Thanks for the replies. I will look on it later. It seems that you refer to
point masses when volume distributions have to be considered.

David

David Jonsson, Sweden, phone callto:+46703000370



On Wed, Mar 3, 2010 at 4:42 PM, Stephen A. Lawrence <[email protected]> wrote:

>
>
> On 03/03/2010 10:27 AM, Stephen A. Lawrence wrote:
> > I don't really understand how tidal and retarded effects can cancel.
> >
> > Tidal effects are only detectable on extended bodies, and the "tidal
> > force" generally (always?) has nonzero divergence.
>
> Actually I think that's wrong -- I don't think it's *divergence* that I
> mean here; the tidal forces "diverge vertically" and "converge
> horizontally" and the result is the net divergence stays zero.
>
> Just fished around a bit on the Web.  You've got tidal forces when the
> Weyl tensor is nonzero.  See, for instance:
>
> http://www.answers.com/topic/weyl-curvature
> http://en.wikipedia.org/wiki/Congruence_%28general_relativity%29
>
> That's from GR but the same general concept is going to apply to
> Newtonian gravity as well, since the theories are essentially identical
> anyplace where conditions are mild enough for humans to live comfortably
> (surface of the Sun, or anyplace inside the orbit of Mercury, are
> examples of places where it's not "comfortable").
>
> I don't think retarding the gravity field results in a nonzero Weyl
> tensor, and in "small field" conditions these tensors are going to be
> combining more or less linearly, so, again, I don't see how the effects
> of retardation can cancel tidal forces.
>
>
> >
> > On the other hand, the retarded gravity effect typically manifests
> > itself as a rotation of the acceleration vector versus what you'd
> > calculate given the (calculated) current position of the gravitating
> > body.  It's detectable by its action on point particles, which don't
> > accelerate as Newtonian theory would predict.
> >
> > But the divergence of retarded gravity is still zero where the mass
> > density is zero.
> >
> > So, again, I don't see how they can cancel.
> >
> > I also question this assertion:
> >
> > [DJ:]
> >> If either of these effects are acting on a body its orbit will become
> >> unstable.
> >
> > I don't understand what you mean by this.  Tidal forces act on all
> > planets, without exception, if they're in orbit.  But as long as the
> > planet's own gravity is larger than the tidal forces acting on it, that
> > doesn't result in instability in its orbit.  In fact the effect of tidal
> > forces can be to "lock" a planet into a particular orbit and rotation
> > rate -- in other words, tidal forces can make the orbit *more* stable.
> >
> >
> > On 03/01/2010 04:13 PM, David Jonsson wrote:
> >> Hi
> >>
> >> My own posting today on Usenet.
> >>
> >> I would be glad if someone could help me with how to calculate this for
> >> some examples to see if there is any reason in it.
> >>
> >> David
> >>
> >> David Jonsson, Sweden, phone callto:+46703000370
> >>
> >>
> >> ---------- Forwarded message ----------
> >> From: *David Jonsson* <[email protected]
> >> <mailto:[email protected]>>
> >> Date: Mon, Mar 1, 2010 at 6:41 PM
> >> Subject: Can retarded gravity be counteracted by tidal acceleration?
> >> To: [email protected] <mailto:[email protected]>
> >>
> >>
> >> Could the accelerating tidal effects
> >> http://en.wikipedia.org/wiki/Tidal_acceleration
> >> be cancelled by retarded gravity effects
> >> http://en.wikipedia.org/wiki/Speed_of_gravity ?
> >>
> >> If either of these effects are acting on a body its orbit will become
> >> unstable. Tidal forces are almost always accelerating and the retarded
> >> gravity effect is decelerating an astronomical body. Maybe there are
> >> conditions when the two effects balances each other and maybe these
> >> conditions form the structure known as the Titius series which is
> >> purely empirical and not yet explained
> >> http://en.wikipedia.org/wiki/Titius–Bode_law
> >> .
> >>  Exoplanets give new cases to test this idea. Moons, rings and pulsars
> >> could also be tested against this idea.
> >>
> >> David
> >>
> >
> >
>
>

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