RF Toolbox

Transmission Line Loss & Delay

Calculates conductor loss, dielectric loss, total insertion loss, and propagation delay for microstrip traces and coaxial cables. Conductor loss is dominated by skin effect and scales as √f; dielectric loss scales linearly with f and loss tangent.

Equations & Parameters ▸
\(R_s = \sqrt{\dfrac{\pi f \mu_0}{\sigma}}\qquad \alpha_c = 8.686\,\dfrac{R_s}{Z_0\,w_{\rm eff}}\;\text{dB/m}\qquad \alpha_d = 8.686\,\dfrac{k_0\,\varepsilon_r(\varepsilon_{\rm eff}-1)\tan\delta}{2\sqrt{\varepsilon_{\rm eff}}\,(\varepsilon_r-1)}\;\text{dB/m}\) \(t_d = \dfrac{L\sqrt{\varepsilon_{\rm eff}}}{c}\)
RsSurface resistance (Ω/sq) — sets skin-effect conductor loss
αcConductor attenuation constant (dB/m)
αdDielectric attenuation constant (dB/m); requires loss tangent tan δ > 0
tdPropagation delay (s); vp = c/√εeff
σConductivity: copper 5.8×10⁷, gold 4.1×10⁷, aluminum 3.5×10⁷ S/m

Microstrip: Hammerstad-Jensen εeff and Z₀. Coaxial: both conductors assumed same σ; result is lower bound (braided/stranded cables have higher loss). Set tan δ = 0 for lossless dielectric.

Line Type
Common Inputs
Microstrip Parameters
Results
Diagram