Sound velocity as a function of depth in marine sediments.

Autor: Hamilton, Edwin L.
Zdroj: Journal of the Acoustical Society of America; 1985, Vol. 78 Issue 4, p1348-1355, 8p
Abstrakt: Additional data from sonobuoys and the Deep Sea Drilling Project (DSDP) justify separating sound-velocity-depth functions and velocity gradients (in the first layer of soft marine sediments) into some geographic areas and sediment types. Based on sonobuoy and core measurements (where V is sound velocity in km/s, and h is depth in sediments in km), the following data are obtained: continental shelf basins off Sumatra and Java-V=1.484+0.710h-0.085h2; U. S. Atlantic continental rise-V=1.513+0.828h-0.138h2; deep-sea terrigenous sediments-V=1.519+1.227h-0.473h2; and siliceous sediments of the Bering Sea- V=1.509+0.869h-0.267h2. Selected DSDP data (through leg 74) in similar areas yield: continental terrace silt-clays-V=1.505+0.712h; deep-sea terrigenous sediments-V=1.510+1.019h; and deep-sea siliceous sediments-V=1.533+0.761h. Computed velocity gradients from sonobuoy measurements are generally supported by the DSDP gradients. Only DSDP data give the following: hemipelagic sediments-V=1.501+1.151h; deep-sea calcareous sediments-V=1.541+0.928h; and deep-sea pelagic clay-V=1.526+1.046h. Where fast sediment accumulation occurs, there has not been enough time to reduce sediment pore spaces under overburden pressure; areas of slow accumulation may have relatively high sediment structural strength. Both cases have lower velocity gradients because higher porosities and consequent lower velocities persist to deeper depths. [ABSTRACT FROM AUTHOR]
Databáze: Complementary Index