Can anyone identify this series trick?

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The discussion revolves around the manipulation of an infinite series in a thesis, specifically transforming the series from one form to another by introducing the frequency difference σr. The author seeks clarification on the transition between the two equations and questions the assumption that n, defined as the ratio of σ to σr, must be an integer. It is suggested that the transformation is aimed at preparing the series for a Fourier expansion. The final form proposed involves redefining variables to facilitate the expansion of u|u| into a Fourier series. The conversation highlights the complexities of series manipulation in mathematical contexts.
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Hi there, I am reading through a thesis and the author takes the infinite series:

\begin{equation}
u(x,t)=u_0(x)+u_1(x)\cos(\sigma t - \phi_1(x)) + u_1'(x)\cos(\sigma' t - \phi'_1(x))+\ldots
\end{equation}

and by letting σr be the difference between the frequencies σ and σ' changes the above to:

\begin{equation}
u=u_0+u_1\cos(n\sigma_rt-\phi_1) + u_1'\cos([n+\beta]\sigma_rt-\phi_1')+\ldots
\end{equation}

where β=±1 and n is an integer. I don't follow the manipulation from the first equation to the other, I just wondered if anyone is familiar with this trick and might be able to talk me through it. Many thanks.
 
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This would be unproblematic is if ##n=\sigma/\sigma_r## is not assumed to be an integer. It seems wrong otherwise, if ##u_1'=0## for example. So either this is wrong or ##n=\sigma/\sigma_r## should be assumed to be an integer, by some reason.
 
Thanks for the reply Erland. The reason for the change is to eventually get u(x,t)|u(x,t)| into a form suitable for a Fourier expansion. I think that by letting θ=σt-Φ1 and α=σrt+Φ11' where σr=σ-σ' to transform (1) in the OP to:

\begin{equation}
u(x,t)=u_0+u_1\cos(\theta)+u_1'\cos(\theta-\alpha)+u_2\cos(2\theta-[\phi_2-2\phi_1])+u_2'\cos(2\theta-2\alpha-[2\phi_1'+\phi_2'-4\phi_1])+\ldots
\end{equation}

should work fine. Then u|u| can be expanded into a Fourier series of θ.
 
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