Acoustic signal propagation and measurement in natural stream channels for application to surrogate bed load measurements: Halfmoon Creek, Colorado

Author(s):  
J Rigby ◽  
Daniel Wren ◽  
Nathan Murray
Author(s):  
D. Keith Wilson ◽  
Daniel J. Breton ◽  
Wesley M. Barnes ◽  
Michael B. Muhlestein ◽  
Vladimir E. Ostashev ◽  
...  

2019 ◽  
Vol 283 ◽  
pp. 02003
Author(s):  
Jun Zhu ◽  
Hanhao Zhu ◽  
Jun Tang ◽  
Guangxue Zheng

Targeted at the issue of extremely low-frequency (<100Hz) acoustic propagation in complex shallow elastic bottom environments. The influence law of different complex elastic bottoms on the acoustic signal propagation at very low frequency by acoustic energy flux has been analyzed with the simulation, which is based on the finite element method. The elastic bottoms which have been studied are the shallow horizontal elastic bottom, and the up-sloping and the down-sloping elastic bottom. The results show that the acoustic signal propagating in the up-sloping and down-sloping elastic bottom environments is more complex than that propagating in the horizontal elastic bottom, and the acoustic energy leaking into those elastic bottoms has very different influence on the acoustic signal propagation, especially in the up-sloping bottom.


Author(s):  
Alban Kuriqi

In this paper is discussed sediment transport as a mechanical process that characterises a natural stream or channel flow regime. The objective of experimental work presented in this paper is to recall and to give another prospect of well-known Meyer-Peter and M&uuml;ller approach for estimation of Shield&rsquo;s number (&theta;_c,&theta;) in laboratory conditions, and calibration of dimensionless MPM number (A). For this purpose two different experiments are conducted, during the first experiment water amount flushed on the flume and bed slope was changed simultaneously until equilibrium state is achieved, meanwhile is estimated the critical Shield&rsquo;s number (&theta;_c). While, during the second experiment, water amount was kept constant, only bed slope of flume was continuously tilted, meanwhile sediment, discharge and Shield&rsquo;s number (&theta;) was determined for given hydraulic conditions. In addition calibration of dimensionless MPM number (A) was performed, where several iteration were considered until for (A=3.42), sediment discharge measured become almost equal with sediment discharge computed by using MPM formula. After these experiments, is concluded that MPM formula can be used also for other certain initial condition and similar procedure may be adopted to calibrate the dimensionless MPM number (A) .


2014 ◽  
Vol 136 (4) ◽  
pp. 2139-2139
Author(s):  
Jericho E. Cain ◽  
Sandra L. Collier ◽  
Vladimir E. Ostashev ◽  
David K. Wilson

2019 ◽  
Vol 65 (3) ◽  
pp. 279-287
Author(s):  
A. N. Rutenko ◽  
D. S. Manul’chev ◽  
S. B. Kozitskii

2012 ◽  
Vol 43 ◽  
pp. 56-63 ◽  
Author(s):  
Ron S. Lewis ◽  
Michèle Drogou ◽  
Peter King ◽  
George Mann ◽  
Neil Bose ◽  
...  

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