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Signal averaging
Signal averaging
from Wikipedia

Signal averaging is a signal processing technique applied in the time domain, intended to increase the strength of a signal relative to noise that is obscuring it. By averaging a set of replicate measurements, the signal-to-noise ratio (SNR) will be increased, ideally in proportion to the square root of the number of measurements.

Deriving the SNR for averaged signals

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Assumed that

  • Signal is uncorrelated to noise, and noise is uncorrelated : .
  • Signal power is constant in the replicate measurements.
  • Noise is random, with a mean of zero and constant variance in the replicate measurements: and .
  • We (canonically) define Signal-to-Noise ratio as .

Noise power for sampled signals

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Assuming we sample the noise, we get a per-sample variance of

.

Averaging a random variable leads to the following variance:

.

Since noise variance is constant :

,

demonstrating that averaging realizations of the same, uncorrelated noise reduces noise power by a factor of , and reduces noise level by a factor of .

Signal power for sampled signals

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Considering vectors of signal samples of length :

,

the power of such a vector simply is

.

Again, averaging the vectors , yields the following averaged vector

.

In the case where , we see that reaches a maximum of

.

In this case, the ratio of signal to noise also reaches a maximum,

.

This is the oversampling case, where the observed signal is correlated (because oversampling implies that the signal observations are strongly correlated).

Time-locked signals

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Averaging is applied to enhance a time-locked signal component in noisy measurements; time-locking implies that the signal is observation-periodic, so we end up in the maximum case above.

Averaging odd and even trials

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A specific way of obtaining replicates is to average all the odd and even trials in separate buffers. This has the advantage of allowing for comparison of even and odd results from interleaved trials. An average of odd and even averages generates the completed averaged result, while the difference between the odd and even averages, divided by two, constitutes an estimate of the noise.

Algorithmic implementation

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The following is a MATLAB simulation of the averaging process:

N=1000;   % signal length
even=zeros(N,1);  % even buffer
odd=even;         % odd buffer
actual_noise=even;% keep track of noise level
x=sin(linspace(0,4*pi,N))'; % tracked signal
for ii=1:256 % number of replicates
    n = randn(N,1); % random noise
    actual_noise = actual_noise+n;
    
    if (mod(ii,2))
        even = even+n+x;
    else
        odd=odd+n+x;
    end
end

even_avg = even/(ii/2); % even buffer average 
odd_avg = odd/(ii/2);   % odd buffer average
act_avg = actual_noise/ii; % actual noise level

db(rms(act_avg))
db(rms((even_avg-odd_avg)/2))
plot((odd_avg+even_avg)); 
hold on; 
plot((even_avg-odd_avg)/2)

The averaging process above, and in general, results in an estimate of the signal. When compared with the raw trace, the averaged noise component is reduced with every averaged trial. When averaging real signals, the underlying component may not always be as clear, resulting in repeated averages in a search for consistent components in two or three replicates. It is unlikely that two or more consistent results will be produced by chance alone.

Correlated noise

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Signal averaging typically relies heavily on the assumption that the noise component of a signal is random, having zero mean, and being unrelated to the signal. However, there are instances in which the noise is not uncorrelated. A common example of correlated noise is quantization noise (e.g. the noise created when converting from an analog to a digital signal).

References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
Signal averaging is a fundamental technique in that enhances the (SNR) of a measured signal by repeatedly acquiring and arithmetically averaging multiple instances of the same signal over time, thereby suppressing random while preserving the deterministic signal components. This method assumes that the noise is uncorrelated and has a mean value of zero, allowing it to cancel out through summation, whereas the coherent signal reinforces proportionally with the number of averages. The mathematical foundation of signal averaging relies on the statistical properties of noise. For n independent measurements, when summing them, the total signal amplitude scales linearly as n times the single-scan signal (S_total = n × S), while the standard deviation of the noise increases as σ_n = σ √n, where σ is the noise standard deviation for a single scan. The signal-to-noise ratio for the summed signal is then SNR = S_total / σ_n = (n S) / (σ √n) = √n (S / σ), improving by a factor of √n relative to a single measurement. Consequently, the SNR improves by a factor of √n, yielding a processing gain of approximately 3 dB per doubling of n (or 10 dB per decade in logarithmic terms). This improvement is most effective for periodic or stable signals where acquisition times are short and the signal remains consistent across repetitions, but it diminishes if the signal or noise exhibits time-dependent drift. In practice, signal averaging finds widespread applications across engineering and scientific domains, including oscilloscopes for visualizing low-amplitude waveforms, biomedical signal analysis such as (ECG) to isolate QRS complexes from , and for enhancing spectral data in techniques like (NMR). Advanced variants incorporate alignment methods, such as or fiducial markers, to handle non-stationary signals, and can be combined with filters like Savitzky-Golay for further smoothing without significant signal distortion. Despite its efficacy, the technique requires sufficient computational resources for large n and is less suitable for real-time processing or non-random sources.

Introduction

Definition and Motivation

Signal averaging is a technique that enhances the detectability of a deterministic signal embedded in noise by arithmetically averaging multiple independent measurements of the same signal. This method relies on the principle that the underlying signal remains consistent across repetitions, while random noise varies unpredictably, allowing the noise to diminish through summation. It is particularly effective for repetitive or time-locked signals, such as evoked responses in biomedical applications. The primary motivation for signal averaging is to improve the (SNR) in scenarios where the desired signal is weak and obscured by substantial , without the need for specialized hardware beyond standard acquisition systems. Intuitively, each averaging iteration reinforces the coherent signal components, which add constructively, while uncorrelated noise terms cancel out on average, leading to a progressive reduction in noise variance. This makes it a cost-effective approach for extracting low-amplitude signals in fields like , where direct measurement is challenging due to inherent physiological noise. Effective signal averaging requires certain prerequisites, including a stationary signal that does not vary systematically across trials and additive that is random, zero-mean, and uncorrelated between measurements. These assumptions ensure that the averaging process isolates the true signal without introducing distortions. The technique originated in the context of analysis in (EEG), pioneered by George D. Dawson, who in 1954 introduced a method to detect small responses to stimuli amid large irregular backgrounds.

Applications

Signal averaging is widely applied in to extract weak physiological signals from noisy recordings. In (EEG), it is used to isolate evoked potentials, such as auditory or visual responses, by time-locking multiple trials to stimuli and averaging them, thereby enhancing the (SNR) of activity patterns buried in background neural noise. Similarly, in electrocardiography (ECG), signal averaging detects low-amplitude late potentials at the end of the , which indicate delayed ventricular depolarization and risk of arrhythmias, enabling non-invasive assessment of myocardial substrate for reentrant . In physics and engineering, signal averaging improves the detection of faint signals in high-noise environments. (NMR) employs it to boost sensitivity for low-abundance nuclei like ¹³C, where multiple scans are accumulated to reduce thermal noise and achieve higher for molecular structure analysis. In , it enhances weak signals by stacking repeated recordings from similar events, suppressing random and revealing subtle ground motions for improved event detection and characterization. In audio and communications, signal averaging serves as a technique. For , it averages multiple utterances or segments to attenuate uncorrelated , improving clarity in environments like teleconferencing or hearing aids, where it helps recover intelligible speech from additive background interference. In systems, pulse integration— a form of coherent signal averaging—accumulates returns from multiple transmissions to increase detection range and reliability of targets amid clutter and thermal . As of 2025, emerging applications integrate signal averaging with for adaptive processing in real-time systems. In wearable health devices, ML algorithms enhance EEG averaging by dynamically weighting trials based on noise estimates, improving seizure detection accuracy from continuous biosignals. A representative example is in clinical EEG for diagnosing neurological disorders, where averaging 100-500 stimulus-locked trials can improve SNR by approximately 20-27 dB, allowing visualization of event-related potentials essential for identifying conditions like or .

Theoretical Foundations

Signal and Noise Models

In signal averaging, the underlying signal is modeled as a deterministic, time-invariant s(t)s(t) that repeats identically across NN independent trials, exhibiting no variability between repetitions. This assumption holds in applications such as recordings, where the signal is triggered by repeatable stimuli, ensuring phase coherence across trials. The component is characterized as additive, zero-mean random ni(t)n_i(t) superimposed on the signal in the ii-th , where i=1,2,,Ni = 1, 2, \dots, N. This is assumed to be stationary with constant variance σ2\sigma^2 and uncorrelated across trials, satisfying E[ni(t)nj(t)]=0E[n_i(t) n_j(t)] = 0 for iji \neq j, and uncorrelated with the signal itself. These properties allow the to cancel out through summation, as its remains zero while its fluctuations diminish. The averaged output signal is given by y(t)=1Ni=1N[s(t)+ni(t)]=s(t)+1Ni=1Nni(t),y(t) = \frac{1}{N} \sum_{i=1}^N \left[ s(t) + n_i(t) \right] = s(t) + \frac{1}{N} \sum_{i=1}^N n_i(t), where the signal term persists unchanged at s(t)s(t), and the noise term has a reduced variance of σ2/N\sigma^2 / N due to the independence of the noise instances. For discrete-time implementations, common in digital signal processing, the models extend to sampled versions ss and nin_i at a sampling rate fsf_s, with the noise often further assumed to be white (uncorrelated across samples) to ensure independence in the discrete domain. The averaging formula becomes y=1Ni=1N[s+ni],y = \frac{1}{N} \sum_{i=1}^N \left[ s + n_i \right], preserving the signal while attenuating the noise variance by 1/N1/N. A critical assumption underpinning these models is that the noise is ergodic, meaning ensemble averages equal time averages, and remains uncorrelated across trials; deviations from these conditions, such as correlated artifacts, can compromise the efficacy of averaging.

Derivation of SNR Improvement

The (SNR) is defined as SNR=10log10(PsignalPnoise)\text{SNR} = 10 \log_{10} \left( \frac{P_{\text{signal}}}{P_{\text{noise}}} \right), where PsignalP_{\text{signal}} is the signal power and PnoiseP_{\text{noise}} is the . In signal averaging, consider a deterministic signal s(t)s(t) corrupted by additive uncorrelated with zero and variance σ2\sigma^2. The signal power remains unchanged after averaging NN independent realizations because the signal adds coherently: the averaged signal is 1Ni=1Ns(t)=s(t)\frac{1}{N} \sum_{i=1}^N s(t) = s(t), so Psignal, avg=s(t)2P_{\text{signal, avg}} = |s(t)|^2. The noise power reduces due to the for uncorrelated noise. The variance of the sum of NN independent noise terms is Nσ2N \sigma^2, and dividing by N2N^2 for the average yields a variance of σ2/N\sigma^2 / N, so Pnoise, avg=σ2/NP_{\text{noise, avg}} = \sigma^2 / N. The improvement in the linear power SNR is thus NN, leading to a decibel improvement of 10log10N10 \log_{10} N. Equivalently, considering the amplitude-based perspective, the ratio Psignal, avg/Pnoise, avg/Psignal/Pnoise\sqrt{P_{\text{signal, avg}} / P_{\text{noise, avg}}} / \sqrt{P_{\text{signal}} / P_{\text{noise}}}
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