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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 υwould the magnetic force balance the electrical force?

Short Answer

Expert verified
  1. The magnetic field isB=μ0συ .
  2. The magnetic force per unit area isfm=μ0(συ)22and the direction of force is upward.
  3. The speed of the upper plate is 3×108 m/s.

Step by step solution

01

Define function

Write the expression for magnetic field of an infinite uniform surface current.

B=μ0K2 …… (1)

Here,μ0is the permeability of the air or free space.

Write the expression for surface current in terms of surface charge density and velocity.

K=συ …… (2)

Here,σis the surface charge density of the conductor andυis the velocity of each plate.

The following diagram shows a large parallel plate capacitor with surface charge +σdensity for upper plate and -σfor the lower plate of the capacitor.

02

Determine the magnetic field 

a)

From the above figure,

Write the expression for the top plate produces a magnetic field which is out page and its below point shows into page.

B=μ0K2

Write the expression for the bottom plate produces a magnetic field which is into page and its below point shows into page.

B=μ0K2

Therefore, the fields due to the plates cancel for point above the top plate and for points below the bottom plate. The fields add up between the plates.

Write the expression for magnetic field between the plates.

B=μ0K2+μ0K2=μ0K

Substituteσυ forK

B=μ0συ …… (3)

Thus, the magnetic field is B=μ0συ.

03

Determine the electric force

b)

Write the expression for the according to Lorentz force acting on the upper plate due to lower plate.

F=(K×B)da …… (4)

Here,K is the surface current andBis magnetic field.

Therefore, write the expression the force per unit area.

f=K×B …… (5)

Substituteμ0K2y^ forBandσυx^ forKin equation (5)

fm=(συx^)×(μ0K2y^)=συμ0K2(x^×y^)=συμ0K2z^

SubstituteσυforKin above equation.

fm=μ0(συ)22

Thus, the magnetic force per unit area isfm=μ0(συ)22and the direction of force is upward.

04

Determine the speed of the upper plate.

c)

Write the expression for electric field due to lower plate.

E=σ20

Here , Eis the electric field and 0is the permittivity.

Write the expression for electric force per unit area feon upper plate.

fe=σ220

Now, balance electric and magnetic forces,

fe=fmσ220=μ0σ2υ22υ2=1μ00υ=1μ00

Substitute 4π×107H/mfor permeability of air free space (μ0)and 8.85×1012C2/Nm2for permittivity of the air or free space.

υ=14π×107×8.85×1012m/s=3×108m/s

Thus, the speed of the upper plate is 3×108 m/s.

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Most popular questions from this chapter

Consider the motion of a particle with mass m and electric charge qein the field of a (hypothetical) stationary magnetic monopole qmat the origin:

B=μ04qmr2r^

(a) Find the acceleration of qe, expressing your answer in terms of localid="1657533955352" q, qm, m, r (the position of the particle), and v(its velocity).

(b) Show that the speed v=|v|is a constant of the motion.

(c) Show that the vector quantity

Q=m(r×v)-μ0qeqm4πr^

is a constant of the motion. [Hint: differentiate it with respect to time, and prove-using the equation of motion from (a)-that the derivative is zero.]

(d) Choosing spherical coordinates localid="1657534066650" (r,θ,ϕ), with the polar (z) axis along Q,

(i) calculate , localid="1657533121591" Qϕ^and show that θis a constant of the motion (so qemoves on the surface of a cone-something Poincare first discovered in 1896)24;

(ii) calculate Qr^, and show that the magnitude of Qis

Q=μ04π|qeqmcosθ|;

(iii) calculate Qθ^, show that

dt=kr2,

and determine the constant k .

(e) By expressing v2in spherical coordinates, obtain the equation for the trajectory, in the form

drdϕ=f(r)

(that is: determine the function )f(r)).

(t) Solve this equation for .r(ϕ)

Suppose you wanted to find the field of a circular loop (Ex. 5.6) at a point rthat is not directly above the center (Fig. 5.60). You might as well choose your axes so that rlies in the yzplane at (0,y,z). The source point is ( Rcos φ',Rsin ϕ',0, and ϕ'runs from 0 to 2JJ. Set up the integrals25 from which you could calculate Bx,Byand Bzand evaluate Bxexplicitly.

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.)

Find the magnetic field at point Pon the axis of a tightly woundsolenoid(helical coil) consisting of nturns per unit length wrapped around a cylindrical tube of radius aand carrying current I(Fig. 5.25). Express your answer in terms of θ1and θ2 (it's easiest that way). Consider the turns to be essentially circular, and use the result of Ex. 5.6. What is the field on the axis of an infinitesolenoid (infinite in both directions)?

Question: Using Eq. 5.88, calculate the average magnetic field of a dipole over

a sphere of radius Rcentered at the origin. Do the angular integrals first. Compare your answer with the general theorem in Prob. 5.59. Explain the discrepancy, and indicate how Eq. 5.89 can be corrected to resolve the ambiguity at . (If you get stuck, refer to Prob. 3.48.) Evidently the truefield of a magnetic dipole is

Bdip(r)=μ04πr3[3(m·r^)r^-m]+2μ03mδ3(r)Bdip(r)=μ04πr3[3m·r^r^-m]+2μ03mδ3(r)

Compare the electrostatic analog, Eq. 3.106.

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