Vp/Vs Ratio Calculator

P-waves travel through rock at a speed set by both the bulk modulus and the shear modulus, while S-waves depend on the shear modulus alone. Dividing one velocity by the other cancels density and leaves a dimensionless number that describes only how the material resists volume change relative to shape change. That is why Vp/Vs and the Poisson ratio carry identical information and convert exactly through nu = ((Vp/Vs)^2 - 2) / (2*((Vp/Vs)^2 - 1)). The limiting cases are instructive: a material with nu of zero gives a ratio of 1.414, the reference Poisson solid with nu of 0.25 gives exactly sqrt(3) or 1.732, and as nu approaches 0.5 the material behaves like a fluid and the ratio grows without bound. The diagnostic value comes from the fact that pore fluids stiffen a rock in compression but not in shear. Replacing brine with gas collapses the bulk modulus while leaving the shear modulus essentially unchanged, dropping Vp sharply and barely touching Vs. Gas-charged sandstones therefore commonly show ratios of 1.4 to 1.6, clean consolidated sands and carbonates 1.6 to 1.8, water-saturated shales 1.8 to 2.0, and soft unconsolidated near-surface sediment above 2.0. The caveats matter: the relation assumes an isotropic elastic solid, so shale anisotropy, fracture alignment, and strong frequency dispersion between sonic-log and seismic bands all bias the result, and a low ratio alone cannot distinguish commercial gas from residual gas saturation.

The elastic framework behind the ratio dates to Simeon Denis Poisson, whose 1829 memoir on elasticity introduced the transverse-to-axial strain ratio that carries his name. The wave velocities themselves follow from the equations of motion for an elastic solid developed through the nineteenth century, and by the early twentieth century seismologists were using P and S arrival times to infer the composition and state of the Earth interior. The practical exploration use began with well logging. George Pickett published work in 1963 on acoustic character logs showing that velocity ratios could discriminate sandstone, limestone, and dolomite from borehole measurements. The technique gained far greater reach after William Ostrander demonstrated in the mid-1980s that gas sands produce a distinctive change in reflection amplitude with source-receiver offset, launching amplitude-versus-offset analysis and making Vp/Vs recoverable from surface seismic data rather than only from wells. In 1985 John Castagna, Michael Batzle, and Raymond Eastwood published an empirical relationship for water-saturated clastic silicate rocks, the mudrock line, giving a baseline against which anomalous ratios could be judged. Fritz Gassmann's 1951 fluid-substitution theory supplied the physics for predicting how the ratio should shift when pore fluid changes, and that combination remains the core of quantitative reservoir interpretation.