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D'Alembert Derived
Setting
, and extending the summation to an integral,
we have, by Fourier's theorem,
 |
(H.14) |
for
arbitrary continuous functions

and

. This is again the
traveling-wave solution of the
wave
equation attributed to d'Alembert, but now derived from the
eigen-property of
sinusoids and
Fourier theory rather than
``guessed''.
An example of the appearance of the traveling wave components shortly
after plucking an infinitely long string at three points is shown in
Fig.H.2.
Figure H.2:
An infinitely long string,
``plucked'' simultaneously at three points, labeled ``p'' in the
figure, so as to produce an initial triangular displacement. The
initial displacement is modeled as the sum of two identical triangular
pulses which are exactly on top of each other at time 0. At time
shortly after time 0, the traveling waves centers are
separated by
meters, and their sum gives the trapezoidal
physical string displacement at time
which is also shown. Note
that only three short string segments are in motion at that time: the
flat top segment which is heading to zero where it will halt forever,
and two short pieces on the left and right which are the leading edges
of the left- and right-going traveling waves. The string is not
moving where the traveling waves overlap at the same slope. When the
traveling waves fully separate, the string will be at rest everywhere
but for two half-amplitude triangular pulses heading off to plus and
minus infinity at speed
.
![\includegraphics[width=\twidth]{eps/f_t_waves_no_term}](http://www.dsprelated.com/josimages/pasp/img1929.png) |
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Wave VelocityNext:
Converting
Any String State to Traveling Slope-Wave Components
written by Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at
Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See
http://ccrma.stanford.edu/~jos/ for details.