Lowfrequency ORT Alexey Stovas IGP NTNU OUTLINE Lowfrequency
- Slides: 21
Low-frequency ORT Alexey Stovas, IGP, NTNU
OUTLINE • Low-frequency properties of layered medium • ORT medium and parameterization • BCH series for ORT • Eigenvalues, multipliers and frequency dependent velocities • Interpretation of dispersion in terms of ORT parameters • Conclusions
Low-frequency properties of the medium ØZero- and infinite-frequency limits ØGiven frequency w=w 0 (non-physical medium) ØLow-frequency approximation + =
ORT: stiffness coefficient matrix Tsvankin, 1997
System matrix for ORT
Upscaling (replacement of Schoenberg-Muir) Zero-frequency limit
The BCH series Roganov and Stovas, 2012
The BCH series [x, y] is a commuting operator a is a volume fraction Roganov and Stovas, 2012
The BCH series Roganov and Stovas, 2012
Weak contrast Isotropic background Weak contrast in elastic and anisotropy parameters Matrix series with respect to contrast
Weak contrast
Weak contrast Matrix series with respect to contrast No second-order contrasts in dispersion terms!
Characteristic equation (eigenvalues)
Characteristic equation (eigenvalues)
Characteristic equation (P-eigenvalues)
Slowness surface dispersion P S 1 S 2 Frequency
Multipliers p 1=0. 1 p 2=0. 1 p 1=0. 05 p 2=0. 2 p 1=0. 2 p 2=0. 05 P wave (down, up) S 1 wave (down, up) S 2 wave (down, up)
Phase velocity, km/s Frequency-dependent phase velocity P-wave S 1 -wave S 2 -wave Frequency, Hz
Wave mode selection Trial series for dispersion coefficient: Three solutions for a 00 that give the wave mode selection.
Quadratic form D 2 D 4
Conclusions • We derive the low frequency approximation for waves propagating in multi-layered orthorhombic model. • The weak-contrast approximation is introduced. • We show that the stop-bands are the result of interaction of different wave modes (P, S 1 and S 2). • The stop-bands are illustrated by multipliers. • By defining the low-frequency effective anisotropic parameters, we perform the sensitivity analysis for intrinsic anisotropy parameters.
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