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<br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br /> <br />"s <br /> <br />~ <br /> <br />1.182 <br />n <br />s <br /> <br />(1 <br /> <br />>'z <br /> <br />(10) <br /> <br />:r: <br />...J f- <br />=> <br />(!) <br />0 <br />0 <br />I?; - ;: <br />I~~ ~ <br />...J(/) ~ <br /><( <br />:r:1II <br />rs~ ~ <br />O~ <br />(f) J.. <br /> J <br /> / <br /> II: <br /> <( J J <br /> LU <br /> >- <br /> g I/~ ! <br /> ~ ~ <br /> \ ~ <br /> '" ~ <br /> <br />o <br />o <br />r<l <br /> <br />in the case of overland flow or from the Manning formula <br /> Q 1.182 ( rz )2/3 4/3 1/2 (9) <br /> ~ A S <br /> ns 1 + Vl":""z2 s <br />as <br /> <br />o <br />lD <br />(\j <br /> <br />o <br /><0 <br />(\j <br /> <br />o <br />v <br />(\j <br /> <br />+ v 1+z2 <br /> <br />Y/3 <br /> <br />1/2 <br />Ss <br /> <br />o <br />(\j <br />(\j <br /> <br />ms <br /> <br />~ <br /> <br />4/3 <br /> <br />( 11) <br /> <br />o <br />o <br />(\j <br /> <br />in the case of flow in a triangular channel. <br /> <br />o <br />lD <br /> <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />-I <br />I <br /> <br />"The model solves the kinematic wave equations by numerical techniques. <br />The details of these techniques have carefully been developed over a <br />period of many years to the point where reliable procedures have been <br />programmed to automatically assure the most economical solution of these <br />equations. These numerical procedures discretize time in steps of t. t <br />and distance in steps of t. x. <br /> <br />o <br /><O~ <br />.S; <br />E <br />Oc <br />~.:.::. <br /> <br />"Over anyone time, i and f are assumed to remain constant. Variables <br />i and f also are assumed to remain constant over x. Variations with <br />x of f can be represented in stepwise changes by a cascade of overland <br />flow segments. Along any stream segment, the variable q changes con- <br />tinuously with time but is assumed constant over the length of the stream <br />segment. II <br /> <br />LU <br />O::!: <br />(\J- <br />-f- <br /> <br />o <br />o <br /> <br />o <br />lD <br /> <br />RUNOFF VOLUMES <br /> <br />In addition to the peak rates of flow presented in Section II I, storm <br />runoff volumes were determined at each design point for each frequency. <br />This was done for both present conditions and future development, and <br />these were found to agree within 5 percent. For this reason, only the <br />runoff volumes for future development are presented below in Table HA-3. <br />Volumes shown are cumulative values at the lower end of each subbasin. <br /> <br />@ <br /> <br />o <br />v <br /> <br />o <br />(\j <br /> <br />TABLE HA-3 <br /> <br />RUNOFF VOLUMES <br /> <br />FUTURE OEVELOPMENT <br />(A II va lues in ac re- fee t) <br /> <br />~u!:!.oif_V~I~m!:io~ ~a~i!?u~ ~r!:q~e!:!.c-'--e~ <br /> <br />o <br />o <br />'D <br /> <br />o <br />o <br />.,. <br /> <br />o <br />o <br />~ <br /> <br />o <br />o <br />(\j <br /> <br />o <br />o <br /> <br />o <br />o <br />o <br /> <br />o <br />~ <br /> <br />o <br />o <br />lD <br /> <br />o <br />o <br />I"- <br /> <br />o <br />o <br /><0 <br /> <br />o 0 <br />o 0 <br />10 v <br />ft. per se c ) <br /> <br />o <br />o <br />"" <br /> <br />o <br />o <br />(\J <br /> <br />o <br />o <br /> <br />o <br />o <br /> <br />DISCHARGE <br /> <br />{in cu <br /> <br />Subbasin <br /> <br />1 <br />2 <br />3 <br />4 <br />5 <br /> <br />5-year 10-year 50-year 100-year <br />10 18 23 26 <br />30 55 70 78 <br />41 74 95 105 <br />51 92 118 131 <br />63 114 147 163 <br /> <br />FIGURE HA-I <br />WRIGHT- MCLAUGHLIN ENGINEERS <br />2420 ALCOTT ST. OENVER.COUC.B02~ <br />