Lorentz Factor Explained for Laymen: Twin Paradox

Santural
Messages
19
Reaction score
0
I looked up Twin Paradox, and I understand the concept of time in SR, and also understand the Einstein synchronization convention concept, but now there is just something I don't get here:
I looked at twin paradoxes and apparently you must use the Lorentz factor (or it's inverse, anyway) to figure out the time a specific journey would take on the Earth rest frame (or along the lines. Can't put it in words.)
So, the only thing is, what does each letter stand for in :
\displaystyle\epsilon=\sqrt{1-v^2/c^2}?

Which I believe is the inverse of the lorentz factor.

Thanks in advance,
Santural : Below the average layman.
 
Last edited:
Physics news on Phys.org
Santural said:
So, the only thing is, what does each letter stand for in :
\displaystyle\epsilon=\sqrt{1-v^2/c^2}?
Are asking what v and c stand for? v = speed of the traveling twin (or moving frame); c = speed of light.
 
Right! Thats part of what I need. However:
Wikipedia says:
Consider a spaceship traveling from Earth to the nearest star system: a distance d = 4.45 light years away, at a speed v = 0.866c (i.e., 86.6% of the speed of light). The round trip will take t = 2d / v = 10.28 years in Earth time (i.e. everybody on Earth will be 10.28 years older when the ship returns. Those on Earth predict the aging of the travellers during their trip will be reduced by the factor \epsilon = \sqrt{1 - v^2/c^2}, the inverse of the Lorentz factor. In this case ε = 0.5 and they expect the travellers to be 0.5×10.28 = 5.14 years older when they return...(goes on and on)
(I added the bold).
What is that epsilon? Where is 0.5 derived from?
 
Santural said:
Where is 0.5 derived from?

By plugging numbers into that formula:

\epsilon = \sqrt {1 - \frac{v^2}{c^2}} = \sqrt {1 - \frac{(0.866c)^2}{c^2}} = \sqrt {1 - 0.866^2} = 0.5

Or have I misunderstood your question?
 
...:rolleyes: hehe...um...:-p ...really, just um...hehe...my bad...

I guess I was being a LITTLE dumb there, sorry.
 
Thread 'Can this experiment break Lorentz symmetry?'
1. The Big Idea: According to Einstein’s relativity, all motion is relative. You can’t tell if you’re moving at a constant velocity without looking outside. But what if there is a universal “rest frame” (like the old idea of the “ether”)? This experiment tries to find out by looking for tiny, directional differences in how objects move inside a sealed box. 2. How It Works: The Two-Stage Process Imagine a perfectly isolated spacecraft (our lab) moving through space at some unknown speed V...
Does the speed of light change in a gravitational field depending on whether the direction of travel is parallel to the field, or perpendicular to the field? And is it the same in both directions at each orientation? This question could be answered experimentally to some degree of accuracy. Experiment design: Place two identical clocks A and B on the circumference of a wheel at opposite ends of the diameter of length L. The wheel is positioned upright, i.e., perpendicular to the ground...
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