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Electrons undergoing cyclotron motion can be sped up by increasing the magnetic field; the accompanying electric field will impart tangential acceleration. This is the principle of the betatron. One would like to keep the radius of the orbit constant during the process. Show that this can be achieved by designing a magnet such that the average field over the area of the orbit is twice the field at the circumference (Fig. 7.53). Assume the electrons start from rest in zero field, and that the apparatus is symmetric about the center of the orbit. (Assume also that the electron velocity remains well below the speed of light, so that nonrelativistic mechanics applies.) [Hint: Differentiate Eq. 5.3 with respect to time, and use .F=ma=qE]

Short Answer

Expert verified

It is proved that the average field over the area of the orbit is twice the field at the circumference.

Step by step solution

01

Write the given data from question.

The electron velocity is remains below the speed of light.

The start is from the rest.

The force on electron is as follows:qE=maF=qE

02

Determine the formula to prove that the average field over the area of the orbit is twice the field at the circumference.

The expression for magnetic force on the electron is given as follows.

FB=Bqv 鈥︹ (1)

Here,B is the magnetic field,q is the charge and v is the velocity.

The expression for centripetal force acting on the electron is given as follows.

Fc=mv2R 鈥︹. (2)

Here,m is the mass of the electron and R is the radius.

The expression for the electric force on the electron is given by,

role="math" localid="1658239700853" FE=qE 鈥︹. (3)

03

Prove that the average field over the area of the orbit is twice the field at the circumference.

The magnetic and centripetal force on the electron is equal.

Bqv=mv2RqBR=mv

Differentiate the above equation with respect to t.

qRdBdt=mdvdt

Substituteafor dvdtinto above equation.

qRdBdt=ma

Substitute qEfor mainto above equation.

qRdBdt=qERdBdt=E 鈥︹. (4)

We know,

Edl=ddtE(2R)=ddtE=12Rddt

Substitute12Rddt for Einto equation (4).

RdBdt=12RddtdBdt=12R2ddtB=121R2+C

Here, Cis constant.

Att=0,B=0,C=0

Therefore,

B(R)=12(1R2)

Hence,the average field over the area of the orbit is twice the field at the circumference.

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Most popular questions from this chapter

A thin uniform donut, carrying charge Q and 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).

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(c) According to quantum mechanics, the angular momentum of a spinning electron is 12 , where is Planck's constant. What, then, is the electron's magnetic dipole moment, in localid="1657713870556" Am2 ? [This semi classical value is actually off by a factor of almost exactly 2. Dirac's relativistic electron theory got the 2 right, 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(localid="1657713972487" (e/2m), where e is the charge of the electron and m is its mass, is called the Bohr magneton.]

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Question: The preceding problem was an artificial model for the charging capacitor, designed to avoid complications associated with the current spreading out over the surface of the plates. For a more realistic model, imagine thin wires that connect to the centers of the plates (Fig. 7.46a). Again, the current I is constant, the radius of the capacitor is a, and the separation of the plates is w << a. Assume that the current flows out over the plates in such a way that the surface charge is uniform, at any given time, and is zero at t = 0.

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Figure 7.46

(c) Repeat part (b), but this time uses the cylindrical surface in Fig. 7.46(b), which is open at the right end and extends to the left through the plate and terminates outside the capacitor. Notice that the displacement current through this surface is zero, and there are two contributions to Ienc.

A long solenoid with radius a and n turns per unit length carries a time-dependent currentl(t) in the^ direction. Find the electric field (magnitude and direction) at a distance s from the axis (both inside and outside the solenoid), in the quasistatic approximation.

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