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GEOLOGICAL SURVEY CIRCULAR 850-1

FOREWORD
v
Mount St. Helens, in southwestern Washington, erupted at 8:32a.m., P.s.t., on May 18, 1980. The north side of the volcano's cone was blown off by a powerful lateral blast, and a huge volume of debris buried land and water features in the drainage area immediately north and northwest of the mountain. Major geomorphic and hydrologic changes extended downstream along the Toutle and Cowlitz Rivers, with mudflows and hydraulic effects reaching the Columbia River (fig. 1). Details of these post-eruption events are described in other reports of this volume.
This report deals with emergency flood hazard situations created by the massive debris avalanche deposit in the North Fork Toutle River valley and by downstream sediment deposition. The debris deposit is up to 600 ft thick; it formed a dam approximately 500 ft high at the outlet of Spirit Lake, creating a set of conditions conducive to overtopping and subsequent downstream flooding. To date (March 1981), this has not occurred. However, Geological Survey hydrologists witnessed and recorded the overtopping and failure of a similar but smaller dam in the North Fork Toutle River near Elk Rock. A flood-hazard assessment made the day before the dam failure proved to be reasonably accurate and useful for the choice of advance protective measures.
The report contains (1) a brief description of the computer models employed to make the dam-failure and flood-threat analyses; (2) analyses of the dam-failure potential at Spirit Lake and at Elk Rock; and (3) hypothetical flood routings from both of these sites.
Modeling methods were employed in an effort to identify and compute the flood hazards associated with the massive post-eruption drainage modifications. Land (1980) described and evaluated available dam-failure, flood-wave computer models and concluded that the model developed by Fread (1980) was the most generally applicable. Land prepared a modified version, named the Dam Break Flood Forecast (DBFF) model, which was utilized for the Mount St. Helens dam-break hazard calculations.
The DBFF modification of Fread's model employs the current understanding of dam-failure mechanics and hydrodynamic flow theory to predict the formation of a dam-failure wave and its downstream movement. The modified model is a practical tool with wide applicability. It can function with input data r3.1\ging from complete and accurate data specification to merely rough estimates of input parameters. The model is economical to run, requiring only nominal amounts - of time on large computers.

The DBFF model consists of three functional parts (Fread, 19.80; Land, 1980): (1) description of the mode of dam failure,. that is, the temporal and geometrical description of the breach; (2) computation of the hydrograph of outflow through the developing breach as governed by the physical and hydraulic features of the reservoir, mainly rates of inflow to the reservoir and its storage characteristics; and (3) routing of the outflow hydrograph · through the . downstream valley to determine discharge hydrograph changes resulting from downstream variations .in valley storage capacity and from frictional resistance to flow.
The DBFF model permits adoption of a variety of breach formation characteristics to simulate either overtopping or piping failure. The user specifies the failure time interval and the final size and shape of the fully developed breach. During model operation, the breach formation commences when the reservoir's water-surface elevation (h) exceeds a critical input stage (hr). An overtopping failure is simulated when hr is set to a value such that a sufficient amount of water is flowing over the crest of the dam to cause· failure. A piping failure is simulated when hr is set to a value below the height of the dam. Overtopping failure modes were assumed for the North Toutle River calculations. The mode of breach failure selected influences the results significantly.
DBFF computes the outflow from the breached dam as the summation of breach flow and flow through spillway outlets. The total outflow hydrograph is a function of water-surface elevation and outlet geometry and is related to depletion of reservoir storage volume. The reservoir routing in DBFF uses either (1) a hydrologic storage routing technique based on the law of conservation of mass; or (2) a hydraulic approach. The hydrologic storage routing technique was used for all reservoir routings described in this report.
After the outflow hydrograph from a breached dam is determined (expressed in terms of stage and discharge by the model), it is necessary to route the hydrograph through the downstream river valley. The DBFF model utilizes a hydraulic routing method based on the two differential equations governing one dimensional unsteady flow, the equations of continuity and momentum. A nonlinear implicit finite-difference algorithm was employed to solve the equations. The computational procedure is capable of simulating both subcritical and supercritical flows.
According to Fread (1980), a distinguishing feature of flood waves generated by dam failure is the great magnitude of the peak discharge compared to runoff-generated flood waves. A dam failure flood is usually many times greater than the runoff flood of record. For example, the most severe flood estimated for a Spirit Lake debris dam failure was about 25 times the maximum flood observed on the Toutle River during a 54-year period. The timespan from the first rise to the peak of the discharge hydrograph generally is very short. This feature can cause serious computational difficulties. In the process of routing dam-failure flood hydrographs down the North Fork Toutle and the Toutle Rivers, considerable time was spent eliminating computational problems introduced by the rapid rise in stage.
An unsteady streamflow simulation model, J879, documented by Land (1978) was used to route flood hydrographs down the North Fork Toutle River, and then down the Cowlitz River to its juncture with the Columbia River. J879 is a computer program for simulating one-dimensional subcritical, gradually varied unsteady flow. It does not perform dam-failure calculations. The program solves the differential equations for unsteady flow, using a linear implicit finite-difference algorithm as the computational method. Details of the J879 computational scheme are contained in a report by Land (1978). Model J879 was employed because the DBFF model did not include the option that would accommodate the correct downstream boundary condition at the Columbia River.
Many uncertainties arose immediately following the eruption of Mount St. Helens concerning the extent of hazards, both geologic and hydrologic. The massive debris blockage- estimated to be 3 to 4 billion cubic yards (Youd and Wilson, 1980)-was
I3 known to block the outlet of Spirit Lake. However, due to poor visibility from aircraft and the dangers of onsite observation, only limited informatioi1 was available on the size of the post-eruption lake and on the stability of the debris dam.
On May 19, Geological Survey hydrologists visited the area and determined that the elevation of the lake surface had been raised about 200ft by the events of May 18. It was thought that the lake represented a possible flood hazard, and the Survey thus initiated work to estimate the downstream flow peaks that would occur if the debris dam failed. The estimates were to be completed within 2 days and, therefore, based largely on initial field observations of water and land conditions. This input information was fragmentary and approximate, particulary for Spirit Lake storage characteristics and the debris dam.
Figure 2 compares an approximate debris-modified bed profile of the North Fork Toutle River compared to the originals bed profile. Figure 3 shows representative channel cross sections constructed from topographic maps and used in the modeling study for the North Fork Toutle and Toutle Rivers. Note the marked variation in channel cross-sectional shape. Although pre-eruption cross-sectional configuration was used in the absence of post-eruption information, vertical elevations of cross section in the first 14.5 mi below the lake outlet were raised in accordance with early estimates of the debris-modified bed profile. The elevations adopted are somewhat lower than those given in the report by Youd and Wilson (1980, fig.
The use of approximate cross-sectional information from small-scale maps was to prove a hindrance to acceptable computational results. The DBFF model computations failed to provide reasonable answers because the actual cross-sectional shapes varied markedly in places from the idealized inputs used for the modeling exercise.

One of the many difficulties encountered in evaluation of the Spirit Lake flood hazard was determination of the most probable mode of failure of the Spirit Lake dam (Youd and Wilson, 1980). In addition to the stability of the debris material forming the dam, the probable mode of failure was dependent on the height and lateral width of the dam, the size and volume of the lake, and the height of water behind the dam. Field information was minimal. Attempts to treat the debris as a dam proved only partly useful. It was finally decided to conceptualize the Spirit Lake hazard as an overtopping, rather than a piping failure or other possible form of breach. Because of the great downstream extent of the debris (14.5 mi), piping or other forms of failure were considered unlikely.
Overtopping conceivably could result from mudflows entering the lake, from snow- and icemelt runoff, or a combination of these events. Water discharged by overtopping failure was visualized to flow over the debris and down the channels carved in the debris mass by the mudflow that followed the May 18 damming of Spirit Lake. -


FIGURE 3.-Selected pre-, May 18, 1980, eruption cross sections of the North Fork Toutle, Toutle, and Toutle River channels
Working from this hypothesis of the mode of failure, calculations were made for overtopping and failure of the Spirit Lake dam throughout the estimated 53.6-mi reach from Spirit Lake (mi 0.0) to the mouth of the Toutle River (mi 53.6). A trapezoidal breach was adopted as the most probable geometric profile, and side slopes of 2 vertical to 1 horizontal were assumed. Three cases were investigated, assuming different sizes and durations of breach development:
The discharges in each case were computed on the basis of estimated reservoir stage and the assumed breach dimensions. CASE I- Duration of breach development equals 1 hr; final breach depth equals 150 ft; maximum width of breach equals 200 ft; discharge at dam equals 1,130,000 ft/s; CASE II- Duration of breach development equals 1 hr; final breach depth equals 100 ft; maximum breach width same as in CASE I; discharge at dam equals 613,000
CASE III- Duration of breach development equals 3 hr; final breach depth equals 50 ft; maximum breach width same as in CASE I; discharge at dam equals 174,000 ft/s.
Results of calculations for the three cases are presented in table 1 a.nd figure 4. The computed range in downstream discharge was wide and convergence of profiles at the mouth was only moderate, indicating little attenuation of the flood wave. Thus, uncertainty in the prediction of potential failure characteristics resulted in corresponding uncertainty in the dam-failure flood-hazard estimates.
The CASE II results shown in table 1 were reported to Geological Survey headquarters as the basis for emergency planning. Subsequently, calculations were made for CASE ll conditions in
the Cowlitz River using the flood-routing program J879. A special river mileage system was adopted for the Cowlitz River flood-routing exercise and the calculations were based on the channel cross sections shown in figure 5. As for the North Fork Toutle and Toutle Rivers, no post-eruption data were available, necessitating the use of pre-eruption configurations. In addition, assumptions were made of a constant flow of 9,000 ft/s from the upper Cowlitz River and a constant Columbia River stage elevation at mile 73.1 (mouth of Cowlitz River) of 5."5 ft above National Geodetic Vertical Datum (NGVD). The Columbia River at this location is affected significantly by tides, but for simplification the average elevation was adopted.
The results of the calculations for CASE II, using J879, from mile 17.0 below Spirit Lake to mile 73.1 are given in table 2. The discharge estimate of 138,000 ft/s at mile 63.4 can be used as a point of context. This discharge corresponds to about a 500-year flood for an unsilted Cowlitz River channel. It is necessary to note, however, that sedimentation following mudflows on May 18-19 markedly reduced the floodwater capacity of the lower Cowlitz River.
A comparison of results obtained using DBFF and J879 was possible below mile 17 on the North Fork Toutle and Toutle Rivers. The flood routing technique in J879 gave considerably more attenuation than DBFF (fig. 4.). The explanation is not obvious and requires further research. It is possible that J879, at least for large, steep-fronted flood waves, may contain some artificial numerical attenuation, especially where reach sizes and time steps are large. The attenuation may be the result of using the linear implicit finite-difference algorithm. The attenuation of the flood wave yielded by the DBFF model was so small that it is somewhat questionable, especially in reaches of the Toutle River downstream from the junction of the North and South Forks.
The surface of the debris clogging in the North Fork Toutle River was highly hummocky, with many depressions and pits, some of which contained ponded water. The debris dammed the mouth of several tributaries of the North Fork, including Maratta and Coldwater Creeks. During July and early August 1980, a small lake impounded at the mouth of Maratta Creek (fig. l) broke through its dam as a result of saturation of the dam material and overtopping. The lake water flowed downstream a short distance where it became trapped behind an obstruction on the hummocky surface of the debris deposit. The obstruction soon failed and the water moved 4 mi farther downstream, where it collected behind another obstruction, forming a 250 acre-foot lake near Elk Rock.
The new lake presented a flood hazard and the Geological Survey personnel, thus, made a series of dam-break calculations using DBFF and input data obtained from onsite observations. The dam was 112 ft high and 215 ft wide. The ponded water was 30 ft deep, placing the pond surface 82 ft above the base of the dam.
The model computations were made on August
- The next day, the dam failed following a
rainstorm. Over a period of several hours, Geological Survey personnel observed the breaching of the dam (which took about 40 min) and the downstream movement of the flood wave. Visual estimates of flood discharge were made by Geological Survey and U.S. Corps of Engineers personnel at several locations, and discharge was measured at two gage sites. Table 3 compares the computed peak discharge at various locations with the estimated and measured peak discharges. The computed discharge at the dam was based on the assumed formation of a near-vertical 30-ft slot (100 percent breach) in the 112-ft high and 215-ft wide plug during a period of 0.1 hr. Calculations were made and results averaged using hypothetical failure widths of 60, 80, and 100 ft. The actual failure occurred progressively but erratically during 40 min, and resulted in an irregular opening about 52 ft high.
Considering the hypothetical assumptions on which the model calculations were based, the comparison between the simulated and the estimated/measured discharges is considered to be good.
The Elk Rock dam failure resulted in damage to channel-maintenance equipment in the North Fork Toutle River, but no loss of life or injuries were incurred. The success of the preevent prediction underscores the utility of computer-based models for estimating flood hazards resulting from dam breaks.
Flood hazards posed by potential dam failures were evaluated under hurried, emergency conditions in order to plan for and minimize dangers of flooding associated with the volcanic eruption and debris flow. Investigations included the debris pile impounding Spirit Lake and the dam formed at Elk Rock. The DBFF model was used to evaluate hypothetical failures and to route flows to the Cowlitz River. A second model (J879) was used to route flow down the Cowlitz to the Columbia River. I7 For both models, uneven levels of data accuracy and completeness hampered computation of reliable hazard estimates.
The Elk Rock dam failed the day following the theoretical failure analysis, providing an opportunity to compare hypothetical and actual results. The comparison between the simuiated and estimated discharge is good, indicating that computer models can play a useful role in the assessment of dam-break flood hazards, even though input data are approximate and incomplete.
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