| 黄花苜蓿收获机吹送装置气流速度场CFD分析 |
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| 引用本文： | 陈树人,肖君,饶师任,吴明聪.黄花苜蓿收获机吹送装置气流速度场CFD分析[J].农业工程学报,2016,32(12):39-46. |
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| 作者姓名： | 陈树人 肖君 饶师任 吴明聪 |
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| 作者单位： | 江苏大学现代农业装备与技术省部共建教育部重点试验室,镇江,212013 |
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| 基金项目： | 江苏高校优势学科建设工程资助项目（苏政办发[2014]37号）；江苏省农业自主创新基金项目（CX(12)3028）。 |
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| 摘 要： | 为了研究黄花苜蓿收获机吹送装置风机转速与吹送气流速度场分布的关系,该文基于CFD模拟技术建立了黄花苜蓿收获机吹送装置气流速度场分布模型,根据实测的黄花苜蓿收获机相关数据,确定了边界条件和模型参数,得到了不同风机转速下吹送气流速度场分布,以及在风机转速为4 000 r/min时,主风管、不同支风管和距离出风口不同距离的气流速度场分布。设计了与模拟条件相同的验证试验,对模拟条件进行了验证分析。研究表明,试验值与仿真值变化趋势一致,试验值比仿真值略小,误差不超过10%,能够准确地反映黄花苜蓿收获机吹送装置的气流速度场分布规律,风机转速为4 000 r/min时,吹送距离在0.22 m波动区间内能够满足黄花苜蓿吹送要求。
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| 关 键 词： | 计算流体动力学(CFD) 模型 装置 气流速度场 风机转速 吹送距离 |
| 收稿时间： | 2015/1/23 0:00:00 |
| 修稿时间： | 2016/3/23 0:00:00 |
CFD numerical analysis of airflow blowing velocity-field of medicago hispida harvester |
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| Chen Shuren,Xiao Jun,Rao Shiren and Wu Mingcong.CFD numerical analysis of airflow blowing velocity-field of medicago hispida harvester[J].Transactions of the Chinese Society of Agricultural Engineering,2016,32(12):39-46. |
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| Authors: | Chen Shuren Xiao Jun Rao Shiren and Wu Mingcong |
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| Institution: | Key Laboratory of Modern Agricultural Equipment and Technology, Ministry of Education and Jiangsu Province, Jiangsu University, Zhenjiang 212013, China,Key Laboratory of Modern Agricultural Equipment and Technology, Ministry of Education and Jiangsu Province, Jiangsu University, Zhenjiang 212013, China,Key Laboratory of Modern Agricultural Equipment and Technology, Ministry of Education and Jiangsu Province, Jiangsu University, Zhenjiang 212013, China and Key Laboratory of Modern Agricultural Equipment and Technology, Ministry of Education and Jiangsu Province, Jiangsu University, Zhenjiang 212013, China |
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| Abstract: | Abstract: In order to study the relationship of fan rotational speed and waft airflow velocity field distribution of Medicago hispida harvester, the waft airflow channel model is established, which is composed of draught fan, duct and waft airflow area by the UG NX8 software; all the parts of the waft airflow channel model are meshed respectively by using the integrated computer engineering and manufacturing code (ICEM), the grids of volute and impeller passage are unstructured, and the entrance of body, the duct and the waft flow area are meshed by hexagonal structured grids; then all the parts are assembled together. Input the model into Fluent, choose the multiple reference frame (MRF) as the coordinate system, connect the whole basin with 3 pairs of interfaces, take the standard turbulence model to simulate and calculate, and get the results of waft airflow velocity field by the way of chart. The results show that: when the speed of draught fan is 4 000 r/min, the blast capacity of the blow system is 0.1265 kg/s, and it is larger than the required capacity (0.1167 kg/s) of Medicago hispida; when the speed of draught fan is 4 000 r/min, the airflow of most of the ducts converges at the distance of 0.2 m from the air outlet, and the speed of waft airflow is 12-14 m/s which is larger than the required speed (11 m/s) of Medicago hispida, while the distance from the air outlet is 0.3 m, the airflow of the ducts converge entirely, but the speed reduces to about 10 m/s which is below the require, so the waft distance is determined to be 0.22 m by analyzing the area between 0.2 and 0.3 m. In order to identify the simulation result of waft airflow velocity field with computational fluid dynamics (CFD), the experiment of determining waft airflow velocity field is carried out under the fan rotational speed of 4 000 r/min. The environment of experiment is indoor without wind so as to reduce interference. The handheld anemometer Kestrel 4000 is used to measure wild speed, whose measurement range and accuracy are 0.4-40 m/s and ±0.1 m/s respectively, and the non-contact tachometer is used to measure fan''s rotational speed, whose accuracy is 1 r/min and measured distance is 50-300 mm. The measure point is signed in the flow area before the test. The test results are compared with the simulation results after the test: the wild speed value from the test is 19.86-23.33 m/s at air outlet, 4.8%-9.3% less than the simulation value, 18.94-20.97 m/s at the distance of 0.1 m from air outlet, 2.1%-9.2% less than the simulation value, 11.94-14.13 m/s at the distance of 0.2 m from air outlet, 2.5%-7.4% less than the simulation value, 7.53-9.35 m/s at the distance of 0.3 m from air outlet, 6.6%-10% less than the simulation value, and 5.6-7.34 m/s at the distance of 0.4 m from air outlet, 6.6%-9% less than the simulation value. The comparison results show that the change trend of experiment value is consistent with simulation value, though slightly smaller than the simulation one. It means that the numerical calculation model established in the research is correct and reasonable, and it can reflect the distribution of waft airflow velocity field truly, so the selection of fan and duct can meet the requirement of blowing of Medicago hispida. |
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| Keywords: | computational fluid dynamics models equipment waft airflow velocity field fan rotational speed blowing distance |
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