Suppose you have two infinite straight line chargesλ, a distance d apart, moving along at a constant speed υ(Fig. 5.26). How great would have tobe in order for the magnetic attraction to balance the electrical repulsion? Work out the actual number. Is this a reasonable sort of speed?

Short Answer

Expert verified

The required speed isυ=3×108m/s and it is not reasonable two wires cannot attain that speed.

Step by step solution

01

Define function

Write the expression for the magnitude of force between two parallel straight current carrying conductors.

F=μ0i1i22πd …… (1)

Here,i1 and i2are currents through the parallel conductors,d is the distance between the two parallel conductors and μ0is the permeability.

Write the expression for the electric filed at distance of due to infinite straight conducting wire.

E=λ2πε0d ……. (2)

Here,λ is the linear charge density and ε0is the permittivity.

02

Determine speed

A line charge moving with speed constitute current that is,

i1=i2=λυ

Now, let’s consider that, one of the wires, then write the expression for the attractive magnetic force on his wire per unit length.

F=μ0i1i22πd

Substitute λυfor i1also λυfor i2.

F=μ0λυλυ2πd=μ0λ2υ22πd

Write the expression for electrostatic repulsion per unit length.

FC=λ22πε0d

The line charges have to balance the magnetic attraction and electrical repulsion.

FC=F …… (3)

Substitute λ22πε0dfor FCandμ0λ2υ22πdfor F in equation (3),

λ22πε0d=μ0λ2υ22πdυ=1μ0ε0

Substitute 4π×10-7H/Mforμ0and 8.85×10-12C2/N·m2for ε0in above equation.

υ=1μ0ε0υ=14π×10-7H/M8.85×10-12C2/N.m2υ=3×108m/s

Thus, the required speed is υ=3×108m/sand it is not reasonable two wires cannot attain that speed.

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Most popular questions from this chapter

A magnetic dipole m⇀=m0z^ is situated at the origin, in an otherwiseuniform magnetic field B⇀=B0z^ . Show that there exists a spherical surface, centered at the origin, through which no magnetic field lines pass. Find the radius of this sphere, and sketch the field lines, inside and out.

A large parallel-plate capacitor with uniform surface charge σon the upper plate and -σon the lower is moving with a constant speed localid="1657691490484" υ,as shown in Fig. 5.43.

(a) Find the magnetic field between the plates and also above and below them.

(b) Find the magnetic force per unit area on the upper plate, including its direction.

(c) At what speed Ï…would the magnetic force balance the electrical force?

A uniformly charged solid sphere of radius Rcarries a total charge Q, and is set spinning with angular velocitywabout the zaxis.

(a) What is the magnetic dipole moment of the sphere?

(b) Find the average magnetic field within the sphere (see Prob. 5.59).

(c) Find the approximate vector potential at a point (r,B)where r>R.

(d) Find the exact potential at a point (r,B)outside the sphere, and check that it is consistent with (c). [Hint: refer to Ex. 5.11.]

(e) Find the magnetic field at a point (r, B) inside the sphere (Prob. 5.30), and check that it is consistent with (b).

A thin glass rod of radius Rand length Lcarries a uniform surface charge σ. It is set spinning about its axis, at an angular velocityω. Find the magnetic field at a distances s冈Rfrom the axis, in the xyplane (Fig. 5.66). [Hint: treat it as a stack of magnetic dipoles.]

(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.)

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