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2016
DOI: 10.1061/(asce)ir.1943-4774.0000971
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Simple Relationships for the Optimal Design of Paired Drip Laterals on Uniform Slopes

Abstract: Microirrigation plants, if properly designed, allow water use efficiency to be optimized and quite high values of emission uniformity to be obtained in the field. It is known that disposing paired laterals, in which two distribution pipes extend in opposite directions from a common manifold, contribute to increasing water use efficiency. Recently, an analytical procedure has been proposed to optimally design paired drip laterals on uniform slopes under the assumption of neglect: (1) the variations of the emitt… Show more

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Cited by 21 publications
(44 citation statements)
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“…Relative errors, RE, calculated by assuming that the corresponding analytical values were true, resulted less than ±2%, demonstrating the applicability of the proposed procedure. Moreover Baiamonte () detected, for any slope of the lateral, the exact position of the manifold (BMP = 0.24), which is necessary to fix for an optimal design. The BMP was defined as the ratio between the number of emitters in the uphill lateral, n u , and the number of emitters in the uphill lateral and in the downhill lateral ( n opt = n u + n d ).…”
Section: Introductionmentioning
confidence: 90%
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“…Relative errors, RE, calculated by assuming that the corresponding analytical values were true, resulted less than ±2%, demonstrating the applicability of the proposed procedure. Moreover Baiamonte () detected, for any slope of the lateral, the exact position of the manifold (BMP = 0.24), which is necessary to fix for an optimal design. The BMP was defined as the ratio between the number of emitters in the uphill lateral, n u , and the number of emitters in the uphill lateral and in the downhill lateral ( n opt = n u + n d ).…”
Section: Introductionmentioning
confidence: 90%
“…These equations are rewritten here by introducing the minor losses terms, expressed according to the classic formula that considers a friction coefficient αmultiplied by a kinetic energy term (De Marchi, ; Jeppson, ; Juana et al, ; Yıldırım, , ), and by highlighting the scale role of the emitter spacing S , for the pressure head, already observed in Baiamonte (). Thus, in the following, the normalized pressure head with respect to the emitter spacing S [m] will be indicated with h * (dimensionless): h*inormalu=h*imaxnormaluK()HnnormalurHnuirαK*normalL()Hnnormalu2Hnui2+i0.5emS0 h*inormald=h*maxnormaluK()HnnormaldrHndirαK*normalL()Hnnormald2Hndi2i0.5emS0 in which r denotes the flow rate exponent of the flow resistance equation, Hnr is the generalized harmonic number of order − r , truncated at n corresponding to Hnr=…”
Section: Deriving Analytical Solution Accounting For Minor Lossesmentioning
confidence: 99%
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