- #1
- 3,766
- 297
I am reading ''Modern Physics`by Tipler and Llewellyn, 4th edition, page 52.
They say something which, unless I am completely confused, is completely wrong.
I cite (Ulysses is the twin in the spaceship, they use [itex] \Delta t_{Earth}= \gamma \Delta_{spaceship}[/itex] and then say:
''...we cannot do the same analysis in the frame of the spaceship because it does not remain in an inertial frame during the round trip; hence it falls outside of the special theory and no paradox arises,. The laws of physics can be formulated so as to be invariant for accelerated observers, which is the role of general relativity''
(emphasis mine).
As far as I understand, this entire paragraph is completely wrong. There is no problem treating accelerated observers in SR. I am surprised to see this in a fairly recent textbook (2003).
Am I totally in the left field?
They say something which, unless I am completely confused, is completely wrong.
I cite (Ulysses is the twin in the spaceship, they use [itex] \Delta t_{Earth}= \gamma \Delta_{spaceship}[/itex] and then say:
''...we cannot do the same analysis in the frame of the spaceship because it does not remain in an inertial frame during the round trip; hence it falls outside of the special theory and no paradox arises,. The laws of physics can be formulated so as to be invariant for accelerated observers, which is the role of general relativity''
(emphasis mine).
As far as I understand, this entire paragraph is completely wrong. There is no problem treating accelerated observers in SR. I am surprised to see this in a fairly recent textbook (2003).
Am I totally in the left field?