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<br />where: <br /> <br />. <br /> <br />"Pl . projected area of the piers (or obstruction, if trash is in- <br />cluded) normal to the direction of flow corresponding to the <br />flow depth Yl at Section 1. <br />Ypl . vertical distance from water surface to centroid of Apl' <br />Koch and Carstanjen suggested that the dynamic force be reduced by one- <br /> <br />third for piers with semi-circular ends. In general terms the dynamic <br /> <br />force can be expressed as <br /> <br />Cn "Pl (i <br />2" V Al gAl <br /> <br />where Cn is a drag coefficient equal to 2 for square pier ends and 1.33 <br />for piers with semicircular ends. Substituting the above expressions <br />for static and dynamic forces in equation (2) and solving for the <br />2 <br />momentum flux (i.e., sum of ~ + Iii ) at Section A, <br /> <br />2 . 2 [ ] <br />MA = ~ + AAYA '" Ail - "Pipl + ~l Al - ~ Apl <br /> <br />(3) <br /> <br />In a similar fashion. momentum theory may be applied between Sections <br /> <br />B and 3, which are located immediately upstre8lll and downstre8lll from <br /> <br />the downstream end of the piers, respectively. In this case, the force <br /> <br />exerted by the piers is in the downstre8lll direction and has only a <br />static component, which is equal to V"P3YP3' where <br />Ap3 '" projected area of piers normal to the direction of .flow <br />corresponsing to the flow depth Y3 at Section 3. <br />YP3 = vertical distance from water surface to centroid of "P3' <br /> <br />5 <br />