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<br />Ihrough a channel of lenglh, L. In order to simplify <br />the analysis, a rectangular channel cross-section was <br />assumed. Appropriate pararnelers of width and depth <br />of flow can be substiluted to represenl a particular <br />storm drainage system. If b is assumed to represent <br />channel width and y the deplh of flow, Ihe cross..ec- <br />tional area of flow, A, is given by: <br /> <br />A=by . . <br /> <br />. (3.15) <br /> <br />and the wetted perimeter, p, is <br /> <br />p=b+2y=b. . . . . (3.16) <br /> <br />Manning's open channel flow equation is <br /> <br />Q=VA=1.49 AR2/3 SI/2 . (3.17) <br />n <br /> <br />in which <br />Q <br />S <br />n <br />R <br />R2/3 <br /> <br />= discharge in cfs <br />= channel slope in ftlft <br />= Manning's rouglmess coefficienl. <br />= hydraulic radius = AlP <br />= (A2/3)1(J>2/3) = y2/3 <br /> <br />Therefore, <br /> <br />Q= 1.49 (by)y2/3 Sl/2 -1.49 bSl/2 (y5/3) <br />n n <br /> <br />. . (3.18) <br /> <br />Solving for y as function of Q, <br /> <br />3/5 <br />Y = f(Q) = ( n ) Q3/5.. (3.19) <br />1.49 bSl/2 <br /> <br />= KQ3/5 <br /> <br />in which <br /> <br />K=( n )315 <br />1.49 bSI/2 <br /> <br />. (3.20) , <br /> <br />T L can Ihen be estimated as a function of instanane. <br />ous discharge by Ihe computer program as: <br /> <br />dislance ~ ~ <br />TL = velocity = LQ Q . (3.21) <br /> <br />Substituting Equation 3.19 into Equation 3.21 yields <br /> <br />T L = L bKQo.6 - L bKQ .0.4 <br />Q <br /> <br />. (3.22) <br /> <br />T L is Ihus given in lerms of readily oblained channel <br />or storm drain design dimensions. Dividing Equation <br />3.22 by 60 gives T L in minules. <br /> <br />By assuming a linear distribution of inflow into <br />the channel or the storm drain syslem along its length, <br />the added Q wi thin a subzone is <br /> <br />Q(+Qo <br />Q 2 <br /> <br />. (3.23) <br /> <br />Narayana et a!. (1969) did not use a lag time <br />concept in Iheir study because a single watershed area <br />was assumed and routing was not required. The Eve- <br />lyn el aI. (1970) study utilized a subzone approach <br />and a lag time parameter which was reduced 10 a con- <br />stant based on subzone characteristics and peak dis- <br />charge rales from individual storm even Is. The dis- <br />charge for each subzone was assumed proportional to <br />the area drained. The lag time parameter for each <br />sub watershed therefore was expressed in lerms of the <br />peak discharge at the outflow point of the most down- <br />slream subzone. The melhod (Evelyn el aI., 1970) <br />gave satisfactory results. This lag lime parameter, in <br />essence, had an attenuation effect on the outflow <br />hydrographs and increased the recession time. The <br />time of the peak discharge was not shifled, however. <br /> <br />In this study, discharge rates are determined <br />for each subzone and used to calculate Ihe lag time <br />parameter. The lag time parameter is applied to cal- <br />culate the time shift due to channel routing effects <br />by dividing the lag time parameter into the time scale <br />and then rounding to the nearest integer. In routing <br />Ihe upstream hydrograph is delayed by the calculated <br />number of lime units. This process is continued for <br />each subzone until the outflow hydrograph is com. <br />puted for Ihe enlire watershed area. <br /> <br />Model Verification <br /> <br />Compuler Synlhesis <br /> <br />The computer model was produced by program- <br />ming the mathematical relationships and logic func- <br />tions described above. The model is analogous to the <br />prolotype to the degree that the mathematical rela- <br />tionships represent real world conditions. A mathe- <br />matical function which describes a basic process, <br />such as evapolranspiration, is applicable to many diff- <br />erent hydrologic models. A simulation modei incor- <br />porates general equations of the various basic processes <br />which occur within the system. The result, therefore, <br />is free of the geometric restrictions characteristic of <br />network analyzers and physical models. The model is <br />applied 10 a parlicular prololype system by estab. <br />lishing, through a calibration procedure appropriate <br />values for the "constants" of the equations used. <br /> <br />Model Verificalion <br /> <br />Hydrologic models require verificalion. Verifi- <br />cation is performed in two steps, namely calibration, <br />or system identification, and testing (described in a <br /> <br />29 <br />