Parameters
Load Preset
R_L — Resistance
Ω
X_L — Reactance (+ind, −cap)
Ω
Z₀ — Char. impedance
Ω
f — Frequency
MHz
εᵣ_eff  (1 = air)
Line Length Preset
Drag to set length 0.1988λ
0λ/4λ/23λ/4λ5λ/43λ/27λ/4
Length (wavelengths)
λ
Length (degrees)
°
Length (mm)
mm
Z_in Result
Input Impedance Z_in
|Z_in|Ω
∠ Z_in°
R_inΩ
X_inΩ
|Γ|
Return LossdB
VSWR
βl°
tan(βl)
λ on substratemm
▪ Transmission Line Input Impedance
Z in = Z 0 · Z_L + j·Z0·tan(βl) Z0 + j·Z_L·tan(βl)
Special Cases βl = 90° (λ/4 line)  →  Z_in = Z₀² / Z_L   (impedance inverter)
βl = 180° (λ/2 line)  →  Z_in = Z_L   (transparent — line invisible)
Z_L = 0 (SC load)  →  Z_in = j Z₀ tan(βl)   (pure reactance)
Z_L = ∞ (OC load)  →  Z_in = −j Z₀ cot(βl)   (pure reactance)
Z_L = Z₀ (matched)  →  Z_in = Z₀   (for any length)
Z_L = R_L + jX_L   load impedance
Z₀ = characteristic impedance of the line
β = 2π/λ   phase constant (rad/m)
l = physical length of line
βl = electrical length in radians
tan(βl) = drives the rotation on Smith chart
Derivation: Using the telegrapher's equations, the voltage and current waves on the line produce V(l) and I(l). Dividing gives Z_in = V(0)/I(0).
For a lossless line: V(x) = V⁺(e−jβx + Γe+jβx), where Γ = (Z_L−Z₀)/(Z_L+Z₀). Evaluating at x = −l (input) and simplifying yields the formula above.
Smith Chart
Z_L (load) TL rotation (constant |Γ|) Z_in
Step-by-Step Working
Enter values — working appears here.