D
dangineer
Guest
MA, I appreciate you taking the time to try to explain your position to me. I really am trying to see things the way you do, so I can understand your opinion.
Relativity doesn't allow for an absolute frame of reference, neither mathematically or conceptually, so I would have to conclude that you choose to not apply relativity to what you observe. But I don't think this is what you are are getting at.
"I choose to consider events in the absolute sense and work with them in the absolute sense, then calculate how they will appear to different relativistic frames."
When you say this, it sounds as if you are considering things in an absolute physical framework (the most common of which is Newtonian mechanics) and then converting them into a relativistic framework. To me this is really confusing, since you cannot convert between the two. Newtonian mechanics is really just a special case of relativistic mechanics. Perhaps this is not what you are saying either, though.
Could you demonstrate your approach through an example? Maybe we can start with a common one, such as the precession of Mercury's orbit.
When Newtonian physics are applied to this situation, what we observe doesn't match what we predict (apohelion of Mercury's orbit doesn't move). But then when we apply GR, the results do match. We've even measured this effect from several different frames of reference through robotic missions to the inner solar system. So I assume that there should be some absolute reference frame where Mercury's orbit doesn't precess.
Relativity doesn't allow for an absolute frame of reference, neither mathematically or conceptually, so I would have to conclude that you choose to not apply relativity to what you observe. But I don't think this is what you are are getting at.
"I choose to consider events in the absolute sense and work with them in the absolute sense, then calculate how they will appear to different relativistic frames."
When you say this, it sounds as if you are considering things in an absolute physical framework (the most common of which is Newtonian mechanics) and then converting them into a relativistic framework. To me this is really confusing, since you cannot convert between the two. Newtonian mechanics is really just a special case of relativistic mechanics. Perhaps this is not what you are saying either, though.
Could you demonstrate your approach through an example? Maybe we can start with a common one, such as the precession of Mercury's orbit.
When Newtonian physics are applied to this situation, what we observe doesn't match what we predict (apohelion of Mercury's orbit doesn't move). But then when we apply GR, the results do match. We've even measured this effect from several different frames of reference through robotic missions to the inner solar system. So I assume that there should be some absolute reference frame where Mercury's orbit doesn't precess.