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Moving Charges and Magnetism Summary

  • The Biot-Savart law asserts that the magnetic field dB due to an element dl carrying a steady current i at a point P at a distance r from the current element is:
magnetic field dB due to an element
  • The constant m0 has the exact value

m0 = 4p x 10-7 T m A-1It is the permeability of free space. It is related to e0, the permittivity of free space and the speed of light in free

space c, by

  • he magnitude of the magnetic field at a distance R from a long, straight wire carrying a current i is given by:
magnitude of the magnetic field of straight wire

The field lines are circles concentric with the wire.

  • The magnitude of the magnetic field due to a N-turn circular coil of radius R carrying a current i at an axial distance x from the center is
magnitude of the magnetic field due to a N-turn circular coil

At the center this reduces to

  • Ampere's Circuital Law: We have discussed a simplified form of this law. If B is directed along the tangent to every point on the perimeter L of a closed curve and is constant in magnetic along perimeter then.

BL = m0 iewhere ie is the net, current enclosed by the closed circuit.

  • Employing Ampere's law one can show that the magnitude of the field B inside a long solenoid carrying a current i is

B = m0 ni

where n is the number of turns per unit length. For a toroid one obtains,

magnetic field of toroid

where N is the total number of turns and r the average radius.

  • The total force on a charge q moving with velocity v in the presence of magnetic and electric fields B and E, respectively is called the Lorentz force. It is given by the expression:
Lorentz force

The magnetic force q (v x B) is normal to v and work done by it is zero.

  • In a uniform magnetic field B, the charge q described in (7) executes circular orbit in the plane normal to B. Its frequency of uniform circular motion is called the cyclotron frequency and is given by:
cyclotron frequency

This frequency is independent of the particle's speed and radius. This fact is exploited in a machine, the cyclotron, which is used to accelerate charged particles.

  • A straight conductor of length l and carrying steady current i experiences a force F in a uniform external magnetic field B,

F = il x B

where |l| = l and the direction of l is given by the direction of the current.

  • Parallel currents attract and anti-parallel currents repel.
  • A planar loop carrying a current i, having N closely, wound turns, and an area A possesses a magnetic moment m where, m = N i A and the and the direction of m is given by the right-hand thumb rule: curl the palm of your right hand along the loop with the fingers pointing in the direction of the current. The thumb sticking out gives the direction of m (and A).

When this loop is placed in a uniform magnetic field B, the force F on it isF = 0

And the torque on it is,

t = m x B

In a moving coil galvanometer, this torque is balanced by a counter - torque due to a spring, yielding.

kf = Ni AB

where f is the equilibrium deflection and k the torsion constant of the spring.

  • An electron moving around the central nucleus has a magnetic moment ml given by:
magnetic moment of electron

where l is the magnitude of the angular momentum of the circulating electron about the central nucleus. The

smallest value of ml is called the Bohr magneton mB and it is

mB = 9.27 x 10-24J/T

Moving Charges and Magnetism
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