Lowfrequency ORT Alexey Stovas IGP NTNU OUTLINE Lowfrequency

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Low-frequency ORT Alexey Stovas, IGP, NTNU

Low-frequency ORT Alexey Stovas, IGP, NTNU

OUTLINE • Low-frequency properties of layered medium • ORT medium and parameterization • BCH

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

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

ORT: stiffness coefficient matrix Tsvankin, 1997

System matrix for ORT

System matrix for ORT

Upscaling (replacement of Schoenberg-Muir) Zero-frequency limit

Upscaling (replacement of Schoenberg-Muir) Zero-frequency limit

The BCH series Roganov and Stovas, 2012

The BCH series Roganov and Stovas, 2012

The BCH series [x, y] is a commuting operator a is a volume fraction

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

The BCH series Roganov and Stovas, 2012

Weak contrast Isotropic background Weak contrast in elastic and anisotropy parameters Matrix series with

Weak contrast Isotropic background Weak contrast in elastic and anisotropy parameters Matrix series with respect to contrast

Weak contrast

Weak contrast

Weak contrast Matrix series with respect to contrast No second-order contrasts in dispersion terms!

Weak contrast Matrix series with respect to contrast No second-order contrasts in dispersion terms!

Characteristic equation (eigenvalues)

Characteristic equation (eigenvalues)

Characteristic equation (eigenvalues)

Characteristic equation (eigenvalues)

Characteristic equation (P-eigenvalues)

Characteristic equation (P-eigenvalues)

Slowness surface dispersion P S 1 S 2 Frequency

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

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,

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

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

Quadratic form D 2 D 4

Conclusions • We derive the low frequency approximation for waves propagating in multi-layered orthorhombic

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.