On Wed, Sep 4, 2024 at 8:08 AM Alan Grayson <[email protected]> wrote:


> *> it seems that the metric tensor FIELD is NOT well defined. AG*



*The metric tensor encodes spacetime curvature, and for every point in
spacetime that you can name I can give you a 4x4 matrix of unique
computable numbers that defines the curvature at that point. What's
ambiguous about that? It's true that I can't do that for points in
spacetime that you cannot name, but that is not a problem because you
cannot get experimental results from points that you cannot name. *

John K Clark    See what's on my new list at  Extropolis
<https://groups.google.com/g/extropolis>
wai





>
> On Wednesday, September 4, 2024 at 6:02:17 AM UTC-6 John Clark wrote:
>
>> On Tue, Sep 3, 2024 at 6:44 PM Alan Grayson <[email protected]> wrote:
>>
>> * > I fail to see how your comments relate to the possibly ambiguous
>>> concept of the latter. The metric tensor field seems ambiguously defined.*
>>
>>
>> *A N dimensional space is composed of an uncountable number of real
>> numbers but it can be unambiguously defined by just N countable rational
>> numbers, you can pair them up one to one. This is possible because there is
>> only a countably infinite number of COMPUTABLE real numbers, the same rank
>> of infinity as the rational numbers. So you can in effect give a rational
>> number name to every real number you are able to find on the number line.
>> You can do this even for a number such as π which is not only irrational,
>> it's transcendental, because it is also computable. You can use an infinite
>> series to get arbitrarily close to π.  *
>>
>> *The vast majority of numbers on the number line are NOT computable (and
>> have no name) but that's not really a problem despite the fact that the
>> vast majority of numbers on the number line are NOT computable because,
>> except for Chaitin's Omega Number, every number that a mathematician has
>> ever heard of is a computable number. Computable numbers can have names,
>> uncomputable numbers can not.*
>>
>

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