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With regard to John Denker's puck on the turntable example, I agree
with Dan that it is not "perverse" to suggest that the acceleration
is "caused by" the force. One can make a very reasonable argument
for making such a suggestion.
Nevertheless, I disagree with Dan that it would be perverse to
suggest that it's the other way. Again, one can make a very
reasonable argument for so suggesting.
Both of those "very reasonable" arguments, however, are *nothing*
more than that. One simply cannot *logically* assign cause and
effect status to F and a. As John D. and others in similar
discussions here in the past have opined, Newton's second law is
simply *not* a statement of cause and effect. Like virtually every
law of physics, it is a statement of equality.
Dan writes:
I can control how much force is applied to the puck without
changing any properties of the puck by changing the properties of
the surface of the turntable. Therefore, it would be perverse to
suggest that the force is caused by the acceleration of the puck.
On the other hand, because I can change the acceleration of the
puck by changing the force, it logically follows that the force
causes the acceleration of the puck.
There's certainly no "logic" involved in reaching that conclusion.
Moreover, one does not in any direct way "control the force" in this
situation and the nature of the surface simply does *not* "determine"
the force. It is the rotation rate and the position of the puck on
the turntable that one both a) most commonly "controls" and that b)
"determine" the acceleration (assuming, of course, that the puck does
not slip.)
It seems to me that there are good pedagogical reasons for writing
Newton's Second Law as a = F/m, but it also seems to me that it is
gravely wrong to actively teach students that any such equation
expresses causality. Indeed, I think it's important to *stress* that
they do not.
I go to some lengths to make clear to students that the process of
solving physics problems involves identifying the physical principles
involved so that one can amass a set of "relationships" between the
parameters of the problem. Once one has those relationships, one can
start the (less interesting) process of asking which ones happen to
be known and which ones can be sussed out from the relationships.
This process of writing down the relationships irrespective BOTH of
what is "known" or "unknown" AND of what might be considered "cause"
or "effect" is what we do first when we *write* good physics
problems. By the same token, it is what students should learn to do
first in order to *solve* good physics problems.
John "Slo" Mallinckrodt
Professor of Physics, Cal Poly Pomona
<http://www.csupomona.edu/~ajm>
and
Lead Guitarist, Out-Laws of Physics
<http://www.csupomona.edu/~hsleff/OoPs.html>
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