Intuitions for Special Relativity
Special Relativity is a theory of space and time that describes how space and time are affected by motion. It follows the natural consequences of the constancy of the speed of light in all reference frames. The special in special relativity refers to the fact that it is a special case of general relativity: situations when objects are moving at constant velocities in a vacuum.
The speed of light is constant in all inertial reference frames, regardless of the motion of the observer or the source of the light. This is a fundamental postulate of special relativity.
Inertial reference frames
The first key insight is to approach the problem with the understanding that motion is relative to the inertial reference frame of the observer. In any situation, we can always choose an inertial reference frame in which one object is at rest and everything else is moving relative to it.
Ash
is a train conductor, and Brock
is waiting for the train to arrive at the
station. The train is moving at speed relative to the station.
From Brock
’s perspective:
- The train is moving towards the station at speed .
- The station is at rest.
Ash
and Brock
experience the world from their respective inertial reference
frames. Each of their observations are true, and they are all valid.
The second key insight is to understand that the speed of light is constant for every observer regardless of their motion or the source of the light.
Here we will ignore the effects of light passing through a medium for the sake of brevity, but know that the physics still holds. This video provides an excellent intuition about how the speed of light can be constant and also how light moves “slower” through a medium.
TLDW; The speed of light is constant in any medium. The “slower” speed is a sort of illusion caused by “phase kicks” between the light and the medium.
The speed of light is constant
The first postulate of special relativity is that the speed of light is constant in all inertial reference frames.
Another way to think about this is to consider a perfect “light clock” that each observer watches. The light clock consists of a photon that bounces between two mirrors once per second. Since the speed of light is constant in all inertial reference frames, an observer watching their clock will always observe the photon moving at the speed of light, .
Let’s give a light clock to Ash
and Brock
and see what happens.
Ash
is a train conductor, and Brock
is waiting for the train to arrive at
the station. The train is moving at speed relative to the station.
Ash
holds a light clock called A
. Brock
also holds a light clock called
B
. Ash
and Brock
both observe the speed of light in their own light clocks
and in each other’s light clocks.
From Ash
’s perspective:
- The station is moving towards the train at speed .
- Light clock
A
is at rest. - The photon in the light clock
A
is moving at speed . - Light clock
B
is moving towards the train at speed . - The photon in the light clock
B
is moving at speed .
From Brock
’s perspective:
- The train is moving towards the station at speed .
- Light clock
A
is moving towards the station at speed . - The photon in the light clock
A
is moving at speed . - Light clock
B
is at rest. - The photon in the light clock
B
is moving at speed .
Light clock A
is moving at speed relative to Brock
, but he observes the
photon inside to be moving at speed , not . How can this be?
It is natural to pause at this point and ask “how can this be true?” or “why is the speed of light constant?”—stop yourself. For a moment, accept that it is true and instead we should ask “what must happen for this to be true?” Trust me, it actually makes more sense to approach the problem this way.
The emergence of time dilation
Let’s follow the math and see what happens when we assume all of the observations are true.
distance traveled in one second
Brock * 0 m
Ash *--* 100 m
Light *~~~~~~~~~~~~~~~~~~~~~~~~~~~~~* 300_000_000 m
In order for the speed of light to be constant in both cases, the elapsed time must be different for each observer!
The time experienced by an observer at rest is called its proper time. Remember that it an observer only ever sees themself at rest. The proper time is always “normal” for the observer. (This is where the twin paradox comes from.)