Stripline vs. Microstrip Delay

A stripline is any trace separated from the air by a solid conductive reference plane on both sides. The electric fields from such a trace are totally contained between the two solid planes, so the speed of propagation for signals traveling on the trace is entirely determined by the dielectric constant of the pcb dielectric material. The speed of propagation for a stripline is independent of the trace geometry or impedance. A stripline need not be symmetrically located between the planes to qualify as a stripline. The term offset stripline is used to describe an asymmetrically positioned stripline (as shown in the pcb cross section in Figure 12.16).

Figure 12.16. The electric field surrounding a microstrip resides partly within the pcb dielectric material and partly within the surrounding air.

A microstrip is any trace fabricated on the outside layer of a pcb. A microstrip has pcb dielectric on one side and air on the other. A microstrip covered with soldermask or more layers of dielectric, but not covered with a solid conductive reference plane, is still called microstrip, although the term embedded microstrip may be used to describe such a trace.

The electric fields surrounding a microstrip reside partly within the pcb dielectric material and partly within the surrounding air. The speed of propagation for signals traveling on the trace is therefore determined partly by the dielectric constant of the pcb dielectric material and partly by the dielectric properties of air. Because the dielectric constant of air is always less than the dielectric constant of the pcb material, mixing a little air into the transmission-line speed equation always speeds up the signal propagation. In simple terms, microstrip traces are always a little faster than stripline traces (Figure 12.16).

Even if you adjust the trace widths on each layer so that the impedances are the same, the speed of propagation on the microstrip layers is always faster. The exact amount of speedup depends on the geometry of the microstrip traces (Table 12.2). A high-impedance, skinny microstrip, high up off the board, has the greatest proportion of its electric field carried in air and the greatest speed. A low-impedance, wide microstrip, pressed down close to the planes, carries more of its electric field in the pcb dielectric, resulting in a trace that is less speedy than its high-impedance counterpart , but still always faster than a stripline.

The only exceptions to the "microstrips are faster" rule would occur on a board with different dielectric materials used on different layers, such as a board built with FR-4 on the outer layers and Rogers RT/duroid 5580 on the inner layers. Such a board might provide exceptional RF properties on one layer without incurring the expense of exotic materials on all the other layers. Inhomogeneous board stack-ups must be thoroughly engineered to avoid difficulties with the different X-Y thermal expansion rates of the constituent materials.

The microstrip configurations listed in Table 12.2 range from 13% to 17% faster than the stripline configuration. Many layout people know about this issue and can automatically adjust trace lengths to compensate, so that at nominal temperature, clocks running on either microstrip or stripline traces will arrive at the same time (Figure 12.17). Trace-length compensation is helpful, but doesn't solve the whole problem with skew between microstrip and stripline layers. To see why, you need to think about variations in the electric permittivity with temperature.

Figure 12.17. On runs of equal length, the top layer may incorporate serpentine traces to equalize the delay between the microstrip and stripline configurations.

Table 12.2. Propagation Delay of Typical Microstrip Traces

Microstrip geometry
h mil	w mil	Impedance W	re
3	3	59.6	3.14
3	4	53.0	3.19
3	5	47.8	3.24
3	6	43.6	3.28
3	7	37.1	3.37
Stripline geometry
h mil	w mil	Impedance W	re
any	any	any	4.30
NOTE ”This table assumes an FR-4 dielectric with r = 4.30 at 1 GHz using copper traces of 1-oz thickness (including plating ) with s = 5.98 10 7 S/m plus a conformal coating (soldermask) consisting of a 12.7- m m (0.5-mil) layer having a dielectric constant of 3.3. The propagation velocity v (m/s) and delay t p (s/m) are found from re , where and c = 2.998 ·10 8 m/s.

Table 12.2 lists only the trace delay at nominal room temperature. Over the temperature range of 0 to +70 °C, the dielectric constant for FR-4 can vary as much as 10%. The trace delay for striplines , being proportional to the square root of the dielectric constant, will vary about 5% over the same temperature range.

Microstrip traces are different, because the surrounding dielectric medium for a microstrip is a mixture of FR-4 and air. When the temperature changes, the portion of the electric field residing in the FR-4 is affected, but the portion of the field in the air is not. The dielectric constant for air is rock solid and does not change with temperature. As a result, the temperature coefficient for microstrip traces (percent change in velocity per degree Celsius) is less severe than for striplines. Fifty-ohm FR-4 microstrip traces suffer a speed variation of only about 3% over the temperature range of 0 to +70 °C.

The difference in temperature coefficients for microstrips versus striplines implies that even if the delays are perfectly matched at nominal room temperature, the traces will still be mismatched by one percent or more at either end of the temperature scale. For a 30-cm (12-in.) trace, the mismatch amounts to a variation of ±20 ps between microstrip and stripline delays. This amount of mismatch represents a small but noticeable portion of a high-speed system skew budget.

For the best speed matching, implement all your clock traces on microstrips or all on striplines, but don't mix and match the two types.

POINT TO REMEMBER

• Given similar dielectrics, signals propagate faster on a microstrip layer than on a stripline layer. For best speed matching, don't mix the two types.