PHYMagnetic Field & Forces
Biot–Savart Law & Field due to Currents
The Biot–Savart law gives the magnetic field produced by a current element, and integrating it (or using Ampere's law as a shortcut) yields the standard results for a straight wire, a circular loop, a point on the loop's axis, a solenoid and a toroid. ISC numericals are almost always direct substitution into one of these standard formulas, so recognising the geometry is the whole skill.
Note that the field always wraps around the current (right-hand rule) and falls off with distance.
Biot–Savart law (magnitude)
current-element length, angle between the element and , distance to the field point, .
Long straight wire
perpendicular distance from the wire; valid for an infinitely long straight conductor.
Centre of a circular coil ( turns)
radius of coil, number of turns, field directed along the axis through the centre.
Axial field of a circular coil
distance of the point from the centre along the axis; reduces to when .
Inside a long solenoid
turns per unit length; field is uniform along the axis inside the solenoid.
Inside a toroid
total turns, mean radius of the toroid; field is confined to the core and zero outside.
- Use in Biot–Savart; use in the loop/solenoid formulas.
- For a circular coil always include the number of turns ; a single loop is the case.
- The solenoid result uses (turns per metre), not the total turns .
- The toroid uses the mean radius and total turns ; the field outside both the core and the toroid is zero.
- All lengths must be converted to metres () before substituting.
- Fields from several wires add as vectors; if two fields are mutually perpendicular the resultant is .
- The straight-wire field circles the conductor; direction is given by the right-hand grip rule (thumb along , fingers along ).
- Dropping the factor for a multi-turn coil, giving an answer times too small.
- Using (straight wire) for the centre of a loop, or vice versa — the loop has no in the denominator.
- Forgetting to convert centimetres to metres, which throws the magnitude off by powers of ten.
- In the solenoid, plugging in total turns instead of turns per unit length.
- Numericalthe loop and solenoid formulasA circular coil of turns and radius carries a current of . Calculate the magnitude of the magnetic field at the centre of the coil.
- Derive / provethe biot–savart lawUsing the Biot–Savart law, derive an expression for the magnetic field at the centre of a circular current-carrying coil of radius having turns and carrying a current .
- Numericalvector addition of fieldsTwo long straight parallel wires, apart, carry currents of and in the same direction. Find the magnitude of the resultant magnetic field at a point midway between the two wires.
- Define / statethe biot–savart law statementState the Biot–Savart law and write the expression for the magnitude of the magnetic field due to a small current element at a point distant from it.
- Give reasonsfield inside vs outside a toroidGive a reason why the magnetic field at any point outside an ideal toroid is zero, while inside the core it is , where is the mean radius.
Written for Sublevo. Question text quoted anywhere in these notes is the Council’s and carries its year and paper; the board’s own diagrams are not reproduced.