Concerned on the relativity of lengths

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Discussion Overview

The discussion centers on the concept of measuring the length of a moving rod as described in Einstein's "The Principle of Relativity." Participants explore the implications of time and position in the context of relativistic length measurement, raising questions about the relationship between time intervals and spatial measurements in a stationary frame of reference.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether the length of the rod can be expressed in terms of the time interval (2:00 am thru 3:00 am) and its velocity v, suggesting a potential relationship.
  • Another participant clarifies that the two ends of the rod are located at different positions at a single time, not at two different times, challenging the initial interpretation of the time interval.
  • A later reply emphasizes that the length of the rod is simply the difference in positions (x2 - x1), indicating that time is not necessary for this calculation.
  • Further, a participant expresses confusion about the necessity of time in the context of the length measurement, questioning how time relates to the positions of the rod's ends.

Areas of Agreement / Disagreement

Participants express differing views on the role of time in measuring the length of the rod, with some asserting that time is not needed while others seek to understand its relevance. The discussion remains unresolved regarding the relationship between time intervals and spatial measurements.

Contextual Notes

Participants rely on specific definitions of time and position, and there is an ongoing exploration of how these concepts interact in the context of relativity. The discussion does not resolve the implications of these definitions on the measurements being discussed.

myoho.renge.kyo
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A. Einstein writes the following on The Principle of Relativity, p. 41:

"Let there be given a stationary rigid rod;and let its length be L as measured by a measuring-rod which is also stationary. We now imagine the axis of the rod lying along the axis of x of the stationary system of co-ordinates, and that a uniform motion of parallel translation with velocity v along the axis of x in the direction of increasing x is then imparted to the rod. We now inquire as to the length of the moving rod, and imagine its length to be ascertain by the following two operations:-"

my concern is the following operation (b):

"(b) by means of stationary clocks set up in the stationary system and synchronizing in accordance with chapter 1, the observer ascertains at what points of the stationary system the two ends of the rod to be measured are located at a definite time. The distance between these two points, measured by the measuring-rod already employed, which in this case is at rest, is also a length which may be designated 'the length of the rod.'"

the present period of time is from 2:00 am thru 3:00 am, 9/5/2006, in burbank, california.

let the observer ascertain that the points of the stationary system (corresponding to the two ends of the rod to be measured) are located at 2:00 am and then at 3:00 am.

the present period of time then is the definite time at which the observer ascertains at what points of the stationary system the two ends of the rod to be measured are located.

shouldn't the "length of the rod" be implied in (2:00 am thru 3:00 am) = ("length of the rod") / v? if not, why? thanks! (2:00 am thru 3:00 am, 9/5/2006)
 
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myoho.renge.kyo said:
A. Einstein writes the following on The Principle of Relativity, p. 41:

"Let there be given a stationary rigid rod;and let its length be L as measured by a measuring-rod which is also stationary. We now imagine the axis of the rod lying along the axis of x of the stationary system of co-ordinates, and that a uniform motion of parallel translation with velocity v along the axis of x in the direction of increasing x is then imparted to the rod. We now inquire as to the length of the moving rod, and imagine its length to be ascertain by the following two operations:-"

my concern is the following operation (b):

"(b) by means of stationary clocks set up in the stationary system and synchronizing in accordance with chapter 1, the observer ascertains at what points of the stationary system the two ends of the rod to be measured are located at a definite time. The distance between these two points, measured by the measuring-rod already employed, which in this case is at rest, is also a length which may be designated 'the length of the rod.'"

the present period of time is from 2:00 am thru 3:00 am, 9/5/2006, in burbank, california.

let the observer ascertain that the points of the stationary system (corresponding to the two ends of the rod to be measured) are located at 2:00 am and then at 3:00 am.
No, the two ends of the rod are located at two different positions at a single time, not at two different times.

the present period of time then is the definite time at which the observer ascertains at what points of the stationary system the two ends of the rod to be measured are located.
Yes, and again the "location" is position not time

shouldn't the "length of the rod" be implied in (2:00 am thru 3:00 am) = ("length of the rod") / v? if not, why? thanks! (2:00 am thru 3:00 am, 9/5/2006)
There is a single time, two different positions, not two different times.
 
thank you for helping me understand. i really appreciate it.

let's say that at t1 (9:00 am) a uniform motion of parallel translation with velocity v along the axis of x in the direction of increasing x is then imparted to the rod, and that at t2 (10:00 am) the observer ascertains that at x1 and at x2 of the stationary system the two ends of the rod to be measured are located.

does the following then imply the "lenght of the rod?":

(9:00 am thru 10:00 am) = (x2 - x1) / v

or

if t1 = 0, then

t2 = (x2 - x1) / v

thank you again. (9:00 am thru 10:00 am, 9/5/2006, in burbank, california)
 
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The "length" is x2-x1. No need for t1.
 
thanks!

but i am confused. at some point in time (let's call it t1) a uniform motion of parallel translation with velocity v along the axis of x in the direction of increasing x is imparted to the rod. and at a later point in time (let's call it t2) the observer ascertains that at x1 and at x2 of the stationary system the two ends of the rod to be measured are located.

why is it that there is no need for t1?

if t1 = 0, and the "length" is x2 - x1, does that mean that t2 = (t2 - t1) = (x2 - x1) / v?

thanks again! (9/10/2006, 8:00 am thru 9:00 am in Burbank, California)
 
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