I'm not sure you can distinguish a "unit of energy". These can be changed
from one for to another. Suppose an atom with an "age" (since it emerged
from the big bang) of 12Gy absorbs a photon with an "age" of 10Gy (although
a CMBR photon would presumably have an age of 400,000 years since no time
elapses for photons!) ... what's the age of the excited atom that results?


On 8 February 2014 17:54, <[email protected]> wrote:

>
> On Saturday, February 8, 2014 4:41:13 AM UTC, Brent wrote:
>
>>  On 2/7/2014 8:16 PM, [email protected] wrote:
>>
>>
>> On Saturday, February 8, 2014 12:26:29 AM UTC, Russell Standish wrote:
>>>
>>> On Fri, Feb 07, 2014 at 03:57:47PM -0800, Edgar L. Owen wrote:
>>> > Ghibbsa,
>>> >
>>> > Let me clarify my previous answer a little.
>>> >
>>> > P-time runs at the same intrinsic rate everywhere in the universe
>>> though it
>>> > doesn't really have a 'rate' in the usual sense since it's prior to
>>> > dimensionality. However that rate is the speed at which the p-time
>>> radial
>>> > dimension of the hyperspherical universe extends. That extension
>>> actually
>>> > is or produces or generates the 'flow' of p-time.
>>> >
>>>
>>> I take it you predict that space has positive curvature (Omega > 1)?
>>>
>>> Note that evidence appears to contradict this, and is widely
>>> considered to be the hard evidence killing Tipler's Omega point idea.
>>>
>>> Or do you conceive of some method to compute this rate from a negative
>>> curvature?
>>>
>>> Furthermore, does your theory impose an embedding dimension for the
>>> spacetime manifold? Because the rate at which the radial dimension
>>> extends is crucially dependent on the embedding dimension.
>>>
>>> Note that General Relativity does not require a Euclidean embedding
>>> space.
>>>
>>> > So p-time runs at the same intrinsic rate and provides the processor
>>> cycles
>>> > of all the computations that produce the current information state of
>>> the
>>> > universe. Part of the results of those computations are the different
>>> > relativistic clock time rates of processes throughout the universe.
>>> >
>>> > Hope that makes it a little clearer....
>>> >
>>>
>>> Not much. How do you connect the clock speed of your hypothetical
>>> computer with the curvature of spacetime?
>>>
>>>
>>>
>>>
>> Hi Russell, I've been scratching around for ways to assemble Edgar's case
>> at its strongest, in terms of relativity, without actually adding anything
>> of my own (i.e. what he has said, just restated).
>>
>> I know this requires a stretch, maybe too far, of what you can do with a
>> frame in relativity. But here goes one possibility.
>>
>> Purely in the sense of how many moments there has been since the big
>> bang, allowing that every piece of energy in the universe (appropriately
>> nodding at dark energy) has its own unbroken history back to it. By
>> whatever measure of a 'moment' we like, shouldn't they all be resolvable in
>> terms of their history to the same number of moments
>>
>>
>> NO!  If each piece of matter carried a clock along (assuming it has
>> indentity) they would all read differently even where they came together
>> because they would have traveled different spacetime paths to that
>> meeting.  That's why I suggested that for any given point you take the
>> longest interval back to the CMB and call that the time-coordinate of that
>> point.  And if you took a set of all such points with the same coordinate
>> that's a way of defining a foliation of spacetime (provided it doesn't have
>> any singular stuff like black holes and cosmic strings in the way).
>>
>> Look at Ned Wright's UCLA tutorial online.  He describes several
>> different ways to define a cosmic "now" (but they don't agree with each
>> other).
>>
>> Brent
>>
>
> Brent I accept that already, but would plead that you are within the
> relativity paradigm there, whereas the paradigm that I stated
> was purely historic, in which we count two moments the same, specifically
> and only where the same defined 'moment' counts back to the big bang at the
> same count. I mean, in reality there's only going to be one and exactly one
> same moment for each unit of energy, or not? Can the distinction you raised
> just there, translate into, for the history that has happened already,
> individual units of energy, in terms of a single number of same defined
> moments since the big bang, can ever have 0 of that same count, or 2 or
> more of that same moment?
>
> Look, I know this is potentially and very likely stepping outside what
> physics tells us. But what I would argue, is that by trying on edgar's
> ideas in the first place, if we're doing so in a reasonably well-motivated
> sort of way, we are already doing that. So why not let's do it right. Start
> by looking for how it could true most generally, which means most
> universally. And apply a sensible standard, which would to look for a sense
> first, that would be true independently of relativity, such that it too
> could be totally true. At least as a starting point.
>
>>
>>
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