Moving charges create magnetic fields, which is the basis for electromagnetism. The study of moving charges in a magnetic field is crucial for understanding electromagnets, electric motors, and generators.
A moving charge in a magnetic field experiences a force called the Lorentz force, given by:
F = q (E + v × B)
where:
The trajectory of a charged particle depends on the direction of its velocity relative to the magnetic field.
When a charged particle moves perpendicular to the magnetic field, it follows a circular path with a radius given by:
r = (m v) / (q B)
The time period of revolution is:
T = (2πm) / (qB)
The particle follows a helical path, with a pitch (distance moved along the field in one cycle) given by:
Pitch = vparallel × T
Biot-Savart Law describes the magnetic field due to a small current element:
dB = (μ₀ / 4π) * (I dl × r̂) / r²
where:
Ampère’s Law states that the line integral of the magnetic field around a closed loop is proportional to the total current enclosed:
∮ B ⋅ dl = μ₀ Ienclosed
The magnetic field at a distance r from a long straight wire carrying current I is given by:
B = (μ₀ I) / (2πr)
At the center of a circular loop of radius R, carrying current I, the field is:
B = (μ₀ I) / (2R)
A solenoid creates a uniform magnetic field inside it, given by:
B = μ₀ n I
where n is the number of turns per unit length.
Two parallel conductors carrying current exert a force on each other. The force per unit length is:
F/L = (μ₀ I₁ I₂) / (2πd)
If the currents flow in the same direction, the wires attract each other; if in opposite directions, they repel.
A current-carrying loop placed in a uniform magnetic field experiences a torque given by:
τ = NIAB si