A velocity is estimated as the slope of a straight line fitted by least squares to…

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Numerical and computational mathematics · Numerical and computational mathematics

Error, Chance and the Machine, Ch Approximating a function: interpolation and differentiation

Problem

A velocity is estimated as the slope of a straight line fitted by least squares to mm readings spaced τ\tau apart and centred on the time of interest. Each reading has independent noise of standard deviation σ\sigma, and the underlying curve has a constant third derivative f′′′f'''. The slope has a noise term σ/[τm(m2−1)/12]\sigma\big/\bigl[\tau\sqrt{m(m^2-1)/12}\bigr] and a truncation term (3m2−7) τ2∣f′′′∣/120(3m^2-7)\,\tau^2|f'''|/120, which add in quadrature in the mean-square error. Let W=mτW=m\tau be the window width. ((a)) For m≫1m\gg1 write both terms in terms of WW, σ\sigma, τ\tau and ∣f′′′∣|f'''|, keeping only the leading power of WW in each. ((b)) Show that the window width that minimises the rms error satisfies W7=14400 σ2τ/f′′′2W^7=14400\,\sigma^2\tau/f'''^2. ((c)) Take σ=1 mm\sigma=1\,\mathrm{mm} and ∣f′′′∣=1 m s−3|f'''|=1\,\mathrm{m\,s^{-3}}. Find the best WW and the rms error of the velocity at 100 Hz100\,\mathrm{Hz} and at 1 kHz1\,\mathrm{kHz}, and say how the best error scales with the sampling interval τ\tau. Compare with the 6.0 mm s−16.0\,\mathrm{mm\,s^{-1}} of the best single difference.

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