Chapter 2: Magnetism

2.1 Introduction to Magnetism

  • Definition: Magnetism is the force of attraction or repulsion experienced by certain materials in the presence of a magnetic field.

  • Not all materials are affected by magnetism.

    • Non-magnetic materials: wood, glass, paper, plastic

    • Magnetic materials (common metals): Iron, nickel, cobalt

2.1.1 Magnetic Field

  • A Magnetic Field (B) is defined as a vector field that exerts a magnetic force on moving electric charges.

  • Steady Magnetic Field: A magnetic field that remains constant over time, resulting from a steady electrical current.

  • Unstable Magnetic Field: A magnetic field that varies over time.

2.1.2 Historical Perspective

  • In 1820, Hans Christian Oersted conducted an experiment demonstrating the relationship between electricity and magnetism.

    • Oersted placed a compass needle near a wire carrying an electric current.

    • When the electric current was activated (switch closed), the compass needle deflected as though influenced by a magnet.

2.1.3 Lorentz Force

  • The Lorentz Force describes the force acting on a moving charge in a magnetic field.

    • The force depends on three factors:

    1. Charge of the particle (electric quantity)

    2. Velocity of the particle

    3. Instantaneous position of the particle

    • This force is always perpendicular to both the magnetic field and the velocity of the charge.

Right-Hand Rule
  • A convention (right-hand rule) to determine the direction of the Lorentz force.

    • Point the thumb of your right hand in the direction of the velocity of the charge.

    • Point the fingers in the direction of the magnetic field lines.

    • The palm will face the direction of the force acting on a positive charge.

2.1.4 Properties of Magnetic Fields

  • The magnetic field strength is characterized by the density of magnetic field lines: more lines indicate a stronger field.

  • Direction of Magnetic Field Lines: Defined to be the direction in which the north end of a compass needle points, tangent to the field lines at any point.

  • Properties:

    • Magnetic field lines cannot cross, indicating a unique magnetic field at any given point.

    • Magnetic field lines form continuous closed loops without beginning or end, distinguishing them from electric field lines that begin and end on charges.

2.1.5 Units of Magnetic Field

  • The unit of magnetic field strength is the Tesla (T).

  • Another smaller unit is Gauss (G):

    • 1 T = 10^4 G

2.1.6 Magnetic Field Strength Examples

  • Pulsar magnetic field: approximately 108T10^8 T

  • Near certain atomic nuclei: 104T10^4 T

  • Superconducting magnet: can generate up to 25T25 T

  • Large laboratory magnets: greater than 2T2 T

  • Earth’s magnetic field: approximately 104T10^{-4} T

  • Indoor magnetic fields: range from 107extto106T10^{-7} ext{ to } 10^{-6} T

  • Human heart: generates a magnetic field of approximately 3imes1010T3 imes 10^{-10} T

2.1.7 Magnetic Induction

  • The integral of magnetic induction over a curved surface within a magnetic field defines magnetic flux.

    • Unit of Magnetic Flux: Weber (Wb)

    • Mathematical representation: extFluxext(Φ)=BimesAext{Flux} ext{ } (Φ) = B imes A where A is the area and B is the magnetic field strength.

2.2 Ampere’s Circulation Law

  • Ampere’s Law states that the line integral of the magnetic field around any closed path equals extμ0ext{μ}_0 times the total steady current passing through any surface bounded by that path.

    • Bdl=extμ<em>0I</em>totalB \bullet dl = ext{μ}<em>0 I</em>{total}

  • This law is essential for calculating magnetic fields in configurations exhibiting high degrees of symmetry.

Applications and Examples
  1. Long Straight Wire:

    • For a straight wire carrying current II, Ampere's Law can be applied to a circular path to find the magnetic field strength at a distance rr from the wire.

    • Inside the wire (r<R):
      B=racμI2extπR2B = rac{μI}{2 ext{π}R^2}

    • Outside the wire (rRr≥R):
      B=racμI2extπrB = rac{μI}{2 ext{π}r}

  2. Infinite Current-Carrying Plate:

    • Considered as multiple infinite straight wires contributing to the overall magnetic field.

    • For such a plate, the magnetic induction can be calculated as being parallel to the plate and perpendicular to the direction of current.

  3. Ideal Solenoid:

    • A long, straight solenoid with closely spaced turns creates a uniform magnetic field inside while being zero outside.

    • Applying Ampere’s Law to the rectangular path leads to uniform field expressions.

Conclusion

  • Understanding the principles of magnetism, magnetic fields, Lorentz force, Ampere's Law, and their applications in various configurations is essential for the comprehensive study of electromagnetism.

  • The unique properties of magnetic fields set them apart from electric fields, forming the basis for various technological applications in science and engineering.