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Sediment rating curve

In many situations, sediment flux is estimated through use of a sediment rating curve (see e.g. Julien, 1998), where a relationship is derived between sampled sedunent... [Pg.248]

The concepts of limited sediment supply to rivers and an upper limit to the capacity of a particular flow rate to transport sediment of a particular particle size distribution and density explain the phenomenon of hysteresis, where sediment concentration for a given flow rate differs on the rising and falling limbs of a flow event. There is thus no simple relationship between flow and concentration, and a sediment rating curve will inherently have wide error bars. [Pg.249]

Fig. 12. The relationship between the mean oceanic residence time, T, yr, and the seawater—cmstal rock partition ratio,, of the elements adapted from Ref. 29. , Pretransition metals I, transition metals , B-metals , nonmetals. Open symbols indicate T-values estimated from sedimentation rates. The sohd line indicates the linear regression fit, and the dashed curves show the Working-Hotelling confidence band at the 0.1% significance level. The horizontal broken line indicates the time required for one stirring revolution of the ocean, T. ... Fig. 12. The relationship between the mean oceanic residence time, T, yr, and the seawater—cmstal rock partition ratio,, of the elements adapted from Ref. 29. , Pretransition metals I, transition metals , B-metals , nonmetals. Open symbols indicate T-values estimated from sedimentation rates. The sohd line indicates the linear regression fit, and the dashed curves show the Working-Hotelling confidence band at the 0.1% significance level. The horizontal broken line indicates the time required for one stirring revolution of the ocean, T. ...
Figure 17, Plot of concentration versus height in a continuous sedimentation device. Curve (1) - low feedrate Curve (2) - high feed rate. Figure 17, Plot of concentration versus height in a continuous sedimentation device. Curve (1) - low feedrate Curve (2) - high feed rate.
Table 1. Sedimentation Rates and Curve Fitting of 210Pb Measurements in Cores Collected at the U. S. Radioactive Waste Disposal Sites Near the Farallon Islands 60 km off San Francisco and at the Hudson Canyon, 350 km off New York City. Table 1. Sedimentation Rates and Curve Fitting of 210Pb Measurements in Cores Collected at the U. S. Radioactive Waste Disposal Sites Near the Farallon Islands 60 km off San Francisco and at the Hudson Canyon, 350 km off New York City.
Due to preferential scavenging and lateral transport of a daughter radionuclide, the activity of daughter Ap can be greater than that of the parent Ap in sediments. The inputs of daughter radionuclides that are not directly from the in situ decay of the parent (supported) are termed unsupported or excess activity. The unsupported Ap is equal to the supported A ) minus the Ap, as shown in the theoretical radionuclide profiles in figure 7.3. Moreover, the curve for the unsupported Ap decreases with depth more than the supported Ap because it is not being produced in situ from the parent. Consequently, the excess activity of a radionuclide can be used to calculate the time elapsed since the particles with unsupported Ap were last at the surface, relative to a particular depth (A). However, to calculate this it must be assumed that the sedimentation rate and supply of unsupported Ap has remained constant over time. [Pg.128]

Results and Discussion. Figure 1 shows the decay in the fraction of cells in solution with the dimensionless time, Pt for various values of the parameter Pt, as predicted by (9). For Pt ->-0, the shape of the curve for practically all finite values of Pt is exponential, as previously predicted by Ruckenstein and Prieve (1975). For Pt > 0, there exists a point on the decay curve, at t = t, before which (t S t ), the rate of deposition increases with time and after which, (t > < ), the rate of deposition decreases with time as in the exponential case. The characteristic shapes of these curves may serve as a useful tool to analyze experimental data. A simple inspection of an experimental curve presenting ijno as a function of time and a comparison between it and the curves in Figure 1 can reveal the relative contribution of the external field and the potential barrier to the kinetics of deposition. This is important in order to avoid misinterpretation of low sedimentation rate as low adhesiveness in studies of cell adhesion. In the analysis of experimental data, the following possibilities should be checked ... [Pg.174]

Figure 11 Calculated asymptotic organic C P ratios plotted as a function of sedimentation rate. Designation of these (C P)org ratios as asymptotic derives from the fact that they represent the composition of organic matter buried below the depth at which the (C P)org increases, and so reflect the composition of buried (preserved) organic matter. Error bars represent the standard deviation of the average asymptotic (C P)org values, or the absolute range of values where their number was less than or equal to 3. Solid curve is the model-predicted asymptotic (C P)org ratio versus sedimentation rate. See text for discussion (after Ingall and Van Cappellen, 1990). Figure 11 Calculated asymptotic organic C P ratios plotted as a function of sedimentation rate. Designation of these (C P)org ratios as asymptotic derives from the fact that they represent the composition of organic matter buried below the depth at which the (C P)org increases, and so reflect the composition of buried (preserved) organic matter. Error bars represent the standard deviation of the average asymptotic (C P)org values, or the absolute range of values where their number was less than or equal to 3. Solid curve is the model-predicted asymptotic (C P)org ratio versus sedimentation rate. See text for discussion (after Ingall and Van Cappellen, 1990).
The amount of carboxylic anhydride used for modification of A1(OH)3 determines the sedimentation rate of filler particles and the increase in water-based slurry viscosity. A limiting value of viscosity is attained at relatively low levels of modifier. This amount of modifier is sufficient to react with the available sites on the A1(OH)3 providing conditions for the breakdown of the aggregates and a separation of individual particles. Since the reaction decreases particle-particle interaction these processes are likely to occur. The sedimentation volume curve can be explained in the same way. [Pg.327]

Fig. 3.2 (a) Depth distribution of total Hg, %C and bacterial sulfate reduction rates (SRR). (b) Sediment mixing curves determined across the landslide layer based on Hg and %C data presented in (a), (c) AVS and pyrite sulfur concentrations at station S-l, October 1984. Dashed lines indicate approximate location of lower and upper boundaries of the landslide. [Pg.71]

Inpolydisperse systems the blurriness of sedimentation boundary is related to both the diffusion and the differences in the sedimentation rates of particles having different sizes. In cases when diffusion is negligible, the c(R) dependence represents the shape of integral particle size distribution curve at any moment of time. [Pg.434]

Figure 12. Sedimentary and geochemical records from oceans, showing dramatic transient shifts in most records in an interval from just before 8 Ma to 4 Ma (shaded), from Filippelli (1997b). Symbols in all records represent averages of 1 Myr intervals, except for normalized sediment flux curve, which represents 0.5 Myr averages. After interval averaging, all records were adjusted to time scale of Cande and Kent (1992) for consistency, (a) Normalized sediment flux in northern Indian Ocean (Rea 1992). (b) Ge/Si ratio in opaline silica from diatoms (Shemesh et al. 1989). (c) of bulk marine carbonates (Shackleton 1987). Although details of different carbon isotope records differ, general trends revealed in this low-resolution record are robust. PDB is Pee Dee belemnite. (d) Phosphorus accumulation rates in equatorial Pacific (Filippelli and Delaney 1994). Peak in accumulation rates is also observed in other parts of Pacific (Moody et al. 1988) and western Atlantic (Delaney and Anderson 1997). These peaks are linked with increased phosphorus input rates from continental weathering (e.g., Filippelli and Delaney 1994). (e) Sr/ Sr record from marine carbonates (Hodell et al. 1990, 1991). (f) of benthic foraminifera (Miller et al 1987). Figure 12. Sedimentary and geochemical records from oceans, showing dramatic transient shifts in most records in an interval from just before 8 Ma to 4 Ma (shaded), from Filippelli (1997b). Symbols in all records represent averages of 1 Myr intervals, except for normalized sediment flux curve, which represents 0.5 Myr averages. After interval averaging, all records were adjusted to time scale of Cande and Kent (1992) for consistency, (a) Normalized sediment flux in northern Indian Ocean (Rea 1992). (b) Ge/Si ratio in opaline silica from diatoms (Shemesh et al. 1989). (c) of bulk marine carbonates (Shackleton 1987). Although details of different carbon isotope records differ, general trends revealed in this low-resolution record are robust. PDB is Pee Dee belemnite. (d) Phosphorus accumulation rates in equatorial Pacific (Filippelli and Delaney 1994). Peak in accumulation rates is also observed in other parts of Pacific (Moody et al. 1988) and western Atlantic (Delaney and Anderson 1997). These peaks are linked with increased phosphorus input rates from continental weathering (e.g., Filippelli and Delaney 1994). (e) Sr/ Sr record from marine carbonates (Hodell et al. 1990, 1991). (f) of benthic foraminifera (Miller et al 1987).
Variance analysis by gravity sedimentation has been carried out to estimate the quality of the resultant products after the preliminary hydrodynamic impact in a turbulent mode and in the reference experiment of microheterogeneous catal) ic systems. Variance analysis data have been processed by the graphic differentiation of the precipitant accumulation curve. The results were used to determine the mass-averaged equivalent raduis r (the radius of a spherical particle with the same sedimentation rate) [35]. [Pg.148]

The microscopic analysis of the synthesised suspensions showed that the BaS04 particles are anisometric (rods with a ratio of length to diameter of 4 1, which explains the sigmoidal appearance of the sedimentation inflection curves). At the initial phase of sedimentation, the rod-like particles may rotate, which provides additional resistance to their movement (similar to an increase in viscosity), and decelerates the sediment accumulation rate. Moreover, during free sedimentation, the aspherically formed particles provide maximum resistance to their own motion. This also decreases the sedimentation rate of the solid particles and complicates the definition of their true size. Therefore, the equivalent radius r (radius of spherical particle, settling at the same rate) was defined according to the results of sedimentation analysis. [Pg.233]

Walling DE (1977) Limitations of the rating curve technique for estimating suspended sediment loads, with particular reference to British rivers. Erosion and Solid Matter Transport in Inland Waters. International Association of Hydrological Sciences Publ. No. 122, pp. 34 8. [Pg.4491]


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