Solenoid inductance with a core
What inductance does this coil have, wound on this core?
- L
- Inductance, H
- μr
- Relative permeability
- N
- Turns
- A
- Area, m²
- l
- Length, m
LaTeX
L = \frac{\mu_0 \cdot μr \cdot N^2 \cdot A}{l}
Method
- Look up the core's relative permeability. Air is 1; a soft ferromagnetic core multiplies the field the same current produces by hundreds or thousands of times.
- Convert the area to square metres and the length to metres.
- Square the turns count — inductance grows with the square of N, not linearly, so doubling the winding quadruples the inductance.
- Multiply μ₀ (4π×10⁻⁷ H/m) by the relative permeability, the turns squared and the area, then divide by the length.
Assumptions
- This is the ideal infinite-solenoid formula: the field is treated as uniform inside the coil and zero outside it. A real, finite coil's inductance is somewhat lower — a long, thin coil (length several times its diameter) is where this approximation is best.
- The core is unsaturated. Relative permeability collapses toward 1 as a ferromagnetic core saturates, and the values used here are the typical low-field figures for each material, not a saturation curve.
- The core fills the coil's cross-section uniformly. A rod that is narrower than the winding, with an air gap around it, has a much lower effective permeability than the bare material figure.