austin0 said:
DO you think that gamma could have a different equation giving different relationships?
Could the metric have a different form and still correspond to the gamma relationship of space and time?
DaleSpam said:
I don't know what you mean by "the gamma relationship of space and time". Gamma is a particular expression: . It is easy to get this expression from the Minkowski metric. As far as I know, it is not possible to get it from other metrics without doing a transform to a (local) Minkowski coordinate system. Although Samshorn's point that v=dS/dt does expand the class of metrics where you can get it.
"the gamma relationship of space and time". is the inherent relationship that as the spatial part of motion increases relative to the temporal component, the temporal part is decreased relative to other inertial frames. It appears that it was this relationship that determined the metric signiture, the only deviation from a Euclidean metric.
would you agree that this seems to be an intrinsic quality of spacetime geometry??
.
austin0 said:
dt (untransformed coordinate time) =====> {BLACK BOX} ======> dtau (transformed time -by the gamma factor)
No matter what may have occurred in the black box, Quija board,quantum computer, whatever, that makes no difference.
It is clear that the final value is related to the initial value by the gamma factor?
do you disagree with this statement?
DaleSpam said:
There is no black box which takes dt as input and gives dτ as output in general. For certain specific problems (constant speed particles) in specific metrics (Minkowski) you can simplify the inputs to the black box as you describe. But in general the inputs to the black box are all of the dxi, not just dt, and in fact in some metrics there is no dt to begin with.
This time I
was presenting an analogy ;-) in this case the black box represented whatever math you cared to employ to achieve your result. that it also entailed a dx was overlooked for simplicity.
The point of course being what was inside the box was irrelevant , The outcome making it clear that in some form the gamma factor had to be present in the box and that the operation itself was functionally a gamma (Lorentz) transformation what ever it might be called.
DaleSpam said:
Of course, I do agree that any physical experiment where the outcome is a function of gamma will have the same outcome regardless of the metric used to analyze the experiment. The point I was making is that the correct outcome can be obtained by simple application of the law as stated, without at any point explicitly bringing gamma into the analysis nor doing any transforms.
Yes you did accomplish your goal without explicitly invoking gamma or doing a transformation within a limited semantic loophole regarding what is called a transformation.
DaleSpam said:
For the first case, the muons in the cyclotron, we can write their worldline as P=(t,r,\theta,z)=(a T, R, a 2 \pi, 0) where a is the number of "laps" around the cyclotron, R is the radius of the cyclotron, and T is the period for one lap. So we have
\tau_P=\int_P d\tau=\int_0^a \frac{d\tau}{da}da=\int_0^a \sqrt{\frac{dt^2}{da^2}-\frac{dr^2}{da^2}-r^2\frac{d\theta^2}{da^2}-\frac{dz^2}{da^2}} \; da=\int_0^a \sqrt{T^2-0-R^2 4 \pi^2-0} \; da =a\sqrt{T^2-4\pi^2 R^2}
Looking at your math it appears to me that at this point =a\sqrt{T^2-4\pi^2 R^2}
you have a distance measurement and a time interval. That you are simply applying the Pythagorean operation to these quantities. the operation itself composites vector components and returns a single value of length. in this case a spacetime length expressed in units of proper time.
The fact that the spatial measurement was not linear does not seem relevant as by this point it is simply a value.
Harking back to an earlier proposition of mine that the gamma was hiding in the pythagorean operation as a geometric gamma function , this seems to be supported by your calculations.
As you say, you did
not explicitly employ the function or a gamma value , yet the end result was in fact, transformed.
Since what
was in the box was the pythagorean operation this would imply that it was the culprit.
This transformation can be easily demonstrated regarding linear motion within the context of Minkowski geometry.
Regarding the other's arguments about integrating with gamma. In this case with motion limited to angular displacement , is integration even necessary?.
wouldn't it be a simple measurement of distance determined by pi?
austin0 said:
Perhaps I am not understanding correctly (quite possible) but to me the term itself , invariant interval necessarily implies a multiplicity of frames to have any meaning.
austin0 said:
It also didn't seem to apply within a single frame as time intervals are automatically proper time within that frame.
T
DaleSpam said:
his is not true in general. For example, consider a rotating reference frame. For large values of r the t coordinate is spacelike.
Wouldn't it be more correct to say it was true in general but not necessarily true in certain limited cases like rotating frames , which I would think was not even an inertial frame. This is SR
austin0 said:
So i understood it to be turning coordinate intervals between events occurring relative to another frame, F ,into a form/value that would agree with all other frames evaluation of that interval relative to F. ------> F's proper time.
Is this incorrect??
DaleSpam said:
I am not certain that I understand what you are saying, but I don't think that is incorrect, just a bit "cumbersome".
Relativity, particularly GR, is a geometric theory. Just think about the spacetime interval as a strange "distance" in spacetime. Distance is a geometric feature, it exists independently of any coordinate system that you might draw on top of the geometric features.
I agree, cumbersome ;-)
yes I understand the spacetime interval,,, the question was; Was determining the interval a transformation.?
austin0 said:
It also seems to me that within a frame the metric is still Galilean/Euclidean.
With the assumption of synchronicity of all clocks within the system.
Functionally equivalent to absolute time.
DaleSpam said:
Not in general, particularly for non-inertial reference frames.
We are talking about SR , inertial frames, Not GR or accelerating frames which are outside the topic of this thread and discussion.
No offense intended whatsoever, but you have a general habit of taking questions and statements that have an explicitly limited context and subject, and either answering them with generalities or refuting them for lack of generality.
austin0 said:
So the Minkowski metric actually only applies to other frames or is this not so?
DaleSpam said:
This is not so. It applies to every inertial frame, not just "other" inertial frames.
Wouldn't it be truer to say it is
applied within every inertial frame regarding every "other" inertial frame.
In any Minkowski diagram the designated rest frame is in a purely Cartesian coordinate structure with a Euclidean metric or do you disagree with this??
If you disagree could you explain what you mean by applying to every frame?