Snow grounds require a layered porous-medium impedance model.

Evidence

The ground sometimes behaves like a layered porous medium, rather than the infinitely thick layer assumed in Eqs. (9) and (10). If we let d be the layer thickness and k2 the wavenumber in the layer, then the resulting impedance of the medium is TM Z = Z2 (Z3 — iZ2 tan k2d) / (Z2 — iZ3 tan k2d), ( 11 ) where Z2 and Z3 are the impedances of the upper and lower materials, respectively, found using Eqs. — Donald G. Albert and John A. Orcutt, Acoustic Pulse Propagation Above…, 26

Categorization

  • DEFINE: Introduces the layered-porous-medium impedance treatment — the exact ‘layered porous-snow model’ gap the polyad flagged.
  • XREF: connects to: Snow exceeds other natural surfaces in sound absorption by a large margin. — Donald G. Albert and John A. Orcutt, Acoustic Pulse Propagation Above…, 6; Effective flow resistivity is the dominant ground absorption parameter. — Donald G. Albert and John A. Orcutt, Acoustic Pulse Propagation Above…, 73; Impedance discontinuities split an arriving wave into reflected and transmitted parts — Ville Pulkki, Matti Karjalainen, Communication Acoustics- An…, 235 (+2 more)

Broader Connections