Relativity visualized
## Space Time Travel |

The special theory of relativity describes space, time and motion. For relativistic effects to become noticeable, motion must occur at nearly the speed of light. Since the speed of light is in excess of a billion kilometers per hour, such motion is far beyond our everyday experience. With fast computers, however, the experience of motion at nearly the speed of light can be simulated. Here we present a simulation using a detailed three-dimensional model of the old city centre of Tübingen. In the simulation we reduce the speed of light in “virtual Tübingen” to 30 kilometers per hour: We can then ride a bike through the city at nearly the speed of light.

One of the fundamental statements of the special theory
of relativity is length contraction. From Albert Einstein's
seminal paper of 1905 on the special theory of relativity
(where *V* is the speed of light):

A rigid body that, when measured at rest, has the shape of a sphere, therefore in motion has - when observed from the frame at rest - the shape of an ellipsoid of rotation with the axes

While the *Y*- und *Z*-dimensions of the sphere (and therefore of
every rigid body of arbitrary shape) do not appear modified by the motion,
the *X*-dimension appears shortened by the factor
, i.e. the more the greater *v*. For *v* = *V* all moving
objects – observed from the frame “at rest” – shrink to two-dimensional
entities.

So should we image a fast moving object to look contracted in the direction of motion? Taken literally, Einstein's statement means just that. And this notion was in fact illustrated by the physicist George Gamov in his 1940 book “Mr. Tompkins in Wonderland” [2,3]. There he writes about a virtual world in which the speed of light is only 30 km/h, so that even a biker can move at nearly the speed of light. This biker sees the houses at the roadside allegedly as shown in figure 1, contracted in the direction of motion.

However, this picture is entirely wrong. It is wong because Gamov did not take the consequences of the finite speed of light into account. In everyday life we may to all intents and purposes pretend that the speed of light is infinite, since we are always concerned with much smaller velocities. But when a velocity close to the speed of light is involved, this is not justified any more. On the contrary, what we should see in this case would be substantially influenced by the fact that light propagates at a finite speed.

The view
that a cyclist going at nearly the speed of light
would “really”
have of houses on the roadside is shown in figures 2 to 4
(in the figure captions
we employ the usual symbol *c* for the reduced speed of light, too).
Figure 2 shows the houses as seen by an observer at rest or in slow
motion.

When moving by at nearly the speed of light,
a *measurement* of the shape of the houses would
reveal them to be contracted in length as described by Einstein.
A view of the contracted houses
according to Gamov is shown in figure 3.

But when the fast cyclist *looks* at the houses,
then she sees them rotated and distorted (figure 4).

Surprisingly, it has taken a long time to realize that an observer at nearly the speed of light must see her surroundings distorted. After all, it was in 1676 that the observations of Olaf Römer established that light propagates with a finite speed. But it was not until 1924 that Anton Lampa [4] described the visual effects for the first time. Later, the work of Roger Penrose [5] and James Terrell [6] was the starting point for a large number of investigations (see [7] for an overview over the literature).

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