Topic 6 of 7
Magnetic force and its direction
A current-carrying conductor in an external magnetic field can experience a force. To predict its direction, identify the field and conventional current separately.
Across the gap between magnet poles, the field points from N to S. Conventional current is opposite to electron motion in a metal. A dot means out of the page and a cross means into it, for the quantity labelled beside the symbol.
Observe the force on a movable wire
Place a straight, movable conducting segment in the gap of a magnet and connect it to a suitable low-voltage d.c. supply, switch and flexible leads. Arrange the current perpendicular to the field and allow the segment to move in the predicted force direction.
Move a current-carrying wire in a magnetic gap
The upper view separates the wire's rear and front ends. Flexible leads allow its straight section to move. Brown arrows show current, teal arrows field, and purple arrows magnetic force.
Only the magnetic force is marked. Weight and support forces still act. The lower end view represents the same wire, not an extra circuit branch.
- With current off, record the segment's position. Gravity and its supports still act; the magnetic force due to current in the segment is absent.
- Close the switch briefly and observe the movement. In the given geometry, the magnetic force is upward.
- Switch off before changing connections. Reverse the current while leaving the magnet arrangement fixed, then switch on and compare: the magnetic force and resulting initial movement reverse.
- Restore the original current direction. Reverse the magnetic field by exchanging the pole positions, keeping the wire geometry comparable. The magnetic force reverses again.
Keep the support arrangement and current magnitude comparable when comparing directions. Current-induced heating can change wire sag or tension, so observe the controlled initial response and limit heating. A movement demonstrates the effect under these conditions; it is not a calibrated measurement of force magnitude.
Use Fleming's left-hand rule
Hold the thumb, first finger and second finger of your left hand mutually perpendicular:
- First finger: field
- Point it along the magnetic field, from N to S across the gap.
- Second finger: current
- Point it along conventional current in the active conductor.
- Thumb: force
- It gives the magnetic force on that conductor.
The right-hand grip rule finds the field produced by a current. Fleming's left-hand rule finds the relative directions of current, an external field and force. Choose the rule for the relationship you are using.
Keep the viewpoint; change one cause
The dot means current out of the page and the cross means current into it. Teal arrows follow the field from N to S. Purple arrows show force on the wire.
Start: field right, current out
Reverse the current only
Reverse the field only
Reverse both
Reversing either current or field reverses the force. Reversing both restores its original direction. No numerical force is represented by arrow length.
| Current in the wire | Gap field | Initial magnetic-force direction |
|---|---|---|
| Out of the page | Right | Up |
| Into the page | Right | Down |
| Out of the page | Left | Down |
| Into the page | Left | Up |
Compare the first and second rows to isolate current reversal. Compare the first and third to isolate field reversal. The last row changes both and returns to the original force direction.
Find a missing direction
The force is downward and the field is rightward
Put your thumb down and first finger right. The second finger points into the page, so that is the required conventional-current direction.
Alternatively, if current is out of the page and force is upward, those two directions require the field to point right. Any two known perpendicular directions can determine the third.
The examples use perpendicular current and field. If a straight segment's current is parallel or opposite to the field, the magnetic force on that segment is zero in this model. Do not force three non-perpendicular directions into the perpendicular-case hand rule.