Background
My question comes from here, it's a response of 1st order LPF RC circuit from an arbitrary periodic input.
How to determine the transient response of a circuit to causal periodic inputs?
Problem
Suppose if I have input signal with period of $T = 10s$
$\displaystyle u(t) = 2t (\theta(t) - \theta(t - 5)) + 0 (\theta(t - 5) - \theta(t - 10) )$
For t from 0 to infinity, there'll be $1-e^{-sT}$ in the denominator.
and then the system transfer function
$ H(s) = \dfrac{1/sC}{R + 1/sC} $
In order to find it's output we need F(s) which is a transfer function for one single period response from the input signal. Inverse it. Multiplies it with unit step since it's a causal signal and system. And then time shifted it by $nT$.
$ F(s) = H(s) U(s) $
$ \displaystyle \begin{align} f(t-nT) \theta(t-nT) &= 2\ \theta(t - nT) \left( RC (e^{-(t-nT)/(RC)} -1) + (t - nT)\right) \\ &+ 2\ \theta(t-5 - nT) \left( (5 - RC) e^{-(t-5-nT)/(RC)} + RC - (t - nT) \right) \end{align}$
Then from periodic summation properties of laplace transform we get $ \displaystyle y(t) = \mathcal{L}^{-1}\left[\frac{1}{1-e^{-sT}} F(s) \right] = \sum_{n=0}^{\infty} f(t-nT) \theta(t-nT) $
Assume if $R = 50k$ and $C = 100uF$, thus time constant of $5s$. This is the plot
Now if I change the time constant into $20s$. This is the plot if we sum it from n = 0 to 20.
Question
How to separate its transient and steady state response? Such as,
$ \displaystyle y(t) = y_{tr}(t) + y_{ss}(t) $
At what time t such that the transient vanishes?
How many period T of input signal does it take for it to be vanished?
I couldn't find any approach since it's difficult to find when the overlapping magnitude became steady. And that depends on the time constant, which results in asymptotic to 0 as t goes to infinity on each summation term.
Analytic expression is what I hope for.