Interesting Question About Relativity and the Absolute

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Discussion Overview

The discussion revolves around the nature of length in the context of special relativity, particularly questioning how lengths, such as the Planck length, can be defined when distances are relative and dependent on the observer's reference frame. The conversation touches on philosophical implications regarding the inherent qualities of objects and their measurements.

Discussion Character

  • Exploratory
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that if distances are relative, it raises questions about defining lengths like the Planck length, which seems to require an absolute reference.
  • Others argue that while space is relative, objects must possess some inherent length, though this length may vary depending on the reference frame.
  • A participant introduces the concept of "proper length," which is described as a body's invariant length measured in its rest frame, suggesting that while lengths change for observers, they remain consistent for the object itself.
  • Another participant emphasizes that the Planck length should be measured in the rest frame for consistency.
  • Mathematical expressions are provided to describe the relationship between proper length and observed lengths, indicating the complexity of measuring length in different frames.

Areas of Agreement / Disagreement

Participants express differing views on the nature of length and its dependence on reference frames, indicating that the discussion remains unresolved with multiple competing perspectives.

Contextual Notes

The discussion includes assumptions about the definitions of proper length and the implications of relativistic effects on measurements, which are not fully resolved.

Curious6
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According to special relativity, distances are relative, as people measuring distance from different reference frames come up with different measurements and are equal on footing as regards their results. However, my question is then: how can we even define a given length, for example, the Planck length to be 10^-33 cm, if it is also subject to special relativity and therefore not even an absolute reference? Also (this is more of a philosophical question), can length even be assigned as a quality of an object or is it just an illusion from our reference frame?

Thanks for your insights.
 
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Let me try to rephrase the question in a more meaningful way: if space is relative, then can we say quarks (or strings, or whatever the smallest constituent of the world is) don't have a length, as it all depends on the reference frame? This however leads me to ask the following: an object existing must have some sort of inherent length to it, or can it vary infinitely depending on the reference frame?

Please, someone help me out, I'm very confused!
 
"Proper length" is the term used for a body's invariant length. Although a body's length will change with respect to an observer, it does have a proper length, and that is a body's length with respect to itself, or its length when at rest.

For example, if you lay down on a spaceship going at 90% the speed of light, you'll look squished up to us because your relative height will be smaller than it was when you were on Earth. But you won't look squished up to yourself. You'll still be able to measure your proper height and you'll measure the same height for yourself on the spaceship as you'll measure on Earth or anywhere (with the exception of extreme gravitational fields that may even distort your point of view).
 
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For consistency the Planck length has to be that measured in the rest frame.

Garth
 
nwall said:
"Proper length" is the term used for a body's invariant length.
...and is in fact the pythagorean sum of measured spatial length: [tex]l_{spatial}=\frac{l_{proper}}{\gamma}[/tex]
and [itex]c[/itex] times the velocity-induced non-simultaneity ("time-length"): [tex]l_{time}=c\frac{\gamma vl_{spatial}}{c^2}=\frac{vl_{proper}}{c}[/tex]

or: [tex]\sqrt{\left(\frac{l_{proper}}{\gamma}\right)^2+\left(\frac{vl_{proper}}{c}\right)^2}=l_{proper}[/tex]

([itex]\gamma=1/\sqrt{1-v^2/c^2}[/itex] as usual)
 
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OK, thanks for clearing up this doubt. It was this concept of 'proper length' I was doubting about.
 

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