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A Physics Quiz of a different type
Last night, the neighbors came over for a visit, and (somehow) we got on the topic of Relativity. One neighbor, a non-science kind of guy (but very intelligent) wanted to know why you can't go faster than the speed of light.
My response was that at one end of E=MC^2 you have pure mass, and at the other end you have pure energy. You can't go past the endpoints. As you go closer to C, M decreases and E increases, since C is decreasing* *That is, since C is relative to a fixed point, as you hit, say, 0.75 C, there is only 0.25 C "left", so C is actually smaller. OK, he accepted that as reasonable , but in my mind, that's not right. So, in one or two sentences, why is there a limit to the speed of light? Thanks. |
Re: A Physics Quiz of a different type
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This is only a theory. Some scientist believe that you can go faster than the speed of light, we just have no idea how to do it. A particle accelerator in Europe actually detected what they believe to be partials that can travel faster than the speed of light. I personal think it will be possible to go faster than the speed of light in the future.
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Someone please correct me if I'm wrong or show a link or reference if I'm right. I can't find where I heard that. I find the Wikipedia explanation pretty good. It should be noted what the gamma factor is (the funny y). The Wikipedia article refers to how it approaches infinity, etc., so it may be helpful to see what it actually is. It often (or almost always) pops up in the math for these types of equations, so they made a variable for it. ![]() Oh, here's a joke. The tachyon is a hypothetical particle that would move faster than light. So... The barkeeper says, "Hey, we don't serve tachyons here," and a tachyon walks into the bar. |
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That's not to say we haven't been wrong about our understanding of the universe before—only that our understanding of the universe today is several orders of magnitude greater than in any other era of history, and because of this, experimental error is the more likely explanation for the results you mention. Besides, any application of faster-than-light anything is still firmly within the realm of speculation (or daydreaming)—in other words, I don't think there's any good reason to believe "it will be possible to go faster than the speed of light in the future". Also, "only a theory" doesn't really mean what you imply. Wikipedia has a dense article on theories, but the important concept is that "theories are collections of hypotheses that are logically linked together into a coherent explanation of some aspect of reality and which have individually or jointly received some empirical support". In other words, calling something a theory doesn't call it into question so much as it indicates that there has been systematic scientific inquiry into the subject. Aside: 4 citations to Wikipedia in 4 replies? That must be a record. (And it's not a bad thing.) |
Re: A Physics Quiz of a different type
I'm no expert mathematician, but I believe Don said he wanted an answer in "one or two sentences", and nobody has provided anything less than a paragraph related to the subject.
Being a high school student that has not taken physics yet, this question is very interesting, and I would also appreciate a short and concise answer, instead of having to read 4 long paragraphs. In conclusion, I would very much be interested in a short answer as to WHY it isn't possible to go faster than the speed of light. Thanks! "In order for knowledge to be understandable, it must be accessible. We live in a world today where people don't want to read long books to learn things. Bring the knowledge to the people, and they will learn it". - Sal Khan, Khan Academy |
Re: A Physics Quiz of a different type
Yeah, you're right on the simplification part.
The Wikipedia article mentioned this, I'll try to sum it up. It takes an increasing amount of energy to approach the speed of light, in a way that you would need an "infinite" amount of energy to travel at the speed of light. The physics of relativistic motion, which deal with speeds comparable to the speed of light, show that the mass (or relativistic mass) increases as you approach the speed of light and the energy of the object approaches infinity. So, it takes more energy to move something more massive, and infinitely so when approaching the speed of light. |
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Cool!
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Particle "A" is traveling at c/2 in the +X direction in inertial reference frame XY. Particle "B" is traveling at speed c/2 in the -X direction in the same reference frame. See Figure 1. In a second inertial reference frame X'Y', particle "B" is at rest. How fast is particle "A" traveling in this second reference frame? See Figure 2. |
Re: A Physics Quiz of a different type
This brings up an interesting situation. If you were traveling at the speed of light with a flashlight in your hand... When you turned it on would no light be emitted? If you are at half the speed of light and turn it on, does the light leave at half the speed of light?
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Wouldn't it be slightly slower than c because of the air and lens of the flash light. :yikes:
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Still has a flash light with a lens, although I suppose he could remove it.
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Of course you still have the glass of the bulb...
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That makes sense.
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I'll take a stab at your problem, Ether.
System 1 (XY): The relative speed of the two particles is c/2-(-c/2) [speed of A - speed of B], which results in 2*c/2 or c, relative to each other, as viewed from a neutral position. System 2 (X'Y'): In this case, the system is fixed onto Particle B in the above problem, which is assumed to be moving at -c/2 (from the reference point in System 1's point of view). The relative speed remains the same, as the motion did not change (if viewed from System 1's reference point), so observers on Particle B see Particle A leaving at speed c. Which brings up the question: Do observers on Particle B really see Particle A, or does it just vanish as it moves? There are some related thought experiments, such as the speed of a bullet fired going forwards versus the speed of a bullet fired going backwards (to an outside observer); in Al's particular case, the real question is does an observer in another reference frame witness light traveling at 2*c? (And if so, does that redefine the speed of light in that observing reference frame? :ahh:) |
Re: A Physics Quiz of a different type
Special relativity all comes from Einstein's two postulates:
1. The laws of physics are the same in all inertial reference frames (keeping this around from Galilean relativity). 2. Light travels at the same speed in all reference frames. Because all of the math and conclusions about various relativistic phenomena are drawn from these, this is the two sentence answer sought by the OP. msimon's original Wikipedia quote basically sums up the theoretical implications of superluminal speeds and why it is generally dismissed as impossible. For more blood and gore, read on. To Al, because light travels at the same speed (in vacuum) in all reference frames, no matter how fast you are going, light will always emanate from a source you are carrying in all directions at the speed of light. To a stationary observer you are passing, the same is true. This is related to the fact that light has no medium (there is no ether), so an source's motion cannot be measured relative to anything meaningful. This was observed in the Michelson-Morley experiment and was a driving force behind Einstein's insight. To Ether, a Lorentz transform will spit out the answer. Let's establish two events in space time (unprimed coordinates are in frame XY, primed coordinates in frame X'Y'): Event 1 with both particles at the origin, x1 = x1' = ct1 = ct1' = 0. Event 2 with particle A after time T in frame XY, x2 = c/2*T, ct2 = cT, x2' = ?, ct2' = ? Frame X'Y' is moving with velocity c/2 to the left so B = -0.5 (B = v/c), y = 1/sqrt(1-B^2) = sqrt(4/3) (Beta and gamma are usually the letters used here but B and y will suffice). The Lorentz transform (which one can derive from the mathematical and physical properties of Einstein's postulates) is: x' = y*x - yB * ct ct' = -yB * x + y * ct So plug in above and x2' = y*cT* (1/2-B) = ycT, ct2' = y*cT * (-B/2 + 1) = 5/4*ycT. Particle A's velocity in frame X'Y', then, is (x2'-x1')/(t2'-t1') = 4/5 c. NOT c as one would expect from Galilean relativity. One could also apply the canned velocity transform (based on this) and get the same result. The increasing mass concept is something I feel is not quite accurate. It exists to reconcile conceptually whats going on with Newtonian physics. Really, the momentum that is conserved is with respect to a proper velocity (because no one can agree on a common clock anymore), and this screws up all our nice F = ma tools (but F is still dp/dt !). As you go faster and faster, space-time is distorted such that the extra acceleration is accounting for more and more energy. Calculating the Energy of a relativistic particle (again from Lorentz transforms) gives K= (y-1)mc^2, where m is always just the rest mass, and the quickly diverging behavior is due to y as opposed to m getting bigger. E = mc^2 is just a statement about the rest mass of particles, since when v = 0, y = 1, so K = 0. The total energy is E = ymc^2. Well that was fun. |
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An observer sitting on Particle B (i.e., in reference frame X'Y') will observe Particle A's speed to be (c/2+c/2)/(1+(c/2)(c/2)/c^2) = 0.8*c |
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And yeah that. That's the velocity transform: u' = (u+v)/(1+uv/c^2), u is the particle's velocity, v is the velocity of the prime frame relative to the non-prime frame. |
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The relativistic addition of velocities is (u+v)/(1+u*v/c^2). |
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Heh, yeah, a little dimensional analysis would tell you that much.... I'm tired.
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As for Al's' thing with the flashlights, an observer standing still would see a solid beam of light, just hanging there in the air, like an infinite, glowing sausage.* *Not really, but it's cool to think about that, no? |
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That means you CAN reach c. Going past c is what requires infinite energy, reaching c needs just a smidgen less than infinity. And yes, we're assuming the object rest mass is nonzero |
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At v=c, B=v/c=1, so y=1/sqrt(1-B^2) is already undefined (or infinity, if that's how you want to define dividing by zero). |
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Its an asymptote.
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Re: A Physics Quiz of a different type
Someone else offered an explanation as well:
As you gain energy, the mass of the object increases, because energy has weight. This includes kinetic energy. So as speed increases, so does mass, requiring more and more energy to maintain acceleration. At some point, it gets really massy, such that you can't push it hard enough to accelerate it. I am told that this "weight gain with energy" has actually been measured, but I can't find that reference. =========== OK, does a photon have mass? If yes, then it cannot travel at the speed of light, but since it does, at rest it must be massless. (Yes, it has momentum, but that's a special case. In theory you can approach the speed of light using a flashlight as your propulsion unit. Might take a while though...) Are there any nonzero-mass particles/objects that travel at c? Can there be? |
Re: A Physics Quiz of a different type
Eh, why try to travel so fast when we could instead slow light to a crawl? The applications for that seem more pragmatic in our lifetimes than attempting to do anything at light speed.
For instance, could we trap light (and thus its energy) in order to accumulate enough for release when we want it? It'd bring a whole new meaning to 'solar energy'. There's been some work already in that direction and it seems at least a little less complicated. |
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When light is reflected, at the point of reflection, is the speed zero? |
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Using a flashlight for propulsion would definitely work (albeit very slowly) because of the momentum of the outgoing photons, but it is no different than any other Newton III interaction; you will still accelerate only asymptotically to the speed of light. |
Re: A Physics Quiz of a different type
Okay, are you ready?
If you go at the speed of light, assuming you can in the first place, you will either dissolve at a sub-atomic level instantaneously, or merge into light. Brings a new meaning to "don't go into the light...", doesn't it? |
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Have you dissolved yet ? |
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