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Re: test problem



Of course you are correct if we have such a "coil bound" spring, which has
no "room" to compress from its relaxed condition. But in the typical
problem a mass on a spring (no gravity - or horizontal) is presumed to be
able to oscillate about its relaxed condition - why should adding gravity
change the presumption in favor of a "coil bound" spring?
"What is gratuituosly assumed can be gratuitously denied." :)

Bob Sciamanda (W3NLV)
Physics, Edinboro Univ of PA (em)
trebor@velocity.net
http://www.velocity.net/~trebor
----- Original Message -----
From: "John Mallinckrodt" <ajmallinckro@CSUPOMONA.EDU>
To: <PHYS-L@lists.nau.edu>
Sent: Wednesday, December 05, 2001 7:29 AM
Subject: Re: test problem


Brian is (as he noted) nitpicking, but his nitpicks are
nonetheless technically correct. I think you are simply
misinterpreting his remarks. He means for us to consider in
particular the case of a spring that is "coil bound" at its
"normal" length, i.e., one that can not be compressed and that
requires a nonzero applied force before it begins to elongate at
all.

Such a coil bound spring will stretch by less than mg/k when the
mass is hung from it and will "run into itself" at the top end of
the oscillation if the oscillation amplitude is greater than the
downward equilibrium displacement caused by the mass.

John Mallinckrodt mailto:ajm@csupomona.edu
Cal Poly Pomona http://www.csupomona.edu/~ajm

On Tue, 4 Dec 2001, Bob Sciamanda wrote:

Brian objected:
No, the questions are unreasonable. If the extra downward
displacement is
greater than the equilibrium displacement, then the possibility of
coil
binding is not excluded on the upward rebound.

I don't understand this objection - I would think coil "binding" (?)
is a
function of other things having to do with the coil design and
structure. As
g is made to go to zero (go to different planets, or just turn down
gravity)
"the extra downward displacement" becomes infinitely "greater than the
equilibrium displacement". You imply this worsens the situation!

For this same reason, the spring constant is not determined by
only
the
force required for a specified displacement.

I understand this statement even less. Surely the static k is still
"determined by only the force required for a specified displacement".
Do
you refer to some "dynamic" k associated with the binding during
oscillation?