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Perturbations in Acoustic Wave Propagation

Dividing the electrical energy density by the strain energy density yields [Pg.31]

The last term is approximately equal to K when 4 1. Thus, the electromechanical coupling coefficient K ) has a second interpretation is approx- [Pg.31]

This relation can be used to relate changes in wave energy density to changes in wave velocity in a lossless medium, i.e., one in which P is constant Implicitly differentiating Equation 2.47 yields [Pg.31]

Example 2.9 If a plane wave propagates in a medium in which the mass density changes, how is wave velocity effected  [Pg.32]

from Equation 2.48, the fractional chan in wave velocity is minus the fractional change in mass density of the medium  [Pg.33]


See other pages where Perturbations in Acoustic Wave Propagation is mentioned: [Pg.31]    [Pg.31]    [Pg.33]   


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