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本文用相空间重构的方法,对竖壁薄液膜流动的液膜厚度时间序列进行了重构,并用分维数对奇怪吸引子的动力特征进行了描述,由此描述了壁面热流率对竖壁薄液膜流动特性的影响。

In this paper, the phase space of falling liquid films was reconstructed byusing the time delay procedure. The fractal dimension of the chaoticattractor of the reconstructed phase space was calculated with the variationof wall heat flux. The calculated fractal dimension showd that the wall heatflux has prominent effect on the dynamic behavior of falling liquid films.

参考文献

[1] Chu K J;Dukler A E .Statistical Characteristics of Thin,Wavy Films: Part III Structure of the Large Waves and Their Resistanceto Gas Flow[J].AICHE Journal,1975,21(03):583-593.
[2] Jayanti S;Hewitt G F .Hydrodynamics and Heat Transfer of WavyThin Film Flow[J].International Journal of Heat and Mass Transfer,1997,40(01):179-190.
[3] Wang BX.;Peng XF.;Zhang JT. .On the effect of lateral thermal convection on freely falling liquid film flow[J].International Journal of Heat and Mass Transfer,1998(23):4031-4033.
[4] J T Zheng;B X Wang;X F Peng .Falling Liquid Film ThicknessMeasurement by Optical-Electronic Method[J].Review of Scientific Instruments,2000,71(04):1883-1886.
[5] ECKMANN J P .Ergodic Theory of Chaos and Strange Attractors[J].Reviews of Modern Physics,1985,57(03):617-655.
[6] Fraser A M;Swinney H L .Independent Coordinates for Strange Attractorsfrom Mutual Information[J].Physical Review A,1986,33(02):1134-1140.
[7] Broomhead D S;King G P .Extracting Qualitative Dynamics fromExperimental Data[J].Physica,1986,20:217-236.
[8] Badii R;Politi A .Statistical Description of Chaotic Attractors: theDimension Function[J].Statistical Physics,1986,40(5-6):725-750.
[9] Schouten J D;Takens F;Bleek C M V .Estimation of the Dimension of aNoisy Attractor[J].Physical Review E,1994,50(03):1851-1861.
[10] B.X.WANG;J.T.ZHANG;X.F.PENG .THERMAL NON-EQUILIBRIUM EFFECT ON STABILITIES OF FALLING LIQUID FILMS[J].International Journal of Heat and Mass Transfer,1999(15):2863-2868.
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