One could consider the rest frame of the CMBR as an "absolute landscape" I
suppose. One over which the Earth is hurtling at some rate, iirc.


On 8 February 2014 16:28, meekerdb <[email protected]> wrote:

>  On 2/7/2014 6:43 PM, [email protected] wrote:
>
>
> On Saturday, February 8, 2014 12:44:30 AM UTC, Brent wrote:
>>
>>  On 2/7/2014 2:45 PM, [email protected] wrote:
>>
>>
>> On Friday, February 7, 2014 10:30:06 PM UTC, Brent wrote:
>>>
>>>  On 2/7/2014 1:37 PM, [email protected] wrote:
>>>
>>>
>>> On Monday, February 3, 2014 6:27:14 AM UTC, Brent wrote:
>>>>
>>>>  On 2/2/2014 10:12 PM, [email protected] wrote:
>>>>
>>>> Namely that however you jig it, there's still going to
>>>> be huge spacetime distortion representing the sun and a tiny one
>>>> representing the earth, which - I thought - had to bias the objectively
>>>> true relation between the sun and the earth for the earth being
>>>> gravitationally dominated by the sun not the other way around.
>>>>
>>>>
>>>> So the question was whether one could just consider the Sun, calculate
>>>> the spacetime metric due to its mass, and then calculate the orbit of the
>>>> Earth as an inertial path in that metric?  In that case of course the
>>>> answer is no.  The metric has to take into account the mass of the Earth as
>>>> well as the Sun.  Just as in Newtonian theory, the Sun and the Earth, and
>>>> Jupiter and the other planets all move around their mutual center-of-mass.
>>>> The center-of-mass is roughly near the surface of the Sun on the side
>>>> nearest Jupiter.
>>>>
>>>> Brent
>>>>
>>>
>>> Hi Brent - Sure, but is it ok to look at the sun and the earth together,
>>> purely as their geometry's in spacetime, and say "that one goes around that
>>> one" to the same sort of accuracy we can say the earth goes around the sun
>>> without invoking relativity. Or is doing that running foul of the basic
>>> principles in play of relativity ?
>>>
>>>
>>> I'm not sure what you're asking.  The corrections to a simple
>>> "stationary Sun, orbiting Earth" due to Jupiter are much bigger than any GR
>>> effect.
>>>
>>> Brent
>>>
>>
>> if  you're willing to keep trying I would also like to...but please be
>> assured I will understand anytime you no longer want to. So trying again
>> here, I would first recap one sense of what this has been about....
>>
>> - I related an experience I had a few years back, when some people much
>> more knowledgeable than I in relativity...at least factually
>> speaking...argued that relativity was a fundamentally different way of
>> explaining the universe (with no dispute from me so far)....such that, you
>> literally could not sensibly talk about frame-free visualizations. I
>> responded that I thought that was only true up to a point, because for
>> example, the spacetime geometry of a much larger and much smaller object,
>> could be visualized as a single landscape for the purpose of saying
>> something very general, like "that one goes around that one".
>>
>> Which they explicitly then ruled out.
>>
>> Of course, this statement was always untrue strictly speaking because
>> both go round a common centre of mass. But the question here, is:
>>
>> - was that more knowledgeable source  correct
>>
>> - was I correct
>>
>> - was one but not the other exclusively correct, if so which one
>>
>> - was there a good chance neither were correct, and you'd have to see
>> what was actually said to be sure
>>
>> - Is what I am saying to you now, which I think is a fairly good capture
>> of what I said then, correct .....so far as it goes
>>
>>
>> My friend Bill Jefferys who used to teach astronomy at Univ of Texas says
>> it doesn't matter what reference frame you choose as far as the physical
>> events go, it just makes the math harder or easier.  So sometimes you use a
>> geocentric frame and sometimes a heliocentric frame and so forth...
>>
>> Brent
>>
>
> but can you throw the relative character out of the window, and speak
> of an 'absolute landscape' implied by relativity theory that is made up of
> all the gravity wells, that definitely suggests a 'reality' that goes
> beyond the principle of equivalence. In that, the landscape shows what's
> big and what's small, so the relation between them, in one big picture.
>
> I ask this in context that acknowledges it wouldn't be any good
> for resolving much useable knowledge about the world. In fact none at all,
> save that reality does imply such a reality is really there.
>
>
> True.  Although this "absolute landscape" would look different according
> to one's perspective (position, motion, etc) it hopefully represents the
> intersubjective agreement of all possible observers.  If you express this
> landscape only in terms of invariants, not coordinates and not relative to
> a particular observer or frame, then you could call it "absolute", but as
> you note that tends to be a messy representation to work with, so we tend
> to use some particular representation; the same way we navigate with flat
> map projections instead of charting courses on globes.
>
> Brent
>
>
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