1) Movie 1 (:20) This is a view of constant acceleration through a starfield. This headlight effect is how space travel at near-light speeds would appear, contrary to the special effects in Star Trek and Star Wars universes. But in this movie and in reality, C, the speed of light, is not and cannot be exceeded.
2) Movie 2 (:09) The sphere's delayed shadow - cast earlier when it was in a different position . Light reflected off the sphere is Doppler-shifted, appearing a different colour.
3) Movie 3 (:12) In a world where the speed of light is only five meters per second, a flickering streetlamp does not instantly illuminate its surroundings; rather it casts expanding shells of light into space around it.
4) Movie 4 (:09) A flash does not instantly illuminate the interior, but slowly travels through the tram. As the light must travel out and back, the illuminated region moves outward at half the speed of light.
5) Movie
5 (:19) The streetlamp turns on and off. Even though the wall
is closer to the streetlamp than the ground, parts of the ground
are lit first. To understand this, we must consider not only the
distance of the surface to the streetlamp, but also the distance
to the eye.
Now, a schematic world where we can track the path of individual
photons. As light makes the trip between the lamp, the surface
and the eye, the light which follows the shortest path will reach
the eye first. As the direct route between lamp and eye is shorter
and thus faster, we see the lamp turn on before anything else
is lit. The route to the wall is longer, so it appears later.
6) Movie 6 (1:24) We now look at moving objects. A tram moving close to the speed of light displays many effects, becoming distorted, and changing colour and brightness. Its shadow also falls at an unusual angle. The effects of distortion,the Doppler effect and intensity can be separately treated, so for the moment we "enhance" our image, correcting it so only distortion appears. This correction occurs within the large rectangle. The tram appears to have been shortened, sheared (with the two ends no longer perpendicular to the sides), and slightly bent. To explain the shear, we again move to the schematic world. As the tram moves close to the speed of light, it is shortened by the Lorentz contraction. As the back side of the tram is further from us than the front side, the light takes longer to reach us. Thus the light we see at any one time must have left the front and back surfaces of the tram at different times. As the tram is moving at a speed comparable to that of light, this time delay also means that we see the front surface of the bus later and further along the track than the back surface, thus we see a shear. This effect is known as the Terrell rotation, as the degree of contraction and shear combine to the exact proportions that a rotation would produce. However, this effect is dependent on the object appearing small and distant. If we are too close to the object it's different parts will appear rotated by different amounts, sometimes resulting in extreme distortion.
7) Movie
7 (:16) Moving with the tram, the world around us shows the
same distortions. This is the Terrell effect. When generalized
to an entire view its known as relativistic aberration.
Also, when we move with the tram, it seems to move faster - time
dilation at work.
8) Movie
8 (:50) To understand relativistic aberration, consider the
ordinary "real" world. When a vehicle moves through
rain, to the vehicle the rain seems to fall at an angle. In an
analogous process, photons "falling" into the camera
appear to come from different angles as the camera moves at different
speeds. As the camera moves faster and faster, photons enter it
at increasingly steeper angles. This means that things that would
appear behind us if we were in their rest frame are wrapped forward
into our field of view. The same, reversed, applies to outgoing
photons. This gathering of light into a narrow circle in the direction
of travel creates a headlight effect forward and a dimming effect
behind.
9) Movie 9 (:15) Terrell rotation or relativistic abberation also explains why the tram appears small as it approaches us, and large as it recedes from us, as seen here in two different views of the tram from the street.
10) Movie
10 (1:19) Accelerating, we see the distortion increasing,
and the sun and clouds rotating into our field of view. The rectangle
in the center of the screen is a computer correction which leaves
out Doppler and intensity effects to improve clarity.
To see what is happening all around us, we use a mercator projection;
a map of everything we can see around us. The map is made by "unwrapping"
a sphere and stretching the areas at the poles to make the map
flat. This is the same kind of common map of the Earth that shows
Greenland stretched to the size of South America. This kind of
map obviously creates distortions of its own which have nothing
to do with relativity. But using this view may help you to understand
the abberation effects of relativity.
Accelerating, we can see that objects behind us increase in size.
Even though we are moving away from the houses at the end of the
street, at the left and right edges, the houses grow larger. The
patch of blue sky overhead shrinks to a small circle ahead of
us. And the clouds and sun rotate into that small circle, appearing
distorted but maintaining their positions in the shrunken scene.
11) Movie
11 (0:49) Returning to the tram we now consider the colour
shift. Even at low speeds, ten percent of the speed of light,
objects change their colour significantly. Lamp posts ahead look
green, but behind they look red. This is the Doppler shift at
work.
Just as the direction of motion of photons change when the camera
moves, so do the frequencies which we perceive as colour. Objects
we move towards appear blueshifted. Objects we move away from
appear redshifted. As we go faster, the effect becomes extreme,
and we see a rainbow effect as any sharp spectral features pass
through the visible band.
This is the cause of red-shift, an observation astronomers made
which showed nearly all stars in the universe are moving away
from us and each other.
12) Movie
12 (:39) Without colour correction, the world ahead turns
blue, and the sun darkens as visible light shifts into ultraviolet
and above. This is matched by a reddening behind. A rainbow ring
appears in the sky as the blue colour is shifted through the regions
of the spectrum our eyes detect as red and green.
We only see light in a narrow range, ROY G BIV, and high speeds
can easily shift visible light above or below visible range.
Doppler shift effects are seen again in this mercator projection.Though
the distribution of energy in spectra means that the Doppler effect
will sometimes make an object look darker, this is not the only
effect changing the brightness of the tram.
13) Movie
13 (:40) At high speeds, extreme intensity effects occur,
with most parts of the scene too dark or bright to see. Aberration
concentrates photons in front and spreads them out behind, so
ahead looks bright and behind looks dim.
Time dilation means the shutter of a moving camera is open longer
- collecting more light and making the image brighter.
This effect means that moving light sources concentrate along
their direction of motion - front and back lights are equal when
stationary.
Accelerating without computer correction, relativity effects swiftly
overtake us. The scene changes colour and becomes very bright
or too dark to make out. At high velocity, the camera is hit by
a beam of high energy radiation.
14) Movie 14 (:11) A subtle effect occurs with shadows. The shadow of the moving tram lies at a steep angle compared with that of other objects. Light moves slowly here, so shadows are not instantaneous. The effects of the blocking take time to reach the surface.
15) Movie 15 (:19) As the tram accelerates, electromagnetic radiation enters more and more directly from in front. This effect, when combined with the doppler shift towards shorter wavelengths of higher frequencies, would produce a lethal high intensity beam of gamma-rays. This is another consequence of traveling near the speed of light usually ignored in science fiction.
16) Movie
16 (:20) Here is the same intensity effect shown in mercator
projection. Note that any information from the outside world enters
through a very restricted kind of porthole.
How would a message carried by laser beam reach the tram ?
How could a message be sent from the tram to the street ?
17 + 18) Movie
17 & 18 (:27) Moving light sources also cast unusual shadows
because they cast different parts of the shadows from different
positions at different times. Note the shadow's curving shape
on the ground. Why does this occur ?
And although of equal intensity, why does the headlight appear
brighter than the tail light as seen from above?
19) Movie
19 (:58) These effects can be seen in the real universe. But
the real speed of light is very fast, three hundred thousand kilometers
per second. Because relativity effects are most pronounced at
very high speeds, the real visual effects of relativity must occur
on a much larger scale than the simulations you've just seen.
For example : light delay in the "light echoes" of exploding
stars, the Doppler shift of fast-moving astronomical bodies, and
the headlight effect in the incredible brightness of gas jets
directed towards us.
Because light is normally so fast, humans do not notice these
effects. Someday, it may be possible, though not practical, to
build a space ship with today's technology that could travel fast
enough to see these effects directly.
Visualising Special Relativity 7 minutes
21) Movie
21 (:49) A trip down a highway without any relativistic effects.
Note that we started from rest, and accelerate uniformly. On the
left, is an unusual speed limit sign. It shows that c, the speed
of light is only one meter per second, or about as fast as a person
walks. The speed of light in our universe is very very fast, which
is why relativistic effects are much more difficult to observe.
These effects, although measuarable at slower speeds with sensitive
equipment, really become noticeable at speeds close to the speed
of light.
Also note the position and orientation of the structures in the
desert. In the next videos , the speeds, accelerations, and positions
of objects will be exactly the same, but visual relativistic effects
will be added.
22) Movie 22 (:49) Let's look at relativistic
rotation. As we accelerate, the angular compression creates an
initial impression of backwards motion.
At the top right is the camera speed relative to the scene, given
as a decimal fraction of the speed of light. Although acceleration
is constant, the number changes less and less as we get closer
and closer to c, the speed of light.
The number at bottom left is the gamma factor, the degree of relativistic
effects. This number starts at 1 and increases as we approach
c.
At bottom right a bird's eye view shows the camera position on
the highway.
As we pass the sign, it seems to rotate. This can be viewed as
a Terrell rotation, or as angular aberration keeping the sign
in our field of view as we pass it. Look at the difference between
our actual postion as viewed from above on the lower right, and
our apparent position. The back walls of the building are also
visible, and extreme distortion is visible on all the objects.
The sky shrinks down to the vanishing point.
23) Movie 23 (:49) We now turn on Doppler
shifting with aberration. The desert is blueshifted ahead, causing
a rainbow effect. As the sky is blueshifted, it drains of visible
colour. The opposite happens at the edges of the image, - the
sky takes on a reddish hue and the road is drained of colour as
the red desert shifts into the infra-red.
Visible light can be shifted out of visible range entirely. If
we recede rapidly from an object, its light will be shifted into
the infrared, producing "red-shift," an observation
astronomers made showing that most galaxies in the universe are
moving away from us.
But approaching, light is blueshifted, even into high frequency
gamma-rays, very unhealthy for speedy travellers without shielding.
24) Movie 24 (:49) With full relativistic
effects the image turns monotone, with objects near the edge of
the screen darkened, and the center brightly illuminated.
These three relativity effects combine here to produce a very
dangerous beam of high frequency radiation aimed directly at the
traveller. Incoming radiation from all directions is rotated more
and more to the front, and is doppler shifted to higher and higher
frequencies.
And as we speed close to light speed, time frames stretch. A camera
shutter set to open for one second on a very fast passing spaceship
would take in much more radiation than if it were on the ground
next to you, even with other relativity effects ignored.
25) Movie
25 (:48) The Terrell effect can be shown with this cube. Doppler
and intensity effects are off. Note the orientation of the cube
change. Compare its apparent position with the actual position
indicated at the lower right. We see the cube as it was, catching
up with photons.
However, these distinctions are meaningless. Even in this universe,
nothing exceeds the speed of light, even when bending, so for
light to travel in a straight line, it would have to exceed its
own speed : impossible. Reality is the distorted cube, and the
bird's eye view is from outside this universe.
On the highway, objects rotated more due to our acceleration.
Since we move past the cube at a constant speed, rotation is constant.
In space flight, effects would also be constant, because spaceships
coast more than accelerating by firing rockets.
26) Movie 26 (:48) If we fly through
the cube at a constant speed, the structures Terrell rotate independently,
seeming to turn the cube inside out. Even when we have exited
the back of the cube, aberration keeps most of it in view.
Here's a few questions to think about :
How would this flythrough change if we started from rest and accelerated
through the cube ?
Once you are physically past the cube, if you were to shine a
laser light ahead, in the direction where you see the cube, where
would the beam end up ?
If you were to throw on the brakes and suddenly stop, what would
the cube look like ?
And how would it be possible to land on the cube itself ? Note
that by the time it appears the cube is closeby, you are completely
out the other side.
27) Movie 27 (1:05) Another interesting
property of the rotations produced by relativity is that it preserves
circles - that is, a sphere will always present a spherical outline
to any observer regardless of their relative motion. This is a
special property of circles, and does not apply to any other shape.
We see this demonstrated by orbiting a camera around the Earth
at a constant high speed. The camera's position can be seen from
above in the lower right hand corner of the screen. Though the
camera is very close to the surface, aberration wraps the Earth
into our forward field of view. But because we are so close to
the earth, we can see only a small portion of its surface so small
regions seem to bulge out and fill the sphere.
These effects are present even in our real world, although to
a much smaller extent because of the great speed of light. Satellites
and space shuttles and Global Positioning Systems all must account
for these effects.