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Local turbulent energy dissipation rate in an agitated vessel: New approach to dimensionless definition

机译:搅拌容器中的局部湍流能量耗散率:无因次定义的新方法

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Using theory of turbulence, particularly using turbulence spectrum analysis, the relations epsilon(*) = epsilon/(u (4)u) = const., v(K)/u = const. and I >/eta(K) = const. were derived. Assuming that u ae (Nd) from this it follows that the widely used dimensionless local turbulent energy dissipation rate defined as epsilon/((N (3) d (2)) is directly proportional to impeller Reynolds number, i.e. epsilon/((N (3) d (2)) ae Re, and length scale ratio I >/d is indirectly proportional to impeller Reynolds number, i.e. I >/d ae Re-1, in an agitated vessel at high Reynolds number. The relations obtained by turbulence spectrum analysis were used for estimation of local turbulent energy dissipation rates experimentally measured by StAhl Wernersson and TragArdh (1998, 1999) covering the range of Re = 87600-910200 and own experimental data covering the range of Re = 50000-189000. The experiments have been performed in tanks of 300 mm and 400 mm in the inner diameter for three different viscosities and for various impeller rotational speeds.
机译:使用湍流理论,特别是使用湍流频谱分析,关系epsilon(*)= epsilon /(u(4)/ nu)=常数,v(K)/ u =常数。并且I> / eta(K)= const。被派生。假设由此得出u ae(Nd),则可得出结论,定义为epsilon /(((N(3)d(2)))的广泛使用的无量纲局部湍流能量耗散率与叶轮雷诺数成正比,即epsilon /((N (3)d(2))ae Re,在高雷诺数下的搅拌容器中,长度比例I> / d与叶轮雷诺数间接成正比,即I> / d ae Re-1。湍流频谱分析用于估算由StA yen hl Wernersson和TragA y rdh(1998,1999)实验测得的局部湍流能量耗散率,覆盖范围Re = 87600-910200,而自己的实验数据涵盖了Re = 50000-189000。实验是在内径为300 mm和400 mm的水箱中进行的,用于三种不同的粘度和不同的叶轮转速。

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