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- Path: sparky!uunet!ogicse!das-news.harvard.edu!husc-news.harvard.edu!blom
- From: blom@husc15.harvard.edu
- Newsgroups: sci.physics
- Subject: Irregular wave motion results
- Message-ID: <1992Nov18.105130.17567@husc15.harvard.edu>
- Date: 18 Nov 92 15:51:29 GMT
- Article-I.D.: husc15.1992Nov18.105130.17567
- Organization: Harvard University Science Center
- Lines: 32
-
- I wrote a simple computer program to simulate waves in a cable fixed at both
- ends as if that cable were a number of springs joined together (320 springs, to
- be exact). I expected to see motion like that predicted by classical wave
- mechanics, obeying the wave equation
-
- d2y 2 d2y
- --- = v ---
- dt2 dx2
-
- from which we find that the shape of a travelling wave pulse does not change
- over time. It occurs to me, though, that this should only work for analytic
- functions. What happens to places on a pulse where the wave comes to a point?
- (i.e. where the function has no definable derivative) In my simulation, it
- seemed that the point smoothed out and left a small disturbance behind the
- pulse, in the form of a low-amplitude, high-frequency standing wave. The pulse
- I was using was part of the sine curve, which therefore came to points at its
- endpoints.
-
- The pulse also deformed with time. Could this be the result of dispersion? My
- model didn't have any special constants or terms in it which would code
- specifically for that effect. Was this just cumulative rounding error? I was
- using 10-byte, 19-digit precision IEEE floating point.
-
- I also did a Fourier analysis of the function looking like /\/\/\/\/\... which,
- over time, had it's points flatten out, and that was the only effect. How
- would a person do a Fourier analysis of, say, a single cosine pulse /~\ over
- time as it breaks into two discrete pulses travelling in opposite directions?
- What happens at the ends of the pulse? Do they flatten out or round off?
-
- Thanks in advance.
- --Eric Blom
- --Harvard University
-