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The input and output of a stable network are related via the following equation. $$\frac{d^2y(t)}{d(t)} + \frac{2*dy(t)}{d(t)} + 10y(t) = \frac{dx(t)}{d(t)} + x(t)$$

x(t) = input, y(t) = output, u(t) = unit function. The input is $$\frac{3u(t)}{e^t}$$

I want to find the zero-state output. Now I have the transfer function as $$\frac{iw + 1}{-w^2 +2(iw) + 10}$$

But I'm not quite sure where to proceed from here. My intuition is to move the transfer function to the time domain through fourier transform, but I'm not sure how I would use that to continue the problem.

Jonathan
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  • u(t) is the standard unit function. Same all the time. – Jonathan Mar 04 '16 at 09:44
  • I am sorry, I do not know any such "standard unit function". The problem is easily solved if you are able to find a function $\phi(t)$ which satisfies $\phi''(t) + 9\phi(t) = 3u'(t)$. – Hugo Mar 04 '16 at 09:48
  • Unit function -> https://en.wikipedia.org/wiki/Unit_function @Hugo – Jonathan Mar 04 '16 at 09:51
  • How did you arrive at that equation? – Jonathan Mar 04 '16 at 09:51
  • Yes, it will still be the same thing. Sorry about that confusion. – Jonathan Mar 04 '16 at 09:55
  • It is not the same thing, since you can not differentiate the function $u(0) = 1$, $u(t) = 0$ elsewhere. Are you looking for a weak solution in the sense of $L^2$, maybe? Got to go to lesson, I will look at the problem later... – Hugo Mar 04 '16 at 09:58
  • I would suggest to use the Laplace transform wrt. the time variable. Since the time integration is from 0 to infinity things are al right if you assume that $u(t)$ is continuous in 0 from the right. – Urgje Mar 04 '16 at 11:52

2 Answers2

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First find the solutions of $y''(t) + 2y'(t) + 10y = 0$. Passing to the characteristic polynomial, it has roots $\lambda_{1,2} = -1\pm 3i$, so every function of the form $$ y_0(t) = Ae^{-t}e^{i3t} + Be^{-t}e^{-i3t} $$ solves the homogenous equation.

Now consider the non-homogenous one. If $u$ is differentiable you get $$ x'(t) + x(t) = 3u'(t)e^{-t}-3u(t)e^{-t}+3u(t)e^{-t} = 3u'(t)e^{-t}. $$

I seek for particular solutions $y(t) = a(t)e^{-t}$. So $y'(t) = a'(t)e^{-t}-a(t)e^{-t}$, $y''(t) = a''(t)e^{-t}-2a'(t)e^{-t} + a(t)e^{-t}$. Substituting into the equation you get $$ a''(t) + 9a(t) = 3u'(t). $$

If you know $u(t)$ there is some chance to solve it, and your solution will be $$ y_0(t) + a(t)e^{-t} $$ for some opportune constants $A,B$.

Hugo
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$$y''(t)+2y'(t)+10y(t)=x'(t)+x(t)$$ The Fourier transform of $y(t)$ will be denoted $\quad F_t[y(t)](\omega) = Y(\omega)\quad$ on a more compact writing.

$\quad F_t[y'(t)](\omega) = -i\omega Y(\omega)$

$\quad F_t[y''(t)](\omega) = -\omega^2Y(\omega)$

$\quad F_t[x(t)](\omega) =F_t[u(t)e^{-t}](\omega) = \frac{1}{\sqrt{2\pi}(1-i\omega) }$

$\quad F_t[x'(t)](\omega) = F_t[\frac{d}{dt}\left(u(t)e^{-t}\right)](\omega) =-i\omega F_t[u(t)e^{-t}](\omega) = \frac{-i\omega}{\sqrt{2\pi}(1-i\omega) }$

$$-\omega^2Y(\omega)-2i\omega Y(\omega)+10Y(\omega)=\frac{-i\omega}{\sqrt{2\pi}(1-i\omega) }+\frac{1}{\sqrt{2\pi}(1-i\omega) } = \frac{1}{\sqrt{2\pi}}$$

$$Y(\omega)=\frac{1}{\sqrt{2\pi}\left(-\omega^2-2i\omega+10 \right)}$$

The inverse Fourier transform leads to :

$$y(t)=\frac{1}{3}e^{-t}\sin(3t)u(t)$$

Zero state output : $\quad y(0)=0$

JJacquelin
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