At frequencies so high that the wavelength of the signals conveyed shrinks to a size comparable with the crosssectional dimensions of a transmission line, strange nonTEM modes of propagation appear. These modes do not by themselves portend a loss of signal power, but they can create objectionable phase distortion (i.e., dispersion of the rising and falling edges) that limits the maximum speed of operation (Section 3.2).
3.9.1 Boundary of WaveguideDispersion Region
If you attempt to operate a transmission line at such a high frequency that the wavelengths of the signals conveyed approach the dimensions of your conductors, strange modes of propagation begin to appear. These modes have to do with the possibility of signal power bouncing back and forth between two interfaces within the transmission structure. These bouncing modes are called nonTEM modes (see Section 5.1.5, "NonTEM Modes").
In a coaxial cable the critical dimension of interest is the diameter of the shield. In a stripline configuration it's the spacing between the planes. In a microstrip it's the thickness of the dielectric.
At frequencies high enough that the signal wavelength becomes comparable with the critical dimension, a fullwave analysis of the situation predicts received waveforms that have what looks like severe overshoot and ringing, even if the line is perfectly terminated .
The frequency at which fully developed nonTEM modes may exist within a transmission structure is
Equation 3.145
where 
w c appears in units of rad/s, 
b is the interplane spacing of a stripline, m, 

h is the dielectric thickness of a microstrip, 

k is a constant in the range of 1/10 to 1/6, 

d 2 is the inner diameter of a coaxial shield, m, 

c is the speed of light, 2.998 ·10 8 m/s, and 

r is the relative dielectric constant of the insulating material, as measured in the vicinity of frequency w c . 
Microstrips suffer more than other configurations from nonTEM modes because the bouncing modal power does not get a clean bounce off the dielectrictoair interface. The properties of this interface introduce a significant phase shift into the modal equations with the result that nonTEM distortion appears in a noticeable way for microstrips at frequencies much lower than for other configurations. This peculiar form of nonTEM behavior is called microstrip dispersion .
For ordinary digital signaling on FR4 printed circuit boards at 10 Gbps you may use microstrip trace heights up to 20 mils without encountering significant microstrip dispersion. At lower frequencies you can use correspondingly bigger traces. Above 10 Gbps, you must use correspondingly smaller ones.
POINTS TO REMEMBER
Fundamentals
Transmission Line Parameters
Performance Regions
FrequencyDomain Modeling
Pcb (printedcircuit board) Traces
Differential Signaling
Generic BuildingCabling Standards
100Ohm Balanced TwistedPair Cabling
150Ohm STPA Cabling
Coaxial Cabling
FiberOptic Cabling
Clock Distribution
TimeDomain Simulation Tools and Methods
Points to Remember
Appendix A. Building a Signal Integrity Department
Appendix B. Calculation of Loss Slope
Appendix C. TwoPort Analysis
Appendix D. Accuracy of Pi Model
Appendix E. erf( )
Notes