The Origin of Matter and Time | Space Time | PBS Digital Studios
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-----Original Message-----
From: 'Brent Meeker' via Atoms and the Void <atv...@googlegroups.com>
To: atvoid <atv...@googlegroups.com>
Sent: Fri, Aug 2, 2019 1:20 am
Subject: Re: What Is Thing-ness?
Neat! But I didn't like his explanation of the twin paradox. Special relativity works just fine for accelerated world lines. It's just that non-geodesic world lines are shorter than geodesic ones.
Brent
You're right, BUT in some sense you can still invoke acceleration if you think about it carefully.
Feynman invokes acceleration in his essay on the twins paradox, so this can't be too crazy. The standard refutation of acceleration as an explanation is the three clock scenario , an example where no physical clock experiences any acceleration.at all. However, this still involves a change of frame for an "effective" clock which is the clock with less duration. A frame change can't be had without acceleration.
So the accelerated effective clock ages slower.
--The effective clock must end up in the same frame as the clock that truly experienced no frame change , hence no acceleration. In SR time is a "personal" parameter. It makes no sense to compare the "time rate" of clocks in different frames to get any objective measure of duration.
Bob Zannelli
On 8/1/2019 5:57 PM, spinozalens via Atoms and the Void wrote:
--The Origin of Matter and Time | Space Time | PBS Digital Studios
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Feynman invokes acceleration in his essay on the twins paradox, so this can't be too crazy. The standard refutation of acceleration as an explanation is the three clock scenario , an example where no physical clock experiences any acceleration.at all. However, this still involves a change of frame for an "effective" clock which is the clock with less duration. A frame change can't be had without acceleration.
So the accelerated effective clock ages slower.
--The effective clock must end up in the same frame as the clock that truly experienced no frame change , hence no acceleration. In SR time is a "personal" parameter. It makes no sense to compare the "time rate" of clocks in different frames to get any objective measure of duration.
Bob Zannelli
On 8/1/2019 5:57 PM, spinozalens via Atoms and the Void wrote:
--The Origin of Matter and Time | Space Time | PBS Digital Studios
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Feynman invokes acceleration in his essay on the twins paradox, so this can't be too crazy. The standard refutation of acceleration as an explanation is the three clock scenario , an example where no physical clock experiences any acceleration.at all. However, this still involves a change of frame for an "effective" clock which is the clock with less duration. A frame change can't be had without acceleration.
Sure it can. That's the three clock example. The elapsed time measure is just "handed off" to a different inertial frame.
But that's the point. You can't "hand it off" without a frame change. How it handed off? One rocket sends am EM signal in frame 1 to be observed in frame 2. The EM signal involves acceleration. You have an effective clock that changes frame.

-----Original Message-----
From: 'Brent Meeker' via Atoms and the Void <atv...@googlegroups.com>
To: atvoid <atv...@googlegroups.com>
Sent: Fri, Aug 2, 2019 2:00 pm
Subject: Re: What Is Thing-ness?
On 8/2/2019 10:00 AM, spinozalens via Atoms and the Void wrote:
Feynman invokes acceleration in his essay on the twins paradox, so this can't be too crazy. The standard refutation of acceleration as an explanation is the three clock scenario , an example where no physical clock experiences any acceleration.at all. However, this still involves a change of frame for an "effective" clock which is the clock with less duration. A frame change can't be had without acceleration.
Sure it can. That's the three clock example. The elapsed time measure is just "handed off" to a different inertial frame.
But that's the point. You can't "hand it off" without a frame change. How it handed off? One rocket sends am EM signal in frame 1 to be observed in frame 2. The EM signal involves acceleration. You have an effective clock that changes frame.
The outgoing rocket passes the ingoing rocket and the ingoing rockets clock is set to match that of the outgoing clock as they pass. They are at the same place at that moment (B on the diagram).
I don't see that any acceleration is involved. The only thing that must change frames is information. Of course information is physically embodied, but that's true when the sender and receiver are relatively stationary too. We don't think of that as involving acceleration.
Brent
This is not the three rocket example you need to show different duration of clocks. These clocks were never synchronized to start. What they read for time is irrelevant
Bob Zannelli
?? I don't understand that remark. I thought it would go without saying that the red rocket and Earth clocks are identical and they are set together at A. The grey rocket also has an identical clock which is set to agree with the red rocket clock as they pass one another at B (set to 2011). Then when the grey rocket passes Earth, its clock reads 2015 while the Earth clock reads 2017. Why is that irrelevant? It's the twin paradox, but without any acceleration.


-----Original Message-----
From: 'Brent Meeker' via Atoms and the Void <atv...@googlegroups.com>
To: atvoid <atv...@googlegroups.com>
Sent: Fri, Aug 2, 2019 3:17 pm
Subject: Re: What Is Thing-ness?
Brent
This is not the three rocket example you need to show different duration of clocks. These clocks were never synchronized to start. What they read for time is irrelevant
Bob Zannelli
?? I don't understand that remark. I thought it would go without saying that the red rocket and Earth clocks are identical and they are set together at A. The grey rocket also has an identical clock which is set to agree with the red rocket clock as they pass one another at B (set to 2011). Then when the grey rocket passes Earth, its clock reads 2015 while the Earth clock reads 2017. Why is that irrelevant? It's the twin paradox, but without any acceleration.
Brent I quickly corrected my comment in a second post
Here it is again
Sorry I didn't notice the stationary state. However, notice that the "effective " clock at point B has changed frame. to be able to get back to the same ( approx) spacetime point at the stationary state to compare clocks.
Bob Zannelli