig. 5.47), that the

scalar potential cannot be single-valued (that is, U(a)U(b), even if they represent the same physical point). As an example, find the scalar potential for an infinite straight wire. (To avoid a multivalued potential, you must restrict yourself to simply connected regions that remain on one side or the other of every wire, never allowing you to go all the way around.)

The magnetic field on the axis of a circular current loop (Eq. 5.41) is far from uniform (it falls off sharply with increasing z). You can produce a more nearly uniform field by using two such loops a distanced apart (Fig. 5.59).

(a) Find the field (B) as a function of z, and show that Bz is zero at the point midway between them (z = 0)

(b) If you pick d just right, the second derivative of B will also vanish at the midpoint. This arrangement is known as a Helmholtz coil; it's a convenient way of producing relatively uniform fields in the laboratory. Determine d such that 2B/z2=0 at the midpoint, and find the resulting magnetic field at the center. [Answer:8μ0I55R ]

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