Special Relativity Spacetime Intervals

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Discussion Overview

The discussion centers on the nature of spacetime intervals in the context of special relativity, specifically addressing why the spacetime interval is defined with a negative time component. Participants explore the implications of this definition and its invariance across different reference frames.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions why the spacetime interval is defined as Δs² = -c²(Δt²) + Δx² + Δy² + Δz², suggesting an alternative formulation that treats time similarly to spatial dimensions.
  • Another participant argues that the negative time component is essential for maintaining frame invariance, citing the Lorentz Transformation to illustrate that the interval remains consistent across different frames.
  • A third participant emphasizes that the spacetime interval is designed to yield consistent results regardless of the observer's frame, contrasting this with the proposed alternative formulation.
  • A later reply reiterates the importance of the spacetime interval's definition, incorporating graphical representations to explain why traditional geometric approaches like the Pythagorean theorem do not apply in this context.
  • This participant also introduces a conceptual perspective on the relationship between the observer's motion and the geometry of spacetime, suggesting that the orientation of coordinates plays a critical role in understanding the invariance of the speed of light.

Areas of Agreement / Disagreement

Participants express varying viewpoints on the definition and implications of the spacetime interval. While some agree on the necessity of the negative time component for invariance, others propose alternative interpretations, indicating that the discussion remains unresolved.

Contextual Notes

Some assumptions regarding the interpretation of spacetime geometry and the implications of observer motion are not fully explored, leaving room for further inquiry into the foundational aspects of the spacetime interval.

swashtecher
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Just a quick question on spacetime intervals in spacetime. Why is the spacetime interval between two events given by Δs^2 = -c^2(Δt^2) + Δx^2 + Δy^2 + Δz^2, rather than c^2(Δt^2) + Δx^2 + Δy^2 + Δz^2 (as if it were the distance between two points in four spatial dimensions)? Or more succinctly, why is the time component of the spacetime interval negative?
 
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Because the first one is frame invariant (it takes the same value in every frame), whereas the second one is not.

Take the Lorentz Transformation:

\Delta x'=\gamma (\Delta x-v\Delta t)
\Delta t'=\gamma (\Delta t-v\Delta x/c^2)

Now try calculating (\Delta x')^2-(c\Delta t')^2. You'll find that (\Delta x')^2-(c\Delta t')^2=(\Delta x)^2-(c\Delta t)^2.

If you try doing the same thing with (\Delta x')^2+(c\Delta t')^2 you'll see that (\Delta x')^2+(c\Delta t')^2 \neq (\Delta x)^2+(c\Delta t)^2
 
The whole point of the spacetime interval is to arrive at something analogous to a distance in space and/or a period of time that comes out the same no matter what frame you do the calculation in. If you use the second formula, it doesn't come out the same in all frames whereas the first one does.
 
swashtecher said:
Just a quick question on spacetime intervals in spacetime. Why is the spacetime interval between two events given by Δs^2 = -c^2(Δt^2) + Δx^2 + Δy^2 + Δz^2, rather than c^2(Δt^2) + Δx^2 + Δy^2 + Δz^2 (as if it were the distance between two points in four spatial dimensions)? Or more succinctly, why is the time component of the spacetime interval negative?

elfmotat and ghwellsjr summed it up pretty well. Here's basically the same point they've made using some graphics.
4_D_Metric_SpaceE.jpg

From this point of view you can see why the Pythagorean theorem doesn't work for the blue guy when he tries to compute an invariant value for a red interval.

In a way, the root cause of this situation (from the standpoint of the space-time diagram) has to do with the unique orientation of the blue and red X1 and X4 coordinates. For example, the direction the blue guy moves in the 4-dimensional universe determines the slope of his world line (his X4 coordinate slope with respect to the black rest system).

Now, the mysterious aspect of special relativity is that blue's X1 coordinate (his 3-D cross-section view of the 4-D universe) rotates such that the 45-degree photon world line always bisects the angle between X4 and X1. This is a perfectly general phenomenon, regardless of the observer's speed, holding for any observer moving relative to the black rest system. Accordingly, this explains why the speed of light is always c, for any frame of reference.

So, in a way, you could ask of nature: Why is it that the observer's X1 axis always rotates in that special manner when the X4 rotates? One possible answer that has been suggested is that consciousness can only pick out a cross-section view of the 4-D universe that is intelligible. And The 4-dimensional objects are arranged geometrically so as to present symmetric relationships among objects that are consistent with the laws of physics. Some would argue that this underlies the discovery of laws of physics. And this is consistent with the fact that the laws of physics are the same in all Lorentz frames.
 
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