In mathematics, the evolution of a differential equation is defined as a two-parameter mapping given by:
Φ
{\ displaystyle \ Phi}
x
′
(
t
)
=
f
(
t
,
x
(
t
)
)
{\ displaystyle x '(t) = f (t, x (t))}
Φ
t
,
t
0
x
0
: =
x
(
t
)
{\ displaystyle \ Phi ^ {t, t_ {0}} x_ {0}: = x (t)}
in which
In words: Evolution maps the value of any solution curve at the point in time to the value of the solution curve at the point in time . So it describes the further development of the solution starting from the starting point .
x
0
{\ displaystyle x_ {0}}
x
{\ displaystyle x}
t
0
{\ displaystyle t_ {0}}
x
(
t
)
{\ displaystyle x (t)}
t
{\ displaystyle t}
x
0
{\ displaystyle x_ {0}}
The evolution of the differential equation has the following properties:
Φ
t
0
,
t
0
x
0
=
x
0
{\ displaystyle \ Phi ^ {t_ {0}, t_ {0}} x_ {0} = x_ {0}}
d
d
τ
Φ
t
+
τ
,
t
x
|
τ
=
0
=
f
(
t
,
x
(
t
)
)
{\ displaystyle {\ frac {d} {d \ tau}} \ Phi ^ {t + \ tau, t} x | _ {\ tau = 0} = f (t, x (t))}
Φ
t
2
,
t
1
Φ
t
1
,
t
x
0
=
Φ
t
2
,
t
x
0
{\ displaystyle \ Phi ^ {t_ {2}, t_ {1}} \ Phi ^ {t_ {1}, t} x_ {0} = \ Phi ^ {t_ {2}, t} x_ {0}}
for ( transitivity ).
t
≤
t
1
≤
t
2
{\ displaystyle t \ leq t_ {1} \ leq t_ {2}}
In the case of autonomous differential equations , the start time is arbitrary. It then writes instead of simply and designated as phase flow .
x
′
=
f
(
x
)
{\ displaystyle x '= f (x)}
t
0
{\ displaystyle t_ {0}}
Φ
t
,
t
0
{\ displaystyle \ Phi ^ {t, t_ {0}}}
Φ
t
{\ displaystyle \ Phi ^ {t}}
Φ
t
{\ displaystyle \ Phi ^ {t}}
<img src="https://de.wikipedia.org/wiki/Special:CentralAutoLogin/start?type=1x1" alt="" title="" width="1" height="1" style="border: none; position: absolute;">