Hilbert–Huang transform, Hurst and chaotic analysis based flow regime identification methods for an airlift reactor

Abstract The flow regimes and their transitions in an internal loop airlift reactor were investigated. The Hilbert–Huang transform (HHT) was applied to analyze the energy–frequency–time distribution of the pressure signal. It was found that the Hilbert spectrum of the pressure signal was closely related to the superficial gas velocity. The stochastic behaviors of intrinsic mode functions (IMFs) extracted from the pressure signal were studied using the Hurst analysis. Two different Hurst exponents were obtained for each pressure signal: one was smaller than 0.5, while the other was larger than 0.5, representing the anti-persistent and persistent hydrodynamic behaviors, respectively. The evolution of the larger Hurst exponent clearly indicated flow regime transitions in the downcomer. The wavelet transform combined with the autocorrelation analysis were applied to extract chaotic components of the pressure signal. Two flow regime transition points were successfully detected from the evolution of chaotic parameters, i.e. the largest Lyapunov exponent, correlation dimension and Kolmogorov entropy.

[1]  P. Grassberger,et al.  Measuring the Strangeness of Strange Attractors , 1983 .

[2]  Li Yingmin,et al.  Analysis of earthquake ground motions using an improved Hilbert–Huang transform , 2008 .

[3]  N. Huang,et al.  A new view of nonlinear water waves: the Hilbert spectrum , 1999 .

[4]  Hsiaotao Bi,et al.  Characterization of dynamic behaviour in gas–solid turbulent fluidized bed using chaos and wavelet analyses , 2003 .

[5]  Cor M. van den Bleek,et al.  Early warning of agglomeration in fluidized beds by attractor comparison , 2000 .

[6]  P. Tse,et al.  A comparison study of improved Hilbert–Huang transform and wavelet transform: Application to fault diagnosis for rolling bearing , 2005 .

[7]  Naoko Ellis,et al.  Hydrodynamics of three-phase fluidized bed systems examined by statistical, fractal, chaos and wavelet analysis methods , 2005 .

[8]  L. Cao Practical method for determining the minimum embedding dimension of a scalar time series , 1997 .

[9]  Cor M. van den Bleek,et al.  Deterministic chaos: a new tool in fluidized bed design and operation , 1993 .

[10]  Wen‐Teng Wu,et al.  Flow regime transitions in an internal-loop airlift reactor , 2007 .

[11]  P. Grassberger,et al.  Estimation of the Kolmogorov entropy from a chaotic signal , 1983 .

[12]  J. Cusido,et al.  Fault detection by means of Hilbert Huang Transform of the stator current in a PMSM with demagnetization , 2010, 2007 IEEE International Symposium on Intelligent Signal Processing.

[13]  J. Markoš,et al.  Scale influence on the hydrodynamics of an internal loop airlift reactor , 2004 .

[14]  Xingang Li,et al.  Origin of pressure fluctuations in an internal-loop airlift reactor and its application in flow regime detection , 2009 .

[15]  Yong Yan,et al.  Hilbert–Huang transform based signal analysis for the characterization of gas–liquid two-phase flow , 2007 .

[16]  N. Huang,et al.  The empirical mode decomposition and the Hilbert spectrum for nonlinear and non-stationary time series analysis , 1998, Proceedings of the Royal Society of London. Series A: Mathematical, Physical and Engineering Sciences.

[17]  Lijia Luo,et al.  Hydrodynamics and mass transfer characteristics in an internal loop airlift reactor with different spargers , 2011 .

[18]  John R. Grace,et al.  Characteristics of gas-fluidized beds in different flow regimes , 1999 .

[19]  J. Heijnen,et al.  A simple hydrodynamic model for the liquid circulation velocity in a full-scale two- and three-phase internal airlift reactor operating in the gas recirculation regime , 1997 .

[20]  Xingang Li,et al.  Identification of regime transitions in an inner-loop airlift reactor using local bubble-induced pressure fluctuation signals , 2010 .

[21]  S. Hahn Hilbert Transforms in Signal Processing , 1996 .

[22]  Rajamani Krishna,et al.  Characterization of regimes and regime transitions in bubble columns by chaos analysis of pressure signals , 1997 .

[23]  E. Ali,et al.  Prediction of regime transitions in bubble columns using acoustic and differential pressure signals , 2007 .

[24]  Jc Jaap Schouten,et al.  Monitoring the quality of fluidization using the short-term predictability of pressure fluctuations , 1998 .

[25]  Gabriel Wild,et al.  Study of hydrodynamic behaviour in bubble columns and external loop airlift reactors through analysis of pressure fluctuations , 2000 .

[26]  Lijia Luo,et al.  CFD simulations to portray the bubble distribution and the hydrodynamics in an annulus sparged air‐lift bioreactor , 2011 .

[27]  Yongrong Yang,et al.  Multiscale resolution of fluidized‐bed pressure fluctuations , 2003 .

[28]  Chris Chatfield,et al.  The Analysis of Time Series: An Introduction , 1981 .

[29]  M. Rosenstein,et al.  A practical method for calculating largest Lyapunov exponents from small data sets , 1993 .

[30]  H. Hurst METHODS OF USING LONG-TERM STORAGE IN RESERVOIRS. , 1956 .

[31]  Tsao-Jen Lin,et al.  Predictions of flow transitions in a bubble column by chaotic time series analysis of pressure fluctuation signals , 2001 .

[32]  Lijia Luo,et al.  Identification of flow regime transitions in an annulus sparged internal loop airlift reactor based on higher order statistics and Winger trispectrum , 2011 .