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<br />r, <br /> <br />tion'geometry values from the original slope area measure- <br />ment. The high water marks and cross sections of the channel <br />from the original survey are assumed to define the crest of the <br />wave that produced the peak discharge and the channel ge' <br />ometry at that time, Wave heights were determined by sub, <br />tracting the computed water surface elevations (D,) from the <br />surveyed flood mark elevations (D,), Instantaneous discharge <br />of the largest waves (Q._) was computed as the product of <br />the cross-sectional area of the waves and the corresponding <br />velocity (V._) using the equation by Brater and King (1954), <br />For the average conditions at the cross sections and using <br />a roughness coefficient of 0,030, the average wave height of <br />1.37 m [Table I, column (2)] is the same as the average height <br />of the largest waves observed by Fancher, The computed wave <br />velocity [Table I, column (6)] for these conditions, using the <br />equation by Brater and King (1954), is also in close agreement <br />with Fancher's observations. This close agreement suggests <br />the total instantaneous peak discharge may have been 2,740 <br />m'ls or 32% more than the published discharge of 2,082 <br />m'ls [Table I, column (7)], <br />An estimated hydrograph for Q, and an "envelope" hydro' <br />graph for total instantaneous peak discharge were determined <br />(Fig, 2), The wave envelope depicts the instantaneous wave <br />discharge for approximately 30 translatory waves at 4-5,min <br />intervals for about 2 h on the basis of Fancher's account, <br />Nearly all of the runoff volume is depicted by the hydrograph <br />for Q, because the wave envelope depicts only the instanta- <br />neous discharge for approximately 30 waves, and total wave <br />volume was estimated to be about I % of the total runoff, The <br />hydrograph and wave envelope (Fig, 2) are intended to rep- <br />resent only the general runoff and wave conditions for the <br />flood as reported by Fancher and were developed from both <br />discharge and flow instability computations, <br /> <br />'1 <br />I <br />I <br />I <br /> <br />ANALYSIS <br /> <br />Supercritical Flow and Translatory Waves <br /> <br />Reports of pulsating waves in steep flood channels and lab- <br />oratory flumes are fairly common and have been documented <br />by Holmes (1936), Thompson (1968), Brock (1969), Foley <br />and Vanoni (1977), and Kranenburg (1992), How common are <br />supercritical flow and translatory waves in natural channels? <br />McGee (1897), Glancy and Harmsen (1975), Belcher (1976), <br />Phillips and Hjalmarson (1996), and Hjalmarson (1987) doc- <br />umented eyewiiness accounts of possible translatory waves <br />(supercritical flow) in natural channels, Perhaps the occurrence <br />of pulsating flow in natural channels is more common than <br /> <br />indicated because (I) The potential for observations has been <br />small because of the sparse population in the areas where <br />many steep wide channels are found; (2) the cause of walls of <br />water in arid lands has been erroneously attributed to intra- <br />event damming and breaching (Schick and Lekach 1989); and <br />(3) the waves have not been clearly recognized by hydraulic <br />engineers involved in the collection and analysis of flood-peak <br />discharge data who have assumed that the flow was gradually <br />varied and stable, <br />For example, the observation of waves in the channel up' <br />stream from U,S, Highway 93 bridge was mentioned to the <br />original USGS survey crew immediately following the Bronco <br />Creek flood but was not considered in the computation of peak <br />discharge, Another example is the catastrophic flood of Sep- <br />tember 14, 1974, in Eldorado Canyon, Nevada, which killed <br />at least nine people and destroyed many homes, vehicles, and <br />boats (Glancy and Harmsen 1975), The flood had a computed <br />peak discharge of 2,152 m'ls, a drainage area of 53,3 kIn , and <br />similar to the Bronco Creek flood, the highwater marks in the <br />slope area reach may have been produced by translatory waves <br />(Glancy and Harmsen 1975), Following are some statements <br />by observers of flow in the steep sand channel of Eldorado <br />Canyon: "," a 6-8 ft-high (1.83-2.44 m) approaching <br />wall. . ." and ", . . initial wave followed by several wavelike <br />surges. . ." <br />McGee (1897) documents his eyewitness account of a sheet- <br />flood wave on the western piedmont slopes of the Tortolita <br />Mountains north of Tucson, Arizona. According to McGee, <br />the floodwater spread beyond the confines of a channel at <br />"race-horse speeds" with a wall of water 15 - 30 cm high, and <br />within the flood, transverse waves formed breakers, The trans- <br />verse waves may have been similar to the reflected waves <br />reported by Thompson (1968) for wave development in su' <br />percritical flow. The steep incised channels of some alluvial <br />fans with slopes of about 3% or greater in the southwestern <br />United Stales are possible sites for the formation of potentially <br />hazardous waves. <br /> <br />Wave Development <br /> <br />The translatory waves in Bronco Creek may have been <br />formed where the channel bed changes gradually from bedrock <br />to sand (Fig, 1) because, according to Koloseus and Davidian <br />(1966), the degree of flow stability is inversely proportional <br />to the channel width-depth ratio and directly proportional to <br />channel roughness, Peak discharge estimates at (I) The paleo- <br />flood sites of 750 m'ls (House and Pearthree 1995); (2) the <br />channel conveyance'slope sites of 1,082 m'ls (H. W. Hjal- <br /> <br />TABLE 1. Results of Slope Ares snd Wsve Computstlonslor Flood 01 August, 19, 1971, In Bronco Cresk <br /> <br /> Total instantaneous <br />Cross-section Wavs hslght Q,~ Vt",.1C QWfl'llllC Vwrnax- peak discharge <br />number (m) (m'/s) (mls) (m'/s) (mls) (m'ls) <br />(1) (2) (3) (4) (5) (6) (7) <br /> <br /> (a) n = 0,030 <br />Average 3-4 10,06 2.739b <br />Average 3-4 1.37 799 6,60 1,943 12,51 2,742' <br /> (b) n = 0.040 <br />Average 3-4 7,64 2,082b <br />Average 3-4 1.13 799 5,47 1,433 11.05 2,232' <br /> (c) Average of Ernest Fancher's observations <br /> 1.37 I I 11.33 <br /> <br />Note: [Q....,., maximum base discharge; Vi....,.. mean velocity of the maximum base discharge; Q......,., instantaneous discharge of the largest waves; <br />V..mu, average velocity of the largest waves. Dashes indicate no data. <br />-Computed using (4) except for Fancher's observations. <br />bComputed using slope area method. <br />CComputed using translatory wave techniques. <br /> <br />JOURNAL OF HYDRAULIC ENGINEERtNG I JUNE 1997/573 <br />