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首页> 外文期刊>Journal of the Taiwan Institute of Chemical Engineers >The observation of air bubble entrapment for water droplets impinging on parafilm surface
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The observation of air bubble entrapment for water droplets impinging on parafilm surface

机译:气泡夹杂在薄膜表面的水滴的观察

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摘要

The formation of an entrapped air bubble for a water droplet impinging on a parafilm surface was studied by using a high-speed video camera system. The images were taken sequentially immediately after the droplet impingement. The relaxation of impinging droplets from both the top and side views was monitored, and a formation mechanism of the entrapped air bubble was proposed in this work. An investigation of droplets with different sizes (D _0) and impact velocities (V _i) was performed, and it was found that the formation of the entrapped air bubble was observed only at (i) V _i=0.35-0.56m/s for droplets with D _0=2.14mm, (ii) D _0=1.93-2.14mm for V _i=0.57±0.02m/s, and (iii) D _0=2.30-2.46mm for V _i=0.52m/s. The fluid flow inside the droplet during the formation of air bubble entrapment was examined by performing two sets of droplet impact experiments: (i) droplets with various V _i at a fixed droplet size and (ii) droplets with various volumes at a fixed V _i. Once the water droplet touched the parafilm surface, the drop spread, and the central cone of the impinging droplet descended. After a few milliseconds, the central cone disappeared, an air cavity formed, and the droplet started to retract. The retraction generated an inward, radial flow mainly to the top and bottom of the central air cavity. A crucial condition for the formation of an entrapped air bubble in this work is the inward flow over the top of the air cavity closes earlier than the upward movement of the fluid below the central cavity.
机译:通过使用高速摄像机系统研究了撞击在石蜡膜表面上的水滴的夹带气泡的形成。液滴撞击后立即连续拍摄图像。从顶视图和侧视图都监测了撞击液滴的松弛,并且在这项工作中提出了夹带气泡的形成机理。研究了具有不同尺寸(D _0)和冲击速度(V _i)的液滴,发现仅在(i)V _i = 0.35-0.56m / s时才观察到夹带气泡的形成。 D _0 = 2.14mm的墨滴;(ii)V _i = 0.57±0.02m / s的D _0 = 1.93-2.14mm,以及V _i = 0.52m / s的(iii)D _0 = 2.3.2-4.46mm通过执行两组液滴撞击实验来检查在形成气泡截留过程中液滴内部的流体流动:(i)具有固定液滴大小的各种V_i的液滴和(ii)具有固定容积V_i的各种体积的液滴。一旦水滴接触到parafilm表面,水滴就会散开,撞击水滴的中心锥下降。几毫秒后,中心锥消失,形成气孔,液滴开始缩回。缩回产生向内的径向流,该流主要流向中央空气腔的顶部和底部。在这项工作中形成夹带气泡的关键条件是,空气腔顶部上方的向内流动要比中心腔下方的流体向上运动更早地关闭。

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