44
Chapter 1
A Closed-Form Solution
It is interesting to notice that, when the production function is
Cobb–Douglas and the saving rate is constant, it is possible to get a closed-form solution
for the exact time path of
k. Equation (1.28) can be written as
˙
k ·
k
−
α
+
(n +
δ) ·
k
1
−
α
=
s A
If we define
v ≡
k
1
−
α
, we can transform the equation to
1
1
−
α
· ˙
v +
(n +
δ) ·
v =
s A
which is a first-order, linear differential equation in
v. The solution to this equation is
v ≡
k
1
−
α
=
s A
(n +
δ)
+
[
k
(0
)]
1
−
α
−
s A
(n +
δ)
·
e
−
(1−
α) ·
(n+
δ) ·
t
The last term is an exponential function with exponent equal to
−
(1 −
α) ·
(n +
δ). Hence,
the gap between
k
1
−
α
and its steady-state value,
s A
/(n +
δ), vanishes exactly at the constant
rate
(1 −
α) ·
(n +
δ).
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