  By analyzing data from a car-following experiment, it is shown that drivers
control their car by a simple scheme. The acceleration $a(t)$ is held
approximately constant for a certain time interval, followed by a jump to a new
acceleration. These jumps seem to include a deterministic and a random
component; the time $T$ between subsequent jumps is random, too. This leads to
a dynamic, that never reaches a fixed-point ($a(t) \to 0$ and velocity
difference to the car in front $\Delta v \to 0$) of the car-following dynamics.
The existence of such a fixed-point is predicted by most of the existing
car-following theories. Nevertheless, the phase-space distribution is clustered
strongly at $\Delta v=0$. Here, the probability distribution in $\Delta v$ is
(for small and medium distances $\Delta x$ between the cars) described by
$p(\Delta v) \propto \exp(-|\Delta v|/\Delta v_0)$ indicating a dynamic that
attracts cars to the region with small speed differences. The corresponding
distances $\Delta x$ between the cars vary strongly. This variation might be a
possible reason for the much-discussed widely scattered states found in highway
traffic.
