In isotropic elasticity, P-wave displacement is longitudinal, whereas in anisotropic elasticity the quasi-P (qP) polarization is generally oblique to the wave normal. We quantify the resulting difference between exact elastic qP propagation and a longitudinally constrained model for homogeneous VTI media in the symmetry plane. The qP dynamics is the invariant spectral restriction of the full elastic operator; the longitudinal dynamics is a conservative Galerkin restriction to curl-free fields. An exact identity shows that the longitudinal squared-speed deficit equals the qP–qSV spectral gap times the squared polarization mismatch. Under weak anisotropy η , the modal/polarization error is O (η), while the phase-speed error is O (η2). Their propagated-field contributions are orthogonal and satisfy a bounded-time estimate O(|η|+tη2). Strong L2 limits on t=O(η−1) and t=O(η−2) identify, respectively, the polarization–phase crossover and order-one long-time dephasing. Exact Fourier experiments verify the asymptotic coefficients and limiting curves. The results provide a mechanical validity criterion for longitudinal P-wave models: short-time accuracy is limited by polarization leakage, whereas sufficiently long propagation is controlled by accumulated phase error.

Longitudinal versus quasi-P waves in weakly anisotropic VTI media: A 2D analysis of modal error and long-time dephasing

S. MIcheletti
2027-01-01

Abstract

In isotropic elasticity, P-wave displacement is longitudinal, whereas in anisotropic elasticity the quasi-P (qP) polarization is generally oblique to the wave normal. We quantify the resulting difference between exact elastic qP propagation and a longitudinally constrained model for homogeneous VTI media in the symmetry plane. The qP dynamics is the invariant spectral restriction of the full elastic operator; the longitudinal dynamics is a conservative Galerkin restriction to curl-free fields. An exact identity shows that the longitudinal squared-speed deficit equals the qP–qSV spectral gap times the squared polarization mismatch. Under weak anisotropy η , the modal/polarization error is O (η), while the phase-speed error is O (η2). Their propagated-field contributions are orthogonal and satisfy a bounded-time estimate O(|η|+tη2). Strong L2 limits on t=O(η−1) and t=O(η−2) identify, respectively, the polarization–phase crossover and order-one long-time dephasing. Exact Fourier experiments verify the asymptotic coefficients and limiting curves. The results provide a mechanical validity criterion for longitudinal P-wave models: short-time accuracy is limited by polarization leakage, whereas sufficiently long propagation is controlled by accumulated phase error.
2027
Anisotropic elasticity, Long-time asymptotics, Mode separation, Quasi-P waves, Spectral projectors, Weak anisotropy
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11311/1330426
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