Compute core parameters: effective area (Ae), magnetic path length (le), AL value (nH/N²), inductance for given turns, required turns for target inductance, and peak flux density (Bpeak) to avoid saturation. Ideal for power inductors, common-mode chokes, and transformer designers.
A ferrite ring (toroid) core is widely used in power electronics, EMI filters, and signal transformers due to its closed magnetic path, high permeability, and low leakage inductance. The core’s geometry determines key parameters: effective cross-sectional area Ae, effective magnetic path length le, and the inductance factor AL. These values allow engineers to predict inductance, design windings, and avoid saturation.
AL = μ0 · μr · Ae / le
with μ0 = 4π·10−7 H/m, Ae in m², le in meters. AL is expressed in nH/N².
For a rectangular cross-section toroid: Ae = h × (OD − ID)/2, le = π × (OD + ID)/2 (mean circumference).
Saturation check: Bpeak = (L · Ipeak) / (N · Ae) [Tesla]. Keep Bpeak below core material limit (typically 0.3 T for MnZn ferrites).
Designing high-frequency inductors or transformers requires reliable core characterization. By inputting basic dimensions and material permeability, this tool instantly provides AL and inductance. It helps engineers compare cores, optimize windings, and validate prototypes without expensive LCR meters. In educational settings, the visual representation of ring geometry reinforces electromagnetic theory.
Take a toroid with OD = 20 mm, ID = 12 mm, height = 6 mm, μr = 2000 (typical N87 material).
Ae = 6 × (20-12)/2 = 24 mm² = 24×10−6 m². le = π·(20+12)/2 = 50.27 mm = 0.05027 m.
μ0 = 4π×10−7 => AL = (4π×10−7×2000×24e-6)/0.05027 × 1e9 ≈ 1200 nH/N².
For N = 50 turns → L ≈ 1200×2500/1000 = 3000 µH (3 mH). Target 2 mH would need N = sqrt(2000×1000/1200) ≈ 40.8 → 41 turns.
Important saturation check: With Ipeak = 2 A, Bpeak = (3000e-6 * 2) / (50 * 24e-6) = 5.0 T. This value is far above the typical ferrite saturation limit (0.3 T). The core would saturate deeply, causing inductance to collapse. To avoid saturation, either increase the number of turns (e.g., N = 200 → Bpeak ≈ 0.25 T) or reduce the peak current. Our calculator instantly highlights such saturation risks.
| Ferrite Material | μr (initial) | Typical Application |
|---|---|---|
| 3C90 / N87 | 2000 – 2300 | Power transformers, SMPS inductors |
| Fair-Rite #43 | 800 | EMI suppression, wideband transformers |
| Fair-Rite #77 | 2000 | Common-mode chokes, pulse transformers |
| 3E5 / N49 | 10000 – 15000 | Low-frequency high-μ applications |
| 4A11 (MnZn) | 1500 | High saturation flux density |
⚠️ Permeability varies with frequency, temperature, and flux density. Use typical μr values for initial design, then verify with prototypes.
This calculator assumes a uniform winding, negligible fringing flux, and rectangular cross-section toroid. For round or chamfered cores, the effective Ae and le may slightly differ, but the formulas remain industry-standard approximations. The permeability μr is considered linear (unsaturated, low excitation). For high-level designs, refer to manufacturer datasheets (e.g., TDK, Ferroxcube, Magnetics Inc.) which provide AL values directly.