What is a transmission line?
A transmission line is a pair of conductors whose length is a significant fraction of a wavelength, so voltage and current vary along it as traveling waves. It is modeled by per-unit-length resistance R, inductance L, conductance G and capacitance C. The characteristic impedance is Z0 = √((R + jωL)/(G + jωC)), which is √(L/C) for a lossless line, and the propagation constant is γ = α + jβ = √((R + jωL)(G + jωC)).[1]
What are the telegrapher's equations?
dV/dz = −(R + jωL)I and dI/dz = −(G + jωC)V. Their solution is a forward wave V+e−γz plus a reflected wave V−e+γz. The ratio V−/V+ at the load is the reflection coefficient ΓL = (ZL − Z0)/(ZL + Z0).[1]
How does loss behave?
For low loss, α ≈ R/(2Z0) + GZ0/2 Np/m (multiply by 8.686 for dB). R rises as √f because of skin effect; G = ωC·tan δ rises as f, so dielectric loss dominates at high frequencies on lossy laminates.[1]
What types of transmission line are used?
| Type | Mode | Typical use |
|---|---|---|
| Coaxial | TEM | Cables, connectors |
| Microstrip | Quasi-TEM | PCB outer layers |
| Stripline | TEM | Inner PCB layers |
| Coplanar waveguide | Quasi-TEM | mmWave PCB, MMICs, probing |
| Rectangular waveguide | TE10 | High power, low loss, mmWave |
| Twisted pair, twin-lead | TEM | Balanced lines |
What is phase velocity?
vp = ω/β = 1/√(LC) for a lossless line, equal to c/√εeff. Group velocity equals phase velocity on a dispersionless TEM line; microstrip and waveguide are dispersive.[1]
Frequently asked questions
When is a trace a transmission line?
When its length exceeds roughly a tenth of the wavelength, or for digital signals when delay exceeds a fraction of the rise time.
Does Z0 depend on length?
No, characteristic impedance depends on geometry and materials, not length.
What is a matched line?
One terminated in its characteristic impedance, so there is no reflection.
See also
References
Online sources accessed October 21, 2026; printed works cited by edition. See all sources.
- “Microwave Engineering, 4th ed.”. D. M. Pozar, Wiley. 2012.