Differential Pair Impedance Calculator
Calculate differential microstrip and stripline impedance. Optimize for USB, HDMI, LVDS.
Key Formulas
Z0: 87/√(εr+1.41)×ln(5.98H/0.8W)
Zdiff: 2Z0(1-0.48e-0.96S/H)
Frequently Asked Questions
What does the Differential Pair Impedance Calculator compute?
This tool calculates the characteristic differential impedance (Zdiff) of tightly coupled microstrip or stripline PCB trace pairs, based on physical geometry and material properties. It also computes the corresponding single-ended impedance (Zodd) and coupling coefficient (kc). The results help ensure signal integrity in high-speed digital interfaces.
Which applications is this calculator optimized for?
It’s tailored for common high-speed serial protocols including USB 2.0/3.x (90 Ω), HDMI (100 Ω), LVDS (100 Ω), PCIe, and MIPI D-PHY. The interface includes preset target impedances and practical parameter ranges aligned with industry layout guidelines for these standards.
What do the input parameters — W, S, H, εr, and T — represent physically?
W = trace width (center-to-center width of one conductor); S = edge-to-edge spacing between traces; H = distance from trace to reference plane (for microstrip) or between planes (for stripline); εr = relative permittivity of the PCB substrate; T = copper thickness (affects effective width via sidewall etching and current crowding).
What are typical values for trace width (W), spacing (S), and height (H) in 4-layer PCBs?
For FR-4 boards: W and S commonly range from 0.1–0.5 mm; H is typically 0.15–0.25 mm for top-layer microstrip (e.g., 1oz copper over prepreg), and 0.4–0.8 mm for inner-layer striplines. Tighter coupling (S ≈ W) improves common-mode rejection but increases crosstalk sensitivity.
Why does changing copper thickness (T) affect impedance even though it’s not part of ideal transmission line formulas?
Copper thickness influences the effective trace cross-section and current distribution—especially at high frequencies due to skin effect and manufacturing taper (trapezoidal trace profile). Thicker copper slightly reduces resistance and increases effective width, lowering impedance by ~2–5% across typical T = 12–35 µm (½–1 oz) ranges.
How accurate is this calculator compared to field solvers like HFSS or ADS?
It uses well-established closed-form approximations (e.g., Hammerstad & Jensen for microstrip, Schneider for stripline) with <5% error for typical PCB geometries. While less precise than 3D EM solvers, it provides fast, reliable first-pass design guidance—ideal for layout iteration before final sign-off simulation.
What should I do if my calculated Zdiff deviates significantly from the target (e.g., >10% error)?
First verify units (mm, µm, dimensionless εr) and ensure S ≥ 2×T to avoid fabrication shorting. Adjust W and S iteratively—increasing W lowers Zdiff, while increasing S raises it. For fixed routing area, consider switching from microstrip to stripline (more stable Zdiff vs. process variation).
Can this tool be used for edge-coupled versus broadside-coupled differential pairs?
Yes — it models edge-coupled (same layer) microstrip/stripline configurations, which dominate PCB design. Broadside coupling (traces on adjacent layers) is not supported, as it requires different field solutions and is rarely used due to poor manufacturability and uncontrolled coupling.
How does dielectric constant (εr) tolerance impact impedance accuracy?
FR-4 εr varies ±0.3–0.5 across frequency, temperature, and batch—causing up to ±7% Zdiff shift. For critical designs, use controlled dielectrics (e.g., Isola FR408HR, εr = 3.66 ±0.05) and validate with TDR measurement. This tool assumes nominal εr; adjust input conservatively for worst-case analysis.
Is there a relationship between differential impedance and common-mode impedance?
Yes: Zdiff ≈ 2×Zodd and Zcommon ≈ Zeven/2, where Zodd and Zeven are odd- and even-mode impedances. High coupling (low S/W) increases Zdiff–Zsingle separation and improves common-mode noise rejection—critical for EMI compliance.