Sand transport in Lido and Chioggia inlets was measured using modified Helley-Smith sand traps equipped with 60-micron nets. The traps had an efficiency of about 4% only but provided enough material for analysis. Very fine sand (0.07 < d < 0.11 mm) only was collected in the traps. Transport of sand was greatest in the bottom 10% of the water column and followed a Rouse profile. Sand extended to a height of about 4 m above the bed during peak flows corresponding to the estimated thickness of the boundary layer; and observed in synoptic ADCP profiles. The sand in the benthic boundary layer was largely inorganic (>95%); above this layer, organic content varied widely and was greatest near the surface. The movability number Ws=U* showed a linear relationship to dimensionless grain diameter (D*): (Ws/U*) = (D*/10); D*< 10. Sand concentration in suspension was simulated by a mean Rouse parameter of -2.01 +/- 0.66 (Lido inlet) and -0.82 +/- 0.27 (Chioggia inlet). The b parameter (Hill et al., 1988) was correlated with D* and movability number in the form: b = 2:07 - 2:03D* + 59(Ws=U*)^2 (r^2 = 0.42). Von Karman's constant was back-calculated from a Law of the Wall relationship as a test on the accuracy of U* estimates; a mean value of 0.37 +/- 0.1 (compared to the accepted value of 0.41) suggest U* was accurate to within 10%. The constant of proportionality (g = 3.54 x 10^-4) between reference concentration (Ca) and normalized excess bed shear stress was in line with the published literature.

The measurement of sand transport in two inlets of Venice lagoon, Italy

Zaggia;Umgiesser;Mazzoldi;Rizzetto;
2010

Abstract

Sand transport in Lido and Chioggia inlets was measured using modified Helley-Smith sand traps equipped with 60-micron nets. The traps had an efficiency of about 4% only but provided enough material for analysis. Very fine sand (0.07 < d < 0.11 mm) only was collected in the traps. Transport of sand was greatest in the bottom 10% of the water column and followed a Rouse profile. Sand extended to a height of about 4 m above the bed during peak flows corresponding to the estimated thickness of the boundary layer; and observed in synoptic ADCP profiles. The sand in the benthic boundary layer was largely inorganic (>95%); above this layer, organic content varied widely and was greatest near the surface. The movability number Ws=U* showed a linear relationship to dimensionless grain diameter (D*): (Ws/U*) = (D*/10); D*< 10. Sand concentration in suspension was simulated by a mean Rouse parameter of -2.01 +/- 0.66 (Lido inlet) and -0.82 +/- 0.27 (Chioggia inlet). The b parameter (Hill et al., 1988) was correlated with D* and movability number in the form: b = 2:07 - 2:03D* + 59(Ws=U*)^2 (r^2 = 0.42). Von Karman's constant was back-calculated from a Law of the Wall relationship as a test on the accuracy of U* estimates; a mean value of 0.37 +/- 0.1 (compared to the accepted value of 0.41) suggest U* was accurate to within 10%. The constant of proportionality (g = 3.54 x 10^-4) between reference concentration (Ca) and normalized excess bed shear stress was in line with the published literature.
2010
Istituto di Scienze Marine - ISMAR
sand transport
tidal inlets
Venice lagoon
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/72577
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