- Number of turns
- 100
- Coil radius
- 1cm
- Coil length
- 5cm
78.9568µH
Open with these values78.9568µH
Result: 78.9568 µHInductance grows with the square of the turns and with the cross-section, and falls as the coil gets longer: 100 turns on a 1 cm radius over 5 cm gives about 79 µH. This is the long-solenoid formula, so it overstates short, fat coils.
78.9568µH
Open with these values355.3058µH
Open with these values49.3480µH
Open with these valuesL = µ0 × N² × π × r² ÷ l
| Turns, radius, length | Shape of the coil | Inductance |
|---|---|---|
| 50, 2, 8 | Short and wide — expect an overstatement | 49.3480 |
| 100, 1, 5 | Five times as long as it is wide | 78.9568 |
| 500, 0.5, 20 | Long and thin, closest to the model | 123.3701 |
| 200, 1.5, 10 | Length just over three diameters | 355.3058 |
| 1000, 2, 30 | A large former, densely wound | 5263.7890 |
Multiply the magnetic constant by the square of the turns and by the cross-sectional area, then divide by the winding length. Doubling the turns quadruples the inductance; doubling the length halves it.
It assumes a long solenoid whose field is uniform inside and zero outside. A coil as long as it is wide comes out roughly a third too high; one five times longer than wide is within a few per cent.
From the axis to the middle of the wire, not to the outside of the winding. The area term is squared, so a small error here is doubled in the answer.
Yes, considerably. This calculator assumes an air core; a magnetic core multiplies the inductance by its relative permeability, which is often in the hundreds.
The formula does not apply. It describes a single layer of turns along a cylinder, and a multi-layer winding needs a different treatment entirely.
Information, not professional advice.
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