Quote:
Originally Posted by NewOldGuy
The reasoning there is still confusing.
First it is simply "agreed" that the speed of light will be 299,792,458 meters per second. This is not measured, it is just agreed to as the standard by international consensus.
Then from that, we derive the length of a meter as the distance traveled by light in 1/299,792,458 seconds.
The only thing that makes it not circular is that C is not based on a measurement at all, but just on an agreed constant value. Without measurement, how is this assumed? With measurement, the definition becomes circular. The official explanation seems to get around this by making it clear it is not a measured value.
The two definitions absolutely depend on each other and neither can exist without the other. They are jointly defined to be in agreement, and neither one is independently defined.
Your objection is noted, but it’s not unique to using c to define lengths. The original standard for the meter was a metal bar that was defined to be one meter long (actually the bar was longer but had two marks on it defined to be one meter apart. That is irrelevant to the point, though, so I will refer to this as a meter bar). How did we know the length of the meter bar was 1 meter without measuring it?
The question, while it seems to be a valid question is actually not a legitimate question. The confusion lies in that you seem to think there’s somehow a “true” meter out there that we can use to check our definition of the meter to see if it really is a meter. No such “true” meter exists; we define our standard units any way we find useful. The old meter bar had a length of one meter precisely because we all agreed that it did. There is no deeper meaning than that.
That’s an incredibly important step, though. The agreement upon a standard is what allows measurements in the first place. A measurement is really nothing more than a comparison of an observed quantity to a standard quantity. With our meter bar in hand, we could now go out and measure the lengths of all kinds of stuff. One of the things we wanted to measure is the wavelength of light. We developed ways to measure it very accurately. In fact our measurements got so good, the limiting factor holding us back from making even better measurements was our meter bar. It made sense to scrap the meter bar at that point and define the meter in terms of wavelengths of light. Technically we picked light generated in a particular way and defined its wavelength. How do we know it actually had that wavelength? No better reason than “Because we said so.”
Continuing in similar vein, we used our new standard to measure other lengths. One thing we wanted to measure is c. This isn’t a length, but a velocity. Nonetheless a velocity is just a ratio of length to time, so measuring a velocity involves measuring a length (and a time of course). Again we got good at it, so good that the measurement accuracy was limited by our standard wavelength, so scrap the standard wavelength and define the value of c.
In some regard, this is actually a much better standard. There is no standard length in nature. That is, there’s no phenomenon in nature that always involves the same distance. There is a standard velocity though, namely c. This standard velocity is actually much more fundamental than just being the speed at which photons move. The constant c is a defining constant in the geometry of flat spacetime. It also is involved in the fine structure constant, which gives the strength of the electromagnetic force. Being the speed at which photons move is almost an afterthought regarding the role c plays in physics. In short if c isn’t constant the universe would be a very different place; we’d notice, and it would not be just that the speed of light was different.
This is also the case for other values in nature, such as the quantum of action, given by Planck’s constant, h and also the gravitational constant G, which relates energy to spacetime curvature. Most notably, these constants h,c and G can be mathematically combined to give values with units of mass, time, and length. We could theoretically define our units therefore by simply defining these three constants. These are the true fundamental definitions of our units.