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Force Wave Variables

Force Equation:

$\displaystyle f_m(t) + f_{1m}(t) + f_{2m}(t) = 0,
$

Traveling-Wave Decomposition of String Force:

\begin{eqnarray*}
f_1(t,x)&=&f^{{+}}_1(t-x/c)+f^{{-}}_1(t+x/c)\\
f_2(t,x)&=&f^{{+}}_2(t-x/c)+f^{{-}}_2(t+x/c)
\end{eqnarray*}

String Force:

$\displaystyle f(t,x) \isdef -Ky'(t,x)
$

where Note that string force pulls up to the right.
That is, a string segment with negative slope pulls ``up'' to the right and ``down'' to the left:

\begin{figure}\centering
\input fig/stringslope.pstex_t
\\ {\LARGE }
\end{figure}

In the present problem, our force equation

$\displaystyle f_m(t) + f_{1m}(t) + f_{2m}(t) = 0,
$

becomes, in terms of mass inertial force and string forces:

$\displaystyle m\dot v(t) + K\,y'_1(t,0) - K\, y'_2(t,0) = 0
$

or, using string force-wave notation:

$\displaystyle \zbox{f_m(t) - f_1(t) + f_2(t) = 0}
$

These force relations can be checked individually:


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Download MassString.pdf
Download MassString_2up.pdf
Download MassString_4up.pdf

``Ideal Mass Colliding with an Ideal String'', by Julius O. Smith III, (From Lecture Overheads, Music 420).
Copyright © 2007-03-01 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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