Re: What causes time dilation?
From: Old Man (nomail_at_nomail.net)
Date: 08/30/04
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Date: Sun, 29 Aug 2004 20:08:25 -0500
"Edward Green" <spamspamspam3@netzero.com> wrote in message
news:eca320d0.0408290353.6b821f59@posting.google.com...
> "Old Man" <nomail@nomail.net> wrote in message
news:<FuGdnVs954KCCrPcRVn-pw@prairiewave.com>...
> > "hunkahunkaburninluv" <some@where.come> wrote in message
> > news:2p75lgFhs9v9U1@uni-berlin.de...
> > > First, I am not a physicist. I do desktop publishing as a profession,
but
> > am
> > > an avid sci-fi reader.
> > >
> > > Two related questions. What causes time to slow down as a ship
approaches
> > > the speed of light? Is there any possibility that we could create the
> > effect
> > > on a stationary object? Imagine a room in which time was slowed down
to
> > say
> > > 1% normal. One year might in it might equal 100 years.
> >
> > Sure you can do that by modification of the space-time
> > metric, that is, by increasing the curvature of space, for
> > some limited region of space. For, example, see to it
> > that the gravitational field is increased in that special
> > room of yours.
> >
> > Actually, a field isn't required. All you need is a huge
> > amount of gradient-free, negative gravitational potential.
> > You can do that by constructing a massive spherical
> > shell about yourself. Then, through peepholes in the
> > shell, you can watch time fly by on the shell's outer
> > surface, all in weightless comfort.
>
> That's a very cute idea, Old Man.
>
> You could use that as a refrigerator: Say your peach is ripe. You
> just pop it in your massive spherical shell, and, a week later, when
> you want to eat it, you take it out, a few minutes older. Better than
> a refrigerator.
>
> I wonder somewhat about the physics of watching time fly by, though.
> If a some light at frequency f came down your peephole, would its
> frequency on receipt be slowed by the same factor?
>
> No, I guess that's not so: light climbing out of a gravity well is
> red-shifted -- i.e., _not_ speeded up to the frequencies we would
> expect for its particular spectral transmission. It carries the
> stigmata of its slow birth. So I guess the reverse is true, and light
> falling in would be blue shifted to the internal observer. Which does
> solve a queueing problem for all the light which would otherwise be
> waiting around to fall in your peephole. Not to mention the even more
> significant precognition problem for light climbing out.
>
> > However, for a large factor in time-rates between you
> > and those on the surface, the people on the surface
> > would be living (?) in a huge gravitational field. So, lets
> > put them out in space, almost an infinite distance away.
> > Then the ratio in time rates between you and them is
> > given by
> >
> > delta_t (you) / delta_t (them) = sqrt[ 1 - 2 M / R c^2 ]
> >
> > where M and R are the mass and radius of the shell,
> > and G is the universal gravitational constant. Note that
> > your time approaches zero (their time approaches infinity)
> > as the mass of the shell, M, approaches that of a black-
> > hole of radius, R, but everyone lives in free-fall comfort.
> >
> > See: "Gravity: An Introduction to ... " by J.B. Hartle
> > ISBN 0-8053-8662-9
>
> Should be banned by the GR technicians, of that is an example of its
> teachings: it was clearly comprehensible! :-)
>
> (P.S. He asked about kinematic time dilation, not gravitational. But
> yours was a lovely answer anyway ;-).
Hartle's book is pretty neat. Rather than plowing through
the GTR formalism, he provides conceptual shortcuts via
the space-time metric and 4-vector length invariance.
[Old Man]
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