If a current carrying conductor is held in the right hand with the thumb pointing in the direction of the current, the direction in which the fingers encircle the wire gives the direction of the magnetic lines of force around the wire
If a corkscrew is screwed along a conductor in the direction of current, the direction in which the ends of the handle move gives the direction of lines of magnetic force
In a current-carrying circular coil, when the direction of current is downward, the direction of magnetic lines of force is clockwise. When the direction of current is upward, the direction of magnetic lines of force is anticlockwise
Thumb, first finger, and second finger of the left hand at right angles
First finger indicates the direction of the magnetic field, second finger indicates the direction of current, thumb indicates the direction of force on the conductor
Forefinger, middle finger, and thumb of the right hand at right angles
Forefinger points in the direction of the magnetic field, thumb denotes the direction of motion of the conductor, middle finger points in the direction of induced current
Electric charges can be positive or negative, while electric current is always considered as flowing from positive to negative.
A moving charge produces an electric current, which generates a magnetic field around it.
The magnetic field lines are always perpendicular to the direction of motion.
The direction of the force on a charged particle depends on its velocity and the direction of the magnetic field.
An electron with velocity v has a magnetic moment m = -ev/2c (where c is the speed of light).
Magnetic moments have units of ampere-metres squared (Am^2) or joules per tesla (JT^-1).
Magnetic moments have units of ampere-metres squared (Am^2) and are measured using a magnetometer.
In a solenoid, the magnetic field inside is uniform and parallel to its axis.
In a uniform magnetic field, the torque experienced by a dipole is given by T = mB sinθ, where B is the magnitude of the magnetic field and θ is the angle between the dipole axis and the field vector.
A current loop can be considered as an equivalent magnetic dipole.