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
;
2˛
Œ.˛
C
1/c
1
.x
1
C
x
2
/
˛
1
2˛
Œc
1
.˛
C
1/.x
1
C
x
2
/
˛
1
1
1
J.x
1
;x
2
/
D
2˛
Œc
2
.˛
C
1/.x
1
C
x
2
/
˛
1
1
2˛
Œ.˛
C
1/c
2
.x
1
C
x
2
/
˛
1
1
2
1
computed at the equilibrium becomes
0
2˛
h
.˛
C
1/c
1
c
2
1
i
2˛
h
c
1
.˛
C
1/
2
˛
c
2
1
i
1
1
2
1
2
˛
1
c
1
C
c
1
C
@
2˛
h
c
2
.˛
C
1/
2
˛
c
2
1
i
2˛
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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