What Is the Frame of Reference for Measuring Velocity?

In summary: So 1/30th the speed of light is still in the range where the simple addition still gives a result that is very close to the correct value. But if you go to 0.9 c or 0.99 c, the error is huge. In short, if you are not sure, ask a physicist.In summary, The speed of an object relative to another object can never reach or exceed the speed of light, regardless of their individual speeds relative to a third object. This is due to the principles of Special Relativity, which state that the speed of light is constant for all observers. This leads to effects such as time dilation and length contraction, which have been observed and
  • #1
DrWarezz
33
0
Hi all,
I'm pretty young, and thus don't understand any of the relativity theory, well; it's more of a case of "I don't understand WHY..", if you know what I mean :eek:\

Basically, going to the rule that no mass can equal/breach the speed of light, well, I'm confused here. Not about the most obvious of; "WHY?" (I'll tackle that another time I think :uhh: ), but, what do you measure an objects velocity relative to?

For example:

Planet A (Moving < way) Planet B ('still') Mass C (Moving > way)

Let's say that 'Mass C' 'took off' from planet B. And is traveling at over half the speed of light (possible). And Planet A, is moving in the opposite direction to the Mass C at over half the speed of light (possible). Well, a problem occurs here; Mass C's velocity is over the speed of light, relative to Planet A.

I understand this is a common question, but I hope that someone can explain to me, ie; what you measure the masses velocity relative to? And clear up any other 'mess'? :biggrin:

Thanks a lot in advance,
[r.D]
 
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  • #2
Even though A and C each move over half the speed of light in opposite directions relative to B, the speed of C relative to A is still less than the speed of light. Funky huh? Counter-intuitive, totally unobvious, yet Einstein made this totally coherent mathematically. Let us know if you want the equations.
 
  • #3
Yes please :)
Thanks - [r.D]
 
  • #5
Let v and w be the speeds of A and C relative to B, then the speed of C relative to A (or vice-versa) is u :

[tex]u = \frac{v + w}{1 + \frac{vw}{c^2}}[/tex]

Clearly, with speeds we are used to (much less than c), the denominator is nearly 1, so that what we have learned prior to relativity is still the best way to calculate in most practical cases. (don't confuse c = speed of light and C = your flying object)
 
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  • #6
Thanks, I'm still not clear though :confused:
Even though A and C each move over half the speed of light in opposite directions relative to B, the speed of C relative to A is still less than the speed of light.

I don't quite understand why the speed of C relative to A is still less than c :confused:

I've found a website using Doc Als' link, which explains einsteins velocity addition, but I haven't read it yet. I will later :smile: -- I'm guessing that that will explain it a bit more clearly?

Thanks alot,
[r.D]
 
  • #7
Yup. If you insert v = 0.5c (A going half the speed of light relative to B) and w = 0.5c (C going half the speed of light relative to B), you get u = 0.8c (C going 80% the speed of light relative to A, not 100% as a simple addition would predict). Any other v and w you insert that is less than c will give u < c.
 
  • #8
:smile: Thanks alot, Gonzolo!
Is the reason for why no object relative to any other object can breach the speed of light related to Time Dilation? If so, could you elaborate a little on how?

Thanks alot, have a good weekend,
[r.D]
 
  • #9
Oh yes, another thing:
You say that the simple addition works with small numbers/velocities. What range of numbers would you say are 'small'? ie; What number onwards should you use this theory, etc, on?
ta - [r.D]
 
  • #10
DrWarezz said:
:smile: Thanks alot, Gonzolo!
Is the reason for why no object relative to any other object can breach the speed of light related to Time Dilation? If so, could you elaborate a little on how?

Thanks alot, have a good weekend,
[r.D]

This is all intimately related. So is "length contraction" - a 10-ft dragster car going near c might only be 8 ft long for the spectator.

All these effects are consequences of the postulate ( = an educated guess = hyposthesis, = the basis of Special Relativity) that the speed of light c is always the same for anyone in any situation. This means that for the spectator, the speed of the light emitted from the dragster's headlights is c, not "dragster speed + c". And for the driver, it is also c.

Now suppose there is a light on the left of the dragster that sends a pulse towards a mirror on the right and comes back. For the driver, it takes a time t = carwidth/c to go back and forth. But for the spectator, the lightpulse will have moved obliquely so that it will have traveled a greater distance. Since c = d/t is a constant, the time it has taken is also greater. So for the spectator, intervals of time (the time it takes for light to go from the left to the right and back) in the car are greater than they are for the driver. Each reflexion can be considered to be the tick of a clock. This is time dilatation. I believe it has been verified experimentally with very sensitive (atomic) clocks on board aircrafts (not cars) flying for an extended period of time and comparing these to identical atomic clocks on the ground.

The speed equation is another consequence of the postulate. I won't demonstrate it now, but as you can see, putting the dragster speed w in the equation and the speed of light v = c, it will give :

[tex]u = \frac{c + w}{1 + \frac{cw}{c^2}} = (\frac{c + w}{1 + \frac{w}{c}})\frac{c}{c} = \frac{c + w}{c + w}c = c[/tex]

... still c. Adding a velocity to c, still gives c, just like I said earlier.

For your second question, note the number [tex]\frac{vw}{c^2}[/tex] in the speed equation. When v and w are each 0.1 c = 30 000 000 m/s, the whole denominator becomes 1.01 (= 1 would mean regular speed additions, from the numerator). So below about 10 000 000 m/s, it's no use taking about special relativity. Experiments can be done with aircrafts only because atomic clocks are extremely sensitive.
 
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  • #11
Wicked. Thanks a lot for all the help, Gonzolo.
I think I get it :D

ta,
[r.D]
 
  • #12
Gonzolo said:
... For the driver, it takes a time t = carwidth/c to go back and forth...

That should be t = 2*carwidth/c. :grumpy: But the reasoning remains the same.
 
  • #13
This what theory of relativity all about. the calculation you did was in accordance to he Newtonian mechenics. according to thery of relativity , on order to keep c the maximum speed the time start dilating also change occurs in distance too to keep 'c' the maximum speed.
 
  • #14
Thanks.

Is there a reason why c = 299 792 458 ms, that we know?
Like; why not: 299 792 459 ms? (assuming it's actually not). Is there some sort of formula which explains this velocity?

Thank you.
[r.D]
 
  • #15
Not that I know of. I explain it to myself by saying that we wrongly chose the lengths of a meter and a second. You can do all of physics with c = 1 "some other speed unit" (1 light-year per year or whatever). The physics is independant of the units.

You could say that [tex]c = 1/ \sqrt{\epsilon \mu}[/tex], but this only displaces the question to why do [tex]\epsilon[/tex] and [tex]\mu[/tex] have their own values? Physicists are usually better off using c to explain the rest of physics, rather than the other way around.
 
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  • #16
Thanks :) lol

Oh, also: This is kind of embarrassing to ask, but; What is 'mass' exactly? What differs it from matter, and what happens when an objects mass increases? :eek:\

Thanks alot,
[r.D]
 
  • #17
Trying to answer "what is mass" can open up quite a pandora's box. Here are a few related notions, depending on which theory you use :

= related to inertia (classical, Newton etc.)
= quantity of matter (classical, Newton etc.)
= depends on the number of atoms, nucleons (this displaces the question to what is the mass of a nucleon?)
= caused by Higgs boson (particle physicist's domain)
= causes space-time curvature (general relativist's domain)

Someone else may want to answer how space-time curvature and Higg's boson are compatible, this fringes on the limits on what is observable and thus on the limits of what is solidly explainable. Whether there is an "exact" answer, I do not think so.

In special relativity, there are distincly two types of mass : rest mass and relativistic mass. Rest mass is exactly "whatever mass is that we are used to." - an electron has a rest mass of about 10E-31 kg, classically as in relativity. The relation between rest mass and relativistic mass is :

[tex]m = rest mass/\sqrt{1-(\frac{v}{c})^2}[/tex]

So if you accelerate the electron to 0.9 c, its mass is about double or so. 0.99 c : triple etc. (not exactly, but you get the idea). A rough way of putting it is that instead of gaining speed, a particle gains in relativistic mass when it nears c (except within its own frame of course, where it stays = rest mass)

A photon can also be said to have relativistic mass (since [tex]E = mc^2[/tex], [tex]m = E/c^2 = photon energy/c^2[/tex]). But a photon has no rest mass. Trying to find the rest mass of a photon with the first equation gives c/c in the denominator, but dividing by zero is undefined, this implies that the rest mass of something that goes c is undefined. The definition [tex]m = E/c^2[/tex] remains valid though for a photon's relativistic mass.
 
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  • #18
Gonzolo said:
Let v and w be the speeds of A and C relative to B, then the speed of C relative to A (or vice-versa) is u :

[tex]u = \frac{v + w}{1 + \frac{vw}{c^2}}[/tex]

Clearly, with speeds we are used to (much less than c), the denominator is nearly 1, so that what we have learned prior to relativity is still the best way to calculate in most practical cases. (don't confuse c = speed of light and C = your flying object)


sorry, but the only way i could get .8c in your equation was to take out the [tex]c^2[/tex] from the bottom fraction. if you where to put in .5c in both v and w like you gave the example of, you would get [tex]u = \frac{1}{1.25}[/tex] which = .8 i tried using the [tex]c^2[/tex] in the bottom and couldn't get .8. i also tried using 2\2 on the bottom equation to get a similar fraction without using big numbers. like i multiplied .25 (.5 x .5) by 2 and get .5. then i squared 2 and get 4. .5\4 is the same as 1\8 which is .125 and 1\1.125 doesn't = .8. if you could explain how you get it, it'd help out alot. thanks
 
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  • #19
never mind. i figured it out. i messed up when i tried to use 2\2. instead, i should have just used one which would have gotten me .25/1. then you would add the 1 and get 1/1.25. sorry, forget the question.
 
  • #20
Just for fun (I'm getting use to this Latex!) :

[tex]u = \frac{v + w}{1 + \frac{vw}{c^2}} = (\frac{0.5c + 0.5c}{1 + \frac{0.5c * 0.5c}{c^2}}) = (\frac{c}{1 + \frac{0.25c^2}{c^2}}) = (\frac{c}{1 + 0.25}}) = \frac{1}{1.25}c = 0.8c[/tex]
 
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  • #21
ah, i caught another problem that i did lol. when i multiplied .5c by .5c, i forgot to make the change the c to [tex]c^2[/tex].
 
  • #22
Okay..
so, what is ment exactly if an objects mass increases? Do the particles become more compressed?
Thanks alot,
[r.D]
 
  • #23
More massive means more energetic, and it gains in momentum. Its energy and momentum can increase indefinitely (unlike its speed). That's why particle accelerators have been getting bigger and bigger. The bigger and more powerful they are, the more energy you can give to the particles.

With "compression", you might be referring to Lorentz contraction, which is the space equivalent of time dilatation. It is also quite fun. A single particle however doesn't have much of a length. Contraction would apply to objects with a well-defined length, or volume.
 
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1. What is a frame of reference for measuring velocity?

A frame of reference for measuring velocity is a coordinate system that is used to describe the motion of an object. It is a fixed point or set of points that is used to measure the position, velocity, and acceleration of an object at a specific point in time.

2. How is a frame of reference determined?

A frame of reference can be determined by choosing a fixed point or set of points that are considered to be at rest. This can be a stationary object or a specific location on a map. The chosen frame of reference should be stable and not moving in relation to the object being measured.

3. Why is a frame of reference important in measuring velocity?

A frame of reference is important in measuring velocity because it provides a standardized way to describe an object's motion. Without a frame of reference, it is impossible to accurately determine an object's speed or direction of movement.

4. Can a frame of reference affect the measurement of velocity?

Yes, a frame of reference can affect the measurement of velocity. Different frames of reference can result in different measurements of an object's velocity, as the object may appear to be moving at different speeds or directions depending on the chosen frame of reference.

5. How do we choose the most appropriate frame of reference for measuring velocity?

The most appropriate frame of reference for measuring velocity depends on the situation and the object being measured. It is important to choose a frame of reference that is stable, easily identifiable, and relates to the object's motion. For example, the ground may be a suitable frame of reference for measuring the velocity of a car, while the sun may be a suitable frame of reference for measuring the velocity of a planet.

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