How Signals Propagate in Unbounded Conductive Media
Key Takeaways

Transmission lines on a PCB are a form of waveguide, where the boundary along the waveguide forms an open resonator structure.

The nonideal nature of any copper modifies the typical waveguiding behavior in transmission line structures.

The impedance of a general transmission line can be calculated by considering its wave propagation behavior, but only once the nonideal nature of conductors is included.
The rough nature of electrodeposited copper films modifies the ideal impedance of copper and the wave impedance of a waveguide
Transmission lines come in many forms, such as coaxial lines, printed traces on a PCB, or long cables or wires. All of these structures share some similar behavior relating to how an electromagnetic wave travels along the interconnect. Although these structures are fundamental for guiding a propagating electromagnetic disturbance along an interconnect, there is often a misperception as to how signals travel on transmission lines.
In particular, the electromagnetic signal on an interconnect exists around the line, meaning signals are propagating in unbounded conductive media as they travel. In other words, transmission lines are really waveguides, and the structure that supports wave propagation will determine the impedance seen by signals on the line. Once you get to higher frequencies and TEM behavior stops dominating wave propagation, it helps to take a wave impedance perspective to understand signal behavior.
Transmission Line Impedance From the Wave Perspective
Take a look at the Telegrapher’s equations and you’ll see that the definition of signal behavior on a transmission line is in terms of the voltage and current. This is very useful for understanding how voltage and current sourced by a driver component will travel along an interconnect to a receiver component. For PCB designers, this is important information, particularly for understanding how losses reduce signal levels at a receiver.
The reality is that the signal on a transmission line is described by the traveling electromagnetic field in the PCB substrate, not the voltage and current from the Telegrapher’s equations. For this reason, we need to use the wave impedance to understand the actual impedance seen by a traveling electromagnetic wave:
Wave impedance equation
Impedance Is Defined in Terms of Field Strengths
The equation shown above is universal in that it considers the electric and magnetic fields on the interconnect, rather than the voltage and current from the Telegrapher’s equations. Although the results can be made equivalent, the reality is that impedance depends on the ratio of these fields. Here, the wave impedance will vary across the frequency domain and tends to a constant value, just like we would see in a typical transmission line. In fact, this is the definition of impedance used in conformal mapping to determine transmission line impedance equations directly from the wave equation. See the seminal textbook Transmission Line Design Handbook by Brian C. Waddell for some famous results for common PCB trace geometries.
From here, we can describe in full how a signal propagates in unbounded media, including conductive media.
How Signals Propagate in Unbounded Conductive Media
In the above equation, the wave impedance depends on the conductivity of the medium in which it travels. We usually have three possibilities in practice media:
 Insulating dielectric: These are materials that have very low conductivity. For example, we can take the conductivity of a PCB laminate to be zero.
 Semiconducting media: The conductivity of a semiconductor is nonzero and will be slightly nonlinear at high field strength.
 Conductors: A conductor will have very high conductivity, so the wave impedance will be very high.
For an infinite wire in free space, the field exists entirely around the wire, not within the wire. However, the field can propagate around the wire as a plane wave, and the field will perfectly converge to plane wave behavior far from the wire.
Once you bring a ground plane close to your conductor, as is the case in real interconnects, you no longer have signal propagation in unbounded conductive media, and we need to consider how the boundary conditions affect wave propagation.
All Media is Bounded Somewhere
All conductive media and the region surrounding it are bounded and affected by some boundary conditions. The skin effect also arises around conductors due to the interaction between the electromagnetic field and charges in a conductor, but the fields around the conductor will still be affected by the presence of ground references, other conductors, absorbers, and anything else that defines an interface between two media. It is the boundary conditions that will determine the characteristic (lossless) impedance, the wave impedance, and propagation constant for the interconnect.
There are two ways to determine the impedance in any real system:
 Calculate the electric and magnetic fields from the potential field as determined from the Telegrapher’s equation and use these to calculate the wave impedance in the interconnect.
 Calculate the wave impedance directly from the electromagnetic wave equation using a technique like conformal mapping, method of moments, method of characteristics, or using a 3D field solver.
As an example, consider the stripline shown below. Along the yaxis, we have two boundary conditions where the electric fields terminate at the conductive reference planes. Along the xaxis, there is no boundary in this theoretical problem, although we do have a fluxconserving boundary condition at infinity located in the xz plane.
Even a relatively open waveguide cavity like a stripline has some boundary conditions that determine the impedance, propagation constant, and signal losses
Here, the boundary conditions define a dispersion relation that determines the propagation constant in terms of the structure’s eigenfrequencies. The skin effect occurs in all conductive boundaries around the signal, and this will influence the dispersion relation and the resulting wave impedance in the interconnect.
Analytically, this is a complex transformation that accounts for skin effect losses, copper roughness, and dispersion in the PCB substrate. At mmWave and higher frequencies, the wave behavior becomes dominant and the interconnect no longer behaves as a TEM waveguide. This is also very important at lower frequencies used in standard wireless protocols, particularly in antenna design. With the right 3D field solver utility in your PCB design software, you can visualize the electromagnetic field in your interconnects, determine wave impedance and impedance matching, and directly calculate important quantities like power transfer in your interconnects.
When you’re designing highspeed/highfrequency interconnects and you need to account for wave behavior in signal propagation in unbounded conductive media, use Cadence’s PCB design and analysis software to build and evaluate your designs. Cadence provides the industry’s best CAD tools for PCB design and powerful signal integrity analysis tools that help automate many important tasks in systems analysis. Cadence’s suite of prelayout and postlayout simulation features gives you everything you need to evaluate your system.
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