20.4 Magnetic fields due to currents
- Syllabus
- 9702–2028–2029
- Topic
- 20.4
- Level
- A2
| Current source | Required field-line pattern | Strength cue |
|---|---|---|
| long straight wire | concentric circles centred on wire | circles spread farther apart with distance |
| flat circular coil | lines pass nearly parallel through centre, perpendicular to coil plane, then curve around outside in closed loops like a bar magnet | closest near centre |
| long solenoid | straight, parallel, equally spaced lines inside along axis; curved closed loops outside like a bar magnet | strong/uniform inside, weak outside |
For a straight wire, point the right thumb along conventional current; curled fingers give circular field direction. Current into the page gives clockwise arrows; current out gives anticlockwise arrows.
For a circular coil or solenoid, curl right-hand fingers with conventional current around the turns; the thumb points through the coil toward its magnetic north end and gives the internal field direction.
Reversing current reverses every field arrow and swaps the coil/solenoid north and south poles, while leaving the field-line shape unchanged.
The syllabus requires a flat circular coil, not a flat current sheet. Do not draw straight-wire lines parallel to the wire or show a real solenoid as perfectly uniform outside its ends.
For a long solenoid, field strength is approximately proportional to current and turns per unit length; a high-permeability core can increase it further.
Use the right-hand grip rule for polarity and distinguish ideal uniform interior field from fringing at the ends.
Increasing turns per metre or current strengthens the field, while reversing current reverses the poles.
A solenoid is not a permanent magnet by default; its field depends on current and core conditions.
Each current creates a magnetic field that acts on the other conductor, producing attraction for currents in the same direction and repulsion for opposite directions.
Use the field of one wire and F=BIL on the other; the force per length falls as separation increases.
Two long parallel wires carrying equal currents in the same direction pull toward each other.
The force is not an action of one current on itself; it is an interaction between the fields and the other conductor’s current.