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Re: [Phys-l] nifty question (solution)



Some thoughts, for what they're worth:
a catenary lifted at the center to support height provides two similar catenaries of half width and half depth of the original. Two part CoGs at half the original vertical distance from the support level
each carrying half the original hung weight implies increased potential energy.(obviously)
A catenary lifted to support height, where one half has a higher CoG than the other exerts unequal reaction on the center support. An extreme division of cable lengths in each half span reduces the CoG height nearer the original position, and so is energetically favored, for sliding friction low enough at the center support. I suggest the center lifted catenary is always energetically unfavorable for low enough sliding friction at that support.

Brian W

On 9/24/2010 7:26 AM, curtis osterhoudt wrote:
The reason I'd asked "what happens if you pulled up, instead of down?", is that,
for at least some range of up-pulls, I suspect the situation becomes unstable in
equilibrium, and the cable will slip to one side or the other given something to
break the left-right symmetry. I wondered if anyone might venture to show that,
or disagrees with my guess.


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________________________________
From: Carl Mungan<mungan@usna.edu>
To: phys-l@carnot.physics.buffalo.edu
Sent: Fri, September 24, 2010 6:00:35 AM
Subject: Re: [Phys-l] nifty question (solution)

Okay, looks like most people got it, and several people even
anticipated the second question below. Reference for these questions
is given in the last line below.

Consider an ideal (ie. cannot stretch, and can bend freely) cable
suspended from two points of equal height (that are closer together
than the cable's length). The cable adopts the shape of a catenary
(hyperbolic cosine).

Now suppose you hang a weight from the center of the cable. Does the
cable's center of mass move up, down, or remain at the same height?
The center of mass goes up. Here's a simple explanation:

Suppose instead of suddenly attaching the hanging mass m to the
cable, I instead apply a downward force F to the center of the cable
that slowly increases from 0 up to mg. (This guarantees the process
is quasistatic, just like what we do in thermo when we compress a
piston in a gas-filled cylinder.) Clearly I do positive work on the
cable. Thus the energy of the cable increases. Since the process was
quasistatic, there is never any KE of the cable. Further, the cable
is ideal and thus doesn't stretch, so it cannot gain elastic PE. All
that's left is for the cable to gain gravitational PE, and thus its
COM must rise.

> From the same readings, here's another (much easier) nifty question.
Suppose instead of pulling downward on the center of the cable, I
pull upward, until the center of the cable is at the same height as
the two ends of the cable. What upward force F am I applying at that
instant?

Reference: AJP 58:1110 (1990). -Carl