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<br />Expansion in al storm sewer conduit will rl!suI1: in a shearing <br />action between tile incoming high velocity jet and the <br />surrounding sewer boundary. As a result.. much of the kinetic <br />energy is dissipa1::ed by eddy currents and turbulence. The <br />loss of head c:an be expressed as: <br /> <br />HL= Ke (V//2g) [ 1 - AdA, ], <br /> <br />(Equation 6.2) <br /> <br />in which A is the cross section area, V i.s the average flow <br />velocity, and Ke is the loss coefficient. Subscripts 1 and 2 <br />denote the upstream and downstream sections, respecti vely. <br />The value of K" is l:lbout 1.0 for a sudden expansion, and about <br />0.2 for a well d.,~signed expansion trclne:iticm. Table 6-2 <br />presents the expansion loss coefficients for various flow <br />conditions. <br /> <br />2 . <br /> <br />Contraction Losses <br /> <br />The form loss due to contraction is: <br /> <br />HL=Kc (V//2g) [1- (A,)2/A:]' <br /> <br />(Equation 6.3) <br /> <br />where Kc is the contraction coeff icient, ~ is equal to 0.5 <br />for a sudden contraction and about 0.1 for Cl well designed <br />transition. Subscripts 1 and 2 denote thl~ upstream and <br />downstream sections, respectively. Table 6-2 presents the <br />contraction loss coefficients for various flo'... conditions. <br /> <br />3. <br /> <br />Bend Losses <br /> <br />The head losses flJr bends, in excess of that caused by an <br />equivalent length of straight pipe, may be expressed by the <br />relation: <br /> <br />HL = Kb (V'/2g) <br /> <br />(Equation 6.4) <br /> <br />in which K" is the bend coefficient. The bend I::oefficient has <br />been found to be a function of: (a) th,~ rati,) of the radius <br />of curvature of tile bend to the width of the conduit, (b) <br />deflection angle .of the conduit, ~ gE!Ometry of the cross <br />section of flow, and (d) the Reynolds Number and relative <br />roughness. A tabulation of the recommended bend loss <br />coefficients for st:andard bends, radius pipe, a.nd bend through <br />manholes is presented in Tables 6-3 and 6.-4. <br /> <br />4. <br /> <br />Junction and Manhole Losses <br /> <br />more branc:h sewe,rs enter a main <br />The hydrllulic design of a <br />of two o:r more transitions, <br /> <br />A junction occurs \/here one or <br />sewer, usually at. manholes. <br />junction is in effect the design <br /> <br />6-4 <br /> <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />II <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />