I Questions concerning the geometry of spacetime

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The discussion centers on the geometry of a rectangle in a spacetime diagram, specifically questioning its area and whether it represents a 2D Euclidean space. It is established that the rectangle does not have an ordinary area but possesses a "spacetime area," which is defined by its timelike and spacelike sides. The rectangle is confirmed to be in Minkowskian geometry rather than Euclidean geometry, highlighting the need for a broader understanding of "area" in the context of spacetime. The conversation also emphasizes the distinct properties of temporal and spatial dimensions, particularly how they are measured differently. Overall, the complexities of spacetime geometry challenge conventional perceptions of shapes and areas in physics.
  • #61
Dale said:
I am not sure what you mean by “actual distance”. It is a spacetime interval. Why should it be anything other than what it is?
I meant spatial distance.
Dale said:
Spacetime intervals can be either timelike or spacelike. Timelike intervals are measured with clocks and spacelike intervals are measured with rulers. Either way the result of such a measurement can be reported in meters, regardless of the device used.
Yes, that makes sense.
Dale said:
This isn’t the geometrical view. In the geometrical view time is just another dimension. There is a future time direction and a past time direction but there is no time flow. If you draw a line on a page there is no sense that the page flows along the line. The line simply has some extent on the page without requiring the page to move under the line or the line to move on the page.
I agree. Yet we observe changes in the real world. The changes seem to be explained as time flowing by us/observation/consciousness or as we going through time.
 
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  • #62
student34 said:
However, I do not understand what is different about an "elapsed proper time along a world line" which you say can be real. Why are we taking its integral instead of just (-dtf^2)^(1/2)
In the context of special relativity, because the world line may not be a straight line (geodesic).

For example, one would not measure the length of a curving road in ordinary 2 dimensional Euclidean space by taking the square root of the sum of the squared difference between the endpoint coordinates. One would integrate along the path instead.
 
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  • #64
student34 said:
If I am understanding you correctly, you say that if we use the spacetime interval formula then we will get a negative squared spacetime interval between "time-like separated events"
Only in case of the (-+++) convention (##ds^2=-c^2dt^2+dx^2+dy^2+dz^2##), not in case of the (+---) convention (##ds^2=c^2dt^2-dx^2-dy^2-dz^2##). See for this also the 2nd part of posting #30 from @PeterDonis.

student34 said:
However, I do not understand what is different about an "elapsed proper time along a world line" which you say can be real. Why are we taking its integral instead of just (-dtf^2)^(1/2)
See:
https://en.wikipedia.org/wiki/Proper_time#In_special_relativity
 
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  • #66
student34 said:
if we use the spacetime interval formula then we will get a negative squared spacetime interval between "time-like separated events"
If you are using the appropriate signature convention, yes.

student34 said:
which I understand to be an imaginary number.
No. The sign of the squared interval is not taken into account when taking the square root. The sign of the squared interval just labels the interval as timelike or spacelike. It does not mean one of them corresponds to an interval that is an imaginary number.

(If you doubt this, consider that if we are using the timelike signature convention, then a spacelike squared interval is negative. Does that mean ordinary spatial distances are imaginary numbers? Of course not.)
 
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  • #67
student34 said:
I meant spatial distance.
A timelike interval is not a spatial distance.

student34 said:
Yet we observe changes in the real world.
Things change over space as well as time. So the fact that there is change in a particular direction in no way implies that anything is flowing.

student34 said:
The changes seem to be explained as time flowing by us/observation/consciousness or as we going through time
Certainly, that is a possible view which is compatible with the data. However, as I said before, it is not the geometrical view. In this thread you are asking about the geometrical view, so the non-geometrical view doesn’t belong in this thread. Not because it is inherently wrong, but it is just a topic for a different thread.

If you want to discuss time flowing instead of the geometrical view of time then let me know. I can easily close this thread and you can open a new one to discuss that instead.
 
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  • #68
Thanks everyone, it was another helpful discussion.

To see if I learned anything, I will make a closing statement about what I learnt. Please correct me if I am wrong.

I knew there were differences between spatial properties and the temporal properties. However, I did not know that the temporal dimension does not share the same property of spatial distance as the spatial dimensions.

Having said that, I am still quite curious and perplexed about what this temporal dimension is, and how it can share so many spatial properties such as curvature, spatially measurable and intersect with spatial dimensions, yet does not have spatial distance.
 
  • #69
student34 said:
I knew there were differences between spatial properties and the temporal properties. However, I did not know that the temporal dimension does not share the same property of spatial distance as the spatial dimensions.
You still don't seem to have the right conceptual scheme. This might be because you don't even seem to have the right conceptual scheme for ordinary Euclidean geometry in ordinary Euclidean space, so let's start with that first.

What you are calling "spatial distance" is not a property of "spatial dimensions". It's a property of the metric, which, for our purposes here, you can think of as a function that takes two points and gives you a number, which in the case of Euclidean geometry we call the "distance" (or more precisely the "squared distance", since you have to take its square root to get what we normally call the distance). In Euclidean geometry, the metric is basically the usual Pythagorean theorem. A key property of this metric is that it is what is called "positive definite": the squared distance between any two distinct points is always a positive number. But this is not a property of any particular "dimension": it's a property of the geometry as a whole, because the metric is a property of the geometry as a whole.

Now consider the case of Minkowski spacetime, which is the geometry of spacetime in special relativity. The metric in this case is now not positive definite: the metric is still a function that takes two points and gives you a number, but now that number is not always positive. It can be positive, negative, or zero. (Purists would say that this means the thing we're calling the "metric" for Minkowski spacetime is really a "pseudometric", but we won't go into such fine points here.) But still, the metric is not a property of any particular "dimension", nor are the squared distances of different signs properties of different "dimensions". They're all just properties of the geometry as a whole.

student34 said:
Having said that, I am still quite curious and perplexed about what this temporal dimension is, and how it can share so many spatial properties such as curvature, spatially measurable and intersect with spatial dimensions, yet does not have spatial distance.
These questions also mostly come from having the wrong conceptual scheme. Hopefully the above helps.

However, you also mention other properties here: "curvature", "spatially measurable", and "intersect with spatial dimensions". Let's consider those briefly:

Curvature is not a property of a "dimension". It's a property of either a particular curve (curves can be "straight"--the technical term is "geodesic"--or not) or a geometric manifold as a whole (the Minkowski spacetime of SR is flat, but in General Relativity we also consider spacetimes that are curved). The latter kind of curvature is represented by a tensor, the Riemann curvature tensor.

Timelike intervals are not "spatially measurable", so I'm not sure what you're referring to with that.

Timelike curves can of course intersect spacelike curves, but this is not "dimensions" intersecting. "Dimensions", to the extent that concept even means anything in this context, aren't the kinds of things that can "intersect".
 
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  • #70
PeterDonis said:
What you are calling "spatial distance" is not a property of "spatial dimensions". It's a property of the metric, which, for our purposes here, you can think of as a function that takes two points and gives you a number, which in the case of Euclidean geometry we call the "distance" (or more precisely the "squared distance", since you have to take its square root to get what we normally call the distance). In Euclidean geometry, the metric is basically the usual Pythagorean theorem. A key property of this metric is that it is what is called "positive definite": the squared distance between any two distinct points is always a positive number. But this is not a property of any particular "dimension": it's a property of the geometry as a whole, because the metric is a property of the geometry as a whole.

Now consider the case of Minkowski spacetime, which is the geometry of spacetime in special relativity. The metric in this case is now not positive definite: the metric is still a function that takes two points and gives you a number, but now that number is not always positive. It can be positive, negative, or zero. (Purists would say that this means the thing we're calling the "metric" for Minkowski spacetime is really a "pseudometric", but we won't go into such fine points here.) But still, the metric is not a property of any particular "dimension", nor are the squared distances of different signs properties of different "dimensions". They're all just properties of the geometry as a whole.
So then is there a difference between 1 meter of Minkowski spacetime and 1 meter of Euclidean geometry?
 
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  • #71
student34 said:
So then is there a difference between 1 meter of Minkowski spacetime and 1 meter of Euclidean geometry?
Strictly speaking, you can't even compare the two. They're numbers from the metric of two different manifolds.

If there is some physical link between the Euclidean geometry you are considering and the Minkowski spacetime you are considering (for example, if the Euclidean geometry is the geometry of a spacelike slice of Minkowski spacetime--"space" at one instant of "time"), then you can use the same unit for both. Then 1 meter in the Euclidean geometry would be the same as 1 meter of the MInkowski spacetime that it's a spacelike slice of, because you chose the units that way.
 
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  • #72
PeterDonis said:
Strictly speaking, you can't even compare the two. They're numbers from the metric of two different manifolds.

If there is some physical link between the Euclidean geometry you are considering and the Minkowski spacetime you are considering (for example, if the Euclidean geometry is the geometry of a spacelike slice of Minkowski spacetime--"space" at one instant of "time"), then you can use the same unit for both. Then 1 meter in the Euclidean geometry would be the same as 1 meter of the MInkowski spacetime that it's a spacelike slice of, because you chose the units that way.
I think I went off focus when I brought up Euclidean geometry. A better question is what is the difference between a meter of spacelike distance and a meter of timelike distance?
 
  • #73
student34 said:
what is the difference between a meter of spacelike distance and a meter of timelike distance?
That the first is spacelike and the second is timelike. The first is measured with a ruler and the second with a clock.
 
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  • #74
PeterDonis said:
That the first is spacelike and the second is timelike. The first is measured with a ruler and the second with a clock.
I can also measure a meter of space with time, the distance light travels in 1/299792458s. Is there an intrinsic difference between a meter of each?
 
  • #75
student34 said:
I can also measure a meter of space with time
By using light and measuring its travel time, yes. In fact, this is how the meter is currently defined in SI units.

student34 said:
Is there an intrinsic difference between a meter of each?
Yes. The fact that you can use light travel time to measure distance in space does not make spacelike intervals the same as timelike intervals.
 
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  • #76
PeterDonis said:
Yes.
What is the difference?
PeterDonis said:
The fact that you can use light travel time to measure distance in space does not make spacelike intervals the same as timelike intervals.
I agree.
 
  • #77
student34 said:
What is the difference?
That one is spacelike and one is timelike. There is no other answer. The physical fact in relativity is that these two kinds of things are fundamentally different. That's the way spacetime geometry works.
 
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  • #78
student34 said:
What is the difference?
The question seems disingenuous. Physics, like all of the sciences, is experimental in nature.

Time is what clocks measure. We have well established and accurate agreement amount a large number of people and a large number of clocks. Spring clocks, pendulum clocks, crystal oscillators, water clocks, sun dials, sand clocks and atomic clocks. They all measure something. The something that they measure and agree upon is time.

Distance is what distance measuring devices measure. We have well established and accurate agreement among a large number of people and a large number of measuring devices. We use rulers, micrometers, feeler gauges, odometers, dead reckoning, radar, sonar and interferometry to measure distances. They all measure something. The something that they measure and agree upon is distance.

Some of the most precise and reproducible calibrations for distance measuring devices happen to be based on time measurements and an assumed (and well verified) consistency of the speed of light. So yes, there is a relationship between time and distance. But that does not make them the same thing.

I measure the "distance" between the world-line corresponding to Chicago and the world-line corresponding to Cleveland with distance measuring devices (probably an odometer), based in part on the assumption of a coordinate system in which the surface of the Earth is stationary.

I measure the "time" between my departure from Chicago and my arrival in Cleveland along a worldline corresponding to myself with a clock. Possibly a wristwatch, a dashboard clock or a cell phone.
 
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  • #79
student34 said:
I can also measure a meter of space with time, the distance light travels in 1/299792458s. Is there an intrinsic difference between a meter of each?
Then you did this measurement of spatial distance not with a clock alone.

You can always use the combination of a clock and light as a ruler and the combination of a ruler and light as a clock.

Take as example the diagram with the rectangle in your OP. Assume, the vertical red line and blue line are worldlines of clocks, that are at rest in your reference frame, with a distance between each other of 1 meter.

How would you measure the time interval between two ticks of the red clock? I think it is obvious, that this cannot be measured with a ruler alone.
 
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  • #80
PeterDonis said:
That one is spacelike and one is timelike. There is no other answer. The physical fact in relativity is that these two kinds of things are fundamentally different. That's the way spacetime geometry works.
Well then I guess I hit the bottom here.

Does relativity have to go one step further and say that a postulate would be that the two must not be the same in terms of distance?
 
  • #81
student34 said:
Does relativity have to go one step further and say that a postulate would be that the two must not be the same in terms of distance?
What does it even mean to say that two different quantitative measures are "the same in terms of distance"? And is that not a bit self-referential when one of the measures is "distance"?
 
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  • #82
jbriggs444 said:
Time is what clocks measure. We have well established and accurate agreement amount a large number of people and a large number of clocks. Spring clocks, pendulum clocks, crystal oscillators, water clocks, sun dials, sand clocks and atomic clocks. They all measure something. The something that they measure and agree upon is time.

So yes, there is a relationship between time and distance. But that does not make them the same thing.
In relativity, is there known to be an intrinsic relationship. For example, we know that a proton and an electron have an intrinsic relationship of mass.
 
  • #83
Sagittarius A-Star said:
How would you measure the time interval between two ticks of the red clock? I think it is obvious, that this cannot be measured with a ruler alone.
I agree. But that is more of an extrinsic difference. There can be two different ways to measure the same thing.
 
  • #84
student34 said:
Well then I guess I hit the bottom here.

Does relativity have to go one step further and say that a postulate would be that the two must not be the same in terms of distance?

Did you read...

robphy said:
Spacetime Physics (1st edition)
Chapter One
Part One
https://www.eftaylor.com/download.html#special_relativity
It’s time to read “Parable of the Surveyors”

As I suggested earlier, in spite of your enthusiasm,
it's time to read a careful presentation of ideas (like in the above)
to guide your questioning.

In my opinion, it's difficult to field many of your questions because
you seem unaware of the big picture of how these ideas really fit together.
So, you reading a reference like that will likely help you understand the subject better.
...then ask more questions afterwards.

(An introduction to relativity in an introductory-physics textbook
is not sufficient preparation for the spacetime viewpoint. A reference like the above is.)

my $0.02
 
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  • #85
jbriggs444 said:
What does it even mean to say that two different quantitative measures are "the same in terms of distance"? And is that not a bit self-referential when one of the measures is "distance"?
In other words, must relativity imply that 1m of space not be interchangable with 1m of time.
 
  • #86
student34 said:
In other words, must relativity imply that 1m of space not be interchangable with 1m of time.
If you have two events with a space-like separation, you cannot get a physical object to go from one to the other. If you have two events with a time-like separation, you can.

So the two types of separation are not interchangeable in reality. We like our models to match reality.

We usually use experiments that are less binary than "can we get there" and go for quantitative results like in the Bertozzi experiment.
 
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  • #87
student34 said:
Does relativity have to go one step further and say that a postulate would be that the two must not be the same in terms of distance?
There is no "one step further". All of your questions are just rephrasing the same thing in different words: spacelike and timelike are different things.
 
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  • #88
student34 said:
In other words, must relativity imply that 1m of space not be interchangable with 1m of time.
It is pretty obvious that the two are not interchangeable because one is measured with a clock and the other with a meter stick. Therefore any correct theory will imply that; if you want to call this a statement about what the theory “must” do, you may.
 
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  • #89
There are more precise ways of describing what many of us are trying to tell you,
by using dot-products (which could be regarded as a way to geometrically formalize
measurements of physical quantities [modeled as geometrical objects]
with various measuring devices [modeled as certain unit vectors],
then making definitions).

The use of geometric units is done for consistency and convenience,
but one needs sufficient background understanding to see this.

In my opinion, to appreciate this viewpoint,
you need to understand the basics of spacetime geometry,
as presented in
Taylor and Wheeler's "Spacetime Physics (1st ed)" linked above.
However, I think you may benefit from
Bondi's "Relativity and Common Sense" first
because it emphasize the operational definitions of "time" and "space" coordinates
using light-rays and clocks,
and postpones the formulas and formalism (and use of geometric units) until later.

Until then, I think you are just getting caught up in the formalism
because you don't understand what the basics are (why relativity is formulated the way that it is).

Shameless plug? https://www.physicsforums.com/insights/relativity-using-bondi-k-calculus/

my $0.03
 
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  • #90
student34 said:
In other words, must relativity imply that 1m of space not be interchangable with 1m of time.
Well, torque and energy have the same units (Newton-metres). They are not the same thing. One ##Nm## of torque is not interchangeable with one ##Nm## of energy.

Also, if we continue with geometric units in relativity, we have mass measured in metres as well. The mass of the Sun, for example, is about ##1.5 \ km##. That's something different again from a spacelike interval of ##1.5 \ km##.
 
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