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Re: Spring potential energy without Work (sort of)



On Monday, October 15, 2001 9:40 PM, RAUBER, JOEL wrote:

Is this hand-waving somehow worse than the hand-waving
performed to get
v_f^2 = v_i^2 + 2 a Delta x?

[snip]

Furthermore, average velocity doesn't require handwaving, algebra and
geometry alone serve to derive this for constant
acceleration; at least if
you believe geometry implies that the midpoint of a linear line is its
average value, (and don't call that handwaving). But we're
getting into the
realm of taste here, IMO the result is less natural for Delta
x^2; in the
sense that I think it requires knowing the desired answer in
a slightly more
profound way than the Delta v^2.

I readily admit that formally the arguments are identical.

I know you feel it is a matter of taste but I'm curious as to why
you think the result is less natural for Delta x^2?

*[since F = kx, then
F_avg*Delta x = k (x_i + x_f)*(x_f - x_i)/2 = 1/2 k Delta (x^2).]

Good! We don't need calculus for the linear spring! And I
suppose this
answers, perhaps not in pleasing way, Ludwik's question.

Of course, I'll next say, let's consider a non-linear spring, . . .

Are you saying to consider a situation where one cannot use current
methods (i.e., algebra, geometry, graphing, etc.) to determine the
average* force? Well, of course there must be *some* advantage to
knowing calculus. :)

* average over space (not time)

----------------------------------------------------------
| Robert Cohen Department of Physics |
| East Stroudsburg University |
| rcohen@po-box.esu.edu East Stroudsburg, PA 18301 |
| http://www.esu.edu/~bbq/ (570) 422-3428 |
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