Chemistry Reference
In-Depth Information
After adding these two equations, we obtain
2 ˛
c 1 C c 2 :
.x 1 C x 2 / ˛
D
This equilibrium condition shows us that a realistic non-vanishing steady state exists
only if ˛<2. We can use this equation to substitute, for example, x 2
D x 1 C
2 ˛
c 1 C
1=˛
in one of equations (5.57), from which we get the unique non-vanishing
equilibrium x D . x 1 ; x 2 /, with
c 2
2 ˛
c 1 C c 2
˛ c 2 c 1 .1 ˛/
c 1 C c 2
;
1
˛
x 1
D
(5.58)
2 ˛
c 1 C c 2
˛ c 1 c 2 .1 ˛/
c 1 C c 2
:
1
˛
x 2
D
This equilibrium is positive if ˛>1 min f c 1 =c 2 ;c 2 =c 1 g . The study of the stability
of this equilibrium is particularly easy, because the Jacobian matrix for the map
(5.56) given by
2
;
Œ.˛ C 1/c 1 .x 1 C x 2 / ˛
1
Œc 1 C 1/.x 1 C x 2 / ˛
1
1
1
J.x 1 ;x 2 / D
Œc 2 C 1/.x 1 C x 2 / ˛
1
1
Œ.˛ C 1/c 2 .x 1 C x 2 / ˛
1
1
2
1
computed at the equilibrium becomes
0
h C 1/c 1
c 2 1 i
h c 1 C 1/ 2 ˛
c 2 1 i
1
1
2
1
2
˛
1
c 1 C
c 1 C
@
h c 2 C 1/ 2 ˛
c 2 1 i
h C 1/c 2
c 2 1 i
A
J.x 1 ; x 2 / D
1
1
2
1
2
˛
c 1 C
c 1 C
and has the simple characteristic equation
1 C ˛
2
˛
4 D 0:
2
C
Hence the eigenvalues are 1 D 1=2 and 2 D ˛=2. This implies that the equilibrium
.x 1 ; x 2 / is locally asymptotically stable for each ˛ in the range 0<˛<2.
This contrasts with the results obtained for the best reply dynamics with complete
knowledge of the demand function as discussed by Puu (1991), in Example 3.4 with
˛ D 1. It has been shown there that the unique Nash equilibrium is given by (5.58)
with ˛ D 1,thatis
.c 1 C c 2 / 2 .
c 2
.c 1 C c 2 / 2 ;
c 1
x D .x 1 ; x 2 / D
(5.59)
Furthermore, as we have demonstrated in this example the local stability of this
equilibrium under the best reply dynamics depends on the ratio between the marginal
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