Volcano said:
Hi,
I hope asking in right forum.
I'm trying to understand proper time concept but I'm afraid couldn't understand the reason of answer for below question.
"
Figure 37-18 shows two clocks in stationary frame S (they are syncronized in that frame) and one clock in moving frame S'. Clocks C1 and C1' read zero when they pass each other. When clock C1' and C2 pass each other,
(a) Which clock has the smaller reading
and
(b) which clock measures a proper time?
"
What I couldn't understand here is, how can I determine the observer in this type of question. I'm sure those clocks giving the hints about events but how? And yes, (a) and (b) asking the same thing. Proper time always smaller.
Let's start with the S' frame in which the C'
1 clock is at rest at the spatial origin. I have drawn a spacetime diagram to represent this situation:
I'm assuming that the speed of light is one foot per nanosecond and I draw dots at each tick of a clock. Each dot represents an event with its own coordinates in this Inertial Reference Frame (IRF). Does this make sense to you?
Now we want to see what the events for this clock looks like in the S frame. To do that, we have to realize that the S frame is moving to the left with respect to the S' frame and we plug the numbers for each event into the Lorentz Transformation and make a new IRF diagram:
Now we can add in the other two clocks that are at rest in the S frame:
I have labeled a couple tick marks for each clock with colors matching the colors of the worldlines for each clock. You can see that when the C'
1 reaches the C
2 clock, it has less time on it, 8 nsecs compared to 10 nsecs.
As has been pointed out by others in this thread, each clock keeps track of its own Proper Time. The grid lines mark off the Coordinate Time for each IRF which matches the Proper Time for clocks that have been synchronized to the Coordinate Time and remain stationary in the IRF. This would apply to clocks C
1 and C
2 in the last IRF. We don't normally refer to the Proper Time on such clocks since they match the Coordinate Time and are usually included just to visualize the Coordinate Time. I'm guessing this is the point of the problem and so the answer they are seeking is that it is the C'
1 clock that is measuring the smaller Proper Time when it reaches the C
2 clock but technically, all clocks are measuring Proper Time.
Your statement that Proper Time is always smaller isn't complete--smaller than what? The correct answer is that the Proper Time of a moving clock in an IRF is smaller than the Coordinate Time of the IRF (provided that the clock was synchronized to zero at the Coordinate Time of zero). Note that this is true for the entire trip of the C'
1 clock, even when it is not colocated with another clock. There is always a Coordinate Time (and Location) for the moving clock that you can compare its Proper Time to.
As far as observers go, we normally place observers at rest at the spatial origin of an IRF which means that the C'
1 clock would represent an observer in the first IRF diagram and the C
1 clock would represent an observer in the last IRF diagram. The problem didn't mention any observers. What is your interest in observers?