柴油機(jī)冷卻水套內(nèi)流體流動(dòng)過程CFD分析
[Abstract]:The requirement of energy saving and environmental protection drives modern diesel engine to adopt more new efficient and clean combustion technology, and the power of diesel engine is strengthened continuously, and the requirement of diesel engine cooling system is more and more high. In the cooling system, the cooling water jacket carries the important function of heat transfer. Three-dimensional numerical simulation CFD method has the advantages of low design cost, short cycle and so on, and can effectively face the challenge of the intense market competition in the research and development cycle. Now, it has gradually become the basic tool to study the performance of cooling water jacket in diesel engine industry. The main work of this paper is as follows: (1) before CFD analysis, the parameters of some key points of diesel engine water jacket, such as flow rate, water pressure, water temperature and so on, are obtained by test method. According to the experimental data and three dimensional model of cooling water jacket, the CFD simulation analysis of diesel engine water jacket shows that the flow of each cylinder is uneven, the right six cylinders are higher than the left six cylinders, the flow velocity in the cylinder head water jacket is lower, and there is a flow dead zone. The flow velocity in the water jacket is low and the flow is not good in the middle. (2) according to the results of CFD analysis, the original scheme is improved, the flow rate of water pump is increased, and the structure of the intake of water jacket is optimized (the position is moved up, the direction of the inlet is adjusted to the tangential direction of the cylinder liner). After the improvement, the flow uniformity of each cylinder is improved, the maximum flow deviation value is reduced to 15.95. The flow velocity of the coolant under the exhaust duct of the water jacket in the cylinder head increases obviously, and can reach 2m s-1.The velocity of the coolant between the inlet and the exhaust valve seat is raised to 0.6ms-1. The coolant velocity in the nasal beam area between the exhaust valve seat and the injector hole is increased to 1.2m s-1, and the intermediate region is up to 2m s-1. The velocity of the upper part of the water jacket is more than 0.5 m s ~ (-1), and the velocity of part of the area is 1 m ~ (-1). The velocity at the bottom of the water jacket increased to 1 m s ~ (-1), and the velocity at the inlet increased to 0.8 m ~ (-1). The heat transfer coefficient of most areas is 3000W (M2K) -1, especially in the upper part of the water jacket. The heat transfer coefficient is increased from 1900 ~ 2000W (M2K) -1 to 3000W (M2K) -1.
【學(xué)位授予單位】:江蘇大學(xué)
【學(xué)位級(jí)別】:碩士
【學(xué)位授予年份】:2016
【分類號(hào)】:TK423
【參考文獻(xiàn)】
相關(guān)期刊論文 前10條
1 段敏;王俊文;張磊;閆鵬斌;魏薇;;某四缸柴油機(jī)冷卻水套CFD分析[J];汽車實(shí)用技術(shù);2016年01期
2 衛(wèi)之龍;王金華;舒新建;謝永亮;王錫斌;黃佐華;;合成氣預(yù)混層流火焰結(jié)構(gòu)的實(shí)驗(yàn)和數(shù)值研究[J];西安交通大學(xué)學(xué)報(bào);2014年07期
3 薛冬薪;張文倩;李維;;基于KIVA和SYSNOISE的柴油機(jī)燃燒振蕩數(shù)值模擬計(jì)算[J];內(nèi)燃機(jī);2012年04期
4 閻超;于劍;徐晶磊;范晶晶;高瑞澤;姜振華;;CFD模擬方法的發(fā)展成就與展望[J];力學(xué)進(jìn)展;2011年05期
5 谷芳;崔國起;吳華杰;李斌;楊志毅;;柴油機(jī)缸蓋水套冷卻流場的LDV試驗(yàn)研究[J];汽車工程;2010年08期
6 吳健;徐斌;馬志豪;鮑學(xué)鋒;孫小偉;;基于FIRE的柴油機(jī)燃燒過程模擬分析[J];小型內(nèi)燃機(jī)與摩托車;2010年03期
7 傅松;胡玉平;李新才;陳志忠;李國祥;潘繼紅;;柴油機(jī)缸蓋水腔流動(dòng)與沸騰傳熱的流固耦合數(shù)值模擬[J];農(nóng)業(yè)機(jī)械學(xué)報(bào);2010年04期
8 姚煒;;CFD模擬在發(fā)動(dòng)機(jī)水套設(shè)計(jì)中的應(yīng)用[J];合肥工業(yè)大學(xué)學(xué)報(bào)(自然科學(xué)版);2009年S1期
9 李寶童;洪軍;孫靜;徐海波;邱志惠;潘世翼;;發(fā)動(dòng)機(jī)冷卻液流動(dòng)與傳熱的數(shù)值模擬[J];西安交通大學(xué)學(xué)報(bào);2009年03期
10 葉伊蘇;辛U,
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