Chemistry Reference
In-Depth Information
L
Rx
()
x
Tx
()
aL
x
Ac
−
2
L
Ac
−
−
(
NBN
−
)
−
1
(
NB
−
Fig. 2.3
Example 2.3; linear inverse demand and cost functions and identical capacity constrained
firms. The piece-wise linear map T.x/and reaction function R.x/
equilibrium is either at the boundary of the feasible set Œ0;L or in the interior, and
if the equilibrium is stable. The definition of R..N
1/x/ implies that 0 cannot be
equilibrium, so the equilibrium x is either interior or equals L.
As usual, the steady states of the adaptive adjustment process are the equilibria of
the underlying game, since T.x/
D
x if and only if R..N
1/x/
D
x.However,
the equilibrium might be located on the boundary. We account for this possibility by
writing the unique equilibrium point as
B.N C1/
;L
o
. Its stability, under
the dynamic adjustment process governed by the iteration of the map T , depends on
the derivative of T , which has three segments with two different derivatives: 1
a
and 1
min
n
Ac
x
D
a.N
C
1/
2
. From the results of Appendix B we know that the equilibrium is
globally asymptotically stable of both
j
1
a
j
and
ˇ
ˇ
ˇ
ˇ
ˇ
ˇ
a.N
C
1/
2
1
are less than one,
which is the case if 0<a<
4
N
1
.
We now turn to the asymptotic dynamics of the production sequences gener-
ated by T if, (1) the number of firms in the industry changes, and (2) each firm
is capacity-constrained. Figure 2.4 depicts a bifurcation diagram of output x with
respect to the number of firms N obtained with the parameters A
D
16, B
D
1,
a
D
0:5, c
D
6 and L
D
1 (in all the numerical simulations in this subsection we
select the parameters such that NL
A=B in order to ensure non-negative prices).
Observe that as long as .A
c/=.B.N
C
1// > L,thatisN<9, each firm produces
C
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