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A thin uniform donut, carrying charge Qand mass M, rotates about its axis as shown in Fig. 5.64.

(a) Find the ratio of its magnetic dipole moment to its angular momentum. This is called the gyromagnetic ratio (or magnetomechanical ratio).

(b) What is the gyromagnetic ratio for a uniform spinning sphere? [This requires no new calculation; simply decompose the sphere into infinitesimal rings, and apply the result of part (a).]

(c) According to quantum mechanics, the angular momentum of a spinning electron is role="math" localid="1658120028604" 12, where is Planck's constant. What, then, is the electron's magnetic dipole moment, in role="math" localid="1658120037359" A×M2 ? [This semi classical value is actually off by a factor of almost exactly 2. Dirac's relativistic electron theory got the 2right, and Feynman, Schwinger, and Tomonaga later calculated tiny further corrections. The determination of the electron's magnetic dipole moment remains the finest achievement of quantum electrodynamics, and exhibits perhaps the most stunningly precise agreement between theory and experiment in all of physics. Incidentally, the quantity (e2m ), where e is the charge of the electron and m is its mass, is called the Bohr magneton.]

Short Answer

Expert verified

(a) The gyromagnetic ratio of donut is Q2M.

(b) The gyromagnetic ratio of uniform spinning sphere is also Q2M.

(c) The magnetic dipole moment of electron is 4.61×10-24A×m2.

Step by step solution

01

(a) Step 1: Determine the gyromagnetic ratio

The time period of rotation of donut is given as:

t=2πω

The current in the donut is given as:

I=Qt

I=Q2πω

I=2π

The cross sectional area of the donut is given as:

A=πR2

The magnetic dipole moment of donut is given as:

m=I×A

m=Qa2ππR2

m=QaR22

The angular momentum of donut is given as:

L=MωR2

The gyromagnetic ratio of the donut is given as:

g=mL

Substitute all the values in the above equation.

g=QMωR2

g=Q2M

Therefore, the gyromagnetic ratio of donut is Q2M.

02

(b) Step 2: Determine the gyromagnetic ratio of uniform spinning sphere

The gyromagnetic ratio of the donut does not depend on the geometric feature (radius) of donut so the gyromagnetic ratio of uniform spinning sphere would be same as of donut.

Therefore, the gyromagnetic ratio of uniform spinning sphere is also Q2M.

03

(c) Step 3: Determine the magnetic dipole moment of electron

Consider the expression for the magnetic dipole moment:

me=e4M

Here, meis Planck’s constant and its value is 1.05×10-34J×s, eis the charge of electron and its value is 1.6×1019C, mis the mass of electron and its value is 9.11×1031kg.

Substitute all the values in the above equation.

me=1.6×1019C1.05×1034Js49.11×1031kg

me=4.61×10-24A×m2

Therefore, the magnetic dipole moment of electron is 4.61×10-24A×m2.

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Most popular questions from this chapter

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?

A particle of charge qenters a region of uniform magnetic field B (pointing intothe page). The field deflects the particle a distanced above the original line of flight, as shown in Fig. 5.8. Is the charge positive or negative? In terms of a, d, Band q,find the momentum of the particle.

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)

(a) Check that Eq. 5.65 is consistent with Eq. 5.63, by applying the divergence.

(b) Check that Eq. 5.65 is consistent with Eq. 5.47, by applying the curl.

(c) Check that Eq. 5.65 is consistent with Eq. 5.64, by applying the Laplacian.

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 Bzis zero at the point midway between them (z=0)

(b) If you pick d just right, the second derivative ofBwill 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 dsuch that

2B/z2=0at the midpoint, and find the resulting magnetic field at the center.

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