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<br />2 <br />l\g <br />r:sz:: - - ~, <br />. 1\' <br />. -- -- <br /> <br />\ / <br />HW HWo "'-J <br /> <br />j <br /> <br />. <br /> <br /><l <br />'~ <br />. <br />'~ <br />, <br />J <br /> <br /> <br />-- -----_kG.L h I <br />11.'" -T~------__ __ ~H' HL y~ <br />"'-~ --- <br />____ Ho - __ ZQ__ <br /> <br />------- <br /> <br />SECTION (0 <br /> <br />. <br /> <br />- <br /> <br />~ <br />J <br />J <br />I <br />. <br />A <br />j <br />1 <br />~ <br />, <br />. <br />j <br /> <br />. <br /> <br />TW <br /> <br />. <br /> <br />SECTION 2 <br /> <br />. <br /> <br />. <br /> <br />A <br /> <br />Figure III-S--Full flow energy and hydraulic grade lines. <br /> <br />Figurc III-S dcpicts thc energy grade <br />line and the hydraulic grade line for <br />full flow in a cui vert barrel. The energy <br />grade line represents the total energy <br />at any point along the culvert barrel. <br />HW is the depth from the inlet invert to <br />the energy grade line.The hydraulic grade <br />line is the depth to which water would <br />rise in vertical tubes connected to the <br />sides of the culvcrt barrel. In full <br />flow, the energy grade linc and the hyd- <br />raulic grade line are parallel straight <br />lines separated by the velocity hcad lines <br />cxcept in the vicinity of the inlet where <br />the flow passes through a contraction. <br /> <br />The headwater and tail water condi- <br />tions as well as the entrance, friction, <br />and exit losses are also shown in figure <br />III-S. Equating the total energy at <br />scctions I and 2, upstream and downstream <br />of the culvert barrel in figure III-S, <br />the fOllowing relationship results: <br /> <br />V 2 <br />u <br />HW 0 + -----.- <br />2g <br /> <br />V d2 <br />= TW +--.-- + HL <br />2g <br /> <br />(6) <br /> <br />HW 0 is the hcadwater dcpth above <br />the outlet in vert, ft (m) <br />V u is the approach velocity, ft/s <br />(m/s) <br />TW is thc tailwater dcpth above <br />thc outlet in vcrt, ft (m) <br />V d is thc downstream velocity, <br />[t/s (m/s) <br /> <br />4 <br /> <br />HL is the sum of all losses in- <br />cluding entrance (He)' friction <br />(HI)' exit (Ho) and other <br />losses, (HJ, (H), etc., <br />ft (m) <br /> <br />j <br />~ <br />~ <br />J <br /> <br />, <br />1 <br />< <br />" <br />. <br />~ <br />~ <br />~ <br />~ <br />~ <br />j <br />j <br /> <br />Note that the total available upstream <br />energy (HW) includes the depth of the <br />upstream water surface above the outlet <br />invert and the approach velocity head. <br />In most instances, the approach velocity <br />is low, and the approach velocity head is <br />neglected. However, it can be considered <br />to be a part of the available headwater <br />and used to convey the flow through the <br />cui vert. <br /> <br />. <br /> <br />Likewise, the velocity downstream of <br />the culvert (V d) is usually neglected. <br />When both approach and downstream veloci- <br />tics are neglected, equation (6) becomes: <br /> <br />~ <br />. <br />. <br /> <br />HW 0 = TW + HL <br /> <br />(7) <br /> <br />. <br />. <br />1 <br />. <br />. <br />. <br /> <br />In this case, HL is the difference in <br />elevation between the water surface eleva. <br />tion at the outlet (tail water elevation) <br />and the water surface elevation at the <br />inlet (headwater elevation). If it is <br />desired to include the approach and/or <br />downstream velocities, use cquation (4c) <br />for exit losses and equation (6) instead <br />of equation (7) to calculate the headwater. <br /> <br />36 <br />