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<br />318 <br /> <br />BULLETIN OF THE ASSOCIATION OF ENGINEERING GEOLOGISTS <br /> <br />,. <br /> <br />a 14 <br />Z <br />a <br />u <br />& 12 <br />~ <br />w <br />~ <br />I! 10 <br />t;: <br />~ <br />u , <br />~ <br />~ <br />u <br />~ 6 <br />.. <br />~ , <br />x <br />u <br />~ <br />" 2 <br /> <br /> <br /> <br />o <br /> <br />31 <br /> <br />30 <br /> <br />AUGUST <br /> <br />JULY <br /> <br />Figure 13. Hydrograph showing the effect of a debris flow for <br />Crystal River above Avalanche Creek near Redstone, Coio.. <br />July-August 1959. <br /> <br />PROBLEMS IN ESTIMATING THE WATER <br />DISCHARGE OF SEDIMENT-BEARING <br />FLOWS <br /> <br />The presence of recently eroded channels and <br />coarse deposits may lead some investigators to con- <br />clude that a waterflood has occurred, An indirect <br />discharge estimate then is obtained using common <br />techniques, such as slope-area methods. For ex- <br />ample, the slope-area estimates of discharge along <br />the East River tributary, assuming a water-flood <br />flow for the event on July 24, 1977, are as much as <br />112 to 286 m"/s (3,950-10,000 ft"/s) (Mears, 1979, <br />table I), About 200 m (650 ft) farther downstream, <br />at the toe of the debris fan, 100 m (325 ft) in front <br />of the terminal lobe, our estimate made from high- <br />water marks indicates the peak water flow here <br />was less than 8 m"ls (280 ft"/s). It is unlikely that <br />peak attenuation of such magnitude would have <br />taken place in such a short distance, <br />Downstream of the tributary junction, the flow of <br />the East River was approximately 6 m'ls (200 ft3/s) <br />(well below bankfull) on the day the area was vis- <br />ited (June 21, 1978), A discharge in excess of this <br />amount would have left high-water marks in the <br />channel or on the floodplain below the debris fan, <br />Yet no high-water marks for a stage greater than 6 <br />m"ls (200 ft3/s) were observed on the East River <br />immediately below the debris fan, Therefore, the <br />water runoff from this tributary was most likely less <br />than 8 m'ls (280 ft"/s) , much less than originally re- <br />ported (Mears, 1979). <br /> <br />When such conventional slope-area methods that <br />use Manning's and Bernoulli's equations are mis- <br />takenly applied to debris flows, excessive water- <br />flood flow estimates usually result, Several impor- <br />tant assumptions that are invalid when applying the <br />slope-area method to debris flows are: <br /> <br />I. That the water-flood passage is uniform with <br />steady flow or gradually varied flow, <br />2. That the vertical-velocity distribution is loga- <br />rithmic. <br />3, That the high-water marks (defined by seed <br />lines, drift, and water lines) remaining after the <br />passage of the flood reflect the height of the <br />water flow. For a waterflood, the marks should <br />not indicate any ponding (backwater) resulting <br />from a damming effect common at the front of <br />debris flows, <br />4. That channel erosion should be minimal. <br />5. That Mannings' roughness coefficient "n," <br />which has been determined for water-flow dis- <br />charges, should be used in the computations <br />(Benson and Dalrymple, ]967; Da]rymple and <br />Benson, 1967), <br /> <br />There are hydraulic relations available for use <br />with debris flows, Gol'din and Lyubashevskiy <br />(1966) discuss some formulas proposed by Russian <br />hydrologists to compute the average velocity of <br />mudflows in Crimean river channels. <br />Waterfloods and debris flows are end members of <br />a continuum of a wide range of sediment-water mix- <br />tures in channels. Hooke (1967) believes the differ- <br />ence between waterfloods and debris flows is that <br />(a) the sediment load in waterfloods is varied by <br />deposition or erosion, whereas only the coarsest <br />fragments are deposited by debris flows, and (b) <br />streams (waterfloods) continue to flow so long as a <br />slope exists, but debris flows stop on a finite slope. <br />Thus, a debris flow cannot be converted into a wa- <br />terflood by deposition. A problem exists where wa- <br />terfloods transport large volumes of sediment, or <br />where a debris flow is followed by a more fluid wa- <br />terflood, disrupting the evidence of the debris flow, <br />The problem of making slope-area discharge esti- <br />mates for small mountain streams transporting a <br />large but unknown percentage of sediment is illus- <br />trated in Figure 14 which is a plot of drainage area <br />versus discharge. The curve is an estimate of the <br />500-year discharge for the Rocky Mountains in Col- <br />orado from McCain and Jarrett (1976). Debris-flow <br />slope-area discharge estimates (circles in Figure 14) <br />are discussed in the following section, The triangles <br /> <br />" <br />