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In situ acoustic and laboratory ultrasonic sound speed and attenuation measured in heterogeneous soft seabed sediments: Eel River shelf, California

机译:在异质软海底沉积物中测量的原位声学和实验室超声波速度和衰减:加利福尼亚州埃尔河河架

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We compared in situ and laboratory velocity and attenuation values measured in seafloor sediments from the shallow water delta of the Eel River, California. This region receives a substantial volume of fluvial sediment that is discharged annually onto the shelf. Additionally, a high input of fluvial sediments during storms generates flood deposits that are characterized by thin beds of variable grain-sizes between the 40- and 90-m isobaths. The main objectives of this study were (1) to investigate signatures of seafloor processes on geoacoustic and physical properties, and (2) to evaluate differences between geoacoustic parameters measured in situ at acoustic (7.5 kHz) and in the laboratory at ultrasonic (400 kHz) frequencies. The in situ acoustic measurements were conducted between 60 and 100 m of water depth. Wet-bulk density and porosity profiles were obtained to 1.15 m below seafloor (m bsf) using gravity cores of the mostly cohesive fine-grained sediments across- and along-shelf. Physical and geoacoustic properties from six selected sites obtained on the Eel margin revealed the following. (1) Sound speed and wet-bulk density strongly correlated in most cases. (2) Sediment compaction with depth generally led to increased sound speed and density, while porosity and in situ attenuation values decreased. (3) Sound speed was higher in coarser- than in finer-grained sediments, on a maximum average by 80 m s~(-1) (4) In coarse-grained sediments sound speed was higher in the laboratory (1560 m s~(-1)) than in situ (1520 m s~(-1)), In contrast, average ultrasonic and in situ sound speed in fine-grained sediments showed only little differences (both approximately 1480 m s~(-1)) (5) Greater attenuation was commonly measured in the laboratory (0.4 and 0.8 dB m~(-1) kHz~(-1)) than in situ (0.02 and 0.65 dB m~(-1) kHz~(-1)), and remained almost constant below 0.4 m bsf. We attributed discrepancies between laboratory ultrasonic and in situ acoustic measurements to a frequency dependence of velocity and attenuation. In addition, laboratory attenuation was most likely enhanced due to scattering of sound waves at heterogeneities that were on the scale of ultrasonic wavelengths. In contrast, high in situ attenuation values were linked to Stratigraphic scattering at thin-bed layers that form along with flood deposits.
机译:我们比较了加利福尼亚Eel河浅水三角洲海底沉积物中测得的原位和实验室速度和衰减值。该区域接收大量的河流沉积物,这些沉积物每年都排放到架子上。此外,暴风雨期间大量河床沉积物会产生洪水沉积物,其特征是在40至90 m等深线之间具有可变粒度的薄层。这项研究的主要目的是(1)研究海底过程在地声和物理性质方面的特征,以及(2)评估在声学(7.5 kHz)和实验室在超声(400 kHz)下现场测量的地声参数之间的差异)频率。在水深60至100 m之间进行原位声学测量。使用跨板带和沿板带的大多数粘性细颗粒沉积物的重力核心,获得了海床以下(f bsf)1.15 m的湿散装密度和孔隙率分布图。从鳗el边缘获得的六个选定地点的物理和地声特性显示出以下内容。 (1)在大多数情况下,声速和湿散装密度密切相关。 (2)随着深度的泥沙压实通常会导致声速和密度的增加,而孔隙度和原位衰减值会降低。 (3)较粗颗粒沉积物的声速更高,最大平均值为80 ms〜(-1)(4)在较粗颗粒沉积物中,声速在实验室更高(1560 ms〜(- 1))比原位(1520 ms〜(-1))要大,相反,细粒沉积物中的平均超声波和原位声速仅显示出很小的差异(均为约1480 ms〜(-1))(5)通常在实验室(0.4和0.8 dB m〜(-1)kHz〜(-1))上测量衰减,而不是在现场(0.02和0.65 dB m〜(-1)kHz〜(-1))上测量,并且几乎保持低于0.4 m bsf的常数。我们将实验室超声和原声测量之间的差异归因于速度和衰减的频率依赖性。另外,由于声波在超声波长范围内的异质性上的散射,最有可能增强实验室衰减。相比之下,高原位衰减值与与洪水沉积一起形成的薄层地层散射有关。

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