Why is ct used as the fourth dimension in Special Relativity?

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Discussion Overview

The discussion centers on the use of ct as the fourth dimension in Special Relativity, exploring its implications for the representation of spacetime. Participants examine the reasons for using ct instead of just t, including dimensional consistency, convenience in calculations, and the relationship between time and spatial measurements.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants note that using ct in Minkowski diagrams allows for worldlines of light to be represented at 45 degrees, which is visually appealing and mathematically convenient.
  • It is proposed that both space and time components in spacetime must have identical dimensionality, leading to the use of ct to maintain consistency.
  • Others argue that while ct is convenient, it is not strictly necessary, as calculations can be performed using t with appropriate unit choices, such as light-seconds.
  • Some participants express a preference for using t over ct, suggesting that measuring time may be more fundamental than measuring length.
  • There is a contention regarding the necessity of matching dimensions in spacetime metrics, with some asserting that it is essential for constructing Minkowski and other metrics, while others challenge this view.
  • Participants discuss the nature of time measurement, with examples such as light-clocks and radar measurements being used to illustrate different perspectives on how time can be measured independently of spatial intervals.
  • One participant introduces the idea that if t were used instead of ct, the maximum velocity would be 1 instead of c, linking this to the properties of the 4-velocity vector.
  • Another participant suggests that time intervals can be recorded without spatial measurements, using examples like observing a flashing light.
  • There is a discussion about the relationship between time and spatial measurements, with references to periodicity and the nature of clocks in relativity.

Areas of Agreement / Disagreement

Participants express a mix of agreement and disagreement regarding the necessity and implications of using ct as the fourth dimension. While some support the idea of dimensional consistency, others question its necessity and explore alternative viewpoints on time measurement.

Contextual Notes

Some arguments rely on specific definitions and assumptions about dimensionality and measurement, which may not be universally accepted. The discussion also touches on the implications of different unit systems and their effects on the interpretation of spacetime.

NanakiXIII
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I'm looking for an explanation as to why a lot of results of Special Relativity are described using [tex]ct[/tex] as a fourth dimension instead of just [tex]t[/tex]. Now, I understand that using [tex]ct[/tex] in a Minkowski diagram with identically scaled axes will cause worldlines of light to angle at a nice 45 degrees, and I've seen how [tex]x-ct[/tex], if I remember correctly, is Lorentz invariant, as well as some other cases where it does seem useful to use ct, but the general nature of this usefulness eludes me. Could anyone tell me more about this?
 
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NanakiXIII said:
I'm looking for an explanation as to why a lot of results of Special Relativity are described using [tex]ct[/tex] as a fourth dimension instead of just [tex]t[/tex].
Each component in the decomposition of spacetime in "space" and "time" components must have an identical dimensionality. Both the "space" and "time" components use a measure of "distance". Hence: ct = m/s * s = m

By the way the decomposition in "space" and "time" is observer dependent in relativity.
 
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Also note that with a suitable choice of units, you can use simply t instead of ct in calculations. For example, measure time in seconds and distance in light-seconds (the distance light travels in one second).
 
jtbell said:
Also note that with a suitable choice of units, you can use simply t instead of ct in calculations. For example, measure time in seconds and distance in light-seconds (the distance light travels in one second).
Yeah, but (ct,x,y,z) is easier to write and read than (t,x/c,y/c,z/c)
 
jtbell said:
Also note that with a suitable choice of units, you can use simply t instead of ct in calculations. For example, measure time in seconds and distance in light-seconds (the distance light travels in one second).
Interestingly, in a way we already do that since the meter is defined as the length of the path traveled by light in vacuum during a time interval of 1/299,792,458 of a second. :)
 
DaleSpam said:
Yeah, but (ct,x,y,z) is easier to write and read than (t,x/c,y/c,z/c)

Conceptually, I prefer the latter.
In some sense, measuring a time seems more fundamental than measuring a length. (Radar measurements use a clock.)
In addition, the latter form lends itself more easily to the analyzing the Galilean limit.
 
MeJennifer said:
Each component in the decomposition of spacetime in "space" and "time" components must have an identical dimensionality.

Why?

I don't see the (general) need for any such requirement - but scaling time by c does provide a convenient notation within Minkowski space.

Regards,

Bill
 
Antenna Guy said:
Why?

I don't see the (general) need for any such requirement
One would not be able to construct a Minkowski metric or more advanced metrics in curved spacetimes when the dimensions do not match.

Antenna Guy said:
- but scaling time by c does provide a convenient notation within Minkowski space.
Time is not scaled by c, since both dimensions are different, e.g. s * m/s.
 
robphy said:
Conceptually, I prefer the latter.
In some sense, measuring a time seems more fundamental than measuring a length. (Radar measurements use a clock.)


Eh? I think you've got that precisely the wrong way round, imo. I can't think of a single example of how one could measure an interval of time without *first* having to measure a spatial length.
 
  • #10
shoehorn said:
Eh? I think you've got that precisely the wrong way round, imo. I can't think of a single example of how one could measure an interval of time without *first* having to measure a spatial length.

Refer to "The Interval" chapter (around p.70) in Geroch's General Relativity from A to B
http://books.google.com/books?id=Uk...ty+a&sig=ZwKt1KmtQ_UUElxeSrA1d0iDiTI#PPA72,M1
(see p.72)

The key to a clock is a periodicity.
To perform radar measurements, one makes use of light rays and clocks.
 
  • #11
robphy said:
Refer to "The Interval" chapter (around p.70) in Geroch's General Relativity from A to B
http://books.google.com/books?id=Uk...ty+a&sig=ZwKt1KmtQ_UUElxeSrA1d0iDiTI#PPA72,M1
(see p.72)

The key to a clock is a periodicity.
To perform radar measurements, one makes use of light rays and clocks.

Care to give me an example of a measurement of an interval of time that can be made without measuring a spatial interval then?
 
  • #12
shoehorn said:
Care to give me an example of a measurement of an interval of time that can be made without measuring a spatial interval then?

In a light-clock, one can declare a given separation of mirrors [without "measuring it"] to define a standard tick of this clock. (Allow two mirrors to travel inertially in the same direction. Changing the separation effectively changes the resolution of the clock.) Again, the key is [regular] periodicity of clock. Instead of the light-clock, one could crudely use your heartbeat to measure time [a la Galileo].

The point is that a "wristwatch" time measurement, unlike a "meterstick" measurement that must be extended out, is local to the observer's worldline. This has conceptual advantages in relativity.

From a more practical point of view, distances to remote objects are not done by extending a ruler out to meet it. Radar using light-rays is often used.
 
  • #13
As strange as it sounds... If t was used instead of ct, then the maximum velocity would be 1 instead of c. Of course, I think this is actually done when the speed of light is arbitrarily set to 1 in geometrized units. This follows from the fact that the magnitude of the 4-velocity vector must equal c (or 1) at all times. Where v = 0, t = 1, and so the entire magnitude is due to motion through time (ct = c). At v = c, t = 0, and so the entire magnitude is due to motion through space (ct = 0).
 
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  • #14
shoehorn said:
Care to give me an example of a measurement of an interval of time that can be made without measuring a spatial interval then?

Watch a flashing light.
Record the time of flash one.
Record the time of flash two.
You just recorded a time interval with no spatial measurements.

This also gets to the essence of time measurement.
It's matching world events to clock (reference) events.

Like matching an object to a ruler to measure length.
 
  • #15
shoehorn said:
Care to give me an example of a measurement of an interval of time that can be made without measuring a spatial interval then?

I think the duration of a photon (single complete wave [clarification: passing through a plane of reference]) would constitute both a time and space interval measured by a clock. f=1/t, l=c*t

Conversely, the spatial measurement of one period of a standing wave (segment of a continuous stream of photons) can be used to calculate t.

Regards,

Bill
 
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