CBSE Class 12-science Answered

For any general shape of the wire, magnetic field due to current carrying wire is given by Biot Savart Law:

where is a vector tangent to the current wire equal to dy  for a straight wire along y-axis.

Consider a circular loop of radius r carrying a current I.

Since, dl

Applying Biot- Savart law:

For entire closed circular loop;

For n turns of a coil;

The magnetic field lines due to a circular wire form closed loops. The direction of the magnetic field is given by right hand thumb rule.

The current carrying loop produces a magnetic field around it, whose magnetic moment is given as I x A(here, I is the current through the loop and A is the area of cross-section; hence it behaves like a magnet.

OR

The principle behind the working of a cyclotron is that in a uniform magnetic field, charged particle executes uniform circular motion with a frequency that is independent of its radius (which depends on the energy of the particle)

A cyclotron has a uniform magnetic field spread over a circular region split in two halves by two semi-circular D's, D₁ and D₂.

Let us assume for definiteness that the particle has positive charge. Then, as it comes around in D₁ clockwise to point P, D₁ and D₂ are so connected to an alternating voltage that at this point, D₁ is at a higher potential than D₂. This accelerates the particles, so that it gains kinetic energy by T = q(V₁ - V₂) where V₁ and V₂ are potentials of D₁ and D₂ respectively.

This increases the radius of circular motion since and is proportional to square root of kinetic energy.

Since frequency of circular motion, given by  is independent of r, the frequency of alternating voltage is made twice f_c, so that when the particle reaches point Q, V₂ and V₁ flip and D₂ is at higher potential than D₁, so that particle is accelerated again. This goes on till the kinetic energy is high enough and consequently the radius is large enough so that the particle is ejected out tangentially from the magnetic field with high energy.

Frequency  is independent of the energy or the speed of the charged particle.

Upper limit is relativistic speeds. The cyclotron is limited by relativistic effects due to which the mass of the accelerating particle increases with energy and so fc changes after each cycle.

Also, for light charged particles, fc is enormously high and difficult to maintain. Also, it is not easy to maintain uniformity of the magnetic field. To add to that, a charged particle in circular motion (even if it is uniform) is accelerating and all accelerated charges radiate electromagnetic energy, thereby losing energy.