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<br />4. The equations should not be used for reaches of stream affected <br />by backwater from downstream obstructions. <br /> <br />5. The hydraul ic radius does not include the wetted perimeter of <br /> <br />the bed particles. <br />6. These equations are applicable to streams having relatively <br /> <br />clear water and low suspended sediment. <br /> <br />n = 0.39(0.02)0.38 (7)-0.16 = 0.065 <br /> <br /> <br />APPLICATION OF THE PREDICTION AND REGIME EQUATIONS <br /> <br />An example of the appl ication of equations 10, 11, and 12 to a <br />single depth of flow in a steep-gradient stream is as follows: The <br />reach under study has the following hydraulic properties at one repre- <br />sentative c~oss section obtained from a transit-stadia survey. The <br /> <br /> <br />-channel is straight, high-banked, and trapezoidal in shape, and contains <br /> <br /> <br />boulder-size bed material. Cross-section subdivision is not required. <br /> <br /> <br />No additional factors affect roughness, so that nT is equal to n. The <br /> <br /> <br />cross-sectional area is 1 ,000 ~quare ft (92.9 square meters), the slope <br /> <br /> <br />of the water surface for the reach at the time of the survey was 0.02, <br /> <br /> <br />and the hydraulic radius was computed to be 7 ft (2.1 1m). Assuming <br /> <br /> <br />uniform flow at the section and using equation 10 to solve for Manning's <br /> <br /> <br />n, the value obtained is: <br /> <br />The solution is also shown graphically in figure 5. <br /> <br />w <br />