Magnetism

Jul 20, 2024

Magnetism Lecture Notes

Basic Principles of Magnetism

  • Bar magnets have North and South poles.
  • Like poles repel, while opposite poles attract.
  • Each bar magnet generates a magnetic field that emanates from the North pole to the South pole.
  • Magnetic fields cancel out in regions of repulsion and add up in regions of attraction.

Creation of Magnetic Fields

  • Moving electric charges create magnetic fields.

  • A current-carrying wire generates a circular magnetic field around it.

  • The right-hand rule helps determine the direction of the magnetic field around a wire.

  • Formula to calculate magnetic field strength around a wire:

    [ B = \frac{μ₀ I}{2 π r} ]

    • B: Magnetic field strength (Tesla)
    • μ₀: Permeability of free space (4π imes 10^{-7}Tm/A)
    • I: Current (Amps)
    • r: Distance from the wire (meters)

Magnetic Force on a Current-Carrying Wire

  • Magnetic force (F): A magnetic field exerts a force on a moving charge or current-carrying wire.

  • Formula for magnetic force on a wire:

    [ F = ILB , \sin \theta ]

    • I: Current (Amps)
    • L: Length of the wire in the magnetic field (meters)
    • B: Magnetic field strength (Tesla)
    • θ: Angle between current direction and magnetic field
  • Right-hand rule is used to determine the direction of the magnetic force.

Example Problems

Example 1: Calculating Magnetic Field 2 cm from Wire Carrying 45 Amps

  • Given:

    • I = 45 Amps
    • r = 2 cm = 0.02 meters
  • Calculate:

    [ B = \frac{4π imes 10^{-7} imes 45}{2π imes 0.02} = 4.5 imes 10^{-4} T ]

Example 2: Distance to Produce Magnetic Field of 8 × 10⁻⁴ Tesla with 10 Amps

  • Given:

    • B = 8 × 10⁻⁴ T
    • I = 10 Amps
  • Calculate:

    [ r = \frac{4π imes 10^{-7} imes 10}{2π imes 8 imes 10^{-4}} = 2.5 imes 10^{-3} m = 2.5 mm ]

Magnetic Force on a Moving Charge

  • Formula: For a moving charge in a magnetic field, the magnetic force is given by:

    [ F = Bqv , \sin \theta ]

    • B: Magnetic field strength (Tesla)
    • q: Charge of the particle (Coulombs)
    • v: Velocity of the particle (m/s)
    • θ: Angle between velocity and magnetic field
  • Example: Proton moving east at 4 × 10⁶ m/s in a 2 × 10⁻⁴ T magnetic field

    • Calculate magnetic force:

    [ F = 2 imes 10^{-4} imes 1.6 imes 10^{-19} imes 4 imes 10^{6} = 1.28 imes 10^{-16} N ]

Magnetic Force in a Circular Path

  • A charged particle in a perpendicular magnetic field will move in a circular path.

  • The radius of such a path can be determined using:

    [ r = \frac{mv}{Bq} ]

  • Example: Proton with speed 5 × 10⁶ m/s in a 2.5 T magnetic field

    • Calculate radius:

    [ r = \frac{1.673 imes 10^{-27} imes 5 imes 10^{6}}{2.5 imes 1.6 imes 10^{-19}} = 2.09 imes 10^{-2} m = 2.09 cm ]

Interaction Between Parallel Wires

  • Attraction: Parallel wires carrying current in the same direction attract each other.

  • Repulsion: Parallel wires carrying current in opposite directions repel each other.

  • Magnetic field created by one wire affects the other.

  • Formula to calculate force per unit length between two wires:

    [ F/L = \frac{μ₀ I₁ I₂}{2π d} ]

Example: Force Between Two Wires

  • Given:

    • I₁ = I₂ = 50 Amps
    • L = 30 meters
    • d = 2 cm = 0.02 meters
  • Calculate:

    [ F = \frac{4π imes 10^{-7} imes 50 imes 50 imes 30}{2π imes 0.02} = 0.75 N ]

Ampere's Law

  • Ampere's Law relates the integrated magnetic field around a closed loop to the electric current passing through the loop:

    [ \oint \mathbf{B} , \cdot d \mathbf{l} = μ₀ Iₑ ]

  • Helps derive the magnetic field for different geometries like a solenoid.

  • Solenoid: A coil of wire with many loops; magnetic field strength inside is given by:

    [ B = μ₀ n I ]

    • n: Number of turns per meter
    • I: Current (Amps)

    Example: Magnetic Field in Solenoid

    • Given:
      • Length = 15 cm = 0.15 m
      • Turns = 800
      • Current = 5 Amps
    • Calculate: Turns per meter

    [ n = \frac{800}{0.15} = 5333 , \text{turns/meter} ]

    • Calculate magnetic field:

    [ B = 4π imes 10^{-7} imes 5333 imes 5 = 0.0335 T ]

Torque on a Current-Carrying Loop

  • A current-carrying loop in a magnetic field experiences a torque:

    [ \tau = n I A B , \sin \theta ]

    • τ: Torque
    • n: Number of loops
    • I: Current
    • A: Area of the loop (length × width for rectangular)
    • B: Magnetic field strength
    • θ: Angle between normal to the loop and magnetic field
  • Maximum torque occurs when angle θ = 90°.

Example: Maximum Torque on a Circular Coil

  • Given:

    • Radius = 30 cm = 0.3 m
    • Loops = 50
    • Current = 8 Amps
    • Magnetic Field = 5 Tesla
  • Area:

    [ A = πr^2 = π imes 0.3^2 = 0.2827 m^2 ]

  • Calculate torque:

    [ \tau = 50 imes 8 imes 0.2827 imes 5 = 565.5 , \text{N.m} ]

Conclusion

  • Recap of key formulas and concepts:
    • Magnetic field around wire: ( B = \frac{μ₀ I}{2πr} )
    • Magnetic force on wire: ( F = ILB , \sin \theta )
    • Magnetic force on charge: ( F = Bqv , \sin \theta )
    • Radius of particle path: ( r = \frac{mv}{Bq} )
    • Force between parallel wires: ( F/L = \frac{μ₀ I₁ I₂}{2π d} )
    • Magnetic field inside solenoid: ( B = μ₀ n I )
    • Torque on loop: ( \tau = n I A B , \sin \theta )

Always remember to use the right-hand rule to determine the direction of magnetic fields and forces.