- #71
yoron
- 295
- 2
No, I'm not taking it too seriously, I hope? It just bugs me :
And yes, I also wondered about it DA.
But assuming both in uniform motion and that 'locality' of 'c' holds (using 'c' as your 'clock'), and that 'B' doesn't start measuring until he gets the message defining the 'time rate' from 'A'. Starting from its arrival for example. Then it seems to me that as 'B' receives the message from 'A', they have a 'timing' protocol that will work relative those two? That is, they have set up a 'causality chain' of sorts, that will hold relative them.
That we can have a third observer defining it differently doesn't change the relation in between 'A' and 'B', does it? Neither does it change the way they now can 'time it' from the arrival of that message, assuming them both moving uniformly. To assume that this relation won't hold seems, to me, to imply that 'B' can answer 'A' and that 'A' then could get this answer even before he sent his message in a worst case. And that one can't be correct.
As for the entanglement? Doesn't the measurement define all of it? If 'A' measure a momentum, won't 'A:s' interaction with the entanglement, measuring it, impart a added momentum, and also redefine the momentum for 'B' after he received the message that he can start his?
I'm ignoring the Hotta injection for this, just asking if you can define it otherwise than that A:s interaction measuring the momentum will add a momentum from A:s measurement, that is valid for the whole entanglement? No matter how HUP treats it, the idea should hold, or?
==
To make it somewhat easier to think about, let us assume that they are uniformly moving, of a identical mass distribution/gravity, and at rest relative each other. 'Time dilations' are hard to avoid :)
And yes, I also wondered about it DA.
But assuming both in uniform motion and that 'locality' of 'c' holds (using 'c' as your 'clock'), and that 'B' doesn't start measuring until he gets the message defining the 'time rate' from 'A'. Starting from its arrival for example. Then it seems to me that as 'B' receives the message from 'A', they have a 'timing' protocol that will work relative those two? That is, they have set up a 'causality chain' of sorts, that will hold relative them.
That we can have a third observer defining it differently doesn't change the relation in between 'A' and 'B', does it? Neither does it change the way they now can 'time it' from the arrival of that message, assuming them both moving uniformly. To assume that this relation won't hold seems, to me, to imply that 'B' can answer 'A' and that 'A' then could get this answer even before he sent his message in a worst case. And that one can't be correct.
As for the entanglement? Doesn't the measurement define all of it? If 'A' measure a momentum, won't 'A:s' interaction with the entanglement, measuring it, impart a added momentum, and also redefine the momentum for 'B' after he received the message that he can start his?
I'm ignoring the Hotta injection for this, just asking if you can define it otherwise than that A:s interaction measuring the momentum will add a momentum from A:s measurement, that is valid for the whole entanglement? No matter how HUP treats it, the idea should hold, or?
==
To make it somewhat easier to think about, let us assume that they are uniformly moving, of a identical mass distribution/gravity, and at rest relative each other. 'Time dilations' are hard to avoid :)
Last edited: