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<br />e <br /> <br />. <br /> <br />. <br /> <br />; <br /> <br />e~ <br /> <br />where <br /> <br />MEASUREMENT OF PEAK DISCHARGE AT CULVERTS BY INDIRECT METHODg <br /> <br />fi <br /> <br />O=the discharge coefficient, <br />A,=the flow area at the control section, <br />V, = the mean velocity in the approach <br />section, <br />a,=the velocity-head coefficient at the <br />approach section, and <br />h/,_.=thehead loss due to friction between <br />the approach section and the inlet <br />=L~(Q'fK1K,), and <br />K= conveyance = (1.486fn) R'!3A , (6) <br /> <br />Other notation is evident from figure 1 or it <br />has been previously explained. The discharge <br />coefficient, 0, is discussed in detail in the ~ection <br />entitled "Coefficients of Discharge." <br /> <br />Type 2 "ow <br /> <br />Type 2 flow, as shown on figure 2, passes <br />through critical depth at the culvert outlet, <br />The headwater-diameter ratio does not exceed <br />1.5, and the barrel flows partly full. The slope <br />of the culvert is less than critical, and the tail- <br />water elevation does not exceed the elevation of <br />the water surface at the control section, h,. <br />The discharge equation is <br /> <br />Q=CA,~2g (hl+ a~" -d,-h"_.-h,,.,} (7) <br />where <br /> <br />h/,.3=the head loss due to friction in the <br />culvert barrel=L(Q'fK,J(,), <br /> <br />Flow with backwater <br /> <br />When backwater is the controlling factor in <br />culvert flow, critical depth cannot occur and the <br />upstream water-surface elevation for a given <br />discharge is a function of the surface elevation <br />of the tailwater. If the culvert flows partly full, <br />the headwater-diameter ratio is less than 1.5; or <br />if it flows full, both ends of the culvert are <br />completely submerged and the headwater- <br />diameter ratio may be any value greater than <br />1.0. The two types of flow in this classification <br />are 3 and 4. <br />Type 3 flow <br /> <br />Type 3 flow is tranquil throughout the length <br />of the culvert, as indicated on figure 2. The <br />headwater-diameter ratio is less than 1.5, and <br /> <br />the culvert barrel flows partly full. The tail- <br />water elevation does not submerge the cuh-ert <br />outlet, but it does exceed the elevation of crit.;cal <br />depth at the terminal section. <br />The lower limit of tailwater must be such that <br />(1) if the culvert slope is steep enough that <br />under free-fall conditions critical depth at the <br />inlet would result from a given elevation of <br />headwater, the tailwater must be at an elevation <br />higher than the elevation of critical depth at tbe <br />inlet; and (2) if the culvert slope is mild enough <br />that under free-fall conditions critical depth at, <br />the outlet would result from a given elevation of <br />headwater, then the tailwater must be at an <br />elevation higher than the elevation of critical <br />depth at the outlet. <br />The discharge equation for this type of flow is <br /> <br />Q=CA3~2g (h,+ a'~"-h,-h/l-2-h,,_,} (8) <br /> <br />Type 4 flow <br /> <br />In this classification the culvert is submerged <br />by both headwater and tailwater, as is shown <br />in figure 2. The headwater-diameter ratio can <br />be anything greater than 1.0. No differentiation <br />is made between low-head and high-head flow <br />on this basis for type 4 flow. The culvert flows <br />full and the discharge may be computed directly <br />from the energy equation between sections 1 <br />and 4. Thus, <br /> <br />[h,+h.,=h,+h.,+h'l-2+h, <br />+h"., +h/3-4 +(h., -h..)], <br /> <br />where <br /> <br />h.=head loss due to entrance contraction. <br /> <br />In the derivation of the discharge formula <br />shown below, the velocity head at section 1 <br />and the friction loss between sections 1 and 2 <br />and between sections 3 and 4 have been ne- <br />glected, Between sections 3 and 4 the energy <br />loss due to sudden expansion is assumed to be <br />(h.,-h..). Thus, <br /> <br />h,=h.+h.+h,..,+h." <br /> <br />or <br /> <br />Q= OA ~ 2g(h,-h.) , (9) <br />o 290'n'L <br />1+ Ro'!3 <br />