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Multi-scale particle dynamics of low air velocity in a horizontal self-excited gas–solid two-phase pipe flow
► The particle fluctuation velocities in a self-excited gas–solid two-phase flow are measured by PIV. ► Multi-scale particle fluctuation velocity is analyzed by wavelet multi-resolution method. ► The largest contribution of fins to the fluctuating energy is from the components of low frequency. ► Th...
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Published in: | International journal of multiphase flow 2013-07, Vol.53, p.114-123 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | ► The particle fluctuation velocities in a self-excited gas–solid two-phase flow are measured by PIV. ► Multi-scale particle fluctuation velocity is analyzed by wavelet multi-resolution method. ► The largest contribution of fins to the fluctuating energy is from the components of low frequency. ► The contribution of fins from the high frequency is smaller than that of non-fin.
The particle fluctuation velocities of a horizontal self-excited gas–solid two-phase pipe flow with soft fins near MPD (minimum pressure drop) air velocity are first measured by high-speed PIV in the acceleration and fully-developed regimes. Then orthogonal wavelet multi-resolution analysis and power spectrum are used to reveal multi-scale characteristics of particle fluctuation velocity. It is observed that the pronounced peaks of the spectra of axial and vertical fluctuation velocities appear in the range of low frequency near the bottom of pipe. These peaks of spectra become larger and their frequencies decrease by using fins. In the range of low frequencies (3–25Hz), the wavelet components of the fluctuating energy of axial particle velocity make the main contribution accounting for 87% and 93% respectively for non-fin and using fins near the bottom of pipe. In the range of relatively high frequency (50–400Hz), however, the wavelet components of using fins, accounting for about 49%, become smaller than that of non-fin, accounting for about 72%, in the suspension flow regime near the top of pipe. The skewness factor of axial particle fluctuation velocity indicates that the wavelet components follow the Gaussian probability distribution as the central frequency decreases. |
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ISSN: | 0301-9322 1879-3533 |
DOI: | 10.1016/j.ijmultiphaseflow.2013.02.005 |