<p><BR/>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'>because I am talking here partly of new physics I'll say it with the qualifier - given current physics - both are impossible, that means that if one seemingly requires length expansion that something is wrong with current physics (SR) or with my analysis of the problem, you know where I stand</DIV></p><p>I don't understand how you conclude a length expansion is required by a photon chasing an astronaut.</p><p>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'>I don't understand that, 'the observer from the source' must see moving ship and everything on it as contracted, moving objects are contracted</DIV></p><p>The observer doesn't physically see anything contracting. Only upon taking a measurement and comparing results with the astronaut could contraction be inferred. Let me put it this way... Contraction can be measured and experienced. It is a very real phenomena, but you can't visually see it or photograph the reality of it.</p><p>The speed of light is a measureable quantity. Photons emitted simultaneously in a moving object's rest frame will not be recieved simultaneously. In order for the eye or a camera to process the image of an object, it must essentially believe it is recieving the light simultaneously. In the non-relativistic world it is interpreted as and appears to be simultaneous, but not at relativistics speeds. </p><p>Take a meter stick and look at it. Stationary, you recieve light from the front end before the back end and, with light being so fast, you interpret it as simultaneous and you recieve the full image. Now, say it is approaching you at near light speed. In order for you to see the entire meter stick, the far end of the stick would have to emit it's light <strong>before</strong> the front end to catch up with the moving front end. By the time that light catches up to the front end so it can emit its light (to make the image simultaneous), the meter stick will have moved, thus elongating the image and negating the contraction. The image will always be a distortion of reality.</p><p>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'>don't try to find something complicated in my example</DIV></p><p>I'm not. Special Relativity is complicated enough on its own. I actually think you are over simplifying your though experiment without realizing the complications of SR. </p><p>Replying to:<BR/><DIV CLASS='Discussion_PostQuote'>I am talking about explanations commonly used when explaning SR to laymen or to begining students, my point is everybody is always interested in dealing with oncoming ray of light because without SR we would have the astronaut measure higher than speed of light and everybody always want's to show that is not so, however catching up light is not so sexy becasue astronaut is in no danger of measuring higher than light speed and typically nobody takes it up or thinks about it BUT it is just as important, SR has to pass all such tests so that it is integrated theory, it can ill afford any hanging ends much less contradictory ones <br /> Posted by vandivx</DIV><br /><br />I've fallen pray to some of the 'commonly used' explanations... they are not always correct or can be so simplified that you can lead yourself down the wrong road. The Big Bang balloon and gravity rubber sheet analogies are 2 that are quite simple, yet often misleading. I have no illusions of being well versed in SR, but I think I have a handle on some of the basics. I even grasp some of the less complicated equations.</p><p>Let's go back to your light catching up concept:</p><p>Let's take an astronaut that leaves Earth travelling at .99C for 100 years. After one year, I, here on Earth, emit a beam of light in the direction of the travelling astronaut. What I will see is the light beam finally catch up to the astronaut right at 99 years. I will see that the astronaut has been travelling for 100 years, covered .99 light years distance and the beam of light caught up to him after it has been travelling for 99 years (remember, i waited one year to shine my light).</p><p>What the astronaut sees. At .99C will give a gamma factor of 7 (I think it's 7.1, but for ease of math, i just round). Time will pass for him at 1/7th the pace and length contraction is 7 times what I experience in my rest frame. So the length and time of his trip is ~14 light years distance at ~14 years time when the light reaches him.</p><p>Considering we synchronized our clocks prior to his departure, he now looks at his watch after 1 year (a time we agreed on), he turns around a looks at Earth, he will see that Earth is 7 light years distance away. From this new (apparent) stationary reference frame, it would appear the earth is speeding away from him slowing the Earth's time down by a gamma factor of 7. He is 7 light years distance away when, after my time dilated 1 year (according to him), I shine my light. He looks at his clock and odometer and realizes that it is, in fact, he who has the gamma factor of 7, he realizes he can easily solve the twin paradox and understand the reality of the situation.</p><p>Essentially, from each of our perspectives, we will disagree (yet both be correct) what time I shone my light and how far away the astronaut was when I did.</p><p>The astronaut in his reference frame, still looking back at earth, will see the beam begin when he is 7 light years distance. Given the constancy of photons in a vacuum, this beam of light will reach him in about 7 years travelling 7 light years distance (still his stationary reference frame looking backwards) and the Earth will have sped away an additional 7 light years distance. Thus, the astronaut will measure that he is 14 light years distance from Earth when the light reaches him. </p><p>Obviously, from this perspective, it still takes 14 years for the light to reach the astronaut. His "real" reference frame looking forward, it also take 14 years. Either way you look at it, it takes 14 years and light is travelling at a constant in which ever reference frames he chooses.</p><p>No paradox and no legnth expansion. At least, that's how I see it... I could always be wrong. <img src="http://sitelife.space.com/ver1.0/content/scripts/tinymce/plugins/emotions/images/smiley-laughing.gif" border="0" alt="Laughing" title="Laughing" /> </p> <div class="Discussion_UserSignature"> <div> </div><br /><div><span style="color:#0000ff" class="Apple-style-span">"If something's hard to do, then it's not worth doing." - Homer Simpson</span></div> </div>