Topic 7 of 7
Why a current-carrying coil turns
Opposite sides of a current-carrying coil carry current in opposite directions. In a magnetic field, the forces on those sides can form a pair that turns the coil.
A moment is the turning effect of a force about a pivot or axis. It depends on the force and the perpendicular distance from the axis to the force's line of action. Use Fleming's left-hand rule to find each magnetic force.
Follow the current around one coil
The two active sides are parts of one conducting loop. Current runs along one side and back along the other, so their directions are opposite. View the coil along its axle, with the magnetic field directed right.
Two active sides belong to one connected coil
First trace the current. Then look from the near end along the axle to work out the two forces.
A carries current from far to near. B carries the same current from near to far. The opposite directions are two parts of one circuit.
End view: the forces make a clockwise turning pair
Green arrow: magnetic field. Brown dot/cross: current. Purple arrows: forces. Blue curve: turning sense. The force arrows use one qualitative scale.
Explain the rotation
Field right, left current out, right current in
- For the left side, rightward field and out-of-page current give upward force.
- For the right side, rightward field and into-page current give downward force.
- Upward force on the left gives a clockwise moment about the axle. Downward force on the right also gives a clockwise moment.
- The turning effects add, so the coil tends to turn clockwise in this view.
In the symmetric model, the forces are equal and opposite, so their resultant force is zero. Their lines of action are separated, however, so their moments do not cancel. Zero resultant force does not establish zero turning effect.
Reversing the current with the field fixed reverses both forces and the turning direction at this orientation. Reversing only the field has the same effect. Reversing both preserves the original turning direction.
As the coil turns, the perpendicular distances from the axle to the force lines change. At an orientation where those lines pass through the axle, there is no turning moment from them. Opposite forces produce a turning pair only when their lines of action have the required separation.