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Room 3
100
60
75
Exit
50
25
40
0
20
20
20
Room 1
Room 2
40
40
60
Fig. 5. Static floor field (right) for a rather complex geometry (left).
k S , the coupling to the static field, can be viewed as a measure of the knowl-
edge about the location of the exit. A large k S implies an almost deterministic
motion to the exit on the shortest possible path. For vanishing k S , the individ-
uals will perform a random walk and just find the exit by chance. So the case
k S 1 is relevant for processes in dark or smoke-filled rooms where people
do not have full knowledge about the location of the exit. For fixed sensitivity
parameter k D , the evacuation time decrease monotonically with increasing k S
(see Fig. 6(a)). k S can be interpreted as some kind of inverse temperature for
the degree of information about the inanimate surrounding.
40000
7000
ks=0.4
ks=1.0
ks=10.0
kd=0.0
kd=10.0
6000
30000
5000
20000
4000
10000
3000
0
2000
0
2
4
0
2
4
6
8
10
ks
kd
Fig. 6. Averaged evacuation times for a large room with an initial particle density of
ρ =0 . 3 and δ =0 . 3, α =0 . 3 for (a) fixed k D , and (b) fixed k S .
The parameter k D controls the tendency to follow the lead of others. A large
value of k D implies a strong herding behaviour as observed in panics [18]. For
fixed k S (see Fig. 6(b)), the evacuation times converge to maximal values for
 
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