Bathymetry, Flow Field and Wave Field Measurement in Upper Yahara River, Madison, WI Flow Field The flow field can be discussed as follows: Bathymetry Mapping Modeling Surface Water Modeling System (SMS) is a software to create one-, two, and three-dimensional hydrodynamic modeling. We used this software to plot the bathymetry in our study site. The software can make bathymetry grid in rectangular/Square grids and triangular grids. Triangular grid system was used to plot the bathymetry to ensure better and more accurate coverage of the area. Detailed literature on the working of the software is available on line (http://www.emsi.com/SMS/sms_8_1_new_features.html) but the general procedure for making the grid is as follows: · · Input in the form of x,y,z coordinates of points required to be mapped. · selection of system of interpolation between points to make a grid. · Applying mesh quality checks to ensure max value of interior angles, maximum allowable vertical slope between the elements etc. · Plotting the contours and visual inspection of the bathymetry grid to find out some undesired nodes and then correcting them before taking the output to be run in the FVCOM. The mesh/bathymetry map generated for our study site was as shown below( the vertical scale has been exaggerated 20 times for better assimilation) Bathymetry Mapping Use of SMS 8.1 (Figure 2 , Bathymetry Mapping ) Surface water modeling software 8.1 (SMS 8.1) was used to plot the bathymetry. The software can make bathymetry grid in rectangular/Square grids and triangular grids. Triangular grid system was used to plot the bathymetry to ensure better and more accurate coverage of the area. Detailed literature on the working of the software is available on line (http://www.emsi.com/SMS/sms_8_1_new_features.html) but the general procedure for making the grid is as follows: Input in the form of x,y,z coordinates of points required to be mapped. selection of system of interpolation between points to make a grid. Applying mesh quality checks to ensure max value of interior angles, maximum allowable vertical slope between the elements etc. Plotting the contours and visual inspection of the bathymetry grid to find out some undesired nodes and then correcting them before taking the output to be run in the FVCOM. The mesh/bathymetry map generated for our study site was as shown below( the vertical scale has been exaggerated 20 times for better assimilation): The area of our major focus was north of bridge at HW 113, which has the following bathymetry shape: Modeling Finite Volume Coastal Ocean Model (FVCOM) has been used to simulate flow in the river for 3 days and the wave characteristics have been calculated at following seleted node which represent particular conditions in a specific reach of the river: FVCOM was originally developed for the estuarine flooding/drying process in estuaries and the tidal-, buoyancy- and wind-driven circulation in the coastal region featured with complex irregular geometry and steep bottom topography. Node 639, 510: Entrance to the lake Mendota. Node 509: Inside the jetty areas. Node 516: Near the Bridges. Node 843, 921, 875: Areas in the north of HW 113. The results for wave characteristics will be discussed the wave field. However, to ascertain the impact of different Fetch lengths on the resultant wave height (H)and Wave Time period (T) a point up in the north near the start of River was selected where already some wetland restoration plantation has been done. The fetch length was considered in five different directions as indicated in the figure below: JONSWAP method was used to calculate wave height and wave time period. Main steps involved use of this method are Step (1) Given F, U10, td Step (2) Compute F* = g F/U102 t* = gtd/ U10 F* eff = {t*/68.6}1.5 Step (3) if F* < F* eff ~ Fetch Limited H*s =gHs/ U102 =0.0016(F* eff)0.5 Tp* = gTp/ U10 = 0.286 (F*)0.333 if F* > F* eff ~ Duration Limited Step (4) Fully developed H*s =gHs/ U102=0.243 Tp* = gTp/ U10 = 8.13 Inputs Ua = 5 ,10 ,15 m/sec (assumed) Duration 1 hour, ( assumed) Fetch o North : 368 m o South : 720 m t* = gtd/ U10 = 71500 o o o East : 192 m West : 176 m South West : 2656 m Out puts Ua (m/sec) 5 10 15 20 Fetch length direction (m) N 368 S 720 E 192 W 176 Limit Wave Height Hs (m) Wave Time Pd (sec) Fetch Fetch Fetch Fetch 0.04 0.04 0.04 0.04 0.67 0.67 0.67 0.67 SW N S E W 2656 368 720 192 176 Fetch Fetch Fetch Fetch Fetch 0.04 0.23 0.23 0.23 0.23 0.67 1.58 1.58 1.58 1.58 SW N S E W 2656 368 720 192 176 Fetch Fetch Fetch Fetch Fetch 0.23 0.61 0.61 0.61 0.61 1.58 2.60 2.60 1.58 2.60 SW N S E W 2656 368 720 192 176 Fetch Fetch Fetch Fetch Fetch 0.61 1.24 1.24 1.24 1.24 2.60 3.71 3.71 3.71 3.71 SW 2656 Fetch 1.24 3.71 Producer scheme Wind can strongly affect the behavior of water waves (Especially, the wave period (Ts) and wave height (Hs). In order to account wind into our calculation, we downloaded the wind information (for Madison area) of October from NOVVA. The average daily wind speed (‘Ua’) and the wind direction (‘dir’) are listed in table 1. The average daily wind speed is also listed in table. The average wind speed for October , 2008 is 5.54 mph (2.47 m/s) Linear and progressive waves are assumed for our calculation. The water depth (d) and surface velocity (v) are obtained from FVCOM. Wave length (L), relative depth (d/L), wave height (H) due to the water depth (H mean) and the maxim wave height (Hmax) are calculated as general prosperities. Group velocity (Cg) is calculated as to determinate how the wave energy propagated. We also calculated the wave energy density (Ebar) and wave power (p), because we like to see if wave can be use as an energy source at this region. The average value for three days is listed in table 4.