Calculate quality factor from frequency, inductance, and resistance. See reactance, impedance, losses, and resonance instantly. Export neat results for testing, design reviews, and records.
The core inductor quality factor formula is Q = XL ÷ R. The inductive reactance is XL = 2πfL. Here, f is operating frequency, L is inductance, and R is the effective series resistance.
When temperature rise is supplied, the calculator adjusts resistance with Radjusted = R × (1 + αΔT). That lets you compare the room temperature Q value with a warmer operating estimate.
The impedance magnitude uses |Z| = √(R² + XL²). The phase angle uses θ = tan⁻¹(XL ÷ R). Estimated bandwidth uses BW = f ÷ Q for a resonant interpretation.
If parasitic capacitance is entered, the estimated self resonant frequency uses SRF = 1 ÷ (2π√LC). This helps show when the simple inductive model starts losing accuracy.
For current based values, copper loss uses P = I²R. Peak stored magnetic energy for a sinusoidal current is approximated here as E = L × Irms².
| Frequency | Inductance | Resistance | XL | Q |
|---|---|---|---|---|
| 100,000 Hz | 47.0000 µH | 0.35 Ω | 29.530971 Ω | 84.374203 |
| 500,000 Hz | 68.0000 µH | 0.62 Ω | 213.628300 Ω | 344.561775 |
| 1,000,000 Hz | 100.0000 µH | 1.0000 Ω | 628.318531 Ω | 628.318531 |
| 5,000,000 Hz | 22.0000 µH | 0.9 Ω | 691.150384 Ω | 767.944871 |
Q factor helps compare how much useful inductive reactance an inductor provides against its loss. A higher Q usually means lower effective loss for the same operating frequency and inductance.
Real components rarely behave like ideal parts across wide frequency spans. Core material, skin effect, proximity effect, winding geometry, and parasitic capacitance all shape the measured Q curve.
This calculator is strong for quick engineering estimates, datasheet checks, test review, and design screening. For final validation, compare these outputs with impedance analyzer or network analyzer measurements.
Inductor Q factor compares stored magnetic energy behavior against resistive loss at a chosen frequency. It is commonly estimated by dividing inductive reactance by series resistance.
Inductive reactance increases with frequency, so Q often rises at first. After that, skin effect, core loss, proximity loss, and parasitic capacitance can reduce the practical Q value.
Not always. Higher Q usually lowers loss, but some circuits need controlled damping, wider bandwidth, or better stability. The best value depends on the full design target.
Parasitic capacitance helps estimate self resonant frequency. Near that region, the inductor no longer behaves like a simple ideal inductance, so Q calculations need more caution.
Use the effective series resistance at the operating condition when possible. A room temperature DC resistance can be a starting point, but AC loss and heating may raise the practical value.
The bandwidth output uses the resonant relation BW = f divided by Q. It gives a useful estimate for tuned circuits, not a universal bandwidth for every application.
Higher temperature usually raises conductor resistance. Since Q equals reactance divided by resistance, increasing resistance tends to reduce Q when the operating frequency and inductance stay fixed.
Yes, for estimates and early checks. Still, RF parts often need measured S parameters, impedance curves, and parasitic modeling because high frequency behavior can depart from simple formulas.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.