(a) A phonograph record carries a uniform density of "static electricity" σ.If it rotates at angular velocity ω,what is the surface current density Kat a distance r from the center?

(b) A uniformly charged solid sphere, of radius Rand total charge Q,is centered

at the origin and spinning at a constant angular velocity ωabout the zaxis. Find

the current density J at any point r,θ,ϕwithin the sphere.

Short Answer

Expert verified

(a) The surface current density of a phonograph record carrying a uniform density of "static electricity" σand rotating at angular velocity ωis σωr.

(b) The current density of a uniformly charged solid sphere, of radius Rand total charge Q, centered at the origin and spinning at a constant angular velocity ωabout the zaxis is 3Qωrsinθ4πR3.

Step by step solution

01

Given data

A phonograph record carries a uniform density of "static electricity" σand rotates at angular velocity ω.

A uniformly charged solid sphere, of radius Rand total charge Q,is centered

at the origin and spinning at a constant angular velocity ωabout the zaxis.

02

Surface and volume current density

The surface current density of a surface charge density σmoving with a speed v is

K=σv.....(1)

The volume current density of a volume charge density ρmoving with a speed v is

J=ρv.....(2)

03

Surface current density of charged phonograph

The speed of the charge density rotating with angular velocityωin a circle of radius r is

v=ωr

Substitute this in equation (1) to get

K=σωr

Thus, the surface current density is σωr.

04

Volume current density of charged sphere

The volume charge density of a sphere of radius R uniformly charged with a charge Q is

ρ=Q43πR3=3Q4πR3

The speed at any point in the sphere rotating with angular velocity ωabout the z at a radial distance r and making angle θwith the z axis is

v=ωrsinθ

Substitute these in equation (2) to get

J=3Q4πR2×ωrsinθ=3Qωrsinθ4πR3

Thus, the volume current density islocalid="1657774147962" 3Qωrsinθ4πR3.

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Most popular questions from this chapter

Analyze the motion of a particle (charge q, massm ) in the magnetic field of a long straight wire carrying a steady current I.

(a) Is its kinetic energy conserved?

(b) Find the force on the particle, in cylindrical coordinates, withI along thez axis.

(c) Obtain the equations of motion.

(d) Supposez. is constant. Describe the motion.

(a) Prove that the average magnetic field, over a sphere of radius R,due to steadycurrents inside the sphere, is

Bave=μ04π2mR3

wheremis the total dipole moment of the sphere. Contrast the electrostatic

result, Eq. 3.105. [This is tough, so I'll give you a start:

Bave=143πR3Bdτ

WriteBas×A ,and apply Prob. 1.61(b). Now put in Eq. 5.65, and do the

surface integral first, showing that

1rda=43πr'

(b) Show that the average magnetic field due to steady currents outsidethe sphere

is the same as the field they produce at the center.

For a configuration of charges and currents confined within a volume

V,show that

VJdτ=dpdt

where pis the total dipole moment.

Suppose you wanted to find the field of a circular loop (Ex. 5.6) at a point r that is not directly above the center (Fig. 5.60). You might as well choose your axes so that r lies in the yz plane at (0, y, z). The source point is (R cos¢', R sin¢', 0), and ¢' runs from 0 to 2Jr. Set up the integrals25 from which you could calculate Bx , By and Bzand evaluate Bx explicitly.

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.

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