Chemistry Reference
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2.A
c
2
/
2
.N
C
1/
p
.N
C
1/.N
1/.A
c
2
/
:
'
2
D
As a numerical example, consider A
D
16;c
1
D
10 > 8
D
c
2
D
:::
D
c
N
.Then
using the expressions given in (2.37) we obtain the unique equilibrium
7
N
p
8N
2
9
x
1
D
C
14N
4
;
x
2
D
:::
D
x
N
D
p
8N
2
C
14N
4
;
which shows that for N>7 firm 1 stops producing and we have a boundary
equilibrium
r
8
N
2
1
:
For N
D
7, total equilibrium industry output becomes Q
D
p
6 and the correspond-
ing equilibrium price is f. Q/
D
10; which obviously equals the marginal cost of
firm 1. However this is not the end of the story. Figure 2.17 shows a bifurcation dia-
gram of outputs obtained for the model (2.36) with speeds of adjustment a
1
D
0:5,
a
2
D
0:4, capacity limits L
1
D
L
2
D
0:4 and bifurcation parameter N in the range
Œ3;10 (notice that L
1
C
.N
1/L
2
x
1
D
0 and
x
2
D
:::
D
x
N
D
A in the whole range, so that non-negativity of
prices is ensured). The bifurcation diagram of Fig. 2.17 confirms that x
1
goes to zero
for N>7.However,forN
D
10 a positive stable cycle of period 2 characterizes the
long-run dynamics and it appears that firm 1 resumes production. Mathematically,
this stable cycle is created through a border collision bifurcation between N>9
and N>10, and at its creation it coexists with the stable boundary equilibrium. So,
0.4
x
1
0
0.4
x
2
0
3
4
5
6
7
8
9
10
N
Fig. 2.17
Example 2.5; quadratic price and linear cost function. The semi-symmetric case. Bifur-
cation diagrams of x
1
, x
2
with respect to the number of firms N. Illustrating how x
1
can go to zero
for some values of N
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