Mailing List lml@lancaironline.net Message #35406
From: Brent Regan <brent@regandesigns.com>
Sender: <marv@lancaironline.net>
Subject: Re: Avionics=Black Art
Date: Sun, 23 Apr 2006 18:39:51 -0400
To: <lml@lancaironline.net>
Shields Up!

Imagine water flowing through a thin walled rubber tube. A small part of the water volume is "lost" as the pressure in the tube increases because the tube "inflates" slightly with an increase in pressure. This water is "recovered" when the pressure drops and the tube "deflates". Likewise,
when a current flows through a wire a magnetic field "inflates" or expands around that wire. The field is proportional to the current flowing through the wire. Unlike the tube analogy, if the magnetic field crosses another conductor it generates a voltage in that conductor and if the other conductor is part of a circuit then a current starts to flow and some of the energy from the first conductor is lost to the second conductor. Transformers depend on, and are optimized for, this energy transfer. The ratio of the induced voltage to rate of current change is called inductance. If the current is changing rapidly then a significant portion of the energy flowing through the wire is lost to this inductive resistance, called impedance, and impedance is proportional to frequency.

When you measure the resistance of a wire with an ohm meter you are measuring the resistance of that wire to a direct current flow that is stable with respect to time. If you pass an alternating current through that wire you will also have impedance to that alternating current. That impedance is low at low frequencies and higher at high frequencies.

Now imagine a wire conductor as a bundle tiny strands. The strands in the center of the conductor have a lot of neighbors that want to steal some energy but the strands on the surface only have less than half as many thieving neighbors. The strands in the center therefore have a higher AC impedance than the strands at the surface. This effect becomes more pronounced the higher the frequency so that at high frequencies the impedance at the center of the wire is much higher on the surface. This "skin effect" means that at high frequencies almost all of the energy flowing is following the path of least resistance, which is on the surface, or skin, of the wire.

Cable shields act as a protective skin that intercepts the high frequency energy and drains it to ground before it can get into, or out of, the cable it surrounds. The shield's location and geometry make the preferred path for high frequency energy.  What is essential is that there is a low resistance AND low impedance path from shield to ground. A length of 22 gauge wire may have a low DC resistance but it may have a high AC impedance such that, at high frequencies, if the shield is connected to ground through a small wire then the shield loses most of its effectiveness because its connection to ground has a big resistor (the wire) in series.

The shield will work with only one end tied to ground because, like an antenna, the circuit is partially copper and partially an oscillating magnetic field. However, energy intercepted at the far end of the shield must transverse the length of the cable, and all its DC resistance, before finding ground. If there is a ground at both ends then the energy only has to travel, at most, half as far, and there are two parallel paths to take.

Now imagine you have a device that draws 3 amps at 14 volts and is connected by a 24 gauge 25 foot power cable. The DC resistance of 25' of 24 gauge wire is 0.66 ohms. Multiply this times 3 amps and the voltage drop in the wire is 2 volts. 2 volts in the power wire AND 2 volts in the ground wire. This means that if you put a volt meter between the aircraft ground and the case of the device you would see a 2 volt potential. Now imagine you need to pass a digital signal from the device and that signal is referenced to ground.  When the device sets the signal to "low" it may be ground at the device but it will be at 2 volts at the other end of the cable so the receiver may not interpret the signal as "low". Remember that the signal path does not have significant current flow so there is not the voltage losses that are present in the power cable.

This difference in ground reference is the source of "ground loops" which are unwanted currents flowing between devices that are not tied to ground with a sufficiently low resistance connection. As Hamid said, if DC current is flowing through the shield of a cable it is a symptom of a problem elsewhere, not the source of that problem.

Twenty years ago the only high frequency devices in an airplane were the radios. Now, with the introduction of computers with their high frequency  signals there are new challenges to keeping things electrically "quiet". It does not surprise me that engineers who design audio panels recommend terminating a shield at a pin. They are concerned with audio frequencies only, so if you can't hear it it is not important to them.  The bottom line is that the better you can connect all the grounds of all the chassis and all the shields the better "damped" and electrically quieter the airplane will be.

Many engineers do not sufficiently understand or appreciate the issues. For example, Hamid and I designed a tablet computer for Canadian Marconi Electronics (CMA-1100 Pilot View) and as part of that effort, took the system to a test facility to verify the electromagnetic radiation of the system was within limits.  The closest the system got to busting the radiation limit was 3db (1/2 the allowed power) at about 150 MHz. When CMC repeated the test with a CMC built system they reported their system was over the limit by more than 3 db, 4 times the emissions we measured.  Many phone calls and thousands of dollars in travel and chamber time later we discover that CMC did not follow our recommendation for terminating the power and serial communication shields directly to the connector body at both ends. Rather, they terminated using the CMC standard method of soldering the shield to a 22 gauge wire and then grounding the other end of the two inch long wire. Replacing the cable with one that had properly terminated shields fixed the problem.  CMC did not believe this to be true until we did side by side tests at an independent facility with a CMC engineer present.

The above is a very brief review. I have omitted and simplified much for the sake of brevity.

Regards
Brent Regan
Subscribe (FEED) Subscribe (DIGEST) Subscribe (INDEX) Unsubscribe Mail to Listmaster