Dealing with high impedance sources and maintaining high impedance inputs without compromising reliability has its own set of challenges. This article offers qualitative and quantitative discussions of issues associated what high impedance circuits, what types of sensors are high impedance, and what devices are available for buffering and protecting high impedance circuits. An application is discussed in which going higher impedance helps.
If I had the option, I wouldn't use high impedance sensors. They are so easily affected by external noise, solder flux residue, particle tracking, bias currents, and distant charges, that it can be difficult to get repeatable results. High impedance sensors have some upsides though – they don‟t self load, and they are inherently low power. For quantifying properties such as pH, light, acceleration, or humidity, the most practical sensors available are high impedance. Nature offers them, so expediency urges that we utilize them. With careful attention to design, their tendency to be adversely affected by the world around them can be drastically reduced. As an interesting note about impedance, with the advent of practicable superconduction, impedance has an infinite achievable range. Of what else can that be said?
Reference Resistors and the Fear of High Impedance
Any circuit looking into a high impedance sensor should be characterized with a high impedance source, so every engineer should have some high value reference resistors available. Vishay Techno offers surface mount resistors to 50GΩ, with samples in 1GΩ and 2GΩ values available off the shelf (when last I checked). I also have some very nice leaded 10GΩ and 100GΩ resistors in the “Mini-MOX” series from Ohmite (www.ohmite.com). What is amazing about these ridiculously high value resistors is that they are actually quite “stiff”. For example, I was warned not to touch the resistor body lest the deposits from my skin oil “reduced the impedance”, and this compelled an experiment. Applying a Keithley Model 614 electrometer across the resistor leads resulted in a meter reading of 9.9 to 10.0GΩ. I proceeded to thoroughly touch and squeeze the resistor body from lead to lead with my oily fingers, and then backed away. The meter returned to precisely where it had been, 9.9 to 10.0GΩ. But this shows only that my human oils are not an immediate threat to these particular reference resistors. Sound laboratory methodology would still exhort cleanliness of components, pcb's, and insulators to ensure reliability over time and humidity. Skin oil conductivity is known to vary among humans. For cleaning, Ohmite recommends isopropyl alcohol and lint free wipes and a 75°C bake for 1 hour to drive off moisture.
When performing an impedance measurement like this, bear in mind that the insulator in the cable is entirely in parallel with the resistor under test. To maintain a 1% accuracy on a 100GΩ resistor measurement requires an overall insulator impedance of no less than 10TΩ. The only way around this limitation is to perform an open circuit calibration so that any shunt resistance can be measured and calculated out. The Keithley 614 does not have this feature, but still performs well. This reinforces the fact that, compared to an insulator, a 10GΩ resistor is indeed relatively stiff.
The Enemies of High Impedance Circuits
Impedance is high when leakages, current noises, bias currents, and static voltage dominate the errors. So dealing with high impedance circuits means minimizing those quantities. The most common and addressable form of leakage is that due to solder flux residue. Boards supporting high impedance circuits should be well cleaned so that all flux is removed. Third party board manufactures can have contaminated washers, so a clean wash may need to be specified as a production requirement. Traces should be spaced beyond the minimum design rules as real estate allows. For insulators, I have never found FR-4 to cause any problem, although it does absorb moisture, while Teflon and glass do not. Some designers have had recourse to Teflon posts or wells, but this may be due to their inherent resistance to surface tracking and other effects such as dielectric absorption, rather than their purely insulative properties. To keep surface impedances high in imperfect environments may require sealing or conformal coating, but this can reduce serviceability. Traces connected to high impedance sources and inputs should be guarded by traces at similar potentials. There are many practical considerations. For example, a dual op amp has non-inverting inputs at pins 3 and 5. It is easier to protect pin 5 because it is in the corner, while pin 3 is adjacent to the negative supply.
Bias current and current noise in active devices are sources of error. Bipolar transistors require a DC base current in order to operate. FETs have input leakage. In both cases, a current noise is induced due to electron quantization through junctions (note that this is not true for current generally, but for currents through junctions.) For FETs, current noise rises with frequency because of Miller effects (see sidebar below). While the temptation is to jump immediately to FET based input structures for their low bias currents, there are instances where super-beta bipolar input structures offer an advantage, particularly operating at high temperatures. FET input leakage doubles every 10°C, while super-beta bias current remains relatively stable. In either case, chopping techniques can be applied to remove the effects of both offset voltage and bias current. For impedances below a few MΩ, don't jump immediately to a FET input amplifier without first considering exceptionally precise and low bias current op amps like the LT6010, or LTC2054. Sometimes a better offset voltage can help defray a slightly worse bias current specification. For a given source impedance, the overall input error will be VOS + IBIAS*Rsource. As source impedance rises, the bias current term dominates, making a MOSFET input solution more attractive. This has become truer in recent years as the specifications of CMOS op amps have improved.
Another fascinating problem encountered with high impedance circuits is their sensitivity to motion. Static charges generated by shoes on a carpet can be at kilovolt levels, so even the tiniest capacitive coupling generates significant charge injection. When taking measurements, stand back and hold still. Shielding helps of course, but mechanical vibrations will modulate the capacitance (microphonics) between pcb traces and any local metalwork and cause charge injection. This is true even if the metalwork voltage itself is not changing, but simply at a different DC voltage than the traces. So shield your circuit, but not too closely. When mechanical motion or stress induce voltages on insulators at microscopic levels, they are usually referred to as triboelectric or piezoelectric effects. High impedance sources may require the use of low triboelectric noise cable, such as Belden type 9239 in high vibration environments.
Device and Amplifier Considerations
Discrete MOSFETs offer poor leakage specifications, but in fact they can outperform their specifications by up to six orders of magnitude. The familiar 2N7002 for example specifies channel leakage of 1µA max and gate leakage of 0.1µA max. But looking at these devices in the lab with 20V on the drain and a grounded gate and source, you will find a total combined leakage of only about 1pA! Obviously the specifications are not reflective of what the device does, but rather of the cost of production test time and resolution. Better specifications require more test time and better test equipment, so you'll pay for it. Of course better specifications will also eventually impact yield.
Ultralow leakage matched pair JFETs are available from Linear Integrated Systems (http://www.linearsystems.com) in their LS830, and from InterFET (http://www.interfet.com) in their IFN424. My favorite single JFET is the Philips BF862 for its 3pA gate current, its sub-nanovolt noise density, and its easy-to-deal-with -0.6V pinchoff voltage. The 2N4416 is also popular, especially for its sub-picofarad input capacitance and respectable noise density, but it has that large and wildly variant pinchoff voltage (2V – 6V!) that has been the bane of the JFET world.
CMOS op amps have been available for many years, but the specifications have been poor and the actual results even worse. Linear Technology has recently introduced two very good CMOS amplifiers – the (precision micropower) LTC6078 and the (higher speed) LTC6241. The LTC6241 offers an input leakage current of 4pA max at 25°C, and at 70°C guaranteed under 75pA. There have also been JFET input based “electrometer grade” op amps on the market for many years, but these are relatively expensive. In the end, no op amp or semiconductor device is perfect, so the best DC results are achieved with relays and calibrating or chopping techniques.
The circuit of Figure 1 is one example, incorporating two instances of a force-balance nulling technique. To follow the operation, assume all the switches are open, then close S2 and S3. This engages ultra-precision integrating amplifier A2, forcing A1's output to ground. A1's input offset appears at its +input, and 101 times its offset is stored on C1. Opening S3 allows A1 to function normally again, but with 1µV of effective offset and a drift of about 1µV/second. Now, opening S2 puts feedback resistor R1 in the circuit and causes an output voltage equal to IBIAS * R1 – typically 1mV. Closing S4 and S5 nulls A1's output again, but this time through A3. A1's bias current is delivered now through R2, and stored as a voltage on C2 at 60mV/pA. Opening S4 ends the nulling phase and closing S1 connects the input drive, shown in this case as a resistor under test (RUT) and a voltage source. But while the amplifier is now near perfect, it will not be for long. Drift on capacitors C1 and C2 will require a new nulling phase within several seconds or the amplifiers specifications may degrade beyond those of an unaided LTC6241. Figure 2 shows a much simpler method. Rather than trying to perfect the amplifier, this circuit instead chops the excitation so that the amplifier contributions can be subtracted out. Also, the RUT has been moved to the feedback path so that the output is proportion to RUT resistance rather than RUT admittance. Rise time was measured at 10ms (10-90%) with a 1GΩ RUT, so excitation should be no faster than about 10Hz to ensure adequate settling.
Protecting a High Impedance Circuit
But how can you protect a high impedance circuit without affecting its input impedance? Well, strictly speaking you can't, but you can come close. One of the best ways is to use a series resistor and some series inductance, even if it's just a length of trace. The inductance and parasitics will spread out an ESD pulse and improve the odds that it will jump to the chassis before it gets to anything sensitive. You can further improve those odds by introducing a spark gap in the layout near the connector pin to be struck. This is cheap and effective, but it can cause problems in higher density digital designs. The spark gap re-emits a strong EMI wave (including some nice eerie blue), and I have seen this crash an on-board but distant ‘486 repeatably. Fortunately the hardware was unharmed, so it depends on what level of immunity is specified for the design. In our case this was a failure, as PC reset interventions were not allowed. For analog designs or simple digital designs, spark gaps should not be a problem. Gas discharge tubes are also available as components.
Pretty much anything you do with diode clamps will cause leakage effects. Schottkys will probably be out of the question, as they tend to be leakier. Ultralow leakage diodes are available such as the CMPD6001 series from Central Semiconductor (http://www.centralsemi.com), and the BAS416 from Philips (http://www.semiconductors.philips.com); but the maximum leakage specifications are actually quite high: 500pA to 5nA, and that's at cold. The hot specifications are even worse, often running into microamps. For the lowest leakage, JFET junctions still outperform diodes. The 2N4393 leaks typically 5pA at room and 3nA at 100°C, and is available from Vishay in a SOT-23 package. Compare this to the maximum specified bias current of 75pA at 70°C for the LTC6241. Adding even good diodes or JFETs can cause a significant degradation. Some design work can help offset this problem however. For example, consider the tracking limiter circuit shown in Figure 3. The diodes are back-biased by A2 with the average DC voltage stored on C1. Overvoltages and spikes will be shunted to the reservoir capacitor, but the DC is allowed through (with unity gain). This protects the inputs, and also improves input overload recovery time. Where DC gain is desired, simply short C1 and move the input of A2 to the inverting input of A1. Inverting circuits are easier to protect because the diodes can simply be taken to ground.
Sidebar: Current Noise Measurements
Measuring something is easy when there is lots to measure, and difficult when there's little to measure. Good FETs have very little current noise, especially at low frequency, and that makes it inherently difficult to measure. At high frequency, FET input current noise rises due to either Miller effects in the drain or tail current noise blowing back through the gate-source capacitance, depending on circuit topology. The fact that there is more current noise at high frequency would make it easier to measure, but for the fact that bandwidth rolls off in any practical high impedance circuit.
For the low frequency measurement, simply configure the op amp (I'll limit my discussion to op amps for simplicity) as a unity gain buffer with a 10GΩ source resistor to ground, as shown in Figure 4. Use batteries and enclose the circuit in a cookie tin with a BNC through connector to access the output. Measure the output DC voltage and make sure that it's reasonable given the op amp's typical specified bias current (IBIAS = VOUT/10GΩ). If it looks reasonable, then make a note of the measured value. (If it's not an LTC op amp, you may have to correct for offset voltage first.) Now look at the low frequency output content, using a spectrum analyzer. Make sure you are looking below the rolloff of the input circuit. An input capacitance of 3pF acting on a 10GΩ source will cause a lowpass -3dB rolloff down at 5.3Hz. Below that frequency, and using averaging because noise is noisy, you should be able to see the 13µV/√Hz (at room temperature) noise density of the 10GΩ resistor take shape, as in Figure 5. Properly functioning and shielded, any additional output noise is due to input current noise acting on the 10GΩ source, because the amplifier's input voltage noise is relatively miniscule.
This single plot of output noise gives us two measurements: low frequency input current noise and input capacitance CIN. The low frequency input current noise is derived from the 13.6µV/√Hz output noise density measured at 0.22Hz (Figure 5, DUT is the LTC6241). Subtracting the expected 13µV/√Hz resistor noise RMS-wise leaves a net 4µV/√Hz [sqrt(13.6^2 – 13^2) = 4] attributed to op amp current noise. Dividing the 4µV/√Hz by 10GΩ arrives at an input current noise measurement of 0.4fA/√Hz. This number can be compared with the expected theoretical current noise density of sqrt(2*q*IBIAS), where q is the electron charge 1.6e-19 Coulombs, and IBIAS is the bias current measured above. The input capacitance CIN can be derived from the -3dB point of 4.3Hz shown in the same plot. The -3dB point occurs at CIN=1/2pi*R*f, where R=10GΩ and f=4.3Hz, giving us CIN=3.7pF.
Using the same circuit, but looking at higher frequency, you can also see the effect of the rising current noise – Figure 5a.
Note that the output voltage noise goes flat at high frequency. This is because although the current noise is rising, it is looking into the input capacitance which has falling impedance with frequency. So the product is flat. At 100kHz the 3.7pF input capacitance looks like 430kΩ. So the 50nV/√Hz output noise divided by 430kΩ must be due to 116fA/√Hz of input current noise at 100kHz. We can now plot the input current noise as a function of frequency (thus far measured only at the +input) as in Figure 5b. At low frequency it is a flat 0.4fA/√Hz, rising at a rate of 116fA/√Hz per kHz at high frequency. (Or put in more fundamental units, the rate of rise of current noise with frequency is 1.16attoAmps*Hz-3/2).
But for the high frequency case, many engineers prefer to have a test circuit that is closer topologically to the intended application circuit. A transimpedance circuit is most commonly employed because it is the most frequent application circuit for low current noise high impedance circuits (usually applied to photodiodes). Refer to Figure 6. This circuit emulates a transimpedance photodiode amplifier with C2 taking the place of a 1.5pF photodiode and C1 being a short circuit at high frequency. The bandwidth rolls off due to the combination of finite op amp gain bandwidth and the noise gain of the R2:C2 feedback network increasing with frequency. This is much more complicated than the single RC input encoutered previously! Fortunately the current noise rises with frequency, which is usually undesirable except when trying to measure it. Figure 7 shows the circuit's raw output noise spectrum with VIN open. The flat region at left is dominated by the 20MΩ resistor noise at 582nV/√Hz, and the noise figure there is very near 0dB. The noise clearly rises with frequency, but this could be due to either rising current noise or to voltage noise and rising noise gain. A quick calculation can help decide if either one is dominating, but first we should perform a gain calibration with frequency. R1 and C1 provide the window for excitation and thereby a gain measurement.
At a glance the whole circuit of Figure 6 is an integrator followed by a differentiator, so it should have flat response. In fact, at low frequencies response rolls off because the R1:C1 integrator has no gain. But we're not interested in low frequencies. At frequencies well above R1*C1, the current through C2 goes constant with frequency (as with an ideal photodiode) and the gain does indeed go flat as shown in figure 8. The midband gain factor is R2*C2 / R1*C1, or about 30mV out per 1V excitation in. This is easy to confirm in the lab, and with an accurate measurement the component tolerances become unimportant and the measured gain (attenuation in fact) can be normalized. At still higher frequencies, the differentiator starts to have bandwidth trouble due to the finite gain bandwidth of the op amp and the noise gain of the circuit, and the parasitic capacitances around R2. The result is that the gain drops with frequency – but we knew it would and that's why we're measuring it.
The important thing is that the output noise is measured with exactly the same circuit as the gain, including the op amp and the parasitics, but with the excitation removed. Taking the resulting output noise versus frequency data and dividing by the normalized gain versus frequency data yields a bandwidth-corrected version of output noise, as if the op amp had infinite gain bandwidth and the feedback resistor had no parasitics. Some signal analyzers, such as the HP3562, do an excellent job of waveform divides and plot generation while maintaining correct units for this analysis. But unfortunately I don't have one and it is still confusing for novices anyway, so I offer a sample calculation instead. If you can perform the calculation at one frequency, eventually it becomes easy to perform them at all frequencies.
Again using an LTC6241 as the DUT, I measured a midband gain of 0.0290 at 4kHz (down from the nominal 0.030, probably due to C2 tolerance) as shown in Figure 8. At 100kHz, the gain has rolled off to 0.0212, or about 0.73 of the midband gain. We can now apply this gain correction to the noise measurement at 100kHz.
Refer again to Figure 7. At high frequency, the noise is rising even though the response is falling. At 100kHz, we measure 1.61µV/√Hz output noise. To correct for the gain rolloff, we divide by the 0.73 from the gain curve and get 2.20µV/√Hz, still output referred. This would be the output noise with an infinitely fast op amp and no shunt capacitance around the feedback 20MΩ resistor. In order to refer this noise to the input, many TIA designers simply divide by the 20MΩ feedback impedance, for a 110fA/√Hz input referred current noise.
But this neglects the fact that some of the output noise is due to input voltage noise. We need to perform the calculation mentioned earlier to determine which noise is dominant. The voltage noise of the op amp gets to the output multiplied by the noise gain. The LTC6241 input capacitance of 3.5pF (Cdm + Ccm) combines with C1 to make 5pF. Let's assume 1pF of additional parasitics for a total of 6pF. At 100kHz, this looks like 265kΩ. Noise gain is 1+Zf / Zshunt, or 1+20MΩ/265kΩ = 76. The input voltage noise of the LTC6241 is 7nV/√Hz, so at the output it would contribute 76*7nV = 532nV/√Hz. Subtracting this RMS-wise from the 2.20µV/√Hz gives 2.13µV/√Hz. This is not an appreciable correction at all, but it does reduce the 110fA/√Hz current noise calculated above to 107fA/√Hz.
When measuring an op amp's current noise in this way, it is critical to sift out the effects of voltage noise. The circuit of Figure 5 did not have this complexity because the voltage noise was swamped in all cases, the noise gain was a solid unity, and the bandwidth was uncompromised. So the fact that the two measurement techniques on two different devices on two different inputs yield current noise results within 10% of each other reveals that the op amp has a good symmetric input structure and repeatability device to device, and that the techniques are reliable. The odds are small that everything is haywire and we still managed to fool ourselves.
Charge Amp Tradeoffs for Piezoelectric Accelerometers – How Going Higher Impedance Actually Helps
Figures 9 and 10 show two different approaches to amplifying signals from a capacitive sensor. The sensor in both cases is a 770pF piezoelectric shock sensor accelerometer, which generates charge under physical acceleration. Figure 9 shows the classical “charge amplifier” approach. The op amp is in the inverting configuration so the sensor looks into a virtual ground. All of the charge generated by the sensor is forced across the feedback capacitor by the op amp action. Because the feedback capacitor is 100 times smaller than the sensor, it will be forced to 100 times what would have been the sensor's open circuit voltage. So the circuit gain is 100. The benefit of this approach is that the signal gain of the circuit is independent of any cable capacitance introduced between the sensor and the amplifier. Hence this circuit is favored for remote accelerometers where the cable length may vary. Difficulties with the circuit are inaccuracy of the gain setting with the small capacitor, and low frequency cutoff due to the bias resistor working into the small feedback capacitor.
Figure 10 shows a non-inverting amplifier approach. This approach has many advantages. First of all, the gain is set accurately with resistors rather than with a small capacitor. Second, the low frequency cutoff is dictated by the bias resistor working into the large 770pF sensor, rather than into a small feedback capacitor, for lower frequency response. Third, the non-inverting topology can be paralleled and summed (as shown) for scalable reductions in voltage noise. The only drawback to this circuit is that the parasitic capacitance at the input reduces the gain slightly. This circuit is favored in cases where parasitic input capacitances such as traces and cables will be relatively small and invariant.
When you calculate the bias resistance required for the desired low frequency cutoff, consider that you may want to make the bias resistor still larger. This reduces the noise floor at low frequency. For example if we want to support frequencies down to 10Hz at -3dB, the bias resistor would work out to 1/2pi*10Hz*770pF = 20MΩ. At 10Hz, the 20MΩ resistor would contribute 580nV/√Hz of noise, and be -3dB down just like the signal. Making the resistor 1GΩ as shown, its 4000nV/√Hz voltage noise would be attenuated down to effectively 80nV/√Hz by the accelerometer capacitance, while the signal would barely be attenuated at all. Sometimes going higher impedance than conventionally required can actually help!
Devices and materials are available to support and protect very high impedances. Dealing with high impedances requires a knowledge of what are otherwise miniscule phenomena. Sometimes quantization of these phenomena – such as current noise – can be challenging in itself. But with the right circuit techniques, measurements become meaningful and repeatable. A proper breakdown of error sources such as leakage, settling time, voltage noise and current noise, help the circuit designer to know what to expect, and to get it.