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Re: [Phys-l] waves on a string



Carl:

I wasn't familiar with equation 3 in the article to which you refer but
equation 4 makes sense. It is consistent with the notion that each
infinitesimal bit of mass dm of the string is undergoing simple harmonic
moton so

dE = 1/2 k y^2 + 1/2 dm (dy/dt)^2

where k (determined by setting 1/2 k ymax^2 = 1/2 m vmax^2 where vmax =
2 pi f ymax) is given by

k = dm (2 pi f)^2

-------------

where:

k is the force constant of a ficticious spring that would provide a
force on the bit of string equal to the net force being exerted on the
bit of string by its neigboring string.

f is the frequency of the wave

-------------

I prefer writing his equation 4 as:

dE = 1/2 [mu dx (2 pi f)^2] y^2 + 1/2 (mu dx) (dy/dt)^2

so it looks more like the energy 1/2 k x^2 + 1/2 m v^2 of a simple
harmonic oscillator but it amounts to the same thing.


-----Original Message-----
From: phys-l-bounces@carnot.physics.buffalo.edu [mailto:phys-l-
bounces@carnot.physics.buffalo.edu] On Behalf Of Carl Mungan
Sent: Thursday, December 09, 2010 11:00 AM
To: phys-l@carnot.physics.buffalo.edu
Subject: [Phys-l] waves on a string

In the past, we've discussed questions of energy and momentum
transfer for waves on a string. (Try typing "Benumof" into the PHYS-L
archive searcher for example.)

Anyhow, there's a recent Letter paper by Burko in Eur. J. Phys.
31:L71 (2010) claiming the usual textbook formula for energy of a
string wave is wrong. The gist is that instead of the square of dy/dx
in the PE term, one should have y * second deriv. of y w.r.t. x.

find this Letter near the bottom of: http://iopscience.iop.org/0143-
0807/31/5

I wonder if some others on the list can look at this Letter and see
what they think. -Carl

--
Carl E Mungan, Assoc Prof of Physics 410-293-6680 (O) -3729 (F)
Naval Academy Stop 9c, 572C Holloway Rd, Annapolis MD 21402-1363
mailto:mungan@usna.edu http://usna.edu/Users/physics/mungan/
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