The special theory of relativity is the result of two postulates:
- 1. The laws of physics are the same in all inertial
reference frames.
- Extention from the Newtonian principle of relativity:
- the laws of mechanics are the same for all observers in uniform motion.
- The speed of an object depends on the reference frame,
- however the speed of light in space is the same.
This java applet invites you to the world of space and time in special relativity.
There are two devices that utilize photons to measure time differences (some kind of clock).
- A mirror will reflect the photon when it reaches the top or bottom
of the device.
First, press Start button to begin the animation. Both devices are synchronized.
- Two Light pulses emitted from the ends (yellow rings)
- reach the center of the device at the same time.
Now, change the relative velocity from the selections ( 0.6c or 0.8c ) ,
- where c is the speed of light in
space.
You can change your frame of reference by moving your mouse button,
- within the area of the blue device or out of it.
The width of the moving device becomes smaller, ( From the marks, figure out the shinking factor! )
and the photons are not synchronized.
Light from the two devices is initiated when the sources touch each other.
Two light cones (in yellow) from two ends will reach the center of the device
- in your frame of reference at the same time.
So those two events are simultaneous in your frame.
So, those two events are not simulataneous in the moving frame.
- There is no such thing as absolute simulataneity.
Try to change your frame of reference by moving your mouse
- in and out of the moving device. ( The timing in your frame of reference
will reset to 0.)
- is not all happening at the same moment.
- even though the light from them arrived on the film at the same instant.
- an observer from some other galaxy.
The period of the clock in your frame is 1.0 s.
The number T at the left shows the period
for the photon's motion measured in your rest frame.
The period of the moving frame large than 1.0s , so the moving
clock runs slower.
An observer at rest with the clock sees the pulse moving up and down
with speed c.
The picture is very different when viewed from the other frame.
- As seen by the obeserver who is stationary with respect to the moving
device,
the pulse travels a distance given by ( c t' ). ( red path in the following figure)
In your frame, the pulse travels a longer diagonal path (white path ).
The speed of light is the same to all observers in inertial frames.
The pulse seen by you must take a longer time t,
- to traverse the longer distance ( c t ).
It follows from the Pythagorean Theorem that
( c t )2
= ( v t )2 + ( c t' )2
t'2 = t2 ( c2 - v2 )/c2
t = ( 1 - (v/c)2 )-1/2 t'
=
t'
- the clock is moving must be greater than the corresponding
time interval
seen by the inside observer with respect to whom the clock is stationary.
Your suggestions are highly appreciated! Please click hwang@phy03.phy.ntnu.edu.tw
Author: Fu-Kwun Hwang, Dept. of physics, National Taiwan Normal UniversityLast modified : More physics related java applets
Thank you Prof. Fred Trexler , for your suggestions to this web page.
Fred Trexler Professor of Physics , Spring Arbor College, MI U.S.A.