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Local Turbulent Energy Dissipation Rate in an Agitated Vessel: Experimental and Turbulence Scaling1

机译:搅拌容器中的局部湍流耗能率:实验和湍流缩放比例1

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The hydrodynamics and the flow field in an agitated vessel were measured using 2-D time resolved particle image velocimetry (2-D TR PIV). The experiments were carried out in fully baffled cylindrical flat bottom vessels 300 and 400 mm in inner diameter. The 300 mm inner diameter tank was agitated by a Rushton turbine 100 mm in diameter, and the 400 mm inner diameter tank was agitated by a Rushton turbine 133 mm in diameter. Three liquids of different viscosities were used as the agitated liquid: (i) distilled water (nu = 9.35 x 10(-7) m(2)/s), (ii) a 28 vol % aqueous solution of glycol (nu = 2 x 10(-6) m(2)/s), and (iii) a 43 vol % aqueous solution of glycol (nu = 3 x 10(-6) m(2)/s). The velocity fields were measured at an impeller rotation speed in the range from 300 to 850 rpm, which covers the Reynolds number range from 50000 to 189000. This means that fullydeveloped turbulent flow was reached. The experiments were performed to investigate the applicability of the following relations: epsilon* = epsilon/(u (4)u) = const, vK/u = const, I /eta K = const, tau(I )/tau(K) = const, epsilon* = epsilon/((Nd)4u) = const, I /d ae Re-1, eta K/d ae Re-1, vK/(Nd) = const, N tau(I ) ae R-1, N tau(K) ae Re-1, and epsilon/(Nq) ae Re. These formulas were theoretically derived in our previous work, using turbulence theory, in particular, using turbulence spectrum analysis. The correctness of the proposed relations is investigated by statistical hypothesis testing.
机译:使用2-D时间分辨粒子图像测速仪(2-D TR PIV)测量搅拌容器中的流体动力学和流场。实验在内径为300毫米且直径为400毫米的完全折流的圆柱形平底容器中进行。通过直径为100mm的Rushton涡轮搅拌300mm内径的罐,并且通过直径为133mm的Rushton涡轮搅拌400mm的内径的罐。将三种不同粘度的液体用作搅拌液:(i)蒸馏水(nu = 9.35 x 10(-7)m(2)/ s),(ii)28 vol%的乙二醇水溶液(nu = 2 x 10(-6)m(2)/ s)和(iii)43 vol%的乙二醇水溶液(nu = 3 x 10(-6)m(2)/ s)。在300至850 rpm的叶轮转速下测量了速度场,该范围涵盖了从50000至189000的雷诺数范围。这意味着可以达到充分发展的湍流。进行实验以研究以下关系的适用性:epsilon * = epsilon /(u(4)/ nu)=常数,vK / u =常数,I> / eta K =常数,tau(I>)/ tau (K)=常数,epsilon * = epsilon /(((Nd)4 / nu)=常数,I> / d ae Re-1,eta K / dae Re-1,vK /(Nd)=常数,N tau (I>)ae R-1,N tau(K)ae Re-1,和ε/(Nq)ae Re。这些公式是在我们以前的工作中使用湍流理论,特别是使用湍流频谱分析从理论上推导的。建议的关系的正确性通过统计假设检验进行研究。

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