韓延成,初萍萍,梁夢媛,唐 偉,高學(xué)平
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冰蓋下梯形及拋物線形輸水明渠正常水深顯式迭代算法
韓延成1,初萍萍1,梁夢媛1,唐 偉1,高學(xué)平2
(1. 濟(jì)南大學(xué)資源與環(huán)境學(xué)院,濟(jì)南 250022;2. 天津大學(xué)水利工程仿真與安全國家重點(diǎn)實(shí)驗室,天津 300072)
隨著冬季用水量的增加,越來越多的輸水工程在冬季冰蓋下輸水,冰蓋下輸水已經(jīng)成為一種常態(tài)化輸水方式,但目前對明渠正常水深的顯式計算方法的研究主要針對不結(jié)冰渠道的,缺少對冰蓋下輸水時正常水深的顯式計算方面的研究。該文推導(dǎo)了梯形斷面冰蓋下輸水時正常水深和流量關(guān)系,提出了正常水深的簡易顯式迭代算法,并經(jīng)過證明,此迭代算法是收斂的。用同樣的方法,推導(dǎo)了拋物線形斷面冰蓋下輸水時正常水深和流量關(guān)系,提出了計算正常水深的簡易顯式迭代算法。算例表明,該文提出的冰蓋下梯形斷面和拋物線形斷面的顯式迭代算法具有形式簡單、計算量小、精度高,收斂性好的特點(diǎn),一般需要3~5次迭代就可使誤差小于0.01 m,當(dāng)增大迭代次數(shù)時,誤差進(jìn)一步減小。研究為冰蓋下輸水渠道正常水深計算提供了便捷的計算方法,對冰期輸水渠道的設(shè)計及運(yùn)行管理具有理論和實(shí)踐意義。
渠道;水力學(xué); 設(shè)計; 明渠; 冰蓋下輸水;正常水深;顯式迭代算法
中國北方受蒙古高壓寒冷氣流的控制,冬季寒冷,北方10月以后大部分地區(qū)氣溫都會降到0℃以下,水體表面會發(fā)生結(jié)冰現(xiàn)象。隨著冬季反季節(jié)農(nóng)業(yè)種植規(guī)模的擴(kuò)大以及城市的發(fā)展,冬季需水量大幅增加。越來越多的工程采用常年輸水或冬季輸水。例如引黃濟(jì)青工程為冬季輸水渠道,輸水期為10月至翌年3月。南水北調(diào)東線山東段輸水期為10月至翌年5月。另外南水北調(diào)中線、引灤入津、引黃濟(jì)津、萬家寨引黃調(diào)水、新疆烏什水水庫引水工程等在結(jié)冰后也采用冰蓋下輸水的模式。除此之外,東北、西北、華北等地許多引水發(fā)電工程也采用冰蓋下輸水。冬季冰蓋下輸水已經(jīng)成為一種重要的渠道輸水方式[1-2]。
正常水深的計算是渠道水力學(xué)計算的重要內(nèi)容之一,在渠道設(shè)計、運(yùn)行管理、輸水調(diào)度過程中大量使用[3]。但是正常水深與流量之間為復(fù)雜的非線性函數(shù)關(guān)系,不能直接求解,不方便工程應(yīng)用[4-6]。學(xué)者們對正常水深的顯式求解方法進(jìn)行了大量的研究,趙延風(fēng)等[4,7]提出了梯形斷面的迭代算法,Bijankhan等[8]給出了蛋形斷面正常水深的迭代算法,Liu等[9]研究了馬蹄形斷面的正常水深的迭代算法,Li等[10]提出了拋物線形斷面正常水深的迭代算法。張新燕等[11]研究了拋物線形斷面的正常水深計算公式,張寬地等[12]研究了圓形隧洞正常水深的牛頓迭代算法,張新燕等[13-14]采用SAS軟件研究了U形渠道和圓形隧洞無壓流正常水深直接求解公式,武周虎[15]提出了蛋形斷面明渠正常水深的簡化算法。
這些顯式或直接計算方法,極大地方便了渠道設(shè)計者和運(yùn)行管理者。但是已有的正常水深計算方法和公式是針對不結(jié)冰渠道的,對冰期輸水渠道,冰蓋的形成導(dǎo)致過流能力下降[16],其正常水深計算需要考慮冰蓋阻力的影響;因此那些不結(jié)冰條件下正常水深的顯式計算公式是不適應(yīng)的。目前還缺少對冰蓋下輸水時正常水深的顯式計算方法研究,對冰蓋下輸水渠道的運(yùn)行和管理帶來了不便,研究冰蓋下正常水深的計算對冰期輸水渠道設(shè)計、運(yùn)行具有重要意義。本文以梯形斷面、拋物線形斷面為研究對象,推導(dǎo)冰蓋下輸水時正常水深和流量之間的關(guān)系,提出梯形斷面、拋物線形斷面正常水深的簡易顯式迭代算法,對方便冰期輸水渠道在運(yùn)行、設(shè)計中正常水深的計算具有現(xiàn)實(shí)意義。
由于冰蓋密度較水小,且柔性較大,冰蓋一般浮在水面。冰蓋下均勻流一般用曼寧公式表示為[17]
將式(2)代入式(1)得到冰蓋下輸水正常水深計算公式為
注:為水深,m;為底寬,m;為邊坡系數(shù);下同。
Note:is water depth, m;is bottom width, m;is side slope; Same as below.
圖1 冰蓋下梯形渠道斷面示意圖
Fig.1 Schematic of cross section of trapezoid channel under ice cover
由式(9)可以看出,冰蓋下輸水糙率不是常數(shù)[2],其與水深有關(guān)。將式(4)、(8)、(9)代入式(1),得到冰蓋下均勻流輸水流量的計算公式為
因此迭代公式可表示為
編制數(shù)值求解程序,采用埃特金迭代法或擬牛頓法[23],求解式(10),得到正常水深h=3.745 138 7 m。將其作為理論參考值。
為了檢驗迭代公式的收斂性,采用不同初值0=0.01、0.1、1.0、2.0、5.294 2、10、100 m(其中,=5.294 2 m為根據(jù)水力最優(yōu)斷面得到的正常水深),代入式(13)迭代得到結(jié)果如表1所示??梢钥闯?,本迭代公式具有很好的收斂性,一般需要3~5次就可使誤差小于0.01 m。取水力最優(yōu)斷面為初值時,只需要3次可使誤差小于0.01 m。除了上述初值,也用其他初值經(jīng)過檢驗,不論初值多少,公式均具有良好的收斂效果。當(dāng)增大迭代次數(shù)時,不論初值為多少,均能收斂于理論值。
表1 梯形斷面不同初值時正常水深的迭代結(jié)果
注:0為初始值,h為第次迭代結(jié)果,h理論參考值。下同。
Note:0is the initial value;his the value of thethiteration for normal depth,his the theoretical value of normal depth. Same as below.
學(xué)者們普遍認(rèn)為拋物線形斷面(見圖2)具有拐點(diǎn)少、應(yīng)力集中點(diǎn)少、裂縫少、滲漏小,另外具有穩(wěn)定性好、過流能力大,水力學(xué)特性優(yōu)良的特點(diǎn)[24-27]。巴基斯坦的High Level渠,西班牙Genil-Cabra渠等采用了拋物線形斷面[28]。
拋物線形斷面形狀可表示為[17,29-31]
注:為水面寬度;為水深,m。
Note:is width of water surface, m;is water depth, m.
圖2 冰蓋下拋物線形渠道斷面特性
Fig.2 Cross section characteristics of parabolic channel under ice cover
濕周包括渠床濕周和冰蓋造成的濕周,分別表示為
將式(22)代入式(2),可以得到綜合糙率為
將式(21)~式(23)代入曼寧公式(1),簡化后得到流量和水深的關(guān)系式為
根據(jù)式(25),構(gòu)造的迭代公式為
為了減小迭代次數(shù),初值可取非冰蓋下拋物線形最優(yōu)斷面得到的水深[26-27]
用同樣的方法,可以證明式(26)是收斂的,在此不在贅述。
編制數(shù)值求解程序,采用埃特金迭代法或擬牛頓 法[23],均可得到正常水深h=3.846 841 14 m。將其作為理論參考值。
根據(jù)水力最優(yōu)斷面公式(27),得到水力最優(yōu)斷面條件下0=3.040 4 m。取不同初值(0=0.01、0.1、1.0、5.0、10.0、100、3.040 4 m),根據(jù)迭代公式(26)得到結(jié)果如表2所示。
可以看出,本迭代公式具有很快的收斂速度,一般需要3~5次就可使誤差小于0.01 m。取最優(yōu)斷面為初值時,只需要3次可使誤差小于0.01 m。當(dāng)增大迭代次數(shù)時,不同初值,均能收斂于理論值。
表2 拋物線形斷面不同初值正常水深迭代結(jié)果
本文推導(dǎo)了冰蓋下輸水時梯形斷面和拋物線形斷面綜合糙率及流量計算公式,根據(jù)理論推導(dǎo)提出了冰蓋下梯形斷面和拋物線形斷面正常水深顯式迭代算法,得到如下結(jié)論:
1)提出了冰蓋下梯形斷面和拋物線形斷面的新的迭代公式,具有形式簡單,計算方便的特點(diǎn),采用不同初值,均能收斂于理論值。
2)通過理論證明,本文提出的冰蓋下梯形斷面和拋物線形斷面正常水深的迭代公式是收斂的。
3)實(shí)例表明,本文提出的迭代公式具有很好的收斂性,一般需要3~5次就可使誤差小于0.01 m。增加迭代次數(shù)后都能收斂到理論值。
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Explicit iterative algorithm of normal water depth for trapezoid and parabolic open channels under ice cover
Han Yancheng1, Chu Pingping1, Liang Mengyuan1, Tang Wei1, Gao Xueping2
(1.250022,; 2.300072,)
With the increase of water demand in winter in northern China, more and more open-channel water diversion projects transport water under the ice cover in winter such as the Middle Route of South-to-North Water Diversion Project. The method of transporting water using open channel under the ice cover has become increasingly common to delivery water from reservoirs, rivers and lakes to cities. The normal water depth is an important parameter in channel design, operation, flood control, and flow measurement and maintenance of the open channel or sewage systems. The explicit calculation algorithms of the normal water depth for the open channel are mainly for free-ice channels. This paper proposed algorithm of normal water depth of open channel under ice cover. The expression of the synthesis roughness for the flow of the channel under the ice cover was determined based on the studies of Sabaneev. The relationship between the normal water depth and the flow rate of the trapezoid section under the ice cover was derived. A simple explicit iterative algorithm to compute the normal water depth was then proposed. It proved that the new iterative algorithm was convergent using the convergence theory of iteration. The formula to getting the initial value was proposed using the best hydraulic section. The application examples were given to compute the normal depth under the ice cover by using the new iterative algorithm. The results showed that the explicit iterative algorithm proposed had a fast convergence speed. In general, the error would be less than 0.01 m with only 3-5 times iterations. The number of the iteration decreased when using the initial value from the best hydraulic section. When the number of iterations was increased, the iterative value would be closer to the theoretical value of the normal depth. By using the same method, the relationship between the normal water depth and the flow rate under the ice cover was derived for the parabolic section, and a simple explicit iterative algorithm for calculating the normal depth of water was proposed too. The examples showed that the explicit iterative formula of the parabolic section proposed was simple and had a fast convergence speed too. In general, the error would be less than 0.01 m with only 3-5 times iterations as well as trapezoid section. The study of this paper provides a convenient method for the calculation of the normal water depth of the water conveyance channel under the ice cover. The research has theoretical and practical significance for the design, operation and management of the water conveyance channels under the ice cover because the normal depth is most widely used in the water conservancy project.
canals; hydraulic; design; open channel; water transport under ice cover; normal depth of water; explicit iterative algorithm
10.11975/j.issn.1002-6819.2018.14.013
TV 131.4
A
1002-6819(2018)-14-0101-06
2018-01-31
2018-05-10
國家“十二五”科技支撐計劃(2015BAB07B02-6);山東省自然科學(xué)基金(ZR2017LEE028); 山東省重點(diǎn)研發(fā)計劃(2016GSF117038)
韓延成,甘肅武威人,副教授,主要從事水力學(xué)及河流動力學(xué)方面的研究。Email:stu_hanyc@ujn.edu.cn
韓延成,初萍萍,梁夢媛,唐 偉,高學(xué)平.冰蓋下梯形及拋物線形輸水明渠正常水深顯式迭代算法[J]. 農(nóng)業(yè)工程學(xué)報,2018,34(14):101-106. doi:10.11975/j.issn.1002-6819.2018.14.013 http://www.tcsae.org
Han Yancheng, Chu Pingping, Liang Mengyuan, Tang Wei, Gao Xueping. Explicit iterative algorithm of normal water depth for trapezoid and parabolic open channels under ice cover[J]. Transactions of the Chinese Society of Agricultural Engineering (Transactions of the CSAE), 2018, 34(14): 101-106. (in Chinese with English abstract) doi:10.11975/j.issn.1002-6819.2018.14.013 http://www.tcsae.org