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Re: [Phys-l] Equations



It seems to me, that the concern here is using an equation (relationship) to express a conceptual understanding of motion (at a Newtonian level). I suspect most teaching at the conceptual level, even the intro science level, can get a little casual with the strict mathematical meaning of equations.

My approach is to deal with Newton's First Law as expressing the causation--accelerations are caused by forces. [Try to accelerate something without a force!]

Newton's second law is, to me, primarily a prescription for calculating the acceleration--given the net force and mass of the object. That relationship between the variables also allows me to find the net force if I happen to know the acceleration and the mass, or even the mass if I know the net force and the acceleration. I, like others, like to present the relationship as a = F/me as the most often used form, but I talk through this 'equation' always as 'the acceleration of an object is directly proportional to the net force acting on it but inversely proportional to the mass of the object'.

Newton's third law is about finding the forces. Recognizing that they come in pairs (equal and opposite) can help us identify forces in certain situations where we might otherwise get stumped. My prime example here is to have the class tell me how to walk--using Newton's Laws. That I need a net force in the direction of my (accelerated) motion becomes tricky until the third law is applied to the frictional force between my foot and the floor.

I, in my Newtonian mode of thinking, will still hold out for the notion that accelerations are caused by forces.

Rick (who is seldom called on to think 'outside' the Newtonian mode anymore!)


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Richard W. Tarara
Professor of Physics
Saint Mary's College
Notre Dame, Indiana
rtarara@saintmarys.edu
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----- Original Message ----- From: "John Mallinckrodt" <ajm@csupomona.edu>
To: "Forum for Physics Educators" <phys-l@carnot.physics.buffalo.edu>
Sent: Thursday, April 27, 2006 12:39 PM
Subject: Re: [Phys-l] Equations


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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