Chemistry Reference
In-Depth Information
X
N
a
k
r
k
h
k
.
C
a
k
.r
k
C
1//
1
C
1
D
0:
(5.38)
m
k
C1
T
k
p
k
k
D
1
In the general case computational methods can be used to locate the roots. In order
to obtain analytic results we will consider the case of symmetric firms, when a
k
a;r
k
r;h
k
h;T
k
T;m
k
m and so p
k
p. In both concave and isoelastic
cases
1<r
0;a > 0 and h>0. Notice that in the isoelastic case at most one
firm can have a positive r
k
value, but in the symmetric case all firms would have
positive derivatives r
k
, which is impossible. Then (5.38) becomes the polynomial
equation
mC1
.
C
a.r
C
1//
1
C
T
p
Narh
D
0:
(5.39)
Our results can be summarized in the following theorem.
Theorem 5.3.
Assume symmetric firms and that
h
1=N:
The equilibrium with
information lag is locally asymptotically stable if
T
D
0;
or
T>0
and
m
D
0:
If
T>0
and
m
D
1;
then
(i) The equilibrium is locally asymptotically stable, if
Nhr
C
8.r
C
1/ > 0
.
8
(ii) The equilibrium is locally asymptotically stable for all
aT
ยค
1
C
Nh
,when
Nhr
C
8.r
C
1/
D
0
.
(iii) Otherwise the equilibrium is locally asymptotically stable if
aT < .aT/
1
or
aT > .aT/
2
;
where
.aT/
1
and
.aT/
2
..aT/
1
<.aT/
2
/
are given in (5.43), and the equilibrium
is unstable, if
.aT/
1
<aT<.aT/
2
:
At the critical values
aT
D
.aT/
1
, and
aT
D
.aT/
2
Hopf bifurcations occur giving
the possibility of the birth of limit cycles around the equilibrium.
Proof.
Assume first that T
D
0, that is, there is no time lag. Then (5.39) becomes
C
a.1
C
r.1
Nh//
D
0;
with the only root
D
a.1
C
r.1
Nh//.If f
k
is a reasonable approximation
of f ,thenh
'
1,soNh
1 implying that <0and the equilibrium is locally
asymptotically stable.
Assume next that T>0and m
D
0. Then (5.39) is reduces to the quadratic
equation
2
T
C
.1
C
a.r
C
1/T/
C
a.1
C
r.1
Nh//
D
0:
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