The speed of a body falling through a resistive fluid is modelled as

PHYSICS · Subjective · Fermi University Physics · Scientific Practice & Experimental Methods · Data analysis and model fitting in the laboratory · Data analysis and model fitting in the laboratory

Computational Physics, Ch Finding the best parameters: minimisation and fitting

Problem

The speed of a body falling through a resistive fluid is modelled as v(t)=v∞tanh⁡(kt)v(t) = v_\infty \tanh(kt), where v∞v_\infty is the terminal speed and kk is a rate constant. Three speeds are measured, each with the same uncertainty:
tt (s)123
vv (m s−1^{-1})8.013.516.0
Starting from the guess v∞=15.0 m s−1v_\infty = 15.0\,\mathrm{m\,s^{-1}}, k=0.50 s−1k = 0.50\,\mathrm{s^{-1}}, carry out one Gauss-Newton step. You may use ∂v/∂k=v∞t sech2(kt)\partial v/\partial k = v_\infty t\,\mathrm{sech}^2(kt) with sech2(x)=1−tanh⁡2(x)\mathrm{sech}^2(x) = 1-\tanh^2(x). (a) Evaluate the residuals and the two partial derivatives ∂v/∂v∞\partial v/\partial v_\infty and ∂v/∂k\partial v/\partial k at the starting guess, for the three times. (b) Assemble the 2×22\times2 normal equations. (c) Solve for the update and report v∞v_\infty and kk after the step, to three significant figures.

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