Ask the Applications Engineer—14: High Frequency Signal Contamination

Q. I’ve heard that RF can make low-frequency circuits do strange things. What’s that all about?

A. I was once summoned to France because an Analog Devices Voltage-Frequency Converter (VFC), the AD654, suffered from “unacceptable variation of accuracy.” I had measured the offending parts in my own laboratory and found them to be stable and within specification, but when I returned them to the customer with my test jig he was unable to reproduce my results. While considering a site visit to confirm my suspicions, I discovered that the restaurant “La Cognette” in the town where our customer was located had three stars in the Guide Michelin, and the chef was a “Maitre Cuisinier de France” – a title not lightly bestowed. The visit to the customer became doubly necessary. Herman, who was in England to look at data offsets in a Boeing wind tunnel test, offered to come and help – he said it was the interesting technical problem (but just before he offered I saw him earnestly consulting the Guide Michelin).

To drive from the Analog Devices office in Newbury in the South of England to the centre of France involves six hours of driving, a six hour ferry crossing of the English Channel, and a change from the correct side to the right side of the road. Nevertheless, driving is better than flying, because one can take more test gear (and the portable ham-radio station as well – we are both hams).

As we approached the customer’s works we passed an enormous short-wave transmitting antenna, and then another, and yet another. We began to guess what might be wrong, and when we entered the laboratory I was carrying a hand-portable two-metre ham transceiver (an HT or “handy-talky”) in my jacket pocket.

The AD654 was indeed behaving unstably, as the customer had claimed. The VFC’s output frequency varied by an equivalent offset of tens of mV over the space of a few minutes. I quietly reached into my pocket and pressed the transmit button of my HT. The output frequency jumped by an equivalent of 150 mV, thus demonstrating the problem to be high-frequency pickup. More-formal measurements a little later showed that the local transmitters (of the French Overseas Broadcast organization) produced high-frequency (HF) field strengths within our customer’s works of tens or hundreds of mV/m.

Many problems of instability in precision measurement circuitry can be traced to high-frequency interference, but unless there is a loudspeaker in the system that might unexpectedly burst into hard rock music from the nearby radio station, it is common for engineers to overlook this source of inaccuracy and blame the manufacturer of the amplifiers or data converters.

Furthermore, this case was unusual in that it took a high-powered signal to affect the AD654, which is single-ended and also relatively insensitive to RF – it is much more common to see with a differential amplifier in-amp. Both inputs of these types of amplifier have high input impedances to common; they are therefore far more vulnerable and are affected by low-level RF, such as radiation from a personal computer (PC). [This phenomenon is detailed in the Analog Devices system-design seminar notes, available for sale as System Application Guide (1993).]

An important factor is that, in instrumentation amplifiers, common-mode rejection decreases with increasing frequency, starting to roll off at quite low frequencies – and distortion increases with frequency. Thus, not only are high-frequency common-mode signals not rejected; they are distorted, producing offsets. For some applications, where RF interference is a strong possibility, the AD830 difference amplifier has wideband common-mode rejection and is designed for line-receiver applications; it may be a useful substitute for an instrumentation amplifier.

Sensors are often connected to their signal-conditioning electronics by long cables. Radio engineers have a term for such long pieces of wire; they call them antennas. The long feeders from sensors to their electronics will behave in the same way and will serve as antennas, even if we do not wish them to do so. It does not matter if the sensor case is grounded-at high frequencies the reactances of the case and feeders will allow the system to behave as an antenna, and any high- frequency signals (E-field, M-field, or E-M-field) which it encounters will appear across any impedances. The most likely place for them to end up is at the amplifier input. Precision low-frequency amplifiers can rarely cope with large HF signals, and the result is error – commonly a varying offset error.

Q. But this couldn’t happen to me!

A. Never believe it won’t happen to you! An easy free lunch can always be obtained by persuading an innocent to bet on his or her circuit being free of such problems. Using a ham radio HT on the two-metre (144-148-MHz) band, one watt at a distance of one meter for one second will win you your free lunch almost every time. But a less-dramatic test can be equally convincing.

Disconnect the sensor and its leads. Short-circuit the amplifier input terminals to each other and to the amplifier circuit common (probably ground) with the shortest possible links and measure the amplifier output; observe its stability over a few minutes. Now remove the short-circuit, replace the sensor leads and place them in their normal operating environment. Disable the excitation and short-circuit the signal leads at the sensor end. Again measure the amplifier output, and its variation with time. Weep quietly.

It is often possible to see what is happening by using a high-frequency oscilloscope (or a spectrum analyzer, which is more sensitive but less easy to interpret) to measure the HF noise, both normal mode and common-mode, at the amplifier input; but normal mode measurements must be treated with some suspicion, because the oscilloscope itself – and its power- and probe leads – may themselves introduce signals and invalidate the measurement. The effect of the oscilloscope may be minimized by using a simple broadband transformer between the measurement point and the oscilloscope input, as shown in the figure; but such a transformer has fairly low impedance and will load the circuit being measured.

Figure 1

Common-mode signals can be observed quite easily by disabling any sensor excitation and connecting the oscilloscope ground to the ground at the board input and joining all the sensor leads together and to the oscilloscope input. All too often this signal will have an amplitude of several hundred millivolts and contain components from low frequencies to tens or hundreds of MHz.

The world is full of HF noise sources: ham radio operators, police, people with portable phones, garage door openers, the sun, supernovas, switching power-supply and logic signals (e.g., PCs). Since we cannot eliminate HF noise in the environment, we must filter it out of low-frequency signals before they arrive at precision amplifiers.

The simplest type of protection can be used when the signal bandwidth is only a few Hz. A simple RC low-pass filter inserted ahead of an amplifier will afford both normal-mode and common-mode HF protection. A suitable circuit is shown in the figure. There are two important issues to be considered in the choice of components: the resistances R and R´ (shown as 1 kΩ in the diagram, a value suitable for amplifier bias currents of a few nA or less) must be chosen so that they do not increase the offset appreciably as the amplifier bias current flows in them. The normal-mode time constant, (R + R´)C2, must be much larger than the common-mode time constants, RC1 and R´C1´, otherwise the common-mode time constants would have to be very carefully matched to avoid an imbalance that would convert the common-mode to a signal between the differential inputs.

Figure 2

If the signal bandwidth is wider, such simple filters will not be suitable because they remove the desired HF normal-mode signals as well as the unwanted HF common-mode signals. Large HF common-mode signals are very likely to suffer common-mode→normal mode conversion (as well as minor rectification, producing low-frequency errors) if they get to the amplifier, so it is necessary to use a filter which will reject HF common-mode signals but will pass DC and HF normal-mode signals.

Such a filter is shown below. It was devised many years ago by Bill Gunning of Astrodata and is related to the “phantom circuit” used in long-distance telephone circuits. It uses a tightly coupled “trifilar” transformer having three windings in an accurate 1:1:1 ratio. An AC voltage across any winding will also be present on the others.

Figure 3

The guard line is connected to ground at the source end and at the other end to the amplifier’s guard pin (or a comparable derived voltage), which represents what the amplifier “thinks” is common mode, via a capacitor. The high-frequency common- mode signal will appear (by definition) across the bottom winding, and will induce an equal common-mode voltage in the other two, subtracting the common-mode voltage in series with each line and effectively cancelling the HF common-mode signal at the amplifier inputs.

There are, of course, potential problems. A capacitor in series with the transformer is almost essential in the guard circuit to block DC and LF and prevent transformer core saturation by low-frequency currents in the guard circuit. The impedance looking into the amplifier guard terminal must be much lower than the impedance of the transformer windings; and at very high frequencies the capacitances of the transformer will allow signal leakage or may cause phase shift. These issues set incompatible constraints on the design of the transformer, if it must deal with a very wide range of common-mode frequencies.

In such a case double cancellation using two separate transformers as shown might be considered-the one nearer the amplifier having high inductance (and correspondingly high capacitance) and the other having good VHF efficiency.

Figure 4

Other approaches are also possible: the amplifier can be sited closer to the sensor and the long leads be replaced by leads (or optical fibre) carrying digital data, which is less vulnerable; more shielding is often (but not always) helpful; and sometimes (but rarely) it is possible to reduce the possibility of unexpected HF signals (even if you keep away the hams and police, there is always the possibility of the unexpected pizza delivery truck radioing to its base . . .)

The most important consideration, though, is awareness of the possibility of HF interference and readiness to tackle it. If designs are always made in the expectation of unwanted HF, chances are excellent that precautions will be adequate – it’s when you don’t expect it that the trouble starts.

Q. How did it work out with the French customer?

A. His problem was cured with two resistors, three capacitors and a piece of grounded copper foil. We went off to “La Cognette” to celebrate.



James Bryant

James Bryant自1982年起担任ADI公司的欧洲应用经理,直至2009年退休为止。至今仍从事撰写和咨询工作。他拥有英国利兹大学的物理学和哲学学位,同时还是注册工程师(C.Eng.)、欧洲注册工程师(EurEng.)、电机工程师协会会员(MIET)以及对外广播新闻处(FBIS)会员。除了热情钻研工程学外,他还是一名无线电爱好者,他的呼叫代号是G4CLF。


Herman R. Gelbach