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Effect of rear slant angle on flow structures, and pollutant dispersion and concentration fields in the wake of the studied model vehicle

机译:后倾角对模型车尾流结构,污染物扩散和浓度场的影响

摘要

Experimental investigations of the interaction effect of rear slant angle (i.e., α = 25° and 60°) and heated air exhaust jet condition (i.e., Uj and Tj) on flow structures, and pollutant (i.e., scalar) dispersion and concentration fields in the near-wake region of two simplified scale-model vehicles at Reynolds number Reh = 5.8 × 104 were performed in a closed-circuit wind tunnel using laser Doppler anemometry (LDA) and the cold wire thermometry. The results show that the behaviors of flow structures and pollutant dispersion in the near-wake region of the studied model vehicles are highly dependent on the interaction effect of Uj/U∞ and α. For the low value of Uj/U∞ (i.e., the driving mode from 30 km h-1 to 70 km h-1), the wake structure of the two studied model vehicles is almost similar to the case without introducing the vehicular exhaust jet flow, Uj/U∞ = 0, but the scalar concentration is neither sent straight to the wake region nor trapped by the recirculation zone. For higher value of Uj/U∞ (i.e., the driving mode of 10 km h-1), the jet flow perturbation along the central plane of the vehicular exhaust tailpipe causes the disappearance of the lower vortex in the recirculation zone for the studied model vehicle A (α = 25°) while it causes the stretching of the recirculation zone for the studied model vehicle B (α = 60°). The contaminant is mainly straight trajectory along its jet exhaust flow axis. Outside the recirculation zone, the flow field becomes symmetrical and its flow structure depends only on the rear slant angle of the studied model vehicle. The scalar concentration field of the studied model vehicle B is characterized by a two-dimensional flow structure whatever the studied driving modes are. The distribution of the mean normalized temperature excess field (i.e., scalar concentration field) conforms to the velocity vector field for both studied model vehicles. For the studied model vehicle A, the scalar concentration is drawn to the edge of the trailing vortex at the vehicular exhaust jet side. This phenomenon causes a significant reduction of the scalar concentration level whatever the studied driving modes are.
机译:后倾斜角(即α= 25°和60°)和热空气排气条件(即Uj和Tj)对流动结构以及污染物(即标量)扩散和浓度场相互作用的实验研究使用激光多普勒风速计(LDA)和冷线测温法在闭路风洞中进行了两个雷诺数Reh = 5.8×104的简化比例模型车辆的近尾区。结果表明,所研究模型车辆近尾流区的流动结构和污染物扩散行为与Uj /U∞和α的相互作用密切相关。对于Uj /U∞的低值(即从30 km h-1到70 km h-1的行驶模式),这两个研究模型车辆的尾流结构几乎与不引入车辆排气喷嘴的情况相似流量,Uj /U∞= 0,但标量浓度既不直接发送到尾流区域,也不被再循环区域捕获。对于较高的Uj /U∞值(即10 km h-1的驱动模式),沿车辆排气尾管中心平面的射流扰动会导致所研究模型的回旋区中较低涡旋消失。车辆A(α= 25°),同时导致被研究模型车辆B(α= 60°)的回流区伸展。污染物沿其喷射流轴线主要是笔直的轨迹。在再循环区域之外,流场变得对称,其流场结构仅取决于所研究模型车辆的后倾斜角。无论所研究的驾驶模式如何,所研究的模型车辆B的标量集中场均具有二维流动结构的特征。平均标准化温度过剩场(即标量浓度场)的分布均与两种研究模型车辆的速度矢量场一致。对于所研究的模型车辆A,标量浓度被吸引到车辆尾气喷射侧尾随涡流的边缘。无论研究的驱动模式是什么,此现象都会导致标量浓度水平的显着降低。

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