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 perpendicular to the magnetic field will follow a circular path due to the magnetic force acting as a centripetal force.

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

A charged particle moving perpendicular to a uniform magnetic field will move in a circular path due to the magnetic force acting as a centripetal force.

The magnetic field lines around a circular loop of wire carrying current are in the form of concentric circles.

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.

According to Fleming's left-hand rule, the force is perpendicular to both the magnetic field and the direction of current.

Using the right-hand rule, the magnetic field direction at a point above the wire is away from the wire.

When a loop of wire is placed in a changing magnetic field, electromagnetic induction occurs, generating an electromotive force (EMF) in the loop.

Using the right-hand rule, if the magnetic field is into the paper and the charge moves to the right, the force will be upwards.

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

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 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 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 in a magnetic field is maximum when the angle between the velocity and the magnetic field is 90 degrees.

The radius of the circular path is directly proportional to the speed of the charged particle in a uniform magnetic field.

The magnetic force is maximum when the angle between the conductor and the magnetic field is 90 degrees, as sin(90°) = 1.

Magnetic field lines emerge from the north pole and enter the south pole of a bar magnet.

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

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.

The force on a charged particle moving in a magnetic field is maximum when the particle moves perpendicular to the field.

When a magnet is cut into two pieces, each piece becomes a magnet with its own north and south poles, thus maintaining the magnetic field lines.

The magnetic field strength inside a solenoid increases with the number of turns, as it is directly proportional to the number of turns per unit length.

The magnetic field strength inside a solenoid is directly proportional to the number of turns per unit length. Therefore, if the number of turns per unit length is increased, the magnetic field strength also increases.

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

When the current in a wire 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.