Sedimentology (2010) 57, 1126–1146 doi: 10.1111/j.1365-3091.2009.01140.x The partitioning of the total sediment load of a river into suspended load and bedload: a review of empirical data JENS M. TUROWSKI*, DIETER RICKENMANN* and SIMON J. DADSON *Swiss Federal Research Institute WSL Birmensdorf, Zürcherstrasse 111, 8903 Birmensdorf, Switzerland (E-mail: [email protected], [email protected]) Centre for Ecology and Hydrology, Maclean Building, Crowmarsh Gifford, Wallingford, UK Associate Editor – Steve Rice ABSTRACT The partitioning of the total sediment load of a river into suspended load and bedload is an important problem in fluvial geomorphology, sedimentation engineering and sedimentology. Bedload transport rates are notoriously hard to measure and, at many sites, only suspended load data are available. Often the bedload fraction is estimated with ‘rule of thumb’ methods such as Maddock’s Table, which are inadequately field-tested. Here, the partitioning of sediment load for the Pitzbach is discussed, an Austrian mountain stream for which high temporal resolution data on both bedload and suspended load are available. The available data show large scatter on all scales. The fraction of the total load transported in suspension may vary between zero and one at the Pitzbach, while its average decreases with rising discharge (i.e. bedload transport is more important during floods). Existing data on short-term and long-term partitioning is reviewed and an empirical equation to estimate bedload transport rates from measured suspended load transport rates is suggested. The partitioning averaged over a flood can vary strongly from event to event. Similar variations may occur in the year-to-year averages. Using published simultaneous short-term field measurements of bedload and suspended load transport rates, Maddock’s Table is reviewed and updated. Long-term average partitioning could be a function of the catchment geology, the fraction of the catchment covered by glaciers and the extent of forest, but the available data are insufficient to draw final conclusions. At a given drainage area, scatter is large, but the data show a minimal fraction of sediment transported in suspended load, which increases with increasing drainage area and with decreasing rock strength for gravel-bed rivers, whereby in large catchments the bedload fraction is insignificant at ca 1%. For sand-bed rivers, the bedload fraction may be substantial (30% to 50%) even for large catchments. However, available data are scarce and of varying quality. Longterm partitioning varies widely among catchments and the available data are currently not sufficient to discriminate control parameters effectively. Keywords Bedload, sediment transport, suspended load, total load. INTRODUCTION The sediment load of a river is one of the key variables in channel dynamics. Planform pattern, morphology, erosion, deposition and migration of the channel are in a large part determined by the 1126 amount of sediment moved by the flow in relation to the water discharge (e.g. Schumm, 1963; Shepherd, 1972; Montgomery & Buffington, 1997; Madej, 2001; Parker et al., 2007), and many engineering and forestry applications (for example, channel stability, reservoir sedimentation, 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists The partitioning of sediment load bridge pier scouring, hazard mitigation and soil erosion) rely on good knowledge of the transport processes for design, management and maintenance (e.g. Lauffer & Sommer, 1982; Stott & Mount, 2004; Walling & Collins, 2008; Chin et al., 2009). Following the definitions of Einstein (1950) and Vanoni (1975), a river can carry sediment in two distinct modes. In bedload transport, the sediment particles move by rolling, sliding or hops of the length of a few grain sizes (known as saltation), and they are thus in frequent contact with the channel bed. In suspended load transport, on the other hand, the weight of the particles is supported by turbulent forces in the water and they can travel considerable distances without coming into contact with the bed. Herein, the dissolved load, which can be substantial, is ignored (e.g. Alvera & Garcı́a-Ruiz, 2000; Galy & France-Lanord, 2001; Lana-Renault & Regüés, 2007) because the solid load is most important for engineering and sedimentological applications, and because few reliable parallel records of all three quantities are available. The total load is thus the sum of suspended load and bedload. Grains with sizes that cannot be found in the shifting parts of the bed in appreciable quantities are known as wash load which, in general, is a part of the suspended load. Whether an individual particle is transported as suspended load or as bedload depends on particle size, weight and shape, and on the ambient hydraulic conditions. Two methods are commonly used to determine suspended load. In the first method, sediment concentration is determined by sampling the water at a representative point within the crosssection and then filtering and drying the sample and weighing the remaining solids. In the second method, the turbidity of the water is monitored with an optical method and sediment concentration is calculated with a calibration curve. Both methods are based on the assumption that the determined concentration is representative of the whole cross-section. The suspended load is then calculated by multiplying concentration with discharge. More sophisticated sampling integrates over the water depths to collect more representative samples (e.g. Eads & Thomas, 1983; Lecce, 2009). To automate these methods is more or less straightforward, allowing the collection of large quantities of data. On the contrary, measuring bedload is difficult, usually time and staff intensive and thus expensive (Ergenzinger & de Jong, 2003). The most common 1127 method is the use of sampling baskets lowered to the stream bed (Tacconi & Billi, 1987; Bunte & Abt, 2005). These baskets usually need to be operated manually, either by standing in the stream or from a boat, and they allow only point measurements both in space and time. Other methods include the construction of a retention basin to trap the load and the use of tracer particles. Retention basins can only be feasibly realized for small catchments and tracer methods require extensive field work after each transport event to recover the particles. As a result there are vastly more data available on suspended load than on bedload. Total load is often estimated by measuring suspended load, while the bedload fraction is either ignored due to lack of constraints (e.g. Holeman, 1968; Milliman & Meade, 1983; Milliman & Syvitski, 1992) or taken to be a fixed fraction of the total load (e.g. Hindall, 1976; Griffiths & McSaveney, 1986; Whipple & Tucker, 2002; Brocard & van der Beek, 2006). Numbers that can be found frequently in the literature are 10% to 20% bedload fraction of the total load in general (e.g. Simons & Sentürk, 1977; Dietrich and Dunne, 1978; Holland, 1978; Summerfield & Hulton, 1994; Hay, 1998; Basumallick & Mukherjee, 1999; Galy & France-Lanord, 2001; Lavé & Avouac, 2001) and sometimes 20% to 40% for mountain rivers (e.g. Schröder & Theune, 1984; Dadson et al., 2003; Turowski et al., 2007, 2008), often without giving original data or references. These numbers can be traced back to a Letter to the Editor of the Transactions of the American Geophysical Union (Lane & Borland, 1951). These authors adapted a table (often referred to as Maddock’s Table; see Appendix) that was originally published in a virtually unknown earlier report (Maddock & Borland, 1950), claiming that it is: ‘‘probably the best answer to the problem devised to date’’ (Lane & Borland, 1951). However, Lane & Borland (1951) did not give the full reference to the source, the data basis for the numbers, or the reason why they deemed their judgement to be appropriate. In the original publication, Maddock & Borland (1950) stated that their table: ‘‘gives data on estimates of the unmeasured or bedload of streams based on Bureau of Reclamation experience’’ (Maddock & Borland, 1950), without giving further details on methods and data. Thus, it seems likely that the original tables have been devised without any reliable objective foundation and may just have been a compilation of order of magnitude estimates based on the intuition of field workers. A general revision of this material has, to the 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 1128 J. M. Turowski et al. knowledge of the present authors, so far not been attempted. Since the 1950s, little material has been published dealing specifically with the partitioning of total load into bedload and suspended load. Much of the available material has been published in technical reports or conference reports, and is not widely known. In general, the problem can be approached from two sides: (i) the longterm average dynamics, which is needed, for example, to predict reservoir sedimentation rates; and (ii) the short-term variation with hydraulic conditions, necessary to make predictions used, for example, in hazard mitigation. To study the short-term dynamics and the variation of partitioning with discharge, parallel point measurements of suspended load and bedload are taken (e.g. Williams & Rosgen, 1989; Meunier et al., 2006). However, this only allows the long-term average partitioning to be determined if a long series of data with high temporal resolution is available. The most simple method to determine long-term partitioning is by regularly surveying the deposits in a reference area (preferably in a natural or man-made reservoir), which is a sink for all material transported as bedload. Simultaneously, suspended load going in and out of the area needs to be measured (e.g. Kjeldsen, 1983). A different method has been used by Colby & Hembree (1955) in the Niobrara River, Nebraska. Assuming that all transported material moved in suspension there, these authors compared the suspended load fluxes through a narrow and deep channel stretch with highly turbulent flow (total load section) with measurements in unconfined channel stretches. Their aim was to test and improve the Einstein (1950) method of calculating total load. However, their survey method can only be applied in very special circumstances and thus is not suitable for general use. Colby (1957) used the same database, complemented by total load estimated using the Einstein (1950) procedure, to derive a relationship between bedload transport and flow velocity. The aim in this article is to present published material and provide a synthesis of the current empirical knowledge of the partitioning of total sediment load into suspended load and bedload. Comparisons with theoretical models are left out consciously. Many models have been proposed to calculate suspended load, bedload or total load and none of these has yet been accepted to be valid universally (e.g. Gomez & Church, 1989). Thus, the present study concentrates on empirical relationships and the few published methods to estimate the partitioning of total load into suspended load and bedload directly. In the following, observations made at the Pitzbach, a glacially fed mountain stream near the village of Imst in south-western Austria, where independent measurements of suspended load and bedload were taken at high temporal resolution in 1994 and 1995 are discussed first. As the data cover most of the observation period, the study of both long-term and short-term behaviour is possible. Then, the results are compared with compilations of data from the literature, discussing both the short-term behaviour and the long-term average partitioning. THE PITZBACH The Pitzbach is situated near the village of Imst on the southern side of the Inn Valley (Fig. 1). The Tyrolean Water Power Company (TIWAG) maintains a water intake with a gauging station in the stream at an elevation of 1811 m above sealevel (a.s.l.). There, the stream drains a total area of 26Æ8 km2, 60% of which is covered by glaciers. The average discharge is ca 5Æ9 m3 sec)1 during the summer, when discharge varies with the daily cyclicity typical for glacially fed streams (Hofer, 1987). During the summer months, sediment transport is almost continuous and daily transport events occur in spring and autumn. A Tyrolean weir with a width of 6 m in a rectangular cross-section and a rack spacing of 15 cm is located at the gauging station. From the weir, water is separated off into a sediment settling basin with a length of 40 m and a width of 3 m, in order to have clean water for hydropower generation. Grains larger than 15 cm, which do not fit through the grid and are thus Imst Fig. 1. Location map of the Pitzbach near the village of Imst in Austria. 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 The partitioning of sediment load Table 1. Pitzbach data statistics. Data Number Fraction Total With sediment transport With suspended load transport With bedload transport Only suspended load transport Only bedload transport Both suspended and bedload 55 301 35 395 35 204 9576 25 819 191 9385 1 0Æ640 0Æ637 0Æ173 0Æ467 3Æ45 · 10)3 0Æ170 A Suspended load (kg s–1) not measured, account for 0Æ2% to 2% of the total transported bedload (Hofer, 1987). During the measurement campaign, sediment deposition in the retention basin was monitored by five load cells located along the centre line of the basin floor and a water pressure sensor. The weight was recorded every 15 minutes and stored together with the stage level measured at the weir. The deposition basin was flushed out automatically whenever the stored sediment exceeded a predefined weight and all sediment was inserted back into the stream downstream of the weir. The turbidity of the water was measured near the upstream end of the settling basin and converted to sediment loads using a rating curve based on water samples. More detailed information on the hydrology and hydraulics at the gauging station and the Pitzbach in general can be found in the articles by Hofer (1987), Rickenmann & McArdell (2008) and Turowski & Rickenmann (2009). For the Pitzbach, 55 301 data points are available with reliable measurements of both suspended load and bedload (Table 1). Out of these data points, non-zero sediment transport was observed 35 395 times, that is 64% of the time. Bedload transport occurred only 17% of the time. At the Pitzbach, both bedload and suspended load measurements show large scatter (Fig. 2). The fraction of suspended load varies between zero and one and, even for small discharges, high fractions of bedload have been observed. Similar observations were previously reported by Whittaker (1987). To obtain the mean behaviour, the data were classified into logarithmically distributed bins. On average, suspended load is more important, and summed over the whole data set for 1994 to 1995 about 74Æ2% of the total sediment yield was transported as suspended load; this agrees well with earlier estimates of 81Æ1% in 1975 to 1978 (Lauffer & Sommer, 1982) and 78Æ6% in 1981 (Hofer, 1987). The importance of suspended load decreases with increasing discharge and for the largest measured discharges (above 1129 Bedload (kg s–1) B Discharge (m s–1) Fig. 2. Partitioning of total load for the Pitzbach. Grey dots represent individual data points, black dots represent binned means. (A) Suspended load plotted as a function of bedload. The solid line gives the 1:1 relation for comparison. On average, suspended load is larger than bedload, but for individual 15 minute periods, the opposite can be true. (B) The fraction of suspended load scatters widely but, on average, declines with discharge. In A data points without bedload transport are not included in the calculation of averages, leading to slightly different values on A and B. ca 12 m3 sec)1) bedload constitutes almost 50% of the total load on average or more (Fig. 2B). For certain modelling approaches, for example the simulation of transport rates at high temporal resolution, it may be necessary to stochastically model the partitioning of the total load into suspended load and bedload, using a relation between water discharge and the probability density function of the partitioning. In the case of the Pitzbach, the b distribution was chosen (e.g. Johnson et al., 1995) as an appropriate probability density function (pdf) to describe the 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 1130 J. M. Turowski et al. fraction of the total load transported in suspension at a given discharge: pdfðx; a; bÞ ¼ x a1 ð1 xÞb1 Bða; bÞ A Q = 4·27 m3 s–1 ð1Þ Here x is the fraction of the load transported in suspension, and B(a, b) is the b function, which is defined by: Z 1 t a1 Bða; bÞ ¼ dt ð2Þ b1 0 ð1 tÞ The parameters a and b are related to the expected value E(x) and the variance var(x) of the distribution: a ð3Þ EðxÞ ¼ aþb varðxÞ ¼ ab ða þ bÞ2 ða þ b þ 1Þ B Q = 5·36 m3 s–1 ð4Þ There is no compelling physical reason for using the b distribution, but it is defined on the interval between zero and one, as required, and it is sufficiently flexible to handle most empirical data. Although there are other distribution functions with similar properties, for example the Kumaraswamy (1980) distribution, the b distribution is implemented in most commercially or freely available statistics software and thus methods for parameter estimation or random number generation are easily accessible. In general, the b distribution provides a good description of the Pitzbach data (Fig. 3). Mean, standard deviation and the fit parameters a and b as functions of discharge are shown in Fig. 4. In the Pitzbach, for discharges above 3Æ5 m3 sec)1, the coefficient of variation (the ratio of standard deviation and mean) of the fraction of suspended load is approximately constant at a value of 0Æ22 (Fig. 4E). If the mean partitioning can be estimated, a constant coefficient of variation may be a good first modelling assumption. More problematic is the occurrence of only suspended load even at high discharges. The b distribution cannot handle values of zero or one (or rather, assigns them a probability of zero). At the Pitzbach, the fraction of measurements of only suspended load drops steeply with increasing discharge, to an approximate constant of ca 10% at discharges above ca 6 m3 sec)1 (Fig. 4F). However, bedload transport might have occurred at rates below the detection limit for these data points. For modelling purposes, the b distribution should be sufficiently accurate to simulate the stochasticity of Fig. 3. Examples of the distribution of the fraction of suspended load, at discharges of 4Æ27 and 5Æ36 m3 sec)1. At these discharges many data points are available, making the analysis most robust. The b distribution describes the data well (the insets show per cent–per cent plots). the partitioning between bedload and suspended load. PARTITIONING OF SUSPENDED LOAD AND BEDLOAD IN INSTANTANEOUS MEASUREMENTS This section is based mainly on the compilation of parallel measurements of suspended load and bedload from USGS reports by Williams & Rosgen (1989), complemented by some additional data (Nanson, 1974; Métivier et al., 2004; Meunier et al., 2006), if the parameters necessary for the calculation at hand were available. Of course, the measurements are not strictly instantaneous but represent the average transport rates over a few minutes. The term instantaneous was used here to contrast with long-term measurements as discussed below. The data come from 96 streams covering a wide range of conditions in both mountain streams and larger rivers, and comprise 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 The partitioning of sediment load A Mean fraction suspended load 0·9 0·8 0·7 0·6 0 2 4 6 8 10 Standard deviation fraction suspended load B 1·0 C 0·3 0·2 0·1 0·0 D 12 2 4 6 8 10 0 2 4 6 8 10 0 2 4 6 8 10 4 8 Beta Alpha 0 5 10 6 4 3 2 1 2 0 0 0 2 4 6 8 10 E F 0·3 0·2 0·1 0·0 0 2 4 Discharge 8 6 (m3 10 Fraction of measurements without bedload transport Coefficient of variation fraction suspended load 1131 1·0 0·8 0·6 0·4 0·2 0·0 s–1) Discharge (m3 s–1) Fig. 4. Distribution statistics of the partitioning at the Pitzbach as a function of discharge. Results for bins above ca 10 m3 sec)1 were not plotted, as they come from bins with very few data points and are not statistically significant (see Fig. 2B). (A) The mean fraction of suspended load declines with increasing discharge. (B) Standard deviation. (C) Scale parameter a of the b distribution. (D) Shape parameter b of the b distribution. Note that the fitted mean calculated from a and b with Eq. 3 is lower than the sample mean shown in (A), as data points with the suspended fraction equal to one are excluded in the probability fits. (E) The coefficient of variation of the fraction of suspended load, the ratio of standard deviation and mean, is approximately constant at ca 0Æ22 in the range between 3 and 10 m3 sec)1. (F) The fraction of the number of measurements with only suspended load transport declines steeply with increasing discharge to a constant value of ca 10% for discharge higher than ca 6 m3 sec)1. almost 2000 individual data points. The discharges at which the data were taken range over more than six orders of magnitude from 0Æ007 to 15 200 m3 sec)1. Métivier et al. (2004) noted that their suspended load data from the Ürümqi River, Chinese Tian Shan, can be expressed as a power function of the bedload data; and Meunier et al. (2006) confirmed this observation for the Torrent de St Pierre, French Alps. This approach was adopted here for the whole data set (Fig. 5), although the axes were exchanged, as it is more often necessary to predict bedload from suspended load than vice versa. Despite the large scatter, sometimes over more than four orders of magnitude, there is a clear trend. On average, suspended load transport rates correlated with bedload transport rates. A two-part fit with power laws provides a good description of the median trend and can be used as an empirical equation to estimate bedload G from suspended load L: G¼ aLb ; L ða=cÞ1=ðdbÞ cLd otherwise ð5Þ The best-fit values of the constants a, b, c and d for the 25th, 50th and 75th percentiles are given in Table 2. Both power laws fit the binned means with R2 values greater than 0Æ9. At suspended load transport rates around 1 kg sec)1, bedload trans- 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 1132 J. M. Turowski et al. A B Fig. 5. (A) Bedload transport rates plotted as a function of suspended load transport rates for data reported by Nanson (1974), Williams & Rosgen (1989), Métivier et al. (2004) and Meunier et al. (2006). Despite the large scatter, a clear trend is visible. Filled diamonds give the medians of the binned data (large symbols) and the 25th and 75th percentiles are indicated by small filled squares. The solid lines are the fit to the medians according to Eq. 5 (Table 2). (B) Bedload transport rate as a function of suspended sediment load concentration for the same data. Table 2. Fit values for Eq. 5. Parameter Fit: 25 percentile Fit: 50 percentile Fit: 75 percentile a b c d 1 L ¼ ða=cÞdb 0.131 1.340 0.241 0.588 2.249 0.833 1.340 0.437 0.647 0.394 2.653 ± 0.594 (kg sec-1)1-b 1.1425 ± 0.092 1.473 ± 0.518 (kg sec-1)1-d 0.590 ± 0.052 0.345 kg sec-1 ± 0.007 (kg sec-1)1-b ± 0.125 ± 0.131 (kg sec-1)1-d ± 0.062 kg sec-1 port rates constitute almost 50% of the total load on average. For higher and lower suspended load transport rates, bedload is less important. The maximum total volume concentrations of sediment, defined as the total volume transport rates of sediment normalized by discharge, are around 1%. Equation 5 should not be used to estimate bedload transport rates for higher total sediment concentrations, for example for hyperconcentrated floods. However, suspended load concentrations span a large range of values between 1 and 29 100 mg l)1 (Fig. 5B). The Pitzbach data have not been included in the evaluation of Eq. 5, as it comprises almost five times as many data points as for the other streams put together and would thus dominate the trend locally. However, the points fall in the same region as the other data (Fig. 6); this underlines the generality of the relationship. The behaviour of an individual stream may differ considerably from this trend. For example, in the Horse Creek near Westcreek, Colorado (Williams & Rosgen, 1989), bedload transport is more important than suggested by Eq. 5 and in the Trout Creek near ± 0.052 (kg sec-1)1-b ± 0.079 ± 0.210 (kg sec-1)1-d ± 0.076 kg sec-1 Bayfield, Colorado (Williams & Rosgen, 1989), suspended load is more important (Fig. 6). Equation 5 should thus be used with care when attempting to predict the partitioning for a particular stream; however, it may be useful for regional or global sediment budget estimates. There is no general relationship between the fraction of sediment transported in suspension and discharge. For some streams, suspended load becomes less important as discharge increases, for some there is little variation and for some it becomes more important (Fig. 7). The data can be used to directly test the partitioning proposed by Maddock & Borland (1950) and Lane & Borland (1951) (see Appendix). These authors separated the streams into sandbed and gravel-bed, according to the dominant grain size, and assigned the fraction of bedload according to the observed suspended sediment concentration. Here, a river was classified as sand-bed if the median grain size was smaller than 2 mm. On average, at higher suspended sediment concentrations a smaller fraction of the load is transported as bedload (Fig. 8). As before, 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 The partitioning of sediment load 1133 Sand-bed Gravel-bed Fig. 6. Bedload transport rates as a function of suspended load transport rates, based on the data reported by Nanson (1974), Williams & Rosgen (1989), Métivier et al. (2004) and Meunier et al. (2006). The data are differentiated by source and the plot additionally includes the Pitzbach data. Equation 5 gives the general trend of the data (see also Fig. 5) but is not necessarily suitable to describe the relation for individual streams. In certain streams (e.g. Horse Creek, Colorado) bedload is more important than the trend for the medians suggests, while in others suspended load is more important (e.g. Trout Creek, Colorado, Susitna River, Alaska). The Pitzbach data fall on the same general trend. Fig. 7. Some examples of the variation of the fraction of the sediment transported in suspension as a function of discharge. Apart from the Pitzbach, examples come from the data compilation of Williams & Rosgen (1989) and have been chosen purely for their illustrative value. While for some streams the bedload part becomes more important at increasing discharge (e.g. Pitzbach, Oak Creek), for other streams there is little variation for the studied discharges (e.g. Susitna River) or the suspended load becomes more important (e.g. San Antonio River, Redwood Creek). Large scatter can be observed at similar discharges (e.g. Big Lost River, Yentna River). Fig. 8. Fraction of total load transported as bedload plotted as a function of suspended sediment concentration for the data compiled by Williams & Rosgen (1989). Vertical lines give the boundaries of the three concentration classes proposed by Maddock & Borland (1950). Due to the large scatter, the partitioning criteria given by Maddock & Borland (1950) and Lane & Borland (1951) for three classes of suspended sediment concentrations (Appendix, Table 3) will mostly yield poor results. the scatter is very large, especially for low sediment concentrations. The methods proposed by Maddock & Borland (1950) and Lane & Borland (1951) give largely adequate results for sand-bed rivers for the averages, except for the highest concentrations, but under-estimate the bedload fraction for gravel-bed rivers (Table 3). The data compiled by Williams & Rosgen (1989) were used to develop an update to Maddock’s Table (see Appendix) based on field data. Following Maddock & Borland (1950) and Lane & Borland (1951) the data for gravel and sand-bed rivers were separated and 15 classes of suspended sediment concentration were defined. As using absolute values of suspended sediment transport seems to reduce the scatter (see Fig. 5), the same method was employed for absolute transport rates. The results are listed in Tables 4 and 5 and are illustrated in Fig. 9. The fraction transported as bedload decreases both with increasing suspended sediment load and concentration. Interestingly, the mean values for sand-bed and gravel-bed streams are similar for suspended load transport rates above ca 10 kg sec)1. High sediment transport rates are typically associated with floods. For low bed shear stress, conditions of partial transport are often observed in gravel-bed streams (Parker, 1990; Wilcock & McArdell, 1997) and a possible explanation for the convergence of the two curves may be that, around transport rates 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 1134 J. M. Turowski et al. Table 3. Fraction of total load transported as bedload as a function of suspended sediment concentration. Bedload fraction in gravel-bed streams Bedload fraction in sand-bed streams Suspended sediment concentration (p.p.m.) Maddock & Borland (1950) Lane & Borland (1951) Data mean Data standard deviation Maddock & Borland (1950) Lane & Borland (1951) Data mean Data standard deviation <1000 1000 to 7500 >7500 0Æ05 0Æ05 to 0Æ1 0Æ02 to 0Æ08 0Æ05 to 0Æ11 0Æ05 to 0Æ11 0Æ02 to 0Æ07 0Æ26 0Æ055 0Æ088 0Æ27 0Æ085 0Æ054 Up to 0Æ5 0Æ1 to 0Æ2 0Æ1 to 0Æ2 0Æ2 to 0Æ6 0Æ09 to 0Æ26 0Æ05 to 0Æ13 0Æ51 0Æ10 0Æ035 0Æ33 0Æ089 0Æ032 Means and standard deviation were calculated from the data compiled by Williams & Rosgen (1989). Parts per million (p.p.m.) were taken to be by weight, which makes it equivalent to the dimensional quantity mg l)1, if the fluid is water. of ca 10 kg sec)1, all grain sizes are mobilized and the particle size distribution of the transported load approaches the size distribution on the bed. LONG-TERM PARTITIONING OF SUSPENDED LOAD AND BEDLOAD The data set studied here has been compiled from various sources (Table 6). As direct observations are most interesting, contributions were excluded that are based on the evaluation of grain-size distributions of deposited material (specifying a cut-off grain size for suspended load) or on theoretical relationships to evaluate the partitioning such as the Einstein total load equation (e.g. Jowett & Hicks, 1981; Bezzola et al., 1991; Syvitski & Saito, 2007). In addition, some published material was not used because the measured suspended load and bedload partitioning were not given explicitly or could not be calculated from the available data (e.g. Leaf, 1966; Kuhnle et al., 1989; Lu & Li, 1989). The data presented in Table 6 come from many different sources and were collected with different methods and for different reasons. Thus, several potential parameters of interest for the present purpose (most importantly the grain-size distribution or representative grain parameters) were not reported in many studies. Data quality, comparability and methods of observation are discussed explicitly only where it seems necessary. Major assumptions or problems are pointed out in the footnotes to Table 6. The reader is referred to the original publications for further details. The data are discussed in terms of bulk catchment properties such as drainage area, degree of forestation and glaciation, and geology. In the current compilation gravel-bed streams at small drainage areas, located mainly in mountainous terrain, are clearly over-represented. It was not possible to find direct evaluations of the partitioning of the sediment load for more than four streams with drainage areas larger than 10 000 km2: for the Fraser River, Canada, at Mission and Agassiz (McLean et al., 1999), and the lower Ebro River at the Sastago and Mora d’Ebre Bridges on the Iberian Peninsula (Vericat & Batalla, 2006). In addition, Galy & France-Lanord (2001) assessed the sediment transport of the Ganga and the Brahmaputra by geochemical methods. These authors did not measure the bedload fraction directly, but it was estimated at ca 90% of the unmeasured parts based on unpublished observations (see also footnote to Table 6). Alekseevskiy et al. (2008) reported the partitioning for two individual floods in the Lena River, Russia. These measurements were included to complement the data at high drainage areas. Catchments where the fraction of material transported in suspension is close to one can be found at all drainage areas (Fig. 10). The maximal amount carried as bedload decreases with increasing contributing area, from about 90% in the Torlesse stream (Hayward, 1980) at low catchment sizes to ca 1% in the Fraser River (McLean et al., 1999). At larger drainage areas, for the Lena River (Alekseevskiy et al., 2008), the Ganga and the Brahmaputra (Galy & FranceLanord, 2001) the bedload fraction is higher again; however, it needs to be noted that these are the least reliable data points, for the reasons mentioned above. The difference may be explained by differences in grain size. The Fraser River and the Ebro River are gravel-bed streams, while the Ganga, Brahmaputra and Lena rivers have a sandy bed. Similarly, in the Dora Baltea basin (Vezzoli, 2004), a sand-bed stream at the survey site, the bedload fraction of 59% is much higher than for gravel-bed rivers with a comparable drainage area (ca 3300 km2). Thus, a hypothesis suggested by the available data is that for 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 The partitioning of sediment load 1135 Table 4. Partitioning classified by suspended sediment concentration, after the data of Williams & Rosgen (1989). Concentration smaller than (mg l)1) Mean concentration (mg l)1) Mean fraction of bedload Standard deviation Coefficient of variation Number of points Gravel-bedded stream (1294 points) 2 1 4 2Æ5 8 5Æ4 16 11Æ2 31 21Æ5 61 42Æ0 121 85Æ3 240 179Æ5 477 355Æ3 946 688Æ3 1877 1257 3725 2694 7391 4910 14 666 12 450 29 100 19 767 0Æ55 0Æ37 0Æ29 0Æ28 0Æ26 0Æ27 0Æ29 0Æ24 0Æ13 0Æ09 0Æ07 0Æ04 0Æ01 0Æ12 0Æ07 0Æ28 0Æ33 0Æ28 0Æ28 0Æ28 0Æ26 0Æ25 0Æ22 0Æ16 0Æ12 0Æ08 0Æ08 0Æ004 0Æ07 0Æ04 0Æ51 0Æ89 0Æ97 1Æ00 1Æ08 0Æ96 0Æ86 0Æ92 1Æ23 1Æ33 1Æ14 2Æ00 0Æ40 0Æ58 0Æ57 21 81 182 248 212 129 91 70 87 78 51 36 3 2 3 Sand-bedded streams (236 points) 2 1 4 3 8 5Æ2 16 10Æ9 31 20Æ7 61 40Æ8 121 80Æ4 240 160Æ6 477 317Æ1 946 631Æ1 1877 1131 3725 2395 7391 4918 14 666 8006 29 100 23 450 0Æ997 0Æ992 0Æ84 0Æ80 0Æ70 0Æ57 0Æ52 0Æ36 0Æ27 0Æ11 0Æ09 0Æ10 0Æ13 0Æ08 0Æ01 0 0Æ008 0Æ19 0Æ21 0Æ16 0Æ26 0Æ30 0Æ31 0Æ25 0Æ090 0Æ070 0Æ11 0Æ082 0Æ063 0Æ0004 0 0Æ01 0Æ23 0Æ26 0Æ23 0Æ46 0Æ58 0Æ86 0Æ93 0Æ82 0Æ78 1Æ10 0Æ63 0Æ79 0Æ04 1 2 10 22 36 26 20 20 23 22 18 22 4 8 2 All data (1957 points) 2 4 8 16 31 61 121 240 477 946 1877 3725 7391 14 666 29 100 0Æ45 0Æ32 0Æ28 0Æ32 0Æ28 0Æ28 0Æ26 0Æ20 0Æ15 0Æ10 0Æ07 0Æ06 0Æ09 0Æ07 0Æ05 0Æ32 0Æ31 0Æ28 0Æ30 0Æ28 0Æ26 0Æ26 0Æ22 0Æ19 0Æ11 0Æ08 0Æ10 0Æ08 0Æ06 0Æ04 0Æ71 0Æ97 1Æ00 0Æ94 1Æ00 0Æ93 1Æ00 1Æ10 1Æ27 1Æ10 1Æ14 1Æ67 0Æ89 0Æ86 0Æ80 32 120 241 332 328 223 159 131 132 108 73 56 11 6 5 1 2Æ5 5Æ3 11Æ2 21Æ6 42Æ6 86Æ3 176Æ2 348Æ2 690Æ1 1250 2610 5591 10 308 21 240 gravel-bed rivers the fraction of sediment transported as bedload becomes less important as drainage area increases, while for sand-bed channels bedload transport is more important at a given drainage area. This hypothesis is in agreement with the results from the data on short-term partitioning (Fig. 9). However, more accurate long-term data especially for sand-bed channels are needed to validate this hypothesis. Of interest is the data point for the Marsyandi (Pratt-Sitaula et al., 2007). There, long-term sediment deposits in a natural reservoir dammed 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 1136 J. M. Turowski et al. Table 5. Partitioning classified by suspended sediment transport rate, after the data of Williams & Rosgen (1989). Value smaller than (kg sec)1) Mean suspended load (kg sec)1) Mean fraction of bedload Standard deviation Coefficient of variation Number of points Gravel-bedded stream (1294 points) 0Æ0001 0Æ0001 0Æ0004 0Æ0002 0Æ0015 0Æ0008 0Æ0061 0Æ0034 0Æ0242 0Æ012 0Æ0955 0Æ052 0Æ3777 0Æ20 1Æ4933 0Æ76 5Æ9045 3Æ1 23Æ3457 11Æ2 92Æ3066 53Æ9 364Æ9718 207 1443Æ065 727 5705Æ7467 2815 22 560 8237 0Æ29 0Æ25 0Æ21 0Æ19 0Æ29 0Æ34 0Æ40 0Æ38 0Æ30 0Æ32 0Æ21 0Æ10 0Æ05 0Æ02 0Æ01 0Æ19 0Æ27 0Æ25 0Æ22 0Æ31 0Æ29 0Æ29 0Æ27 0Æ24 0Æ23 0Æ17 0Æ11 0Æ05 0Æ03 0Æ00 0Æ65 1Æ07 1Æ21 1Æ18 1Æ07 0Æ84 0Æ74 0Æ69 0Æ80 0Æ71 0Æ80 1Æ07 0Æ90 1Æ28 0Æ48 10 59 130 182 177 177 115 74 58 43 47 79 82 51 10 Sand-bedded streams (236 points) 0Æ0007 0Æ0002 0Æ0023 0Æ0015 0Æ0075 0Æ0049 0Æ025 0Æ016 0Æ084 0Æ061 0Æ28 0Æ15 0Æ93 0Æ58 3Æ1 1Æ8 10Æ3 5Æ6 34Æ4 20Æ9 114 61Æ5 381 237 1270 725 4232 1732 14 100 9960 0Æ99 0Æ99 0Æ91 0Æ88 0Æ87 0Æ70 0Æ62 0Æ64 0Æ53 0Æ25 0Æ15 0Æ11 0Æ09 0Æ05 0Æ01 0 0Æ004 0Æ20 0Æ25 0Æ12 0Æ28 0Æ26 0Æ19 0Æ18 0Æ16 0Æ10 0Æ10 0Æ08 0Æ04 0Æ00 0 0Æ004 0Æ22 0Æ28 0Æ14 0Æ40 0Æ42 0Æ29 0Æ34 0Æ66 0Æ66 0Æ98 0Æ83 0Æ66 0Æ03 1 4 9 9 10 17 22 23 27 22 29 35 21 5 2 All data (1957 points) 0Æ0001 0Æ0001 0Æ0004 0Æ0002 0Æ0015 0Æ0009 0Æ0061 0Æ0034 0Æ024 0Æ0125 0Æ095 0Æ0524 0Æ38 0Æ2037 1Æ5 0Æ7831 5Æ9 3Æ2823 23Æ3 11Æ9569 92Æ3 50Æ724 365 208Æ8199 1443 730Æ3125 5706 2742Æ1818 22 560 8524Æ1667 0Æ29 0Æ25 0Æ20 0Æ20 0Æ29 0Æ36 0Æ36 0Æ36 0Æ34 0Æ29 0Æ16 0Æ09 0Æ06 0Æ02 0Æ01 0Æ17 0Æ27 0Æ25 0Æ25 0Æ33 0Æ30 0Æ29 0Æ29 0Æ25 0Æ22 0Æ14 0Æ10 0Æ06 0Æ03 0Æ00 0Æ60 1Æ09 1Æ24 1Æ25 1Æ12 0Æ83 0Æ81 0Æ78 0Æ74 0Æ77 0Æ89 1Æ07 0Æ96 1Æ22 0Æ48 15 68 164 223 236 233 189 158 130 91 125 146 112 55 12 by a large landslide were dated with the carbon method and the reported partitioning averages over ca 5400 years, the longest period of any of the data points. Rare, large events, which are frequently missed during observation periods of a few years or even decades, often contribute disproportionately large quantities of sediment to the long-term budget (e.g. Sadler, 1981; Kirchner et al., 2001). As the partitioning varies with discharge, such large events may also supply much of the material transported as bedload. With only 64% suspended load, the data point for 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 The partitioning of sediment load A Gravel-bedded Sand-bedded Unknown grain size Gravel means Sand means 1137 transported as suspended load. A is the drainage area in km2. It is clear from the discussion above that, due to the large scatter in the data, such a simple function will not always yield good results. Nevertheless, Eqs 6a and 6b give a good estimate for the median values for drainage areas below ca 5000 km2 (Fig. 10). A non-linear regression to the data for gravel-bed streams (Table 6) yields the equation (Fig. 10, solid line): Fsus ¼ 055 þ 0040 lnðAÞ ð7Þ The lower bound for gravel-bed streams is welldescribed by the equation (Fig. 10, dotted line): Suspended sediment concentration (mg l–1) B Fsus ¼ 008 lnðAÞ Suspended load transport rate (kg s–1) Fig. 9. Bedload fraction plotted as a function of: (A) suspended sediment concentration; and (B) suspended sediment transport rate for the data compiled by Williams & Rosgen (1989). Data have been separated into gravel-bed and sand-bed streams. Means are given for the classified data (Tables 4 and 5); error bars denote 1 SD. the Marsyandi plots at the lower limit at its drainage area for gravel-bed streams, which may reflect the importance of rare events for the bedload contribution at this location (Fig. 10). Beecroft (1983) reported a bedload fraction of higher than two-thirds for a large outburst flood of a water pocket from the Tsidjiore Nouve Glacier (Switzerland); this compares with a long-term bedload fraction of 0Æ44 (Table 6), providing some further evidence for the hypothesis. Schlunegger & Hinderer (2003) proposed a simple logarithmic function to predict the longterm bedload fraction from the drainage area for streams in the European Alps, based on a part of the data used herein (Fig. 10, dashed line; see also the comments of Hinderer 2001, 2005): Fbed ¼ 0525 00506 lnðAÞ ð6aÞ Fsus ¼ 0475 þ 00506 lnðAÞ ð6bÞ Here Fbed denotes the fraction of total load transported as bedload and Fsus the fraction ð8Þ While Eqs 6a to 8 are useful models, they provide only rough estimates and the behaviour of individual streams can be very different. In addition, the partitioning can vary considerably from flood to flood or from year to year. For example, in the Arnás experimental catchment, Spain, the flood-averaged fraction of suspended load varied between 68% and 100% for 11 floods in 2003 to 2005 (Lana-Renault & Regüés, 2007). Similarly, in the Nahal Yael, a flash-flood stream in Israel, the suspended load fraction varied between 17% and 40% in four floods (Lekach et al., 1992). Using the method of Colby & Hembree (1955), Schroeder & Hembree (1956) reported suspended load fractions between 28% and 79% of the load measured upstream of the sampling point at a constricted section (assumed to represent the total load) for transport in the Niobrara River on individual days. For the yearly sediment loads at the Nigardsbreen glacier, the fraction of sediment transported in suspension varied between 24% and 61% (Kjeldsen, 1974, 1975, 1977, 1981, 1983; Bogen, 1989; Hallet et al., 1996). Bogen (1989) stated that in years with long-duration large floods the fraction of bedload to total load decreased. For the Nigardsbreen glacier the range of reported values is comparable in magnitude with the changes after the timber harvest in the Hore catchment. It is thus difficult to separate the influence of catchment properties, changing flood sizes and natural variability. Neither the amount of forest cover or glaciation in the catchment, nor the underlying geology provide a unique predictor of the long-term partitioning. The extent of forest cover may play a role in the partitioning between bedload and suspended load: for the Hore catchment, Wales, 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 Norway Austria Austria Austria Austria Visa River Arzino Kanzingbach Radurschlbach Pitzbach I V Debris retaining dam IV intake KtW IV intake KtW Norway IV intake KtW North Pennines Alberta Vallais Vallais Alptal Taiwan Taiwan Taiwan Taiwan Taiwan Taiwan Taiwan Taiwan Taiwan Taiwan Taiwan Taiwan Switzerland India India Canada Switzerland Switzerland Norway USA New Zealand Austria UK Norway Norway Siberia Siberia Israel Spain Spain Switzerland Country Engabreen Sunmoon Lake Paiho Reservoir Lyiutan Reservoir Wushantou Reservoir Jenitan Reservoir Tapu Reservoir Wushoh Reservoir Feitsui Reservoir Tsengwen Reservoir Techi Reservoir Kukuan Reservoir Shihmen Reservoir Erlenbach Brahmaputra§ (sand-bed) Ganga§ (sand-bed) Hilda Glacier Tsidjiore Nouve– Bas Arolla– Nigardsbreen** Hilda Creek Torlesse Stream Pitzbach Burnham Reservoir Trollbergdalsbreen Bondhusbreen Yakutsk braiding zone Yakutsk braiding zone Lena River* (sand-bed) Lena River* (sand-bed) Nahal Eshtemoa Isaz Catchment Arbúcies Turtmänna Reservoir Gauging station 56 Vallais Location/station Stream Table 6. Long-term observations on sediment partitioning. 245 12Æ6 22 24Æ5 26Æ8 50 3Æ85 26Æ8 17Æ8 4 12Æ6 15 27 53 60 83 100 219 303 481 592 708 763 0Æ7 583 000 1 060 000 2Æ24 4Æ8 7Æ6 65 897 000 897 000 119 0Æ33 106 36Æ6 Drainage area (km2) 2 6 3 1 4 4 20 30 10 15 10 30 30 15 25 25 30 30 7 2 2 2 2 2 25 2 1 1 67 1 4 06Æ06Æ1998 23Æ06Æ1998 15 6 26 32 Survey period (years) 0Æ89 1 0Æ47 0Æ65 0Æ81 0Æ61 0Æ26 0Æ61 1 0Æ48 1 0Æ93 0Æ75 0Æ55 1 0Æ72 1 1 0Æ51 0Æ49 0Æ49 0Æ43 0Æ56 0Æ39 0Æ57 0Æ45 0Æ1 0Æ79 0Æ55 0Æ64 0Æ54 0Æ65 0Æ67 0Æ95 0Æ59 0Æ34 0Æ6 Fraction suspended load 0 0Æ024 0Æ60 0Æ13 0Æ76 0Æ50 0Æ95 0Æ60 0Æ71 0Æ70 0Æ72 0 0 0 0 0 0 0 0 0 0 0 0 0 0Æ56 0 0 Fraction glaciated Alekseevskiy et al. (2008) Alekseevskiy et al. (2008) Alexandrov et al. (2009) Alvera & Garcı́a-Ruiz (2000) Batalla et al. (1995) Colenco (2001), Hartmann et al. (2006) Dadson (2003) Dadson (2003) Dadson (2003) Dadson (2003) Dadson (2003) Dadson (2003) Dadson (2003) Dadson (2003) Dadson (2003) Dadson (2003) Dadson (2003) Dadson (2003) Dürst (1990) Galy & France-Lanord (2001) Galy & France-Lanord (2001) Gurnell (1987) Gurnell et al. (1988) Gurnell et al. (1988) Hallet et al. (1996) Hammer & Smith (1983) Hayward (1980) Hofer (1987) Holliday et al. (2008) Kjeldsen (1974) Kjeldsen (1974, 1981, 1983), Gurnell (1987) Kjeldsen (1977, 1981, 1983), Gurnell (1987) Kjeldsen (1975, 1977) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Source 1138 J. M. Turowski et al. 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 V Debris retaining dam III Bächental III Bächental III KtW V Debris retaining dam II Tegernsee V Kematen I Mauthen III Reichenhall III Sylvenst. Sp. I Gailitz III Forggensee I Oberdraub. I Liezen I Prutz I Magerbach I Rosegg Washington Washington Washington Washington Ködnitzbach Dürrache Dürrache Taschachbach Fischbach Weissach Melach Gail Saalach Isar Gail Lech Drau Enns Inn Inn Drau West Fork Shultz Creek North Fork Hoffstadt Creek Main Hoffstadt Creek Main Shultz Creek Rio Cordon Fraser River§§ Fraser River–– Two O’Clock Creek Basin Marsyandi Nahal Yael Venter Ache Gail Gail Egg Saalach Gailitz Oker Drau Enns Salzach Salzach Drau Maesnant*** Vent Mauthen Rattendorf Hermagor Unterjettenberg Mündung Gross-Schwülper Oberdrauburg Grossreifling Laufen Burghausen Annabrücke Wales Landslide dam Agassiz Mission Location/station Stream Table 6. Continued. Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria USA USA USA USA Italy Canada Canada Canada Nepal Israel Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria Austria UK Country 28Æ4 55 55 60Æ6 82 95 245 349 940 1138 1237 1423 2112 2113 2464 5119 7057 7Æ7 9Æ83 23Æ7 29Æ8 5 218 000 228 000 9 1620 0Æ5 156 349 595 782 940 1237 1740 2112 4020 6108 6649 7566 0Æ54 Drainage area (km2) 2 10 3 4 1 11 1 10 6 5 10 5 10 5 6 6 10 2 2 2 2 15 21 21 1 5400 10 3 10 10 10 41 10 1 10 3 15 40 10 1/3 Survey period (years) 0Æ82 0Æ37 0Æ41 0Æ77 0Æ75 0Æ5 0Æ81 0Æ9 0Æ68 0Æ76 0Æ96 0Æ78 0Æ88 0Æ89 0Æ94 0Æ91 0Æ96 0Æ83 0Æ85 0Æ81 0Æ79 0Æ76 0Æ99 0Æ99 0Æ99 0Æ64 0Æ32 0Æ80 0Æ85 0Æ95 0Æ68 0Æ80 0Æ96 0Æ87 0Æ88 0Æ82 0Æ88 0Æ88 0Æ96 0Æ21 Fraction suspended load 0Æ11 0 0 0 0 0 0Æ05 0 0 0Æ30 Fraction glaciated Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lauffer & Sommer (1982) Lehre et al. (1983) Lehre et al. (1983) Lehre et al. (1983) Lehre et al. (1983) Lenzi et al. (2003) McLean et al. (1999) McLean et al. (1999) McPherson (1971) Pratt-Sitaula et al. (2007) Schick & Lekach (1993) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Schröder & Theune (1984) Stott & Mount (2004) Source The partitioning of sediment load 1139 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 Wales Wales Wales Wales Wales Sastago Bridge Mora d’Ebre Bridge Tanllwyth Hore Cyff Kirkton Monachyle Lower Ebro River Lower Ebro River Dora Baltea Basin (sand-bed) Isar Pitzbach UK UK UK UK UK Spain Spain Italy Austria Austria Country 0Æ89 3Æ08 3Æ1 6Æ9 7Æ7 49 000 84 000 3264 8839 26Æ8 Drainage area (km2) 12 3 12 8 4 2 2 ? 2 2 Survey period (years) 0Æ75 0Æ54 0Æ49 0Æ99 0Æ99 1 0Æ94 0Æ41 0Æ68 0Æ74 Fraction suspended load 0Æ60 0Æ06 Fraction glaciated Stott & Mount (2004) Stott & Mount (2004) Stott & Mount (2004) Stott & Mount (2004) Stott & Mount (2004) Vericat & Batalla (2006) Vericat & Batalla (2006) Vezzoli (2004) Weiss (1996) This study Source Whether a stream is sand-bed is indicated after its name. Unlabelled streams are gravel-bed. *The data for the Lena River are for two individual events, rather than for an extended period of time. It was included because data for large rivers are rare. Batalla et al. (1995) did not measure the loads over 26 years but did weekly sampling during 1991 to 1992 (and more frequently during floods). The long-term sediment yields were then calculated from the long-term discharge time series with a rating curve approach. Dadson (2003) calculated suspended load as the spatial average of around 150 gauging stations in Taiwan. Some of the sites show higher suspended load than total load (assumed to be the volumes deposited in the reservoirs). There are two possible explanations for this: (i) large amounts of sediment were not deposited but flushed through the reservoir. This possibility was excluded by the author. (ii) The mismatch could be due to errors in survey methods, in the conversions from concentrations to loads or from deposited volume (including pore space) to sediment volume, or from the averaging. The last reason seems to be the most likely. For the cases in question, the fraction of suspended load was set to one. §Galy & France-Lanord (2001) used a chemical tracer method that did not allow estimation of the bedload component directly, but only the sum of the unmeasured parts: the material deposited in the flood plain upstream of the survey point and the bedload transported over the measurement cross-section. Unpublished observations and data (e.g. flow velocity measurements; the movement of anchor chains of boats in the stream) suggest that the bedload component makes around 90% of the unmeasured sediment material. This value is consistent with the estimate of deposition rates in the Ganga basin (Métivier et al., 1999), and leads to a fraction of ca 49% suspended load for both streams. –Gurnell et al. (1988) report data from the ablation season (three months in the summer) and estimated yearly loads from these measurements (see also Small, 1987). For the Tsidjiore Nouve the bedload measurements were somewhat uncertain. The median estimate was used here. **All of Kjeldsen (1983), Bogen (1989) and Hallet et al. (1996) reported data for the Nigardsbreen. However, the data are partly inconsistent (e.g. the year associated with the data seems to be shifted by one year in fig. 2 of Bogen (1989) and fig. 1 of Hallet et al. (1996) and some numbers deviate considerably). Here, the values taken from fig. 1 of Hallet et al. (1996) were used, as they were published most recently. The quoted 10% suspended load was given as a maximum estimate by Hayward (1980). The streams surveyed by Lehre et al. (1983) were affected by the outbreak of Mt St Helens in 1980 and presumably showed elevated sediment transport during the observation period. It is unclear whether and how such an event affects the partitioning. §§The drainage area of the Fraser River at Agassiz was estimated from maps and known drainage area at points upstream and downstream of the survey point. ––At Mission, the sub-surface median grain size was reported at 0Æ38 mm; however, most of the fine material is transported as wash load and the stream has a gravel-bed. ***For the Maesnant stream bedload measurements have been conducted over one year and suspended load measurements over three years. It is not clear which part of the survey was done in parallel, and sediment yield is given for the complete survey periods only. Here, the bedload measurements were assumed to reflect the average for the total three year survey period. Bedload volumes were converted to weights using a bulk density of 1600 kg m)3. Plattlingen IV intake KtW Location/station Stream Table 6. Continued. 1140 J. M. Turowski et al. 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 The partitioning of sediment load 1141 Fig. 10. Fraction of suspended load for long-term observations plotted against drainage area. For small catchments, there is large scatter, which reduces as the contributing area increases. All data points result from observation periods of at least one year (Table 6), except the observations for the Lena River, which come from two individual floods. Best fit curves for gravel-bed streams are indicated (Eqs 6a to 8). Data points from sources with more than two data points are highlighted, as well as those mentioned specifically in the text. Fig. 11. Influence of the amount of glaciation of a catchment on the fraction of the sediment load transported in suspension (see also Table 6). the bedload fraction increased from 32Æ6% when mature forest covered the catchment to 50Æ8% after the timber harvest (Stott & Mount, 2004). On the contrary, in the Kirkton catchment, Scotland, the bedload fraction decreased from 3Æ7% to 0Æ5% after harvest (Stott, 1997; Stott & Mount, 2004). However, considering the large variation that can be observed in the same catchment from year to year, it is questionable whether these numbers can really be attributed to changing vegetation within the catchment, or whether the natural variability is the cause. The range of values for the bedload fraction measured at the Nigardsbreen glacier, for example, exceeds the range of values measured in the Hore and Kirkton catchments for different harvest cycles. There seems to be a slight decline in the importance of suspended load transport with increasing rate of glaciation, provided that some part of the catchment is covered by ice (Table 6; Fig. 11). As there are few data with large scatter, this trend cannot finally be confirmed. Large scatter is observed for unglaciated catchments. For assessment of the role of catchment geology, the data reported by Lauffer & Sommer (1982) are useful because they were obtained using the same methods and are thus directly comparable. Basic information on catchment geology is available (Table 7). For each of the three rough classes of rock type (carbonate/solid sediments, igneous/solid metamorphic and soft metamorphites/soft sediments) given by Lauffer & Sommer (1982) basic statistics were calculated (Table 8). Using Student’s t-test, the hypothesis that the data for the groups come from the same distribution can be rejected at the 1% significance level. Assuming that carbonates/solid sediments are the hardest rocks and soft metamorphites/soft sediments the weakest rocks, the amount transported in suspension becomes more important as the substrate material becomes weaker. In addition, the standard deviation decreases for weaker material; this confirms intuitive expectations: weaker rocks are broken down more easily to small particles. For otherwise equal conditions, one would thus expect on average smaller grain sizes in a catchment with weaker substrate, and thus a larger fraction of the grains transported in suspension. However, a detailed evaluation of this result with more extensive data is required. Of course, a high suspended load fraction can be caused by an abnormally low bedload transport rate, an abnormally high suspended load transport rate or a combination of both (cf. 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 1142 J. M. Turowski et al. Table 7. Geology of the catchments studied by Lauffer & Sommer (1982). Fraction suspended load Stream Location/station Geology Arzino Weissach Dürrache Dürrache Lech Isar Saalach I II Tegernsee III Bächental III Bächental III Forggensee III Sylvenst. Sp. III Reichenhall Enns Inn Inn Taschachbach Radurschlbach Pitzbach Kanzingbach Fischbach Melach Gail I Liezen I Magerbach I Prutz III KtW IV intake KtW IV intake KtW V Debris retaining dam V Debris retaining dam V Kematen I Mauthen Drau I Oberdraub. Ködnitzbach Gail V Debris retaining dam I Gailitz Drau I Rosegg Carbonate/solid sediments Carbonate/solid sediments Carbonate/solid sediments Carbonate/solid sediments Carbonate/solid sediments Carbonate/solid sediments Carbonate/solid sediments (soft metamorphites/soft sediments) Igneous/solid metamorphites Igneous/solid metamorphites Igneous/solid metamorphites Igneous/solid metamorphites Igneous/solid metamorphites Igneous/solid metamorphites Igneous/solid metamorphites Igneous/solid metamorphites Igneous/solid metamorphites Igneous/solid metamorphites (soft metamorphites/soft sediments) Igneous/solid metamorphites (soft metamorphites/soft sediments) Soft metamorphites/soft sediments Soft metamorphites/soft sediments (igneous/solid metamorphites) Soft metamorphites/soft sediments (igneous/solid metamorphites) 1 0Æ5 0Æ37 0Æ41 0Æ78 0Æ76 0Æ68 0Æ89 0Æ91 0Æ94 0Æ77 0Æ65 0Æ81 0Æ47 0Æ75 0Æ81 0Æ9 0Æ88 0Æ82 0Æ96 0Æ96 Table 8. Statistics of catchments with different geologies (see Table 7). Fraction suspended load Geology Number of points Minimum Mean Maximum SD Carbonate/solid sediments Igneous/solid metamorphites Soft metamorphites/soft sediments 7 11 3 0Æ37 0Æ47 0Æ82 0Æ64 0Æ80 0Æ91 1 0Æ94 0Æ96 0Æ23 0Æ14 0Æ08 Syvitski & Saito, 2007), and the reported values may be influenced by short-term variations in sediment supply or transport. For example, the streams studied by Lehre et al. (1983) were affected by the eruption of Mount St Helens in 1980, which delivered large amounts of loose material in ash deposits, rock slides and mud flows. Similarly, it is known that extreme hydrological events can cause significant increases in erosion and sediment production (e.g. Gintz et al., 1996; Turowski et al., 2009). It is clear that such events can affect the local grain-size composition and channel morphology, and thus the partitioning of the total load into suspended load and bedload. However, the exact nature of this change remains unclear. CONCLUSIONS Since the publications of Maddock & Borland (1950) and Lane & Borland (1951) appeared, no attempts have been made to review and synthesize the available empirical data on the partitioning of the total sediment load of a stream into suspended load and bedload. Data on longterm and short-term behaviour of the fraction of sediment transported by a stream as suspended 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 The partitioning of sediment load load were compiled. The fraction of sediment transported in suspension fluctuates strongly for a given stream: for the Pitzbach, a mountain stream in Austria, where sediment transport observations are available at 15 minute resolution, the fraction of suspended load varies between zero and one. For the same catchment, the fraction of suspended load is variable from flood to flood and from year to year, even without any obvious changes in catchment conditions such as climate or land use. Similar observations have been made in other streams for short and long time scales. On average, bedload scales with suspended load for short-term observations and an empirical equation (Eq. 5) were proposed to estimate bedload volume from suspended load measurements. The equation describes a general trend in the data; however, it should be used with care, as individual streams may deviate substantially from the described relationship. It may be useful for continental or global sediment budgets or for modelling purposes. To estimate the bedload fraction for individual measurements Maddock’s Table was updated based on the data compiled by Williams & Rosgen (1989) (Tables 4 and 5). Neither drainage area nor the degree of forest cover or glaciation can be used uniquely to predict the long-term average fraction of sedi- 1143 ment delivered as suspended load. As intuitively expected, the limited data suggest that harder rocks in a catchment lead to a larger bedload component. The available data suggest that for gravel-bed channels bedload transport becomes less important with increasing drainage area, while at a given drainage area it is more important for sand-bed channels. However, particularly for the long-term partitioning, data are still rare and, in the current compilation, gravelbed streams at small drainage areas are overrepresented. Partitioning values vary widely among catchments and the available data are currently not sufficient to effectively discriminate control parameters. APPENDIX: MADDOCK’S TABLE The partitioning given in Table A1 was proposed by Maddock & Borland (1950). Lane & Borland (1951) reproduced the table in a slightly altered and expanded form (Table A2) (see also Vanoni, 1975). ACKNOWLEDGEMENTS We thank B.W. McArdell, D. Walling, A. Beer and M. Church for encouraging comments and for pointing out (and the latter for copying and Table A1. Partitioning due to Maddock & Borland (1950). Suspended load concentration Bed material Suspended material Per cent bedload in terms of total load Low Low Medium Medium High High Sand Gravel or rock Sand Gravel or rock Sand Gravel or rock About the same as bed Small amount of sand About the same as bed 25% sand or less About the same as bed 25% sand or less To 50 5 10 to 20 5 to 10 10 to 20 2 to 8 Low: 1000 p.p.m. or less; medium: 1000 to 7500 p.p.m., high: 7500 p.p.m. or more. Table A2. Partitioning due to Lane & Borland (1951). Concentration of suspended load (p.p.m.) Type of bed material forming the channel of the stream Texture of suspended material Per cent bedload in terms of measured suspended load Less than 1000 Less than 1000 1000 to 7500 1000 to 7500 Over 7500 Over 7500 Sand Gravel, rock or consolidated clay Sand Gravel, rock or consolidated clay Sand Gravel, rock or consolidated clay Similar to bed material Small amount of sand Similar to bed material 25% sand or less Similar to bed material 25% sand or less 25 to 150 5 to 12 10 to 35 5 to 12 5 to 15 2 to 8 2010 The Authors. Journal compilation 2010 International Association of Sedimentologists, Sedimentology, 57, 1126–1146 1144 J. M. Turowski et al. posting) literature. The Tyrolean Water Power Company TIWAG supported the measurement campaign at the Pitzbach and made the data available. S. Rice, J. Syvitski and an anonymous reviewer provided thoughtful and constructive comments that helped improve the manuscript. 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