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Question -

(a) A monoenergeticelectron beam with electron speed of 5.20 × 106 m s−1 issubject to a magnetic field of 1.30 × 10−4 T normal to the beamvelocity. What is the radius of the circle traced by the beam, given e/m forelectron equals 1.76 × 1011 C kg−1.

(b) Is the formula youemploy in (a) valid for calculating radius of the path of a 20 MeV electronbeam? If not, in what way is it modified?

[Note: Exercises11.20(b) and 11.21(b) take you to relativistic mechanics which is beyond thescope of this book. They have been inserted here simply to emphasise the pointthat the formulas you use in part (a) of the exercises are not valid at veryhigh speeds or energies. See answers at the end to know what ‘very high speedor energy’ means.]



Answer -

(a)Speed of anelectron, v = 5.20 × 106 m/s

Magnetic field experienced by theelectron, B = 1.30 × 10−4 T

Specific charge of an electron, e/m =1.76 × 1011 C kg−1

Where,

e = Charge on the electron = 1.6 × 10−19 C

m = Mass of the electron = 9.1 × 10−31 kg−1

The force exerted on theelectron is given as:

θ = Angle between themagnetic field and the beam velocity

Themagnetic field is normal to the direction of beam.

The beam traces a circular path of radius, r.It is the magnetic field, due to its bending nature, that provides thecentripetal force for the beam.

Hence, equation (1)reduces to:

Therefore, the radius ofthe circular path is 22.7 cm.

(b) Energy of the electron beam, =20 MeV

The energy of the electronis given as:

This result is incorrect because nothing canmove faster than light. In the above formula, the expression (mv2/2)for energy can only be used in the non-relativistic limit, i.e., for v << c

When very high speeds areconcerned, the relativistic domain comes into consideration.

In the relativisticdomain, mass is given as:

Where,

= Mass of the particle atrest

Hence, the radius of thecircular path is given as:

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