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Written by: BurtJordaan
Tuesday, June 17, 2008

This "perennial" is almost as old as Einstein's special theory of relativity itself. Einstein did not invent the paradox, although it was stimulated by his 1905 paper, where he spoke about the fact that two clocks that were separated, one staying inertial and the other one being moved away from the first one and then brought back again, will not read the same time.

The popular press explained it in terms of twins of closely the same age, where one twin sets off on a long, fast journey and eventually returns home. Special relativity then predicts that the "away twin" will be younger than the "at home" twin.

The "paradox" arises out of an abuse of special relativity's freedom to choose any inertial frame as the reference frame and make all calculations relative to it. The "abuse" on it's part arises out of choosing a non-inertial frame (the away twin) as reference and then making wrong conclusions---like that the home twin can just as well be considered as in motion relative to the away twin. This then means that the home twin should therefore suffer the same amount of time dilation as has been calculated for the away twin and could thus be considered to end up the younger one (or at least both twins still being the same age).

To confuse the issue even further, many explanations of the difference between the two reference frames are very confusing and unconvincing---even some given in reputable technical books. Search the web for "Too Many Explanations: a Meta-Objection" (the author found it on "http://math.ucr.edu") and see for yourself.

None of the one's discussed there is fully convincing either---which may be just another "meta-objection" (what does "fully convincing" mean anyway?) In my eBook "Relativity 4 Engineers" I give three reasonable explanations: (i) a simple "hand waving" argument; (ii) a very relativistic calculation and (iii) a more engineering-like representation and calculation. I will concentrate on the "engineering" solution here, using electromagnetic signals and relativistic Doppler shift.

Pam and Jim are twins that decided to put Einstein to the test. On January 1st, 2007 Pam quickly accelerated her spacecraft to a speed of 0.6c and flew away inertially for 4 years, when she will quickly turn around and head back to Earth at 0.6c again. Jim stays at home and the twins agreed to send each other a New Years greeting on every January 1st until Pam returns safely.

This scenario is illustrated in the Minkowski spacetime diagram, Figure 1, a split image for clarity. This shows a crucial non-symmetry in the signals that the home twin and the away twin receive. Although the amount of stretch and shrinkage of the received periods are the same, the amount of time that the signals are stretched and shrunk is very different between the respective twins.

Twin paradox with Doppler shift
Figure 1

The Doppler shift ratio (period of received signal (Tr) to period of transmitted signal (T) for the outbound leg (opening velocity) is

Tr/T = sqrt[(1+0.6)/(1-0.6)] = 2.0

and the same ratio for the inbound leg (closing velocity) is

Tr/T = sqrt[(1-0.6)/(1+0.6)] = 0.5,

as can be clearly seen in figure 1. The non-symmetry comes from the fact that the away twin receives compressed period signals immediately after turnaround, while the home twin has to wait until the first signal after turnaround arrives at home before noticing the event.

In the four years that Pam heads away from home, she will receive only two New Year's messages from Jim. This is because Jim here represents the T period of 1 year. Pam is the receiver, with the Tr period of 2 years. On her calendar she will receive "happy New Year 2008" only on Jan 1, 2009, and the next one ("happy New Year 2009") on Jan 1, 2011. Weird, but this is due to the increasing distance between them and the time light takes to cross the gap.

During her return trip, the situation is reversed, so in the last four years, she will receive eight New Year's messages from Jim, one every six months! She will receive the last (tenth) message, on New Year's Day 2015 on her calendar, as she makes a close fly-by of Earth.

Does this solve the twin paradox? Not quite, yet.

That was Pam receiving Jim's messages. At what rate will Jim receive New Year's messages from his sister? For the first eight years, he will also have to wait two years for every 'happy New Year' message. This means that it will be 2015 on Earth before Jim gets the message that his sister has sent on New Year's Day 2011, with a note that she has just turned around for the home leg of her trip.

Then, for the last two years, Jim will receive a New Year's message every six months - four of them. Add them up and Jim will receive only eight messages from Pam in the decade that he waited for her return. Conclusion: Pam recorded only eight years during her voyage, while Jim recorded ten years.

I hope this clears up at least some of the confusion that surrounds the "twin paradox".

Burt Jordaan (http://www.relativity-4-engineers.com)




 

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2 comments so far...

Re: The "Twin Paradox"

I'm sorry Burt, but this is about as "clear as mud". I consider myself to be an enlightened layman in the field of relativity, but I don't follow your reasoning. (I do accept the end result, however.) Could you perhaps pick one or more transmissions, both from Jim and from Pam, and calculate when they would be received in each other's "time". I was trying to visualize (say) Jim's 1st transmission. It happened on 1/1/08. Pam was 0.6 light years away at the time. Could you illustrate what her calendar said? I'm thinking that when Pam receives Jim's first signal, she is 0.6 + (1-0.6) = 1 light year away from Jim. I don't know the time dilation equation, but I'd assume Pam's calendar reads 1/1/10 when she gets the 1st signal. OK, I may be alright and may be able to work out the remaining details. I still don't understand this assymetry, however.

By DougJ on   Wednesday, June 25, 2008

Re2: The "Twin Paradox"

Hi Doug, you wrote:

"I was trying to visualize (say) Jim's 1st transmission. It happened on 1/1/08. Pam was 0.6 light years away at the time. Could you illustrate what her calendar said? I'm thinking that when Pam receives Jim's first signal, she is 0.6 + (1-0.6) = 1 light year away from Jim."

The relativistic Doppler ratio solves this scenario without any pain, but if you want to go through it the hard way, just to confirm the Doppler way, here it is:

If Jim could somehow read Pam's calendar when he sent that 1/1/08 signal, he would have seen 10/20/07, being 1/1/07 + 0.8 x 365 days. The 0.8 is Pam's time dilation relative to Jim. You are right that at that time, Jim will find Pam 0.6 ly away from him. In Jim's frame, he will know that his greeting signal travels at 1-0.6=0.4c relative Pam, so it will take 0.6/0.4=1.5 years to reach Pam. That means Jim's calendar will read 1/1/08 + 1.5 y = 7/1/09 when the signal reaches Pam. However, Pam's 0,8 time dilation factor means that on her calendar it takes only 0.8 x 1.5 = 1.2 years. Add that to her 10/20/07 and you get 1/1/09.

Easy, isn't it? ;) Not quite, it can be very confusing working it out this way, while those Minkowski diagrams show it at a glance!

Doug: "OK, I may be alright and may be able to work out the remaining details. I still don't understand this assymetry, however".

The asymmetry is caused the moment Pam ignites her rocket to turn around (year 2011 on her calendar). She will immediately notice a change in the Doppler shift of signals from Jim. Jim's calendar will read 2012 at that time, but he will not notice any change in Doppler shift of Pam's signals until his calendar time has passed the year 2015. Because of the distance, that delay is caused by the time light takes to travel to him from the turnaround point.

Shout if you need more help in wrapping your head around it.

Regards, Burt Jordaan (http://www.relativity-4-engineers.com)

By BurtJordaan on   Thursday, June 26, 2008

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