I Overdamping Condition of Nonlinear Equation

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In case of equation
\alpha y''(x)+\beta y'(x)+\gamma y(x)=0
where ##\alpha>0##, ##\beta>0##, ##\gamma>0##, characteristic equation is
\alpha r^2+\beta r+\gamma=0
and characteristic roots are
r_{1,2}=\frac{-\beta \pm \sqrt{\beta^2-4\alpha \gamma}}{2 \alpha}
If ## \beta^2<4\alpha \gamma## system is underdamped, and
if ## \beta^2>4\alpha \gamma## system is overdamped.
What in the case of equation
\alpha y&#039;&#039;(x)+\beta y&#039;(x)+\gamma \sin[y(x)]=0
when equation is nonlinear? How to find when system is overdamped? Thanks a lot for your help in advance.
 
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How do you define underdamping in such a situation? Is such an equation even solvable? And does it have periodic solutions (i.e. imaginary exponential parts in its solution)?
 
Overdamping is when characteristic roots are real and negative, I suppose. But I am not sure how to see that in case of nonlinear equations. I saw in literature that people discuss overdamped limit in case of nonlinear equations, but I am not sure how to do that. Because of that I asked here in the forum.

This limit is to my mind important to see when term ##\beta y'(x)## dominates over ##\alpha y''(x)##.
 
And just one more question, but very similar that the mentioned. What if we have equation
\alpha y&#039;&#039;(x)+\beta y&#039;(x) +\gamma y(x)=cz+d
If ##c## and ##d## are not functions of ##x##? What's happening with condition in that case?
 
There is the following linear Volterra equation of the second kind $$ y(x)+\int_{0}^{x} K(x-s) y(s)\,{\rm d}s = 1 $$ with kernel $$ K(x-s) = 1 - 4 \sum_{n=1}^{\infty} \dfrac{1}{\lambda_n^2} e^{-\beta \lambda_n^2 (x-s)} $$ where $y(0)=1$, $\beta>0$ and $\lambda_n$ is the $n$-th positive root of the equation $J_0(x)=0$ (here $n$ is a natural number that numbers these positive roots in the order of increasing their values), $J_0(x)$ is the Bessel function of the first kind of zero order. I...
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