Re: Slabinski and Mingst/Stowe disagree in Pushing Gravity
- From: "TC" <tclarke@xxxxxxxxxxx>
- Date: 4 May 2005 05:46:52 -0700
Paul Stowe wrote:
> On 3 May 2005 19:02:12 -0700, "TC" <tclarke@xxxxxxxxxxx> wrote:
> > Then why did you use the word "empirically"?
>
> Because, like Newton & his equation, it is tied directly to
> observation. It is one thing to say,
> q' = (¥2G/c^2)m/r
> and another to solve for ¥, by 'linking it' to an observed value.
You can always make one observation fit a theory by adjusting
a constant [well almost always]
> Like Newton when he said, I observe that,
> F o< Mm/r^2
> And the solves for the magnitude of the proportionality constant
> BY linking it back to measured observations...
Newton had a whole lot, enormously more support,
than you can claim.
> That's the 'empirical' part!
But the form of the equation is based on a theory.
It is not a purely empirical formula like a regression equation.
Better to term it a theoretical formula.
> > [But there must be a mistake somewhere in your paper or in
Slabinski's
> > or else your results would agree with Slabinski.]
> As I told you earlier, now that we've been made aware of this,
> it IS being worked on. My gut says, we're both right. We'll
> see.
OK.
......snip for brevity.....
> > [Paul argues that m/r is the best fit by comparing some
> > heat fluxes from various planets]
> > Thereby he disproves LeSagian gravity (which predicts m
> > dependence) and supports classical theory wherein m/r
> > is deposited in the body from its gravitational collapse
> > and is currently escaping from the body as relict heat.
> Sigh, why do you deliberately distort? You know damned well
> that I've said no such thing.
I know you didn't say that your results support classical
gravity theory.
You say excess heat fits an equation of the form Km/r.
_I_ pointed out that this can be seen as support for classical
gravity theory.
> No,r do I think so. You also
> know damned well that if what you are claiming is true there
> would have never been and issue of 'anomalous excess heat'
> for the gas giant planets.
I just point out that potential energy has form m/r.
I'm really not that familiar with all the possible explanations
people have posited. But any one having an m/r dependence would
fit the same data.
By the way the fit is not all that good.
> Further, you should also know that that very same ¥ term is
> utilized to decompose G into its constitute parts of ¿ & µ.
What does this have to do with the alternative explanation
provided by classical gravity theory? The decomposition is
only part of your theory.
Also, Slabinski does a decomposition and derives an upper
bound from it.
> These in turn, are used in the classic derivation of the drag
> equation, which, just amazingly, matches the precise magnitude
> of that observed in Pioneer & Ulysses spacecraft.
> Two from one, an amazing series of coincidences, eh?
Now you have to tackle the binary pulsar, deflection of
light by the sun, gravitational redshift ...
Tom
.
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