<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 />
|