When a current-carrying conductor is placed in a magnetic field, a force is exerted on the conductor due to the interaction between the magnetic field and the current. This force is known as the magnetic Lorentz force and its direction is perpendicular to both the magnetic field and the current flow. The magnitude of the force depends on the strength of the magnetic field, the current flowing through the conductor, and the length of the conductor exposed to the magnetic field.
The force experienced by a current-carrying conductor in a magnetic field is strongest when the current and magnetic field are perpendicular to each other, maximizing the force according to the right-hand rule.
The force on the electron would be perpendicular to both the direction of its motion and the current flow in the wire. This is described by the right-hand rule for magnetic fields, where the force would point in a specific direction based on the orientations of the current and the electron's motion.
The shape of the magnetic field lines around a straight current-carrying conductor is circular, with the conductor at the center of each circular loop. These magnetic field lines form concentric circles around the conductor, perpendicular to the direction of the current flow.
A straight current-carrying wire produces a magnetic field around it, which can be described as a circular magnetic field perpendicular to the direction of current flow. This magnetic field is responsible for creating a force on any nearby moving charges.
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When a current-carrying conductor is placed in a magnetic field, a force is exerted on the conductor due to the interaction between the magnetic field and the current. This force is known as the magnetic Lorentz force and its direction is perpendicular to both the magnetic field and the current flow. The magnitude of the force depends on the strength of the magnetic field, the current flowing through the conductor, and the length of the conductor exposed to the magnetic field.
When a magnetic field is parallel to a current-carrying wire, there is no force acting on the wire. This is because the magnetic force on a current-carrying wire is perpendicular to both the current and the magnetic field.
It experiences maximum force when it is placed perpendicular to the direction of magnetic field.
The force experienced by a current-carrying conductor in a magnetic field is strongest when the current and magnetic field are perpendicular to each other, maximizing the force according to the right-hand rule.
When the conductor,magnetic field and motion are perpendicular to each other
The circular loop of wire carrying current will align itself in a plane perpendicular to the direction of the magnetic field created by the current flowing through the loop. This is a result of the magnetic force exerted on the current-carrying loop in the presence of the magnetic field.
A current-carrying conductor in a magnetic field experiences a force due to the interaction between the magnetic field and the current. The direction of this force depends on the direction of the current in the conductor and the direction of the magnetic field. The rule that can be used to determine the direction of the force is the right-hand rule, where the thumb points in the direction of the current and the fingers point in the direction of the magnetic field, indicating the direction of the force.
The force due to Earth's magnetic field on a wire carrying a current vertically downward would be perpendicular to both the current flow and the magnetic field lines, according to the right-hand rule. This force would either point to the east or west depending on the direction of the magnetic field lines.
The wire will experience a force due to the interaction between the magnetic field and the current. The direction of the force can be determined using the right-hand rule. This phenomenon is described by the magnetic force equation, F = I * L * B * sin(theta), where I is the current, L is the length of the wire, B is the magnetic field strength, and theta is the angle between the wire and the magnetic field.
Conductor magnitude force refers to the force experienced by a current-carrying conductor placed in a magnetic field. This force is known as the Lorentz force and is perpendicular to both the direction of the current and the magnetic field. It can be calculated using the formula F = BIL, where B is the magnetic field strength, I is the current, and L is the length of the conductor in the magnetic field.
Force perpendicular is equal to the force component that acts perpendicular to a surface or object. It is calculated by multiplying the force magnitude by the sine of the angle between the force vector and the direction perpendicular to the object.