Acoustic and Other Physical Properties of Shallow‐Water Sediments off San Diego

1956 ◽  
Vol 28 (1) ◽  
pp. 1-1 ◽  
Author(s):  
E. L. Hamilton ◽  
George Shumway ◽  
H. W. Menard ◽  
C. J. Shipek
1955 ◽  
Vol 27 (5) ◽  
pp. 1007-1007
Author(s):  
E. L. Hamilton ◽  
George Shumway ◽  
H. W. Menard ◽  
C. J. Shipek

Geophysics ◽  
1956 ◽  
Vol 21 (2) ◽  
pp. 305-319 ◽  
Author(s):  
George Shumway

Sound velocity and attenuation measurements in unconsolidated marine sediments have been made by a resonance method which utilizes a thin‐walled plastic cylinder as a pressure‐release container to hold samples. Velocities were determined from resonant frequencies which lay between 23 and 36 kc/sec for the 2 inch diameter by 4 inch long cylindrical container used. Attenuation was determined from the sharpness of the resonant modes. Relatively undisturbed sediment samples were obtained by diver, in shallow water, using the same plastic containers in which the acoustic measurements are made. Deep sea samples were obtained by cutting sections from cores which were taken in plastic tubes. Velocities for shallow water sediments in the San Diego area ranged from 4,840 ft/sec (0.978 times sea water velocity) for fine silt to 5,680 ft/sec (1.147 times sea water velocity) for medium sand, measured at 60°F. and atmospheric pressure. Velocities in deep‐sea red clay samples ranged between 0.980 and 1.040 times the sea water velocity, at 60°F. and atmospheric pressure. Attenuation coefficients for shallow‐water San Diego sediments varied from about 1 to 4 db/ft for silts, to about 3 to 8 db/ft for sand.


1963 ◽  
Vol 53 (1) ◽  
pp. 27-37
Author(s):  
R. A. Haubrich ◽  
W. H. Munk ◽  
F. E. Snodgrass

Abstract Spectra of seismic and ocean wave recordings near San Diego, California, show closely related features. The wave spectra consist of a sharp peak whose frequency, f(t), increases linearly with time and consistent with the expected dispersive behaviour from a source at 6150 nautical miles (presumably a storm in the Ross Sea). The seismic spectra show peaks at f(t) and at 2 f(t); the double frequency peak contains 100 times the energy of the peak at the primary frequency. A comparison between the peak frequencies and band widths of the seismic and ocean wave spectra, and an estimate of the direction and beam width of the seismic radiation, leads to the following conclusions: that the microseismic generation area is predominantly local, being confined to a distance of 100 miles up or down the coast. For the primary frequencies the generative strip is presumably confined to shallow water; for the double frequencies it extends 200 miles seaward.


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