Signal averaging explained

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

Assumed that

s(t)

is uncorrelated to noise, and noise

z(t)

is uncorrelated :

E[z(t)z(t-\tau)]=0=E[z(t)s(t-\tau)]\forallt,\tau

.

Psignal=E[s2]

is constant in the replicate measurements.

E[z]=0=\mu

and

0<E[\left(z-\mu\right)2]=E[z2]=Pnoise=\sigma2

.

SNR=

Psignal
Pnoise

=

E[s2]
\sigma2
.

Noise power for sampled signals

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

Var(z)=E[z2]=\sigma2

.

Averaging a random variable leads to the following variance:

Var\left(1n
\sum
n
i=1

zi\right)=

1{n
2}
n
Var\left(\sum
i=1

zi\right)=

1{n
2}
nVar\left(
\sum
i=1

zi\right)

.

Since noise variance is constant

\sigma2

:

Var(Navg)=Var\left(

1n
\sum
n
i=1

zi\right)=

1{n
2}

n\sigma2=

1n
\sigma

2

,

demonstrating that averaging

n

realizations of the same, uncorrelated noise reduces noise power by a factor of

n

, and reduces noise level by a factor of

\sqrt{n}

.

Signal power for sampled signals

Considering

n

vectors

Vi,i\in\{1,\ldots,n\}

of signal samples of length

T

:

Vi=\left[si,1,\ldots,si,T\right],si,k\inKT

,

the power

Pi

of such a vector simply is

Pi=

T
\sum
k=1
2}
{s
i,k

=\left|Vi\right|2

.

Again, averaging the

n

vectors

Vi,i=1,\ldots,n

, yields the following averaged vector

Vavg=

1n
\sum
n
i=1

si,k=

1n
\sum
n
i=1
T
\sum
k=1

si,k

.

In the case where

Vn\equivVm\forallm,n\in\{1,\ldots,n\}

, we see that

Vavg

reaches a maximum of

Vavg,identicalsignals=Pi

.

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

SNRavg,identicalsignals=

Vavg,identicalsignals
Navg

=nSNR

.

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

Time-locked signals

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

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

The following is a MATLAB simulation of the averaging process:N=1000; % signal lengtheven=zeros(N,1); % even bufferodd=even; % odd bufferactual_noise=even;% keep track of noise levelx=sin(linspace(0,4*pi,N))'; % tracked signalfor 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; endend

even_avg = even/(ii/2); % even buffer average odd_avg = odd/(ii/2); % odd buffer averageact_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

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).