Wave Momentum

The physical forward *momentum* carried by a transverse wave
along a string is conveyed by a secondary *longitudinal wave*
[394].

A less simplified wave equation which
supports longitudinal wave momentum is given by [394, Eqns. 38ab]

(B.40) | |||

(B.41) | |||

(B.42) |

where and denote longitudinal and transverse displacement, respectively, and the commonly used ``dot'' and ``prime'' notation for partial derivatives has been introduced,

(B.43) | |||

(B.44) |

(See also Eq. (C.1).) We see that the term in the first equation above provides a mechanism for transverse waves to ``drive'' the generation of longitudinal waves. This coupling cannot be neglected if momentum effects are desired.

Physically, the rising edge of a transverse wave generates a longitudinal displacement in the direction of wave travel that propagates ahead at a much higher speed (typically an order of magnitude faster). The falling edge of the transverse wave then cancels this forward displacement as it passes by. See [394] for further details (including computer simulations).

[How to cite this work] [Order a printed hardcopy] [Comment on this page via email]

Copyright ©

Center for Computer Research in Music and Acoustics (CCRMA), Stanford University