Abstract:The continuous measurements of flow velocity/rate and suspended sediment concentration (SSC) in tidal rivers are crucial in estuarine studies. However, the accurate estimates of these terms are difficult and labor-intensive procedures are needed; thus, a robust and efficient method of the measurements is required. The changes of cross-sectional average suspended sediment concentration, tidal bore celerity and flow velocity were measured in the Qiantang River by using acoustic tomography systems. The struser sh… Show more
“…Experimental and numerical analyses showed some transient flow reversal next to the bed and close to the bore passage (Docherty & Chanson, 2012;Khezri & Chanson, 2012b;Koch & Chanson, 2009;Leng & Chanson, 2017a, 2017bLubin et al, 2010); however, this occurrence is relatively weak and related to flow separation and recirculation due to the upward deviation of the main flow at the foot of the bore (Liu et al, 2015;Lubin et al, 2010). In the case of a tidal bore, in which also the bulk flow velocity at the head of the front actually reverses (Furgerot et al, 2016;Masoud et al, 2015;Simpson et al, 2004), the reverse flow is typically much stronger. This is a very important aspect that must be considered in the experimental study of the characteristics of a tidal bore front, in order to properly assess the enhanced mixing and erosion processes related to the flow reversal at the bore passage.…”
A tidal bore is a positive wave traveling upstream along the estuary of a river, generated by a relatively rapid rise of the tide, often enhanced by the funneling shape of the estuary. The swell produced by the tide grows and its front steepens as the flooding tide advances inland, promoting the formation of a sharp front wave, that is, the tidal bore. Because of the many mechanisms and conditions involved in the process, it is difficult to formulate an effective criterion to predict the bore formation. In this preliminary analysis, aimed at bringing out the main processes and parameters that control tidal bore formation, the degrees of freedom of the problem are largely reduced by considering a rectangular channel of constant width with uniform flow, forced downstream by rising the water level at a constant rate. The framework used in this study is extremely simple, yet the problem is still complex, and the solution is far from being trivial. From the results of numerical simulations, three distinctive behaviors emerged related to conditions in which a tidal bore forms, a tidal bore does not form, and a weak bore forms; the latter has a weakly steep front and after the bore formed it rapidly vanishes. Based on these behaviors, some criteria to predict the bore formation are proposed and discussed. The more effective criterion, suitably rearranged, is checked against data from real estuaries, and the predictions are found to compare favorably with the available data.
“…Experimental and numerical analyses showed some transient flow reversal next to the bed and close to the bore passage (Docherty & Chanson, 2012;Khezri & Chanson, 2012b;Koch & Chanson, 2009;Leng & Chanson, 2017a, 2017bLubin et al, 2010); however, this occurrence is relatively weak and related to flow separation and recirculation due to the upward deviation of the main flow at the foot of the bore (Liu et al, 2015;Lubin et al, 2010). In the case of a tidal bore, in which also the bulk flow velocity at the head of the front actually reverses (Furgerot et al, 2016;Masoud et al, 2015;Simpson et al, 2004), the reverse flow is typically much stronger. This is a very important aspect that must be considered in the experimental study of the characteristics of a tidal bore front, in order to properly assess the enhanced mixing and erosion processes related to the flow reversal at the bore passage.…”
A tidal bore is a positive wave traveling upstream along the estuary of a river, generated by a relatively rapid rise of the tide, often enhanced by the funneling shape of the estuary. The swell produced by the tide grows and its front steepens as the flooding tide advances inland, promoting the formation of a sharp front wave, that is, the tidal bore. Because of the many mechanisms and conditions involved in the process, it is difficult to formulate an effective criterion to predict the bore formation. In this preliminary analysis, aimed at bringing out the main processes and parameters that control tidal bore formation, the degrees of freedom of the problem are largely reduced by considering a rectangular channel of constant width with uniform flow, forced downstream by rising the water level at a constant rate. The framework used in this study is extremely simple, yet the problem is still complex, and the solution is far from being trivial. From the results of numerical simulations, three distinctive behaviors emerged related to conditions in which a tidal bore forms, a tidal bore does not form, and a weak bore forms; the latter has a weakly steep front and after the bore formed it rapidly vanishes. Based on these behaviors, some criteria to predict the bore formation are proposed and discussed. The more effective criterion, suitably rearranged, is checked against data from real estuaries, and the predictions are found to compare favorably with the available data.
“…One of the main obstacles in utilizing acoustic instruments for the river discharge measurements, either FATS or ADCP, is the attenuation of acoustic waves [14]. The energy of an acoustic wave is evidently attenuated by increasing the distance from the source, due to the energy absorption by water molecules and the suspended particles.…”
Fluvial Acoustic Tomography System (FATS) as an advanced technology acquires continuous streamflow data in rivers and estuaries even during floods. However, the acoustic signals are dramatically attenuated by suspending sediments which this problem is a new field of study. In this study, we propose a new equation to estimate the maximum applicable measurement distances (MAMDs). It is based on the cross-sectional suspended sediment concentration () and the particle sizes on the 30-kHz FATS. Our study results show that MAMD might be 2,380 m in the clear water. Moreover, the streamflow monitoring can be perfectly done while is less than 12.67 kg/m 3 with the particle radii of 3 μm, when the horizontal distance between two acoustic stations is 100 m. Also, the acoustic signals are not decayed if the particle radii equal to 20 mm and the maximum is 6.6 kg/m 3. This study highlights the performance of FATS in the presence of high and provides a better perspective of applying FATS in different rivers with high variability of .
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