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Re: Double Atwood



Hi David,
I get M = 3 kg . . . do we agree?

Re: your students' concerns:

1) It matters not that the observed objects are accelerating, so long as
we observe them from a non-accelerating frame. It is WE, the observers,
who must not accelerate!

2) This can only be resolved by a careful examination of the geometry. If
the 2 kg mass rises an amount x due to the fall of an amount x by the 3 kg
mass, this will be exactly canceled if the pulley B falls an equal amount
x.

Hope this is of some help. Push it if more discussion will help.

Bob

Bob Sciamanda (W3NLV)
Physics, Edinboro Univ of PA (em)
trebor@velocity.net
http://www.velocity.net/~trebor

----- Original Message -----
From: David Abineri <dabineri@CHOICE.NET>
To: <PHYS-L@lists.nau.edu>
Sent: Friday, October 15, 1999 8:29 PM
Subject: Double Atwood


I wonder if someone might help with the following student comments about
this problem given in my AP class this week.

A pulley (A) is attached to the ceiling with a string passing over it.
On the right end of the string hangs a mass M and on the left side hangs
another pulley (B) with a string holding a mass of 2kg on one side and a
mass of 3kg on the other side. The question is to find the mass M in
order that the 2kg mass remains stationary when the system is released.

I solved this in a pretty conventional manner making the downward
acceleration of pulley B equal to the upward acceleration the 2kg mass.

The student asks two questions:

1. Are the calculated tensions in the string around pulley B really
correct since the system of pulley B and its masses is an accelerating
system? Does this affect the answer to the problem?

2. Isn't pulley B behaving as a simple machine of mechanical advantage 2
so that movements in the string around pulley A are not equal to the
movements of the string around pulley B? Does this affect the answer to
the problem?

Any clarifying thoughts would be appreciated.

Thanks,
--
David Abineri dabineri@choice.net