Concerned on the relativity of lengths

  • Thread starter Thread starter myoho.renge.kyo
  • Start date Start date
  • Tags Tags
    Relativity
myoho.renge.kyo
Messages
37
Reaction score
0
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)
 
Physics news on Phys.org
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)
 
Last edited:
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)
 
Last edited:
I started reading a National Geographic article related to the Big Bang. It starts these statements: Gazing up at the stars at night, it’s easy to imagine that space goes on forever. But cosmologists know that the universe actually has limits. First, their best models indicate that space and time had a beginning, a subatomic point called a singularity. This point of intense heat and density rapidly ballooned outward. My first reaction was that this is a layman's approximation to...
Thread 'Dirac's integral for the energy-momentum of the gravitational field'
See Dirac's brief treatment of the energy-momentum pseudo-tensor in the attached picture. Dirac is presumably integrating eq. (31.2) over the 4D "hypercylinder" defined by ##T_1 \le x^0 \le T_2## and ##\mathbf{|x|} \le R##, where ##R## is sufficiently large to include all the matter-energy fields in the system. Then \begin{align} 0 &= \int_V \left[ ({t_\mu}^\nu + T_\mu^\nu)\sqrt{-g}\, \right]_{,\nu} d^4 x = \int_{\partial V} ({t_\mu}^\nu + T_\mu^\nu)\sqrt{-g} \, dS_\nu \nonumber\\ &= \left(...
In Philippe G. Ciarlet's book 'An introduction to differential geometry', He gives the integrability conditions of the differential equations like this: $$ \partial_{i} F_{lj}=L^p_{ij} F_{lp},\,\,\,F_{ij}(x_0)=F^0_{ij}. $$ The integrability conditions for the existence of a global solution ##F_{lj}## is: $$ R^i_{jkl}\equiv\partial_k L^i_{jl}-\partial_l L^i_{jk}+L^h_{jl} L^i_{hk}-L^h_{jk} L^i_{hl}=0 $$ Then from the equation: $$\nabla_b e_a= \Gamma^c_{ab} e_c$$ Using cartesian basis ## e_I...

Similar threads

Back
Top