Are Everyday Objects Spacelike?

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Discussion Overview

The discussion revolves around the nature of spacelike intervals in the context of everyday objects, specifically using a glass of water as an example. Participants explore the implications of spacelike separation between points on the object and delve into the properties of four-vectors in relation to timelike, spacelike, and null classifications.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that the interval between two points on an object can be considered spacelike if the events at those points occur simultaneously.
  • Others argue that if the events are separated by a time interval long enough for light to travel between the points, then they cannot be spacelike separated.
  • One participant clarifies that objects themselves are not events, and that intervals depend on the coordinates of pairs of events.
  • Another participant discusses the concept of a three-dimensional object sweeping out a world-volume in Minkowski space, indicating that while some points may be spacelike separated, others may not be.
  • A participant presents a classification of four-vectors into timelike, spacelike, and null, providing examples of their component structures.
  • Another participant challenges the correctness of the proposed component structures, explaining that timelike vectors can have non-zero spatial components, and that the classification depends on the relationship between the time and spatial components.
  • There is a discussion about the existence of inertial frames where specific conditions for timelike, spacelike, and light-like vectors can be met.

Areas of Agreement / Disagreement

Participants express differing views on the nature of spacelike intervals and the classification of four-vectors. There is no consensus on the correctness of the proposed component structures for four-vectors, and the discussion remains unresolved regarding the implications of spacelike separation in the context of everyday objects.

Contextual Notes

Limitations include potential misunderstandings of the definitions of spacelike, timelike, and null vectors, as well as the dependence on the choice of inertial frames. The discussion also highlights the complexity of relating everyday objects to concepts in relativistic physics.

Dixanadu
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Hey guys,

Imagine an everyday object, like a glass of water for example. Now imagine two points on the glass, like one near the top and one near the bottom. The interval between these two points, [itex]\Delta X[/itex], is it spacelike because these two "events" are occurring at the same time?
 
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Dixanadu said:
imagine two points on the glass, like one near the top and one near the bottom. The interval between these two points, ##\Delta X##, is it spacelike because these two "events" are occurring at the same time?

If you imagine things that way, then yes. ;) But if, for example, you imagine events corresponding to the top point at some instant of time and the bottom point after an interval of time long enough for light to travel from the top to the bottom, then those two events will not be spacelike separated.
 
Objects are not events, or pairs of events. Intervals are functions of the coordinates of pairs of events.
 
To be more concrete, a three-dimensional object will sweep out a world-volume in Minkowski space. If you just look at two points on the glass, they will be described by world lines. These are going to have points which are space-like separated, but also other points which are not. Like Peter said, if you wait long enough, light from one end of the glass will reach the other.
 
Wow thank you guys for such quick replies!

So the next thing is...I just wana understand the component structure of four vectors. let's take for example a four vector [itex]n_{\mu}[/itex]. It can either be timelike, spacelike or null. Here's how I understand the component structure in each case:
1) TIMELIKE - [itex]n_{\mu}=(1,0,0,0)[/itex] - basically all spatial components are 0
2) SPACELIKE - [itex]n_{\mu}=(0,1,1,1)[/itex] - time component vanishes
3) NULL - [itex]n_{\mu}=(1,1,0,0)[/itex] - everything else apart from the time component and one spatial component vanishes

of course the "1" entries can be anything not just 1.

So: are these correct?

Thanks guys!
 
Dixanadu said:
So: are these correct?

No. A time-like vector may very well have non-zero space-like components. The thing is that it has a positive square (well, this depends on your taste in metrics ...), i.e., the square of the time component is larger than the sum of the squares of the space components. The opposite goes for space-like vectors and for light-like vectors, the square of the time component is equal to the sum of the squares of the space components.

Edit: That being said, there always exists an inertial frame where a time-like vector has all space components equal to zero and there always exists an inertial frame where a space-like vector has zero time component. A light-like vector always has a non-zero time component and at least one non-zero space component.
 
Orodruin said:
Edit: That being said, there always exists an inertial frame where a time-like vector has all space components equal to zero and there always exists an inertial frame where a space-like vector has zero time component. A light-like vector always has a non-zero time component and at least one non-zero space component.

Okay - so in a space where the vector [itex]n_{\mu}[/itex] exists, a Lorentz observer can always find a frame wherein the conditions you wrote are met (depending on whether the vector is timelike / spacelike / lightlike) ?
 

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