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Ludwik is not appeased with accelerations due to rotations, so I must
consider linear acceleration, which I will suppose is always due to
a force of some kind.
It is easy to discount the kinds of electric field which motivate
mechanical force, because at some point a macroscopic object will be
squashed if the acceleration is too great; the force needing to spread
over a wider area of application until a rather thin layer, perhaps
a monatomic layer is the limit.
And so I am finally left with the force of gravity, which it appears may be
multiplied without limit and which would provide an arbitrarily large
acceleration to a particle approaching a hole of sufficient mass.
brian whatcott <inet@intellisys.net>
Altus OK