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<br />SYNTHETIC HYETOGRAPH EQUATIONS <br /> <br />A synthetic hyetograph to be developed for <br />design of drainage facilities is not the one seen or <br />measured in an actual storm. It is rather a temporal <br />pattern with average variation of intensities within the <br />design burst and the most likely sequence of these <br />varying intensities. We all recognize that such a syn- <br />thetic hyetograph derived from the rainfall intensity- <br />duration-frequency data does not generally repre- <br />sent the rainfall in complete storms, but rather <br />represents intense bursts within storms. It is possible <br />that a number of bursts may come at any time within <br />the actual storms with much, or little, additional rain <br />falling in between the bursts. Therefore, without the <br />recorded intense bursts of a given duration, it is <br />unlikely that a hyetograph can be constructed which <br />represents the average rainfall in complete storms, <br /> <br />Since an elemental urban highway cross-section, <br />as described before, is a small watershed with drainage <br />area less than 0,1 square mile, it may be justified to <br />develop a synthetic hyetograph which represents an <br />intense burst rather than a complete stann of a long <br />duration which consists of a series of single intense <br />bursts. This in a sense is equivalent to assuming that a <br />synthetic hyetograph for urban highway watersheds is <br />a single-burst storm pattern having the duration of <br />ralnfall equal to the time of concentration for an <br />entire storm sewer system which drains storm water <br />collected at all dralnage inlets. The basic equations to <br />be used are the rainfall intensity-duration-frequency <br />relationships, Eq. 6 or 7, which can be formulated by <br />using rainfall data in Weather Bureau Technical Paper <br />No, 25 or 40. <br /> <br />Formulation of Hyetograph Equations <br /> <br />As mentioned in the previous section, the <br />rainfall intensity-duratlon.frequency relationship, Eq. <br />6 or 7, can be used to derive a synthetic hyetograph <br />equation which produces the same total amount (or <br />depth) of rainfall as described by the corresponding <br />intensity-duration-frequency curve up to any time, t, <br />for given frequency (or return period), F. <br />Mathematically it is expressed as <br /> <br />J t r dr = r t ....................... (8) <br />o av <br /> <br />in which r is the ralnfall intensity in inches per hour <br />at any time in the synthetic storm; r is the <br /> <br />integration variable for time; and fav is the average <br />rainfall intensity in inches per hour and is assumed to <br />be expressible in the form of Eq, 6 or 7, Because of <br />the reasons as stated previously, only Eq. 6 is used in <br />the present analysis. <br /> <br />The rainfall intensity-duration-frequency <br />formula, Eq. 6, has a parameter, b, the value of which <br />may be either positive or negative. In the case of a <br />negative b, Eq. 6 is not valid for td S Ibl. A <br />preliminary analysis of rainfall data obtained from <br />Weather Bureau Technical Paper Nos. 25 and 40 has <br />indicated that a positive b mainly applies to a large <br />section of the country-perhaps to the portion east of <br />the Rocky Mountains-while a negative b generally <br />applies to the west of the Rocky Mountains. <br />However. in some special meteorological areas such as <br />Hawaii (Weather Bureau Technical Paper No, 43, <br />1962; Cheng and UlU, 1973), the value of b was <br />found to be, or almost, zero. In light of the variety of <br />the b vaIue to be found in nature, it is suggested that <br />Eq. 6 be modified to include the cases of negatlve and <br />zero b. Therefore, Eq, 6 is expressed in the following <br />form in order that the b value is always kept positive, <br /> <br />a <br />r = . . . . . . . . . . . . . .. . . . . . . . . (9) <br />av (td z b)c <br /> <br />Substituting the expression of r av (from Eq. 9 after <br />changing its td to t) into Eq. 8 and then <br />differentiating the result with respect to t yields a set <br />of hyetograph equations for three types of storm <br />patterns, which are defined according to the skewness <br />of the pattern,"'1 , (l.e" the ratio of the time before <br />the peak to the total time duration). Because of the <br />nature of Eq. 9 which also breaks down for tdS bin <br />the case of -b, the hyetograph equations need to be <br />separately formulated for both cases of +b and -b. <br /> <br />Hyetograph equations for positive b <br /> <br />Three types of storm patterns are specified by <br />using the different values of "'1, A completely <br />advanced (initial burst) type storm pattern has "'1 = 0 <br />and a completely delayed (fmal burst) type storm <br />pattern, "'1 = 1. Both types which seldom occur in <br />nature may be regarded as extreme cases of the third <br />type, namely an intermediate type storm pattern, <br />which has 0 < "'1 < 1, Hyetograph equations for the <br />three types are derived and listed as follows: <br /> <br />7 <br />