A charged particle moving perpendicularly to a magnetic field experiences a magnetic force that acts as a centripetal force, causing it to move in a circular path.

A charged particle moving in a magnetic field experiences a force that is perpendicular to its velocity, resulting in circular motion.

According to Fleming's left-hand rule, the force on a current-carrying conductor in a magnetic field is perpendicular to both the current and the magnetic field.

The strength of the magnetic field in a solenoid is primarily determined by the number of turns per unit length and the current flowing through it.

The force experienced by a current-carrying conductor in a magnetic field is directly proportional to the magnetic field strength. Therefore, if the magnetic field strength is doubled, the force also doubles.

The force on a current-carrying conductor is directly proportional to the magnetic field strength, so if the magnetic field strength is doubled, the force also doubles.

The force on a charged particle moving in a magnetic field is maximum when the angle between the velocity and the magnetic field is 90 degrees.

When the current in a solenoid is reversed, the direction of the magnetic field also reverses.

The magnetic field around a long straight conductor decreases with distance. Specifically, it is inversely proportional to the distance from the conductor.

The direction of the magnetic field around a straight conductor carrying current is counterclockwise when viewed from the positive end of the conductor.

Increasing the current in a solenoid increases its magnetic field strength, as the magnetic field is directly proportional to the current.

The magnetic field inside a long solenoid is uniform and parallel to the axis of the solenoid.

Iron is a ferromagnetic material, which means it can be magnetized and has a high magnetic permeability.

Iron is considered a ferromagnetic material, which can be magnetized and retains its magnetism.