PCB Via Inductance Calculator

Calculate parasitic inductance and self-resonant frequency of a PCB via. Estimates voltage drop at high-current transients.

Calculator Electronics Updated Apr 23, 2026
How to Use
  1. Enter via length L (stackup depth between layers the via connects).
  2. Enter via drill radius r (typical 0.1-0.25 mm).
  3. Tool computes self-inductance, impedance at given frequency, and voltage drop at given di/dt.
Input
mm
mm
Hz (MHz, GHz OK)
A/ns
Presets
Via Parasitics
Inductance L
nH
Z at f
Ω
Effective (N vias)
nH
V = L·di/dt
mV

Show Work

Enter via geometry.

Formulas

Via Inductance
L ≈ 5.08 · h · [ln(4h/d) + 1] (nH)
h, d in inches. Rosa 1908 formula.
Metric Form
L ≈ 0.2 · Lmm · [ln(2·L/r) − 0.75] (nH)
L in mm, r in mm.
Impedance at f
Z = 2π·f·L
Inductive reactance.
N Parallel Vias
L_eff ≈ L / N
Ignoring mutual coupling.
Voltage Drop
ΔV = L · di/dt
Switching transient drop.
Typical
0.4-1.5 nH per via
Standard 1.6mm FR4.

History of Via Modeling

The formula for inductance of a straight cylindrical conductor was derived by Edward Bennett Rosa at the US Bureau of Standards in 1908 as part of the bureau's comprehensive study of self- and mutual-inductance of conductors. Rosa's formulas remain the closed-form reference for round-wire and via inductance calculations more than a century later.

PCB via inductance became a first-class signal-integrity concern in the 1990s when CPU and memory interface speeds pushed past 100 MHz. Suddenly the 1-2 nH parasitic inductance of a standard through-hole via created a measurable impedance discontinuity at the vias' self-resonant frequency (typically 1-3 GHz). Modern HDI (high-density interconnect) PCBs use microvias (blind, buried, stacked) to reduce via inductance by 5-10× for high-speed interfaces.

Power-delivery networks (PDNs) rely on many parallel vias to reduce effective L at decoupling capacitors. A single 1 nH via at 1 A/ns load-step produces a 1 V drop on the power rail — unacceptable for 1.0 V core voltages. Ten parallel vias drop that to 100 mV. Modern VRMs use hundreds of via-pairs between output stage and BGA mounting pads to meet PDN impedance targets down to 1 mΩ at 100 MHz.

About This Calculator

Enter via length (stackup depth it traverses), drill radius, and number of parallel vias. Optional: frequency for Z-magnitude readout, di/dt for voltage-drop estimate. The formula is the cylinder-wire approximation from Rosa 1908 — accurate to ~10% for typical PCB via aspect ratios.

For more accurate modeling (especially at multi-GHz frequencies where via stub resonances dominate), use a 3D field solver (Ansys HFSS, CST). For power-delivery PDN design, parallel via count and return-via proximity matter more than the single-via number computed here. Everything runs client-side.

Frequently Asked Questions

Why care about via L?

At high frequencies, via inductance becomes the dominant impedance — not via resistance. A 1 nH via has +j6.3 Ω at 1 GHz. Multi-GHz signals routed through vias see significant impedance discontinuities unless the via is kept short and well-referenced.

How to reduce?

(1) Shorter vias (blind/buried/microvias). (2) Multiple parallel vias (L ∝ 1/N, not 1/N exactly due to mutual coupling). (3) Return vias within 1mm of the signal via.

Signal via vs power via?

Signal vias carry high-frequency edges — inductance matters. Power/ground vias carry DC + switching noise — resistance matters more for DC drop, inductance still matters for switching transients.

Common Use Cases

Decoupling Cap Via

Bulk cap mounting pads to power plane: each mounting via adds ~1 nH. Parallel multiple vias to reduce effective inductance.

High-Speed Signal

PCIe Gen4 (16 GT/s) through 1.6mm FR4 via: ~1.2 nH = ~12 Ω at 1.6 GHz. Significant reflections without careful stackup.

Power Delivery

VRM output to CPU package: many parallel vias minimize L × di/dt voltage droop during load steps.

Last updated: