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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.

Short Answer

Expert verified

The charge qentering a region of uniform magnetic field Band getting deflected by a distance dis positive. The momentum of the charge is qBa2+d22d.

Step by step solution

01

Given data

A particle of charge qenters a region of uniform magnetic field pointing into the page.

The field deflects the particle a distanced above the original line of flight.

02

Define the formula for the force on a charge in a magnetic field and its momentum

The force on a charge q moving with a velocity v in the presence of a magnetic field B is

F=q(v×B)     .....(1)

The momentum of such a particle moving in a circular trajectory of radiusR is

p=qBR     .....(2)

03

Determine the momentum of the given charge

Since V is towards the right and Bpoints into the page, from equation (1) the force must be pointing upwards if the charge is positive. That is indeed the direction of the deflection. Hence the charge is positive.

In the figure, using Pythagoras theorem,

role="math" localid="1657687257870" (Rd)2+a2=R2R=a2+d22d

Substitute this in equation (2) and get

p=qBa2+d22d

Thus, the momentum of the particle is qBa2+d22d.

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Most popular questions from this chapter

Use the results of Ex. 5.11to find the magnetic field inside a solid sphere, of uniform charge density ρand radius R, that is rotating at a constant angular velocity \omega.

Show that the magnetic field of an infinite solenoid runs parallel to the axis, regardless of the cross-sectional shape of the coil,as long as that shape is constant along the length of the solenoid. What is the magnitude of the field, inside and outside of such a coil? Show that the toroid field (Eq. 5.60) reduces to the solenoid field, when the radius of the donut is so large that a segment can be considered essentially straight.

Find the vector potential above and below the plane surface current in Ex. 5.8.

(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.

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.]

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