Depending on the low-distortion needs of an application, the system engineer can choose from plenty of signal amplifiers. The first step in making the right choice is to understand the typical datasheet curves that characterize total harmonic distortion plus noise, THD+N, in amplifiers.
Harmonic distortion versus amplitude is one of the typical datasheet curves that describe THD+N, and it is the topic of this series of articles. Another important typical curve is THD+N versus frequency.1
In the THD+N versus amplitude curve, the first region is noise dominated and is explained in terms of the amplifier's signal-to-noise ratio (SNR). Next is a moderate-distortion region, which is explained in terms of the internal amplifier topology, as well as loading. And last is the clipping-dominated region. Figures 1a and 1b show examples.
In Part 1, we will examine how THD+N is affected by the amplifier's noise and why it seems to improve with amplitude level. First, let's take a brief look at the measurement setup.
THD+N versus amplitude measurement
A distortion analyzer tool is usually used to make THD+N measurements.1 For simplicity, the amplifier is configured in a closed-loop gain of one. I say “simplicity,” because this is not always the case, especially when the distortion components are below the instrument's noise level. We'll have more on this in a subsequent article. For now, we can assume a buffer configuration is good enough for our measurements.
In the setup shown below, the positive input is connected to the instrument's pure sine wave generator, and the amplifier's output is connected back to the instrument for distortion analysis. The frequency of the sine wave is fixed to a single, constant frequency while the amplitude is swept across the dynamic range of the amplifier.
Datasheets usually present the THD+N versus amplitude curve with a fixed frequency of 1kHz and amplitude swept from 100mV-rms up to the amplifier's dynamic range limit. The distortion analyzer's bandwidth setting limits the noise and the number of harmonics the instrument takes into account. Typical settings for the bandwidth are 80kHz and 500kHz. The measurements in this article use a bandwidth of 80kHz.
The tool generates a frequency spectrum for each amplitude in the sweep and uses the following equation to calculate THD+N.
In this equation, V1 is the fundamental of the input signal. This is the variable that is swept. VN is the harmonics, and VNOISE is the amplifier's noise. When the tool completes the amplitude sweep, it has a family of frequency spectra to generate THD+N as a function of amplitude.
The THD+N in the noise-dominated region in Figure 1a decreases (or improves) with increasing amplitude, because the THD+N is reported as a ratio to the increasing amplitude signal. The noise floor of an amplifier for a given bandwidth and frequency is a fixed quantity, so for smaller signal amplitudes, the SNR is the limiting factor for an amplifier's linearity. As the signal amplitude increases, SNR improves, and so does THD+N.
Figure 1b presents THD+N by showing results in absolute values, rather than as a percentage ratio of the amplitude signal. In this case, the units used are V-rms, but they can also be shown in dBV (voltage relative to 1V). Figure 1b uses the following equation to show the results in absolute units.
When THD+N is presented in absolute units, the measurement in the noise dominated region is independent of the fundamental signal's amplitude. This makes it clear that the noise component is constant and unrelated to the signal amplitude. However, at a particular signal amplitude level, the amplifier stages begin to depart from their linear regions, and the THD contribution begins to dominate. At this point, the curve enters the moderate-distortion region. This happens between 3V-rms and 4V-rms in Figure 1b.
Figure 3a shows frequency spectra for three different input signals to further illustrate that the noise component in THD+N is constant and unrelated to signal amplitude. The noise is dominant at signal amplitudes of 100mV-rms and 1V-rms, but at 4V-rms, the amplifier's nonlinear behavior begins to produce harmonics. THD (and not noise) becomes dominant at this point.
The noise-dominated region in Figure 1a can also be understood in terms of the equation shown below. In this equation, the numerator is constant and representative of the dominant noise. THD is insignificant, and x is the increasing signal amplitude. The function f(x) is representative of THD+N in the noise-dominated region.
For this function, a small input value for x yields a large output value, and vice versa . In a log-log scale, the slope of this function is -20dB per decade. Figures 4a and 4b show the results for f(x) = 1/x and f(x) = 0.1/x to illustrate the effects of high and low noise on THD+N.
As soon as the signal becomes large enough and the nonlinearities of the amplifier begin to produce harmonics, the amplifier enters the moderate-distortion region. In my next article, I will take a look at the input and output stages of the amplifier in this region and how they play a role in setting the THD+N.
We initiated this series of articles by discussing the noise-dominated region of the THD+N versus amplitude curve. As you become familiar with this curve, keep in mind that the noise floor of an amplifier for a given bandwidth and frequency is a fixed quantity. For smaller signal amplitudes, the SNR is the limiting factor for an amplifier's linearity.
References and additional information:
- Jorge Vega and Raj Ramanathan, “Harmonic Distortion: Part I – Understanding Harmonic Distortion vs. Frequency Measurements in Op Amps,” En-genius, January 30, 2012.
- David Johns and Kenneth Martin, Analog Integrated Circuit Design , John Wiley & Sons, Inc., 1997.
- OPA1652/54 op-amp datasheet, Texas Instruments.
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