通電ワイヤ上の磁力: 例

A magnetic force acts on a current-carrying conductor when it is placed in a magnetic field. Moving charges in the wire experience a force perpendicular to both the current direction and the magnetic field. The magnitude of this force depends on the current strength, conductor length, magnetic field strength, and the angle between them. Using the right-hand rule helps determine the force direction.

The magnetic force on a current-carrying conductor is determined by the cross product of current direction and magnetic field direction. The right-hand rule provides a quick method: point your fingers along the current direction, curl them toward the magnetic field direction, and your thumb points in the force direction. This perpendicular relationship ensures the force acts at 90 degrees to both vectors.

To find the total force on a conductor with straight and curved segments, calculate the force on each section separately, then add them vectorially. For straight segments carrying current in a uniform field, use F = IL × B. For curved segments, divide them into infinitesimal elements and integrate the force contributions across the entire curve to obtain the total force.

A sufficiently strong magnetic field creates an upward force on a current-carrying wire that can equal and oppose the downward gravitational force. When these forces balance, the tension in supporting leads becomes zero and the wire achieves static equilibrium. The magnetic force magnitude depends on current strength and field strength, allowing precise force control through current adjustment.

The magnetic force magnitude depends on the sine of the angle between current direction and magnetic field direction. When perpendicular, the angle is 90 degrees and force is maximum. For curved conductors, different segments make different angles with the field, so their force components vary. Integration accounts for these varying angles across the curved path.

To find the required current, set up a free-body diagram balancing gravitational and magnetic forces. Use the right-hand rule to confirm the magnetic force points upward. Then equate the weight force to the magnetic force expression: mg = BIL. Solving for current gives I = mg/(BL), where m is mass, g is gravitational acceleration, B is field strength, and L is wire length.

For curved segments, divide the path into infinitesimal elements of length dl at varying angles to the magnetic field. Each element experiences a small force dF = I(dl × B). Integrating this expression over the entire curve from zero to the total angle yields the total force on the curved section. This method handles the changing angle and direction of force components along the curve.