- #1

thehangedman

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What would be the shape of the "plane" when the metric is +1, -1 (Minkowski)?

Is it somehow hyperbolic?

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- Thread starter thehangedman
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In summary, Minkowski space, which is a 2-dimensional space with the metric signature (-+), is flat like a plane. This means that its curvature is zero, its geodesics are straight lines, and its topology is the same as that of a Euclidean plane. However, when looking at the metric structure, it differs from the Euclidean plane in that it uses a different way of assigning distances, similar to how the hyperbola plays the same role as the circle in Minkowski space. This means that while the topology of Minkowski space is the same as the Euclidean plane, its metric structure is different and is related to the concept of Lorentzian structure. The topology of Minkowski space

- #1

thehangedman

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What would be the shape of the "plane" when the metric is +1, -1 (Minkowski)?

Is it somehow hyperbolic?

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One way to think about it is that (using intimidating terminology for a moment) you have topological structure plus metric structure.

Topological structure means whatever is preserved under stretching a rubber sheet. Topologically, Minkowski space is the same as the Euclidean plane, and a coffee cup is the same as a doughnut http://en.wikipedia.org/wiki/Topology#Elementary_introduction , but the plane isn't the same as a doughnut.

Metric structure means how you assign distances, which is different for the Euclidean plane than for Minkowski space. In Euclid's axioms, there is only one that refers to distance measure: given any point to use as a center, and any line segment with that point at an end, you can make a circle with that segment as its radius. The hyperbola plays the same role in Minkowski space as the circle does in the Euclidean plane.

Another way to think about it is that the role played by rotations in the Euclidean plane is played by a certain kind of distortion in Minkowski space: http://www.lightandmatter.com/html_books/0sn/ch07/ch07.html In both cases, the transformations preserve "distances" (Pythagorean or Minkowskian), as well as areas and parallelism.

Topological structure means whatever is preserved under stretching a rubber sheet. Topologically, Minkowski space is the same as the Euclidean plane, and a coffee cup is the same as a doughnut http://en.wikipedia.org/wiki/Topology#Elementary_introduction , but the plane isn't the same as a doughnut.

Metric structure means how you assign distances, which is different for the Euclidean plane than for Minkowski space. In Euclid's axioms, there is only one that refers to distance measure: given any point to use as a center, and any line segment with that point at an end, you can make a circle with that segment as its radius. The hyperbola plays the same role in Minkowski space as the circle does in the Euclidean plane.

Another way to think about it is that the role played by rotations in the Euclidean plane is played by a certain kind of distortion in Minkowski space: http://www.lightandmatter.com/html_books/0sn/ch07/ch07.html In both cases, the transformations preserve "distances" (Pythagorean or Minkowskian), as well as areas and parallelism.

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- #3

Ben Niehoff

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The metric signature (-+) does not make the plane "somehow hyperbolic". It is still a plane, its curvature vanishes, its geodesics are straight lines, etc.

The metric of a hyperbolic plane looks like this:

[tex]ds^2 = \frac{dx^2 + dy^2}{y^2}[/tex]

Notice that this metric still has signature (++).

In general, changing the signature from (++++) to (-+++) is not the same thing as introducing curvature. It's actually something quite a bit more radical. Not every manifold (as a topological space) can be given a metric of indefinite signature in such a way that can be extended over the whole manifold. This is called putting a Lorentzian structure on a manifold. It turns out to be related to whether the manifold can have a continuous, non-vanishing vector field.

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Anything separated by a light cone from some event P has a "distance" i.e. a Lorentz interval, of zero, but only some of those events are in the neihborhood of P, those are the events that have nearly identical coordinates.

So the "open balls" of topology determine the neighborhood. Projected onto some basis, the Lorentz interval gives you proper times and proper distances. In the light beam example, we can tell that the absolute value of the distance equals the absolute value of the time in some local coordinate system, as it must to make the Lorentz interval zero (dx^t = dx^2), but we can't tell how long each is (what is dx, what is dt), until we specify more about the reference frame - basically, we need the velocity of the observer.

- #5

TrickyDicky

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It is worth remembering though that given that the hyperbolic plane can't be embedded in Euclidean space, it must be represented by some model, and among those models there is the hyperboloid model that is a 3-dim Minkowski spacetime. The Minkowski plane can be thought of as a flat model of hyperbolic curve represented as distance.Ben Niehoff said:

The metric signature (-+) does not make the plane "somehow hyperbolic". It is still a plane, its curvature vanishes, its geodesics are straight lines, etc.

The metric of a hyperbolic plane looks like this:

[tex]ds^2 = \frac{dx^2 + dy^2}{y^2}[/tex]

Notice that this metric still has signature (++).

In general, changing the signature from (++++) to (-+++) is not the same thing as introducing curvature. It's actually something quite a bit more radical. Not every manifold (as a topological space) can be given a metric of indefinite signature in such a way that can be extended over the whole manifold. This is called putting a Lorentzian structure on a manifold. It turns out to be related to whether the manifold can have a continuous, non-vanishing vector field.

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Ben Niehoff

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TrickyDicky said:It is worth remembering though that given that the hyperbolic plane can't be embedded in Euclidean space, it must be represented by some model, and among those models there is the hyperboloid model that is a 3-dim Minkowski spacetime. The Minkowski plane can be thought of as a flat model of hyperbolic curve represented as distance.

This is a bit misleading, which is why I avoided the issue (also the way you've stated it is flat wrong).

The hyperbolic plane (of signature ++) can be isometrically embedded in Minkowski 3-space (of signature -++). That is, the hyperbolic plane can be thought of as a particular 2-dimensional curved surface within Minkowski 3-space. But this does not imply that there is anything "hyperbolic" about Minkowski space itself. Likewise, there is nothing "spherical" about Euclidean space, simply by virtue of the fact that we can isometrically embed spheres in Euclidean space.

Additional corrections to your statement:

1. One doesn't need to have an external space in which to embed the hyperbolic plane in order to have a "model" of it. In fact, the metric I gave above is the Poincare metric for the "upper half plane model", which is a model of hyperbolic space drawn on the upper half of an ordinary Euclidean plane, where the geodesics are drawn as circles centered on the x axis. There are additional models, including the hyperboloid model, but also including two different models drawn within the open disc of the unit circle. One model has straight lines as geodesics; in the other model, geodesics are circles that meet the boundary at 90 degrees. In fact, by conformal mapping, you can make any sort of model you want.

2. There is no such thing as a "hyperbolic curve". All 1-dimensional curves are flat.

3. Minkowski space is not a model of hyperbolic space. Every hyperbolic space can be isometrically embedded in Minkowski space of one dimension higher. This is a different statement.

Some other interesting things can be isometrically embedded in Minkowski space as well. For example, we generally think of a cone as something with a deficit angle at a given point. However, one can have cones with an

Excess-angle cones can also be isometrically embedded in Euclidean space, but they will have to be "wrinkled up", and hence their symmetries will not coincide with symmetries of Euclidean space.

- #7

thehangedman

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- #8

TrickyDicky

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Ah, I see when something can be misleading you rather avoid it than clarify it.Ben Niehoff said:This is a bit misleading, which is why I avoided the issue (also the way you've stated it is flat wrong).

This is quite silly, I didn't imply anything, Minkowski space has no curvature, period.Ben Niehoff said:The hyperbolic plane (of signature ++) can be isometrically embedded in Minkowski 3-space (of signature -++). That is, the hyperbolic plane can be thought of as a particular 2-dimensional curved surface within Minkowski 3-space. But this does not imply that there is anything "hyperbolic" about Minkowski space itself. Likewise, there is nothing "spherical" about Euclidean space, simply by virtue of the fact that we can isometrically embed spheres in Euclidean space.

If what you claim is that Minkowski space is totally unrelated with hyperbolic geometry , you are flat wrong. But I won't bother debating this, just read some geometry, ever heard of hyperbolic numbers?

This is ridiculous, I have never said what you attribute me ,nor suggested it. Why do you recur to a "straw man" trick?Ben Niehoff said:Additional corrections to your statement:

1. One doesn't need to have an external space in which to embed the hyperbolic plane in order to have a "model" of it.

You mean 1-dimensional curves have no intrinsic curvature. Surely you are not denying the existence of hyperbolas or of curves in general just because their curvature is extrinsic, are you?Ben Niehoff said:2. There is no such thing as a "hyperbolic curve". All 1-dimensional curves are flat.

I wrote "hyperboloid model", not "Minkowki space model", right? Precisely what you call a different statement is what I was trying to transmit, but I guess I'm sloppy.Ben Niehoff said:3. Minkowski space is not a model of hyperbolic space. Every hyperbolic space can be isometrically embedded in Minkowski space of one dimension higher. This is a different statement.

- #9

thehangedman

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- #10

thehangedman

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Not donuts. Stupid iPhone autocorrect. "it's" ...

- #11

TrickyDicky

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Yes, it's called the Minkowski trick (when going from Minkowski to Euclidean), aka Wick rotation.thehangedman said:

- #12

Ben Niehoff

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TrickyDicky said:Ah, I see when something can be misleading you rather avoid it than clarify it.

My object was to avoid overloading the OP with irrelevant information that only muddles the issue. He was genuinely confused as to whether Minkowski space is or is not flat.

This is quite silly, I didn't imply anything, Minkowski space has no curvature, period.

...

I wrote "hyperboloid model", not "Minkowki space model", right? Precisely what you call a different statement is what I was trying to transmit, but I guess I'm sloppy.

I was responding to what you wrote below, which I feel is highly misleading (emphasis mine):

TrickyDicky said:It is worth remembering though that given that the hyperbolic plane can't be embedded in Euclidean space, it must be represented by some model, and among those modelsthere is the hyperboloid model that.isa 3-dim Minkowski spacetime

Perhaps this was merely a typo, but what you wrote appears to claim that Minkowski 3-space (a flat space of 3 dimensions and indefinite signature) is the same thing as the hyperboloid model (a curved space of 2 dimensions and definite signature).

If what you claim is that Minkowski space is totally unrelated with hyperbolic geometry, you are flat wrong. But I won't bother debating this, just read some geometry, ever heard of hyperbolic numbers?

Of course I have, and I've used split-biquaternions to explore representations of the Lorentz algebra.

"Hyperbolic geometry" merely refers to geometry on spaces that are negatively curved. It is neat that some of these spaces can be isometrically embedded in Minkowski space, but this is not an essential feature.

There are other hyperbolic spaces which cannot be isometrically embedded in Minkowski space. Anti-deSitter space, for example, is a space of signature (1, d) and constant negative curvature. It can be isometrically embedded in [itex]\mathbb{R}^{2, d+1}[/itex], but not in Minkowski space.

You mean 1-dimensional curves have no intrinsic curvature. Surely you are not denying the existence of hyperbolas or of curves in general just because their curvature is extrinsic, are you?

To me, the phrase "their curvature is extrinsic" is incorrect, from a strict mathematical point of view. All 1-dimensional curves are flat. Their

Similarly, an ordinary 2-torus can be given a completely flat metric. The 2-torus can also be embedded in [itex]\mathbb{R}^3[/itex]. However, despite the fact that the 2-torus is flat, its embeddings in [itex]\mathbb{R}^3[/itex] always have extrinsic curvature. Only in [itex]\mathbb{R}^4[/itex] can one embed the torus isometrically, such that the extrinsic curvature is equal to the intrinsic curvature (i.e., zero).

As a manifold, there is no difference between a hyperbola and the real line.

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TrickyDicky

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I think I already clarified that this is not what I was claiming and admitted that my sloppy writing could be misleading. Instead ofBen Niehoff said:Perhaps this was merely a typo, but what you wrote appears to claim that Minkowski 3-space (a flat space of 3 dimensions and indefinite signature) is the same thing as the hyperboloid model (a curved space of 2 dimensions and definite signature).

What is just neat to you might be significative to others, this is purely subjective. What is objective is that there is many connections between Minkowski space and hyperbolic geometry. Not only the embedding "neatness" : The space of velocities in Minkowski spacetime is hyperbolic, there is hyperbolic orthogonality: hyperbolic right angles, etc...Ben Niehoff said:"Hyperbolic geometry" merely refers to geometry on spaces that are negatively curved. It is neat that some of these spaces can be isometrically embedded in Minkowski space, but this is not an essential feature.

You argue as if I was claiming that Minkowski geometry is hyperbolic geometry. I could as well have stressed the close relation between the Minkowskian and Euclidean plane (even more close with the complex plane). But the OP referred to the similarities with the hyperbolic plane, and once it is cleared up the obvious fact that the minkowki plane doesn't have negative curvature, it is perfectly licit to talk about the connections with hyperbolic notions.

Totally irrelevant since I never said that all hyperbolic spaces can be embedded in Minkowski space. I rather tried to stress the fact that hyperbolic spaces can't be embedded in n+1 Euclidean spaces.Ben Niehoff said:There are other hyperbolic spaces which cannot be isometrically embedded in Minkowski space. Anti-deSitter space, for example, is a space of signature (1, d) and constant negative curvature. It can be isometrically embedded in [itex]\mathbb{R}^{2, d+1}[/itex], but not in Minkowski space.

That is why is called extrinsic. Your nitpicking is quite absurd here. Extrinsic curvature is not a mathematically incorrect term at all. It is implicit that is always referred to the embedding. Following your "strict" policy you shouldn't call them curves either because they are flat.Ben Niehoff said:To me, the phrase "their curvature is extrinsic" is incorrect, from a strict mathematical point of view. All 1-dimensional curves are flat. Theirembeddingwithin some other manifold might have extrinsic curvature. But of a 1-dimensional curve, the curvature does not belong to the curve, in the strictest sense; it is a property of the embedding.

Sure, but the discussion was not in terms of manifolds and topology but clearly geometrical.Ben Niehoff said:As a manifold, there is no difference between a hyperbola and the real line.

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TrickyDicky

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In order not to confuse anybody, when I say hyperbolic I'm not referring to hyperbolic geometry but to anything related to or with the shape of hyperbolas.

Minkowski space is a four-dimensional space that is often described as a "hyperbolic paraboloid" or "saddle-shaped". It is a mathematical model used in the theory of relativity to describe the geometry of space and time.

Minkowski space differs from Euclidean space in that it includes a fourth dimension of time, in addition to the three dimensions of space. This allows for the concept of spacetime, where space and time are not separate entities but are interconnected.

Minkowski space is significant in physics because it provides a mathematical framework for understanding the effects of special relativity, which describes the behavior of objects moving at high speeds. It also plays a crucial role in the formulation of general relativity, which explains the effects of gravity.

Minkowski space is often visualized using diagrams called "Minkowski diagrams". These diagrams use coordinates to represent the three dimensions of space and the fourth dimension of time. The shape of Minkowski space can also be represented using mathematical equations and geometric models.

While Minkowski space is primarily used in theoretical physics, it has also found practical applications in fields such as astrophysics and cosmology. It has been used to model the behavior of black holes, gravitational waves, and the expansion of the universe. Additionally, the concept of spacetime has been applied in technologies such as GPS navigation systems.

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