Chapter 6: Problem 4
Often in practice, an approximation of the form $$ u(t)=\gamma_{1} e^{\gamma_{2} t} $$ is sought for a data fitting problem, where \(\gamma_{1}\) and \(\gamma_{2}\) are constants. Assume given data \(\left(t_{1}, z_{1}\right),\left(t_{2}, z_{2}\right), \ldots,\left(t_{m}, z_{m}\right)\), where \(z_{i}>0, i=1,2, \ldots, m\), and \(m>0\) (a) Explain in one brief sentence why the techniques introduced in the present chapter cannot be directly applied to find this \(u(t)\). (b) Considering instead $$ v(t)=\ln u(t)=\left(\ln \gamma_{1}\right)+\gamma_{2} t $$ it makes sense to define \(b_{i}=\ln z_{i}, i=1,2, \ldots, m\), and then find coefficients \(x_{1}\) and \(x_{2}\) such that \(v(t)=x_{1}+x_{1} t\) is the best least squares fit for the data $$ \left(t_{1}, b_{1}\right),\left(t_{2}, b_{2}\right), \ldots,\left(t_{m}, b_{m}\right) $$ Using this method, find \(u(t)\) for the data $$ \begin{array}{|c|c|c|c|} \hline i & 1 & 2 & 3 \\ \hline t_{i} & 0.0 & 1.0 & 2.0 \\ \hline z_{i} & e^{0.1} & e^{0.9} & e^{2} \\ \hline \end{array} $$
Short Answer
Step by step solution
Key Concepts
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