Surface Waves: Rayleigh & Love#
Learning Goals#
Derive dispersion relations for Rayleigh and Love waves
Interpret particle motions (retrograde Rayleigh, transverse Love)
Connect theory to measurements in Labs 4–6
Rayleigh Waves (vertical–radial, retrograde)#
Boundary conditions at the free surface lead to the Rayleigh equation: $\(\left(2 - \beta^2\right)^2 - 4\sqrt{1 - \beta^2}\,\sqrt{1 - \alpha^2 \beta^2} = 0\)\( where \)\beta = c_R / V_S\( and \)\alpha = V_P / V_S$.
Dispersion in layered media: \(c_R(f)\) depends on near-surface \(V_S(z)\).
Love Waves (transverse, SH)#
SH confined to a low-velocity layer over a faster half-space yields:
\[\tan(k_{z1} h) = \frac{\rho_2 k_{z1}}{\rho_1 k_{z2}}\]leading to discrete modes and dispersion curves \(c_L(f)\).
Particle motion: horizontal, transverse to propagation.
Particle Motion & Energy#
Rayleigh: retrograde elliptical in the vertical–radial plane.
Love: purely transverse; no vertical component.
Practical Workflow#
Lab 4 (theory): derive/inspect dispersion relations and particle motion.
Lab 5 (practicum): measure dispersion (MFT, phase/group velocities).
Lab 6 (Love waves): focus on SH-guided waves; compare with Rayleigh.
Use these lecture notes for equations; keep notebooks focused on computation.