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Matt Pitkin edited We_can_define_the_Fourier__.tex
over 8 years ago
Commit id: e3b724112dffcd4e6b5d8f45057b48f60f6ba509
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The second term in this equation involving $(f+f_k)$ is negligible for our purposes, so only the first term is required.
We want to convert this into a more easily \href{http://math.stackexchange.com/a/1470809/95147}{solvable} form e.g.\
\begin{equation}\label{eq:fourier2}
H_k(f) = y_k' e^{i\phi_k-i\pi f \Delta t} \int_{z_1}^{z_2} \exp{\left[i\left( z^3 + \alpha z + \beta \right) \right]} {\rm d}z.
\end{equation}
Firstly, lets put the cubic in equation~\ref{eq:fourier} in the form
\begin{equation}
M = at^3 + bt^2 + ct + d,
\end{equation}
where $a=(\pi/3)\ddot{f}_k$, $b = \pi \dot{f}_k$, $c = 2\pi(f_k-f)$ and $d=0$ and make the substitution $t = Az+B$. To get the derivative ${\rm d}z$ we have
\begin{equation}
H_k(f) \frac{{\rm d}t}{{\rm d} z} =
y_k' e^{i\phi_k-i\pi f \Delta t} \int_{z_1}^{z_2} \exp{\left[i\left( z^3 + \alpha z + \beta \right) {\rm d}z \right]} A,
\end{equation}
so, ${\rm d}t = A{\rm d}z$ and therefore in equation~\ref{eq:fourier2} we have $y_k' = Ay_k$.
%This integral is not analytic, but integral of cubic trigonometric functions (through e.g.\ use of \href{http://docs.sympy.org/latest/index.html}{sympy}) can be written as
%\begin{equation}