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Effect of Measurement Noise

In practice, measurements are never perfect. Let $ \hat{\underline{y}}=\underline{y}+\underline{e}$ denote the measured output signal, where $ \underline{e}$ is a vector of ``measurement noise'' samples. Then we have

$\displaystyle \hat{\underline{y}}= \underline{y}+ \underline{e}= \mathbf{x}\underline{h}+ \underline{e}.
$

By the orthogonality principle [38], the least-squares estimate of $ \underline{h}$ is obtained by orthogonally projecting $ \hat{\underline{y}}$ onto the space spanned by the columns of $ \mathbf{x}$. Geometrically speaking, choosing $ \underline{h}$ to minimize the Euclidean distance between $ \hat{\underline{y}}$ and $ \mathbf{x}\underline{h}$ is the same thing as choosing it to minimize the sum of squared estimated measurement errors $ \vert\vert\,\underline{e}\,\vert\vert ^2$. The distance from $ \mathbf{x}\underline{h}$ to $ \hat{\underline{y}}$ is minimized when the projection error $ \underline{e}=\hat{\underline{y}}-\mathbf{x}\underline{h}$ is orthogonal to every column of $ \mathbf{x}$, which is true if and only if $ \mathbf{x}^T\underline{e}=0$ [84]. Thus, we have, applying the orthogonality principle,

$\displaystyle 0 = \mathbf{x}^T\underline{e}= \mathbf{x}^T(\underline{y}- \mathb...
...nderline{h}) = \mathbf{x}^T\underline{y}- \mathbf{x}^T\mathbf{x}\underline{h}.
$

Solving for $ \underline{h}$ yields Eq.$ \,$(F.8) as before, but this time we have derived it as the least squares estimate of $ \underline{h}$ in the presence of output measurement error.

It is also straightforward to introduce a weighting function in the least-squares estimate for $ \underline{h}$ by replacing $ \mathbf{x}^T$ in the derivations above by $ \mathbf{x}^TR$, where $ R$ is any positive definite matrix (often taken to be diagonal and positive). In the present time-domain formulation, it is difficult to choose a weighting function that corresponds well to audio perception. Therefore, in audio applications, frequency-domain formulations are generally more powerful for linear-time-invariant system identification. A practical example is the frequency-domain equation-error method described in §I.4.4 [78].


Previous: Time Domain Filter Estimation
Next: Matlab System Identification Example

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About the Author: Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See http://ccrma.stanford.edu/~jos/ for details.


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