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Re: The worm problem



Ludwik and Donald objected to my statement of the rubber worm problem as
being ill formed. I went over Ludwik's complaints, but I easily recognized
that he was being ironic. Donald, however, makes me wonder. The problem I
posed is included below. I would appreciate a serious comment on just how
this problem is ill formed.

I call this (inappropriately) "The Rubber Worm Problem": You are provided
with an elastic rope exactly one kilometer in length. At time t=0 a worm
starts to crawl from one end of the rope to the other at a speed of one
centimeter per second. The rope itself is attached to a tractor which
is stretching the rope at a rate of one kilometer per second. The problem
as it was originally stated specifies that the rope lengthens by one
kilometer at the end of each second, and it is this discrete version of
the problem I will continue with here. At the end of one second the worm
had marched one centimeter toward the other end of the rope. At that
instant he is instantaneously transported to the 2 centimeter mark on a
rope which is now two kilometers in length. By calculation you will see
that at the end of the second second he will be three centimeters along
his way on the two kilometer rope, which will then lengthen to three
kilometers, taking the worm to the 4.5 cm point, etc.

First question: Has our worm embarked on a Sisyphusian journey; will he
ever reach the end of his rope? If not, prove that.

Evidently the answer to the first question is "No" as the sophisticate
will recognize. Otherwise, what's the point of the question? The second
question is: How long will it take the worm to reach the end of his rope?

A physicist will assume the worm needs no more than one coordinate to
specify position. The sample calculation certainly makes that clear. How
could this problem possibly be misinterpreted? In my view it comes
nearer being overspecific.

Leigh


I can't help with your question because it seems quite well specified to
me. I would prefer to reformulate it into an equivalent form. Since the
effect of the stretching is not to move the worm backward but to give it a
longer rope to go along, the effect is the same as if instead of stretching
the rope we slowed the worm, so it would be centimetering 1,1/2,1/3,1/4,
.... in successive seconds. So it turns into the question when that series
= 10^5.

Richard Grandy
Philosophy & Cognitive Sciences
Rice University