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<br /> <br />e <br /> <br />e <br /> <br />e <br /> <br />MEA8UREMENT OF PEAK DI8CHARGE BY THE SLOPE-AREA METHOD <br /> <br />5 <br /> <br />weighted conveyance of each su breach on the <br />form as shown on figure 7. First, use the two- <br />section formula given in table 1 to compute <br />directly the discharge for each two-section <br />subreach. The computed values will most <br />lik8ly differ for each subreach. Then, using <br />the appropriate discharge as the "assumed" <br />value on the form, complete for each subreach <br />the computation of the various heads, slope, <br />and "computed" discharge. The "computed" <br />discharge will agree exactly with the "assumed" <br />if computations are made correctly. This <br />procedure provides an interim check and gives <br />considerable insight into the transformation <br />of 8nergy and energy loss from section to section <br />along the reach. Consistency of results among <br />the subreaches is made evident, <br />Use one of the equations shown in table 1 <br />to compute the final value of discharge. These <br />equations are based on the energy equation <br />and the Manning equation applied throughout <br />the reach. The values of k in the equations <br />are 0.5 if t:.h, is positive and 0 if t:.h, is negative <br />in the given subreach. The value of t:.h, for <br />each subreach was determined in the previous <br />computations and may be used to determine <br />the values of k in the multisection equation. <br />After the final value of discharge has been <br />determined, use that value to compute the <br />subsection discharges for subdivided sections, <br />the corresponding velocities, and the mean <br /> <br />velocities for all sections. Enter the compu- <br />tations in the two columns at the right of the <br />computation form. Computed velocities should <br />be compatible with the appearance of the <br />channel after the flood. Gross errors can be <br />recognized in some instances if velocities are <br />greatly different from those expected. <br /> <br />Froude Number <br /> <br />The value of the Froude number should be <br />computed for each cross section after the final <br />discharge has been determined. The Froude <br />number is defined as <br /> <br />V <br />F=-, <br />~ <br /> <br />(9) <br /> <br />where V is the mean velocity and dm is the <br />average depth in the cross section. <br />The Froude number is an index to the state <br />of flow in the channel. For example, in a <br />rectangular channel the flow is tranquil if the <br />Froude number is less than 1.0 and is rapid if <br />the Froude number is greater than 1.0. The <br />slope-area method may be used for both tranquil <br />and rapid flow. The Froude numbers for the <br />various sections or for subsections of compound <br />sections should be examined to determine the <br />state of flow in the reach. <br /> <br />Number of <br />cro.t",edioM <br /> <br />Table: 1 .-Discharge equations ror use: in slope-area measurements <br /> <br />2 <br /> <br /> <br />t:.h <br />K'L K,' [ (A,), (k ] <br />K, +2gA,' -"I Al 1- )+",(I-k) <br /> <br />Q=K, <br /> <br />3 <br /> <br />Y t:.h <br />Q=K3 KKK' A ' A ' <br />K:(K: LI-,+L'-')+2gA.,,[ -"I (A:) (l-k,-oH"'(A:) (k,-3-kl-oHa,(I-k,.,)] <br /> <br />Multiple <br />(n) <br /> <br />Q=K.-V Aa;.B' where <br /> <br />4=K' L,_, +K' 4, + K.'L"_2l-"-ll+ K.'L"_ll~ <br />... n KIK2 1f, K2Ka ... K(Jl.-2)K(n-l) K(rt-l)Kn <br /> <br />B= A~~g [ -"I (~~Y (l-k,-,H", (~:)' (k..,-kHH"3 (:tY (k...-kHH . . . <br /> <br />+""-ll (AA. )' (k"_I)_.-k('_2l_('_l))+".(I-k"_ll~)]' <br />(n-l) <br />