Flood Routing Introduction ◼ ◼ Flood routing is an analytical technique of determining the flood hydrograph at a particular location in a channel or a reservoir resulting from a known flood at some other location upstream. Routing techniques may be classified in two major categories ❑ ❑ Hydrologic routing (based on the equation of continuity and empirical equation. This involves the balancing of inflow, outflow and volume of storage through use of continuity) Hydraulic routing (based on equations of continuity and momentum) Continued….. Reservoir Routing ◼ ◼ ◼ ◼ The main components of Dam are inflow channel, storage reservoir and outflow structures like spillways, tunnels etc. Once a flood enters a reservoir, part of it may be stored in the reservoir and balance safely passes through or over outflow structures. The main function of a reservoir is to store water from which releases are made according to water demands on downstream of reservoir. A multipurpose hydroelectric project has storage of water as well as generation of electricity. Continued….. Reservoir Routing ◼ ◼ The reservoirs may be small or large. An example of small reservoir is pond of a barrage. A small reservoir has small capacity and hence water levels in barrage pond are sensitive. The outflow from a small reservoir is solely a function of pond elevation if the outflow is not controlled. In case of large reservoirs the moderate inflow may not have large impact on reservoir elevation however large floods need to be negotiated keeping in view the operational rules. Continued….. Reservoir Routing ◼ ◼ ◼ ◼ ◼ The reservoir routing may be classified according to outflow control at a particular reservoir e.g. Flood routing in reservoirs with uncontrolled outflow Flood routing in reservoirs with controlled outflow The basic equation applied is storage equation given as Inflow-Outflow = Rate of Change of Storage I - O = ds / dt - - - - - - - - - - - - (1) Equation (1) shows that if inflow is assumed constant the reservoir storage is a simple function of outflow. Continued….. Reservoir Routing ◼ ◼ ◼ ◼ If average values of inflow and outflow are considered for opted time interval ∆t then equation (1) can be written as [(I1+I2)/2]-[(O1+O2)/2]=[(S2-S1)/∆t] - - - - - - - - (2) Where 1 to 2 are the time step values of I, O and S Equation (2) can be rearranged as (I1+I2)+[(2S1/∆t)-O1]=[(2S2/∆t)+O2] - - - - - -(3) As mentioned above the subscripts 1 and 2 denote values of Inflow, Outflow and Storage at beginning and end of ∆t say from 1 to 2. The time ∆t is known as routing period. This period should not be so large that peak of inflow hydrograph is not intercepted. Flood routing in reservoirs with uncontrolled outflow ◼ ◼ ◼ The following steps explain procedure of reservoir routing 1. The Elevation vs Storage of reservoir information should be known. Here storage means volume of water that a reservoir can accommodate at certain elevation. This elevation vs storage information may either be in the form of table or graph. A typical elevation vs storage graph is shown in Figure 1. Continued….. Flood routing in reservoirs with uncontrolled outflow Elevation vs Surface Area Realationship 124 122 120 Elevation (m) 118 116 114 112 110 108 106 104 102 40000 42000 44000 46000 48000 50000 52000 54000 Surface Area (m²) Fig. 1. Variation of Surface Area of a Reservoir with Elevation Flood routing in reservoirs with uncontrolled outflow Flood routing in reservoirs with uncontrolled outflow Flood routing in reservoirs with uncontrolled outflow 2. The discharge capacity of overflow structure with change in water level should be calculated. For this purpose the applicable discharge formula need to be applied. The well known weir equation is: Q = Cd BH3/2 - - - - - - - - - -(3A) Where, Q = Total Discharge Cd = Coefficient of Discharge B = Width of Weir H = Differential head over the crest of the weir neglecting velocity of approach ◼ Continued….. Flood routing in reservoirs with uncontrolled outflow ◼ ◼ The coefficient of discharge depends on degree of submergence of the weir. Its value is determined experimentally e.g. by model tests. The value can also be determined from Gibson’s curve. Its value generally ranges from 1.6 to 2.2. A mean value of 1.70 is often used in SI units. Continued….. Flood routing in reservoirs with uncontrolled outflow ◼ ◼ ◼ For other types of outflow structures like Sluice Gates, Pipes etc. different equations are used for calculations of discharge and can be found in books of hydraulics. Once the outflow is determined for different reservoir elevations, a graph is plotted between storage and outflow. A typical such graph is shown in figure (2). Please note that outflow is taken along y-axis and [(2S/∆t)+O] is taken along x-axis. The quantity [(2S/∆t)+O] is called ‘Storage Indication’. Continued….. Flood routing in reservoirs with uncontrolled outflow 300 Outflow (m³/s) 250 200 150 100 50 - 500 1,000 1,500 Storage Indication 2,000 2,500 [(2S/∆t)+O] 3,000 3,500 4,000 (m³/s) Figure 2 Outflow and Storage Indication Relationship for certain reservoir Continued….. Flood routing in reservoirs with uncontrolled outflow ◼ ◼ ◼ 3. The inflow hydrograph should be known. It may be actual or forecasted flood. The inflow is added for successive values to get I1+I2. Corresponding to the initial outflow value storage indication [(2S/∆t)+O] is found from storage indication curve. To this value double of outflow is subtracted to get [(2S/∆t)-O]. To this value of [(2S/∆t)-O], I1+I2 is added to get next value of [(2S/∆t)+O]. Read out next outflow from storage indication curve and repeat the procedure till whole of inflow hydrograph is used to get outflow values. Continued….. Flood routing in reservoirs with uncontrolled outflow ◼ Now the inflow and outflow hydrographs are plotted. The difference in peak of inflow and outflow hydrograph is known as attenuation and time between two peaks is known as reservoir lag. Stream Channel Routing or River Routing ◼ ◼ ◼ ◼ ◼ The routing in channels involves solution of storage equation as was done in case of reservoir routing. The storage is function of both inflow and outflow. The method of channel routing is known as Muskingum Method. Consider a channel reach having prismatic cross section as shown in Figure 5. Let, S = Storage I = Inflow O = Outflow The storage in the channel reach consists of two parts: ❑ Prism storage equal to KO. ❑ Wedge storage equal to K (I-O). Stream Channel Routing or River Routing Wedge Storage =K(I-O) I O Prism Storage =KO Figure 5. Prism and Wedge Storage in Channel Stream Channel Routing or River Routing ◼ ◼ ◼ Then total storage ‘S’ is therefore sum of prism and wedge storage. That is: S = K [XI + (1-X)O] - - - - - - (6) Where ‘X’ is a dimensionless constant for certain reach or segment of channel. ‘K’ is storage constant having dimensions of time. Both X and K are determined from inflow and outflow hydrographs for reach under consideration. Stream Channel Routing or River Routing ◼ These constants vary from reach to reach and are determined as follows. ❑ ❑ ❑ ❑ ❑ ❑ The inflow and outflow hydrographs are known for the reach. Find values of (I-O) for each time interval. Find the mean and cumulative mean values of (I-O) which is storage. Assume value of ‘X’ and find the term [XI + (1-X) O] for each time interval. The storage value is already calculated against time as explained. Plot [xI + (1-x)O] values against storage. Inspect if data plotted nearly fits a straight line. If not assume new value of x and repeat steps 1-4. The best-fit straight line corresponds to required value of ‘x’. The slope of this straight line is our required value of ‘K’. Stream Channel Routing or River Routing ◼ ◼ Now we proceed for channel flow routing once values of ‘x’ and ‘K’ are known. Routing means finding outflow hydrograph for given inflow hydrograph. The linear relationship is expressed as for Muskingum Method ◼ S = K [(xI) + (1-x) O] Since rate of change of storage in a particular channel reach is given as [I2+I1/2]Δt – [O1+O2/2] Δt = S2–S1 -----------(1) Stream Channel Routing or River Routing ◼ ◼ For if Muskingum Theorem is applied to that change; the equation can be written as in terms of storage ◼ S2–S1 = K [ x (I2+I1) + (1-x)(O1+O2)]---------(2) Now equating equations 1 and 2 we get ◼ (I1/2)Δt+(I2/2)Δt–(O1/2)Δt-(O2/2)Δt = K{(xI2-xI1)+(1-x)(O2–O1)} rearranging the terms we get (I1/2)Δt+KI1x+(I2/2)Δt-KI2x-(O1/2)Δt+O1K-xKO1 = (O2/2)Δt+O2K-xKO2 (0.5Δt+Kx)I1=(0.5Δt-Kx)I2+(K-Kx-0.5Δt)O1 = (0.5Δt+K-Kx)O2 ---------(3) Stream Channel Routing or River Routing ◼ O2= [(0.5Δt+Kx)/(0.5Δt+K-xK)]I1+ [(0.5Δt-Kx)/(0.5Δt+K-xK)]I2+ [(K-Kx-0.5Δt/0.5Δt+K-Kx)]O1 ◼ OR O2 = C0I2+C1I1+C2O1 Where Co = [(0.5Δt-Kx)/(0.5Δt+K-xK)] C1 = [(0.5Δt+Kx)/(0.5Δt+K-xK)] C2 = [(K-Kx-0.5Δt/0.5Δt+K-Kx)] It may be noted that sum of weighing coefficients Co + C 1 + C2 = 1 Knowing values of ‘x’ and ‘K’ these coefficients are determined simply by substitution of values in equations ◼ ◼ ◼ ◼ ◼ ◼ ◼