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<br />DESCRIPTION OF FLOOD-WAVE CHARACTERISTICS <br /> <br />27 <br /> <br />amount of debris. The leading edge of the flood wave was <br />moving at an average of 9.1 mi/h in the Roaring River <br />(fig. 15). The peak probably was very close to the leading <br />edge of the flood wave (see "dam.Break Modeling"). The <br />relatively slow speed of the leading edge was due to <br />retardance by the vegetation and resulting debris dams. <br />The leading edge probably was very similar to the <br />1889 flood that resulted from the failure of South Fork <br />dam near J obnstown, Pa., which claimed 2,209 lives. In <br />the 1889 flood, eyewitnesses described the flood as car- <br />rying extremely large amounts of debris and traveling <br />much slower than expected. <br />From time to time as the flood entered narrow places in the valley, <br />the massed debris acted as a dam and the giant flow seemed to slow <br />and stop; then the front would boil and seethe and huge trees, ejected <br />by overwhelming pressures, would shoot into the air as the flood o~ce <br />more surged ahead. (Clark, 1982, p. 141). <br />Ample evidence of large debris dams remained in the <br />Roaring River (fig. 17). The 1982 flood also carried large <br />amounts of debris, including very large boulders <br />(fig. 1GB). <br />For these conditions, the theory and application of <br />conventional energy and flow-resistance concepts (such <br />as Manning's n-values) probably are not applicable. The <br />occurrence of numerous debris dams caused localized <br />backwater, resulting in predominately subcritical flow. <br />However, when these debris dams break, flow probably <br /> <br />was supercritical for a short distance until another <br />debris dam formed. Thrbulence was extremely high, as <br />observed by Stephen Gillette at Horseshoe Falls, where <br />he saw boulders and trees being thrown into the air. <br />Across the large alluvial fan formed at the base of <br />Horseshoe Falls, water spread. The depth, width, veloci- <br />ty, or cross-sectional area of flow are unknown. Early <br />in the flood, the flow path was down the major axis of <br />the fan. This was the area of the fan where the largest <br />boulders and thickest sediments were deposited. Soon <br />after the flood wave arrived, the main flow path became <br />plugged with sediment and debris; on the falling limb <br />of the hydrograph, the main flow gradually shifted to <br />the right side of the fan. This migration of the main flow <br />effects from the left to right parts of the alluvial fan is <br />indicated by the distinctly finer-grained deposits on the <br />right side of the fan, flow paths visible on large-scale <br />aerial photographs, and the geographic position of the <br />boulder berms formed during the first few minutes of <br />the flood. <br /> <br />FALL RIVER, HORSESHOE FALLS <br />TO CASCADE LAKE DAM <br /> <br />The confluence of the Roaring River with the Fall <br />River is at the upstream end of Horseshoe Park (fig. 1). <br /> <br /> <br />FIGURE 17.-The remains of a large debris dam in the Roaring River valley near river mile 3.21. <br />