Picture of Doug
High Frequency Measurements Web Page
Douglas C. Smith

 Address:  P. O. Box 1457, Los Gatos, CA 95031
 TEL:      800-323-3956/408-356-4186
 FAX:      408-358-3799
 Mobile:   408-858-4528
 URL:      www.dsmith.org
 Email:    doug@dsmith.org

Technical Tidbit - February 2003
Crossing Ground Plane Breaks - Part 3
Immunity to Radiated EMI

board with slit and square loop  

Figure 1.
Radiated EMI Test Setup

Abstract: In this article, the last in a three part series on the effects of paths crossing ground plane breaks, the effects of immunity to impulsive electromagnetic fields are investigated. As one might expect, the data presented shows a significant loss of immunity to EMI for signal paths that cross a ground plane break as compared to paths that remain over a solid ground plane.

Discussion: Figure 1 shows a circuit board placed 20 cm from a source of EMI (~450K pdf file)  that simulates fast pulses caused  by low voltage ESD, a significant problem in custsomer environments. The board itself is shown in Figure 2. The upper path crosses a slot in the ground plane about 5 cm in length. The paths are 24 gauge wire taped down to a circuit board to form approximate 50 Ohm transmission lines terminated by the resistors on the right. The four wire loops soldered to the ground plane facilitate connections to the ground plane for other experiments and are not used in this test.

Board with ground break

Figure 2
. Test Board with 5 cm Ground Break

An oscilloscope screen is shown in Figure 3 for the path over solid ground. The amplitude of the signal due to the radiated interference is about 100 mV, not enough to cause a problem with most logic circuits. Note that the edge rates are very fast, and risetimes are faster than 1/2 ns on the screen. The EMI source produces edges of about 300 ps or faster.

scope image (solid ground plane)

Figure 3
. Signal from Path Over Solid Ground
(Vertical scale = 100 mV/div, Horizontal scale = 5 ns/div)

Compare Figure 3 to the scope screen shown in Figure 4. Figure 4 was taken using the path that crosses the ground break. The amplitude of the signal is over 3 Volts peak (the scale has been changed from 100 mV/div to 1 V/div) in Figure 4!

Figure 4. Signal from Path Over Broken Ground
(Vertical scale = 1 V/div, Horizontal scale = 5 ns/div)

This result could be expected from the analysis of signal currents on the board in the January 2003 Technical Tidbit, "Crossing Ground Plane Breaks - Part 2, Tracing Current Paths."  The article showed a significant loop is formed composed of the signal path and the return path in the ground plane that is forced to go around the end of the ground plane break. As can be seen from the data above, such a loop makes a great antenna.

For related information pertaining to this article on this website see:

The waveforms in this article were taken with an Agilent Infinium 54845a oscilloscope.

Top of page

Questions or suggestions? Contact me at doug@dsmith.org
Copyright © 2003 Douglas C. Smith