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<br />r- <br /> <br />. <br /> <br />758 <br /> <br />HYDRAULIC ENGINEERING '94 <br /> <br />downstream at increased velocities (Clark et al. 1987). Upstream and downstream <br />of Petersburg, the 3050m (10000 ft) wide valley floor narrows dramatically and <br />the South Branch flows through constrictions approximately 152m (500 ft) wide <br />at Petersburg Gap downstream of the city and 114m (375 ft) wide near Marvin <br />Chapel upstream of the city, (Figure I) <br />Using the graphical pre- and post-processor FastT ABS, a finite element <br />mesh representing the flood plain and channel between Marvin Chapel ,and <br />Petersburg Gap was constructed using a combination of HEC-2 cross sectlon input <br />data previously used for the one-dimensional modeling of the area, topographic <br />infonnation from orthophoto maps, and field survey data. Aerial photos were used <br />to reconstruct conditions prior to the 1985 (-400 yr) flood and levee alignment <br />infonnation was digitized from design maps. <br />Modelinil Procedure <br />RMA2 is a numerical model which uses the finite element method to solve <br />the two-.dimensional. vertically averaged Navier-Stokes equations for free surface <br />flow (Thomas and McAnally 1985), The model can generate both steady state and <br />transient solutions which give water depth and velocity at eac;h node in the finite <br />element mesh used to represent the study area. For comparison with the HEC-2 <br />results, steady state solutions were modeled in this study. Meshes are constructed <br />by using combinations of quadrilateral and triangular elements of varying sizes. <br />This allows for more accurate representation of topography and pennits greater <br />mesh density in areas where more detailed information is desired. Manning's n <br />values are assigned for individual elements allowing spatial variation in roughness, <br />and for this study were based on field data collected for the U,S, Anny Corps' <br />flood protection study. Eddy viscosity can also be assigned for individual <br />elements. In order to achieve a solution with accurate representation of flow <br />separdtion. the eddy viscosity values were lowered as far a possible given the <br />constraint of obtaining a stable solution. Wetting and drying of meshes is allowed <br />via tWQ options. both of which were employed in this study. ]n one, when water <br />depth for a node drops below a user-specified level, the node goes dry and is <br />removed from the mesh, creating lateral movement in the mesh boundary. <br />Likewise. when water depth at a node exceeds a certain level. the node is re- <br />incorporated into the mesh, The other option ror wetting and drying is the "marsh <br />element" option. With this option, elements are not removed from the mesh. but <br />as the water surface drops. the area of the element available for flow decreases so <br />that dry elements are effectively removed from the mesh (King and Roig 1988), <br />RMA2 accepts inflows and water surface elevations as boundary <br />conditions, Data from a gage located near the upstream gap and high water marks <br />recorded at the downstream gap were used to formulate boundary conditions to <br />simulate the 1949 (-50 yr), 100 yr, and 1985 floods fnr meshes representing the <br />topography before and after the 1985 flood and with the proposed levees, <br /> <br />. <br /> <br />LEVEE DESIGN-2D MODEL <br /> <br />. <br />759 <br /> <br />I. <br /> <br />Enml Dischanre Hi~h Wat~r Mark <br />1949 Flood (-50yr) IJI2cms 281.5m <br />100 Yr Flood 2208 ems 281.6m <br />1985 Flood (-400 yr) " 3652 ems 281,8m <br />Table 1. Boundary ConWbons used in lhe simulation of the 50 yr tOO d 400 <br />, yr, an yr floods. <br /> <br />RmdIli <br />Several key observations emerge from the modeling efforts: <br />-In several a~e~s of the. mesh, the pattern of flow and the water surface elevation <br />contours exhibit two~dlmensional features that are important ~o d' F <br />' F' 2 resign. or <br />t,,;o~~anson. (g. ,shows .water surface elevations for the 100 yr flood under <br />cXlsllng topographic c~ndltions and the location of the original cross sections <br />used for HEC-2 modehng, <br />. The two-dimensional nature of flow, the effect nf changing topography and the <br />IOfluence of lbe upstream gap are illustrated in Fig, 3, The upstream gap direclS <br />h'gh veloclly flow across the flood plain, In the 1985 flood chann I 'dth' <br />I .. . e WI In <br />Il~t ,:"glon IOcreased by roughly 200%, As illustrated in the figure, an <br />lIlerease 10 channel Width (post-I 985 mesh) decreases the f1 I' <br />h flood I . ow ve oclty across <br />I c pam. <br />.The levees alter both the pattern and velocity of flow as well as th t <br />I I. . e wa er <br />~u.r ace e e~attons. Fig. 4 shows flow pattems and velocities for the 1985 flood <br />~ ~(~ ~nd Without levees in th~ area of the bridge over the South Branch in <br />I c~c~.s~u~g, In general, ~~re IS a decrease in velocity on the flood. plain and an <br />IIKrc. ase In channel velOCIties. The levees effectively fonn an add't' I <br />" h. . . Ilona <br />t.;OJlslncUon W Ich exhibits some of the ~ame features as the gaps. ]n a(krf <br />Ihe computed water surface elevations are different on the north and sout~ 1~~ <br />01 rhe channel. SI <br /> <br />M' As outlined in the above examples, the two-<iimensional modeling provides <br />.1. 1~I.onal mformati.on about ~he pattern of flow and the water surface eJevations <br />rh.lt I~ not captured m a one-dnnensional model, infonnation of use in both <br />~Jt~~lIn.g and evaluati.n~ ~~od pm~tion pl~ns. Additional analyses in preparation <br />. lI~h ,I.oll~~ from thiS 1~ltlal study mclude Investigation of the effect of flood Jain <br />1.:. 'ral.l~I()OS and contractions. evaluation of model sensitivity to boundary P <br />l(J~I.~/I(llo.ns and hydraulic parameters, and the incorporation of digital elevation <br />llltlUC S Into mesh construction. <br />References Cited <br /> <br />1'1 Kd 'T' n~d" I,.P. and Roig, L.e. (1988) ~Two-Dimensional Finile Elemenl Models for Flood <br />.lIn, an I a Wetlands" P d' I ' <br />. f/ A I . ,rocee m8s nternalwnal Conference on Computational Methods <br />,II ''',",' 11(1 ysu, Okflyama. Japan. <br />("mfl'dl"~)mas, W.A. and McAnally, W.H. (1985) Users Manual/or/he Generalized <br />.\, W. .mgram Syst~m, Open Channel Flow and Sedimentation. TABS.2. Deparunenl of the <br />TIly, illcrways Expenmenl Station, Corps of Engineers. <br />1', ltullWt. ~.l~~ A;;~ C(~~Of Engineers, Ballimore Districl and Inlerstate COmmission on the <br />, ('mlll,lity Rt!~ :slRd E ~ Local Flood Protection Petersburg, West Virgini4: Integrated <br />r"T an nVlronmentallmpact Statement. <br /> <br />- <br />