I am trying to derive an expression for the optimal level of consumption in the basic problem:
$ max \hspace{1cm} U_t = E_t \left[\sum_{s=t}^{\infty} \beta^{s-t} \left( C_s - a\frac{Cs}{2}^2 \right) \right] $
$ s.t \hspace{1cm} A_{s + 1} = A_s(1+r) + Y_s - C_s $
The problem leads to the Euler Equation:
$ E_t \left[ \frac{u'(C_s)}{u'(C_{s+1})} \right] = \beta (1+r)$
Assuming $\beta = (1+r)^{-1}$ we have:
$ E_t \left[ \frac{u'(C_s)}{u'(C_{s+1})} \right] = 1$
Which leads to:
$ C_s = E_t[C_{s+1}]$.
Iterating forward the BC and using the trasversality condition I derived the intertemporal BC:
$ \sum_{s=t}^{\infty} \frac{C_s}{(1+r)^{s-t}} = A_t(1+r) + \sum_{s=t}^{\infty} \frac{Y_s}{(1+r)^{s-t}} $
Now, how can I find an expression for $C_t$? If time were finite intuitively (I think) I would have:
$ C_t = \frac{1}{T - t}(A_t + \sum_{s=t}^{T} E_t [Y_s]) $
How do I deal with the infinite horizon to find and expression for $C_t$?
I was wondering if I can use the geometric series, something like:
$C_t \sum_{s = t}^{\infty} \left( \frac{1}{1+r} \right)^{s-t} = C_t \frac{1}{1 - \frac{1}{1+r}} = C_t\frac{1+r}{r} $