An Organized Space for Programming, Writing, and Soldering

AndersonPhoto1

Photo 1—This is Anderson’s desk when he is not working on any project. “I store all my ‘gear’ in a big plastic bin with several smaller bins inside, which keeps the mess down. I have a few other smaller storage bins as well hidden here and there,” Anderson explained.

AndersonPhoto2

Photo 2—Here is Anderson’s area set up for soldering and running his oscilloscope. “I use a soldering mat to protect my desk surface,” he says. “The biggest issue I have is the power cords from different things getting in my way.”

Al Anderson’s den is the location for a variety of ongoing projects—from programming to writing to soldering. He uses several plastic bins to keep his equipment neatly organized.

Anderson is the IT Director for Salish Kootenai College, a small tribal college based in Pablo, MT. He described some of his workspace features via e-mail:

I work on many different projects. Lately I have been doing more programming. I am getting ready to write a book on the Xojo development system.

Another project I have in the works is using a Raspberry Pi to control my hot tub. The hot tub is about 20 years old, and I want to have better control over what it is doing. Plus I want it to have several features. One feature is a wireless interface that would be accessible from inside the house. The other is a web control of the hot tub so I can turn it on when we are still driving back from skiing to soak my tired old bones.

I am also working on a home yard sprinkler system. I laid some of the pipe last fall and have been working on and off with the controller. This spring I will put in the sprinkler heads and rest of the pipe. I tend to like working with small controllers (e.g., the Raspberry Pi, BeagleBoard’s BeagleBone, and Arduino) and I have a lot of those boards in various states.

Anderson’s article about a Raspberry Pi-based monitoring device will appear in Circuit Cellar’s April issue. You can follow him on Twitter at @skcalanderson.

Evaluating Oscilloscopes (Part 1)

Recently, I was in the market for a new oscilloscope. There’s a good selection of devices for sale, but which should you choose? It’s clear from the ads that the “scope bandwidth” and “sample rate” are two important parameters. But are there other things hidden in the specification sheet you should take a look at?

I’ve compiled notes from my own oscilloscope-selection experience and wanted to share them with you. I’ll be pulling in specifications and examples from a few different oscilloscopes. Personally, I ended up selecting a PicoScope device, so I will be featuring it more prominently in my comparisons. But that’s simply because I don’t have a lab full of oscilloscopes to photograph! I don’t work for Pico Technology or have any affiliation with it, and will be attempting to pull in other manufacturers for this online series to provide some balance.

This “mini-series” will consist of four posts over four weeks. I won’t be discussing bandwidth and sample rate until next week. In this first post, I’ll cover some physical characteristics: stand-alone vs PC-based probe types and digital inputs. Next week I’ll discuss the “core” specifications, in particular the bandwidth, sample rate, and analog-to-digital converter resolution. The  third week will look at the software running the oscilloscope, and details such as remote control, fast Fourier transform (FFT) features, digital decoding, and buffer types. The final week will consider a few remaining features such as the external trigger and clock synchronization, and will summarize all the material I’ve covered.

I hope you find it useful!

Topic 1: Do You Want a PC-Based or Stand-Alone Instrument?
There are two fundamentally different types of instruments, and you’ll have to decide for yourself which you prefer. Many people like a stand-alone instrument, which you can place on your bench and probe your circuits to your heart’s content. You don’t need to have your computer nearby, and you have something solely dedicated to probing.

Figure 1: PC-based oscilloscopes make it easier to mount on a crowded bench. This PicoScope 6000 unit is velcroed to my desk, you can see the computer monitor to the upper left.

Photo 1: PC-based oscilloscopes make mounting easier on a crowded bench. This PicoScope 6000 unit is velcroed to my desk. You can see the computer monitor to the upper left.

The other option is a PC-based instrument, which today generally means it plugs in via USB. I’ve always preferred this type for a few reasons. The first is the minimal desk space needed. I can place an oscilloscope vertically and lose little space (see Photo 1). The second is I find it easier to interact with a standard keyboard and mouse, especially if you’re using more advanced features. In addition, you can easily save screenshots or data from the scope without having to transfer them using a USB key or something similar.

There are a few downsides to USB-based instruments. The most common complaint is probably the lack of knobs, although that’s fixable. In Photo 2, you can see a USB-based “knob board” I built, which pretends to be a USB key. Each turn of the knob sends a keystroke and, as long as your PC-based oscilloscope software lets you set custom keyboard shortcuts, can trigger features such as changing the input range or timebase. Most of the time, I still just use the regular PC interface, as I find it easier than knobs. If you’re interested in the design, you can find it on my blog Electronics & More.

Photo: A simple USB-based knob board uses mechanical encoders to control the USB scope via a physical panel.

Photo 2: A simple USB-based knob board uses mechanical encoders to control the USB scope via a physical panel.

Having a PC-based oscilloscope also means you can have a massive screen. A high-end oscilloscope will advertise a “large 12.1″ screen,” but you can purchase a 22″ screen for your computer for $200 or less.  If your PC-based oscilloscope software supports multiple “viewports,” you can more easily set up complex displays such as that in Figure 1.
Again this comes down to personal preference—personally, I like having the oscilloscope display as a window on my computer. You may wish to have a dedicated display separate from your other work, in which case consider a stand-alone device!

Figure 1: PC-based oscilloscopes make it easier for setting up windows in specific positions, due to a combination of much larger screen space and standard mouse/keyboard interaction.

Figure 1: PC-based oscilloscopes make it easier for setting up windows in specific positions, due to a combination of much larger screen space and standard mouse/keyboard interaction.

Topic 2: Where’s the Ground?
One common complaint with the PC-based oscilloscope is that the probe ground connects to USB ground. Thus, you need to ensure there isn’t a voltage difference between the ground of your device under test and the computer.

This is, in fact, a general limitation of most oscilloscopes, be they stand-alone or PC-based. If you check with an ohmmeter, you’ll generally find that the ”probe ground”  in fact connects to system Earth on stand-alone oscilloscopes. Or at least it did on the different Agilent units I tested. Thus the complaint is somewhat unfairly leveled at PC-based devices.

You can get oscilloscopes that have either “differential” or “isolated” inputs, which are designed to eliminate the problem of grounds shorting out between different inputs. They may also give you more measurement flexibility. For example, if you are trying to measure the voltage across a “high-side shunt resistor,” you can do this measurement differentially. The TiePie engineering  HS4 DIFF is one example of a device with this capability. Of course, you can purchase differential probes for any oscilloscope, which accomplish the same goal! Most manufactures make these differential probes (Agilent, Tektronix, Pico Technology, Rigol, etc.).

Topic 3: Input Types
Almost every scope will have either DC-coupled or AC-coupled inputs. You’ll likely want to compare the minimum/maximum voltage ranges the scope has. Don’t be too distracted by either the upper or lower limits unless you have very specific requirements. At the upper end, remember you will mostly be using the 10:1 probe, which means an oscilloscope with ±20 V input range becomes ±200 V with the 10:1 probe.

At the lower end, the noise is going to kill you. If your oscilloscope has a 1 mV/div range, for example, you’ll have to be extremely careful with noise. To probe very small signals, you’ll probably end up needing an active probe with amplification right at the measurement point. This can be something you build yourself, using a differential amplifier chip, for example, if you are attempting to measure current across a shunt.

Besides the actual measurement range, you’ll be interested in the “offset” range too. With the DC-input, most oscilloscopes can subtract a fixed voltage from the input. Thus you can measure a 1.2-V input on a 1-V maximum input range, as the oscilloscope is able to first subtract say 1 V from the signal. This is handy if you have a smaller signal riding on top of some fixed voltage.

Another input type you will encounter is the 50-Ω input. Normally, this means the oscilloscope can switch between AC, DC, and DC 50 input types. The DC 50 means the input is “terminated” with a 50-Ω impedance. This feature is typically found on oscilloscopes with higher analog bandwidth. For example, this allows you to measure a clock signal that is output on a SMA connector expecting a 50-Ω termination. In addition, the 50-Ω input allows you to simplify connection of other lab equipment to your oscilloscope. Want to use a low noise amplifier (LNA) to measure a very small signal? Not a problem, since you can properly terminate the output of that LNA.

If you end up needing DC 50 termination, you can buy “feed-through” terminators for about $15, which operate at up to 1-GHz bandwidth. You simply add those to the front of your oscilloscope to get 50-Ω terminated inputs.

Any given manufacturer will often have a range of inputs for different bandwidths and models. For example, the PicoScope 5000-series, which has up to 200-MHz bandwidth, has DC/AC high-impedance inputs. The 6000-series has DC/AC/DC 50 inputs for 500-MHz bandwidth and below. The 6000 series in 1,000 MHz bandwidth only has 50-Ω input impedance. Other manufacturers seem to follow a similar formula: the highest bandwidth device is 50-Ω input only, medium-bandwidth devices are DC/AC/DC 50, and lower-bandwidth devices will be DC/AC.

Topic 4: Probe Quality and Type
In day-to-day use, nothing will impact you more than the quality of your oscilloscope probe. This is your hands-on interaction with the oscilloscope.

Figure 4: A smaller spring-loaded probe tip is on the left,  and  a standard oscilloscope probe is on the right. Both  probes have removable tips, so if you damage the probe it’s easy to fix them. Not all probes have removable tips, however, meaning if the tip is damaged you may have to throw out the probe.

Photo 3: A smaller spring-loaded probe tip is on the left, and a standard oscilloscope probe is on the right. Both probes have removable tips, so if you damage the probe it’s easy to fix them. Not all probes have removable tips, however, meaning if the tip is damaged you may have to throw out the probe.

Most “standard” oscilloscope probes are of the type pictured to the right in Photo 3. They are normally switchable from 1:1 to 10:1 attenuation, where the 10:1 mode results in a 1/10 scaling of input voltage. It’s important to note that almost every oscilloscope probe has very limited bandwidth in 1:1 mode—often under 10 MHz. Whereas in 10:1 mode it might be 300 MHz! In addition, the 10:1 mode will load the circuit considerably less. Higher bandwidth probes will often only come in 10:1 mode. I assume the physical switch is too much hassle at higher frequencies!

A first thing to check out is if the tip is removable. If you damage the tip, it can be useful to simply replace the tip rather than the entire probe. If you’re probing a PCB, it can be easy to catch a tip in a via, for example. Alternatively, certain probes might come with an adapter, which is designed for use in probing the PCB, rather than just the tip of the regular oscilloscope probe. The older Agilent 1160A probes come with such a tip.

One particular type of probe I really like has the spring-loaded tip shown to the left in Photo 3. This is a much smaller tip than “standard,” and the spring-loaded tip makes it much easier to get a good connection with solder joints. You can apply some pressure to break through the oxide layer, and the spring-loaded aspect keeps the tip right on the joint. In addition, you can even do things such as probe through the solder mask on a via. There are even plastic guard add-ons, which fit standard surface mount device (SMD) sizes (e.g., 1.27 mm, 1 mm, 0.8 mm, 0.5 mm) to probe TQFP/SOIC/TSSOP packages.

The particular probe I’m photographing comes with the PicoScope 6000 series, which is sold separately as part number TA150 (350-MHz bandwidth) or TA133 (500-MHz bandwidth). However, I’ve noticed that Agilent seems to also sell a probe that looks the same—under part number N287xA—right down to accessories. Similarly, Teledyne LeCroy also seems to sell this probe under the PP007 part number, and Rohde & Schwarz sells it under the RTM-ZP10 part number, also with the same accessories. Thus I suspect there is some upstream manufacturer! Depending on your supplier and options, prices range from $200-$400 for the probe if you want to pick it up separately.

Photo 5: The ground spring accessory can be used in a number of ways. If you're lucky, you can insert it into GND  vias on your PCB. If required, you can also solder a small section of wire to the spring.

Photo 4: The ground spring accessory can be used in a number of ways. If you’re lucky, you can insert it into GND vias on your PCB. If required, you can also solder a small section of wire to the spring.

Pomona Electronics sells a similar probe, part numbers 6491 through 6501 (the exact partnumber depending on bandwidth). The 150-MHz version (6493) is available for under $60 from Digi-Key, Mouser, and Newark element14, for example. This probe differs from the previous group of spring-loaded ones, but if you don’t need the higher bandwidth it may be a more reasonable purchase.

If you are dealing with a high-bandwidth probe, you may need to be concerned about the flatness of the frequency response. A probe may be sold with a 1G-Hz bandwidth, for example, which simply means the -3-dB point is at 1GHz. However, shoddy manufacturing may mean not having a very flat frequency response before that point, or not rolling off evenly after the -3-dB point.

When dealing with high bandwidth probes, the grounding will become a serious issue. The classic “alligator clip” probably won’t cut it anymore! The simplest accessory your probe is likely to come with is the spring adapter shown in Photo 4. There may be more advanced accessories available for grounding, too; check documentation for the probe itself. You can see an example of differences in grounding as part of my “probe review”  video.

Don’t be afraid to build your own accessories for the probe. Photo 5 shows a probe holder I built for a $15 adjustable arm. Details of the construction are here.

Here’s a simple 3-D probe holder you can build for $20 or less.

Photo 5: Here’s a simple 3-D probe holder you can build for $20 or less.

Topic 5: Digital Input?
The final item to consider is if you want digital inputs along with analog. This is, again, somewhat of a personal choice: You may wish to have a separate stand-alone digital analyzer, or you may wish to have it built into your oscilloscope.

I personally chose to have a stand-alone digital logic analyzer, which is a PC-based instrument. Digital logic analyzers are available at a fairly low cost from a variety of manufacturers (e.g., Saleae and Intronix). In my experience, the cost of purchasing a separate PC-based logic analyzer was considerably lower than the “incremental cost” of selecting an oscilloscope with logic analyzer capabilities compared to one without. When evaluating this yourself, be sure to look at features such as number of channels, maximum sample rate, buffer size, and what protocols can be decoded by the logic analyzer.

While integrated-device manufacturers claim you should buy a scope/analyzer in one unit to get perfect synchronization between digital and analog, remember many of these devices can output a trigger signal. So if your oscilloscope can output a trigger signal when it starts the analog capture, you can use this to capture the corresponding data on the digital logic analyzer (or vice versa).

Next Week: Core Specifications
This first week I covered physical details of the oscilloscope itself you might want to consider. Next week, I’ll look at the more ‘”core” specifications such as bandwidth, sample rate, and sample resolution.

Author’s note: Every reasonable effort has been made to ensure example specifications are accurate. There may, however, be errors or omissions in this article. Please confirm all referenced specifications with the device vendor.

 

Experimenting with Dielectric Absorption

Dielectric absorption occurs when a capacitor that has been charged for a long time briefly retains a small amount of voltage after a discharge.

“The capacitor will have this small amount of voltage even if an attempt was made to fully discharge it,” according to the website wiseGEEK. “This effect usually lasts a few seconds to a few minutes.”

While it’s certainly best for capacitors to have zero voltage after discharge, they often retain a small amount through dielectric absorption—a phenomenon caused by polarization of the capacitor’s insulating material, according to the website. This voltage (also called soakage) is totally independent of capacity.

At the very least, soakage can impair the function of a circuit. In large capacitor systems, it can be a serious safety hazard.

But soakage has been around a long time, at least since the invention of the first simple capacitor, the Leyden jar, in 1775. So columnist Robert Lacoste decided to have some “fun” with it in Circuit Cellar’s February issue, where he writes about several of his experiments in detecting and measuring dielectric absorption.

Curious? Then consider following his instructions for a basic experiment:

Go down to your cellar, or your electronic playing area, and find the following: one large electrolytic capacitor (e.g., 2,200 µF or anything close, the less expensive the better), one low-value discharge resistor (100 Ω or so), one DC power supply (around 10 V, but this is not critical), one basic oscilloscope, two switches, and a couple of wires. If you don’t have an oscilloscope on hand, don’t panic, you could also use a hand-held digital multimeter with a pencil and paper, since the phenomenon I am showing is quite slow. The only requirement is that your multimeter must have a high-input impedance (1 MΩ would be minimum, 10 MΩ is better).

Figure 1: The setup for experimenting with dielectric absorption doesn’t require more than a capacitor, a resistor, some wires and switches, and a voltage measuring instrument.

Figure 1: The setup for experimenting with dielectric absorption doesn’t require more than a capacitor, a resistor, some wires and switches, and a voltage measuring instrument.

Figure 1 shows the setup. Connect the oscilloscope (or multimeter) to the capacitor. Connect the power supply to the capacitor through the first switch (S1) and then connect the discharge resistor to the capacitor through the second switch (S2). Both switches should be initially open. Photo 1 shows you my simple test configuration.

Now turn on S1. The voltage across the capacitor quickly reaches the power supply voltage. There is nothing fancy here. Start the oscilloscope’s voltage recording using a slow time base of 10 s or so. If you are using a multimeter, use a pen and paper to note the measured voltage. Then, after 10 s, disconnect the power supply by opening S1. The voltage across the capacitor should stay roughly constant as the capacitor is loaded and the losses are reasonably low.

Photo 1: My test bench includes an Agilent Technologies DSO-X-3024A oscilloscope, which is oversized for such an experiment.

Photo 1: My test bench includes an Agilent Technologies DSO-X-3024A oscilloscope, which is oversized for such an experiment.

Now switch on S2 long enough to fully discharge the capacitor through the 100-Ω resistor. As a result of the discharge, the voltage across the capacitor’s terminals will quickly become very low. The required duration for a full discharge is a function of the capacitor and resistor values, but with the proposed values of 2,200 µF and 100 Ω, the calculation shows that it will be lower than 1 mV after 2 s. If you leave S2 closed for 10 s, you will ensure the capacitor is fully discharged, right?

Now the fun part. After those 10 s, switch off S2, open your eyes, and wait. The capacitor is now open circuited, at least if the voltmeter or oscilloscope input current can be neglected, so the capacitor voltage should stay close to zero. But you will soon discover that this voltage slowly increases over time with an exponential shape.

Photo 2 shows the plot I got using my Agilent Technologies DSO-X 3024A digital oscilloscope. With the capacitor I used, the voltage went up to about 120 mV in 2 min, as if the capacitor was reloaded through another voltage source. What is going on here? There aren’t any aliens involved. You have just discovered a phenomenon called dielectric absorption!

Photo 2: I used a 2,200-µF capacitor, a 100-Ω discharge resistor, and a 10-s discharge duration to obtain this oscilloscope plot. After 2 min the voltage reached 119 mV due to the dielectric absorption effect.

Photo 2: I used a 2,200-µF capacitor, a 100-Ω discharge resistor, and a 10-s discharge duration to obtain this oscilloscope plot. After 2 min the voltage reached 119 mV due to the dielectric absorption effect.

Nothing in Lacoste’s column about experimenting with dielectric absorption is shocking (and that’s a good thing when you’re dealing with “hidden” voltage). But the column is certainly informative.

To learn more about dielectric absorption, what causes it, how to detect it, and its potential effects on electrical systems, check out Lacoste’s column in the February issue. The issue is now available for download by members or single-issue purchase.

Lacoste highly recommends another resource for readers interested in the topic.

“Bob Pease’s Electronic Design article ‘What’s All This Soakage Stuff Anyhow?’ provides a complete analysis of this phenomenon,” Lacoste says. “In particular, Pease reminds us that the model for a capacitor with dielectric absorption effect is a big capacitor in parallel with several small capacitors in series with various large resistors.”

Protocol-Decoding Oscilloscope Software

Agilent2Agilent Technologies has introduced the N8819A USB 3.0 SSIC and N8820A MIPI CSI-3 protocol decoders. The software decodes USB 3.0 SuperSpeed Inter-Chip (SSIC) and MIPI Camera Serial Interface 3 (CSI-3) protocols on oscilloscopes. The protocol decoders provide engineers with a fast, easy way to validate and debug SSIC and CSI-3 interfaces.

The N8819A USB 3.0 SSIC and N8820A MIPI CSI-3 protocol decoders are designed to run on 90000 A-, 90000 X-, and 90000 Q-Series oscilloscopes. They decode protocol packets for the SSIC V1.0 and MIPI CSI-3 V1.0 specifications, respectively. The decoders provide accurate timing measurements associated with the protocols.

The software supports correlated protocol decode information with the analog waveforms; symbol, packet, frame, and payload detail of the protocols; high-speed (HS-BURST) and low-speed PWM (PWM-BURST) transmission modes; cyclical redundancy check (CRC) on the packets; and search capability for various frames, sequences, and errors.

Both protocol decoders can be used on Infiniium 90000 Q-Series oscilloscopes, which deliver real-time bandwidth of up to 33 GHz on four channels. The oscilloscopes feature bandwidth upgradability to 63 GHz and low noise and jitter measurement floor performance.

The Agilent N8819A USB 3.0 SSIC and N8820A MIPI CSI-3 protocol decoders cost $3,500 and $3,000, respectively.

Agilent Technologies, Inc.
www.agilent.com

A Look at Low-Noise Amplifiers

Maurizio Di Paolo Emilio, who has a PhD in Physics, is an Italian telecommunications engineer who works mainly as a software developer with a focus on data acquisition systems. Emilio has authored articles about electronic designs, data acquisition systems, power supplies, and photovoltaic systems. In this article, he provides an overview of what is generally available in low-noise amplifiers (LNAs) and some of the applications.

By Maurizio Di Paolo Emilio
An LNA, or preamplifier, is an electronic amplifier used to amplify sometimes very weak signals. To minimize signal power loss, it is usually located close to the signal source (antenna or sensor). An LNA is ideal for many applications including low-temperature measurements, optical detection, and audio engineering. This article presents LNA systems and ICs.

Signal amplifiers are electronic devices that can amplify a relatively small signal from a sensor (e.g., temperature sensors and magnetic-field sensors). The parameters that describe an amplifier’s quality are:

  • Gain: The ratio between output and input power or amplitude, usually measured in decibels
  • Bandwidth: The range of frequencies in which the amplifier works correctly
  • Noise: The noise level introduced in the amplification process
  • Slew rate: The maximum rate of voltage change per unit of time
  • Overshoot: The tendency of the output to swing beyond its final value before settling down

Feedback amplifiers combine the output and input so a negative feedback opposes the original signal (see Figure 1). Feedback in amplifiers provides better performance. In particular, it increases amplification stability, reduces distortion, and increases the amplifier’s bandwidth.

 Figure 1: A feedback amplifier model is shown here.


Figure 1: A feedback amplifier model is shown.

A preamplifier amplifies an analog signal, generally in the stage that precedes a higher-power amplifier.

IC LOW-NOISE PREAMPLIFIERS
Op-amps are widely used as AC amplifiers. Linear Technology’s LT1028 or LT1128 and Analog Devices’s ADA4898 or AD8597 are especially suitable ultra-low-noise amplifiers. The LT1128 is an ultra-low-noise, high-speed op-amp. Its main characteristics are:

  • Noise voltage: 0.85 nV/√Hz at 1 kHz
  • Bandwidth: 13 MHz
  • Slew rate: 5 V/µs
  • Offset voltage: 40 µV

Both the Linear Technology and Analog Devices amplifiers have voltage noise density at 1 kHz at around 1 nV/√Hz  and also offer excellent DC precision. Texas Instruments (TI)  offers some very low-noise amplifiers. They include the OPA211, which has 1.1 nV/√Hz  noise density at a  3.6 mA from 5 V supply current and the LME49990, which has very low distortion. Maxim Integrated offers the MAX9632 with noise below 1nV/√Hz.

The op-amp can be realized with a bipolar junction transistor (BJT), as in the case of the LT1128, or a MOSFET, which works at higher frequencies and with a higher input impedance and a lower energy consumption. The differential structure is used in applications where it is necessary to eliminate the undesired common components to the two inputs. Because of this, low-frequency and DC common-mode signals (e.g., thermal drift) are eliminated at the output. A differential gain can be defined as (Ad = A2 – A1) and a common-mode gain can be defined as (Ac = A1 + A2 = 2).

An important parameter is the common-mode rejection ratio (CMRR), which is the ratio of common-mode gain to the differential-mode gain. This parameter is used to measure the  differential amplifier’s performance.

Figure 2: The design of a simple preamplifier is shown. Its main components are the Linear Technology LT112 and the Interfet IF3602 junction field-effect transistor (JFET).

Figure 2: The design of a simple preamplifier is shown. Its main components are the Linear Technology LT1128 and the Interfet IF3602 junction field-effect transistor (JFET).

Figure 2 shows a simple preamplifier’s design with 0.8 nV/√Hz at 1 kHz background noise. Its main components are the LT1128 and the Interfet IF3602 junction field-effect transistor (JFET).  The IF3602 is a dual N-channel JFET used as stage for the op-amp’s input. Figure 3 shows the gain and Figure 4 shows the noise response.

Figure 3: The gain of a low-noise preamplifier.

Figure 3: The is a low-noise preamplifier’s gain.

 

Figure 4: The noise response of a low-noise preamplifier

Figure 4: A low-noise preamplifier’s noise response is shown.

LOW NOISE PREAMPLIFIER SYSTEMS
The Stanford Research Systems SR560 low-noise voltage preamplifier has a differential front end with 4nV/√Hz input noise and a 100-MΩ input impedance (see Photo 1a). Input offset nulling is accomplished by a front-panel potentiometer, which is accessible with a small screwdriver. In addition to the signal inputs, a rear-panel TTL blanking input enables you to quickly turn the instrument’s gain on and off (see Photo 1b).

Photo 1a:The Stanford Research Systems SR560 low-noise voltage preamplifier

Photo 1a: The Stanford Research Systems SR560 low-noise voltage preamplifier. (Photo courtesy of Stanford Research Systems)

Photo 1 b: A rear-panel TTL blanking input enables you to quickly turn the Stanford Research Systems SR560 gain on and off.

Photo 1b: A rear-panel TTL blanking input enables you to quickly turn the Stanford Research Systems SR560 gain on and off. (Photo courtesy of Stanford Research Systems)

The Picotest J2180A low-noise preamplifier provides a fixed 20-dB gain while converting a 1-MΩ input impedance to a 50-Ω output impedance and 0.1-Hz to 100-MHz bandwidth (see Photo 2). The preamplifier is used to improve the sensitivity of oscilloscopes, network analyzers, and spectrum analyzers while reducing the effective noise floor and spurious response.

Photo 2: The Picotest J2180A low-noise preamplifier is shown.

Photo 2: The Picotest J2180A low-noise preamplifier is shown. (Photo courtesy of picotest.com)

Signal Recovery’s Model 5113 is among the best low-noise preamplifier systems. Its principal characteristics are:

  • Single-ended or differential input modes
  • DC to 1-MHz frequency response
  • Optional low-pass, band-pass, or high-pass signal channel filtering
  • Sleep mode to eliminate digital noise
  • Optically isolated RS-232 control interface
  • Battery or line power

The 5113 (see Photo 3 and Figure 5) is used in applications as diverse as radio astronomy, audiometry, test and measurement, process control, and general-purpose signal amplification. It’s also ideally suited to work with a range of lock-in amplifiers.

Photo 3: This is the Signal Recovery Model 5113 low-noise pre-amplifier.

Photo 3: This is the Signal Recovery Model 5113 low-noise preamplifier. (Photo courtesy of Signal Recovery)

Figure 5: Noise contour figures are shown for the Signal Recovery Model 5113.

Figure 5: Noise contour figures are shown for the Signal Recovery Model 5113.

WRAPPING UP
This article briefly introduced low-noise amplifiers, in particular IC system designs utilized in simple or more complex systems such as the Signal Recovery Model 5113, which is a classic amplifier able to obtain different frequency bands with relative gain. A similar device is the SR560, which is a high-performance, low-noise preamplifier that is ideal for a wide variety of applications including low-temperature measurements, optical detection, and audio engineering.

Moreover, the Krohn-Hite custom Models 7000 and 7008 low-noise differential preamplifiers provide a high gain amplification to 1 MHz with an AC output derived from a very-low-noise FET instrumentation amplifier.

One common LNA amplifier is a satellite communications system. The ground station receiving antenna will connect to an LNA, which is needed because the received signal is weak. The received signal is usually a little above background noise. Satellites have limited power, so they use low-power transmitters.

Telecommunications engineer Maurizio Di Paolo Emilio was born in Pescara, Italy. Working mainly as a software developer with a focus on data acquisition systems, he helped design the thermal compensation system (TCS) for the optical system used in the Virgo Experiment (an experiment for detecting gravitational waves). Maurizio currently collaborates with researchers at the University of L’Aquila on X-ray technology. He also develops data acquisition hardware and software for industrial applications and manages technical training courses. To learn more about Maurizio and his expertise, read his essay on “The Future of Data Acquisition Technology.”