Chemistry Reference
In-Depth Information
L
Rx
()
x
Tx
()
aL
x
Ac
2 L
Ac
(
NBN
)
1
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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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