Time–frequency analysis of tribological systems—part I: implementation and interpretation

Abstract A novel technique adapting the time–frequency analysis has been utilized to characterize stationary and non-stationary signals from tribological interactions. This representation displays time, frequency, and signal magnitude to decipher signals emanating from such interactions. Short-time Fourier transform, Wigner, Coi–Williams, and Zhao–Atlas–Marks distributions are suited to represent stationary and non-stationary signals. Some of the most complex tribological phenomena involve head–disk interactions in magnetic recording systems. Examples drawn from practical head–disk interface tests are analyzed by using the fast Fourier transform algorithm to illustrate the dynamic features of various distributions. Time–frequency representation of output spectrums of laser doppler vibrometer (LDV), strain gage sensor, and acoustic emission (AE) sensor obtained from head–disk experiments giving evidence of stationary and non-stationary behavior are investigated.

[1]  J. Bolton,et al.  The use of the Wigner Distribution to analyze structural impulse responses , 1990 .

[2]  L. Cohen Generalized Phase-Space Distribution Functions , 1966 .

[3]  M. Riley Speech Time-Frequency Representations , 1989 .

[4]  Robert J. Marks,et al.  The use of cone-shaped kernels for generalized time-frequency representations of nonstationary signals , 1990, IEEE Trans. Acoust. Speech Signal Process..

[5]  Mj Martin Bastiaans The Wigner distribution function applied to optical signals and systems , 1978 .

[6]  William J. Williams,et al.  Improved time-frequency representation of multicomponent signals using exponential kernels , 1989, IEEE Trans. Acoust. Speech Signal Process..

[7]  D. Bogy,et al.  Dynamics of Gas-Lubricated Slider Bearings in Magnetic Recording Disk Files—Part I: Experimental Observation , 1986 .

[8]  E. Wigner On the quantum correction for thermodynamic equilibrium , 1932 .

[9]  K. Ono Dynamic Characteristics of Air-Lubricated Slider Bearing for Noncontact Magnetic Recording , 1975 .

[10]  Tetsuya Hamaguchi,et al.  Measurement of Impulsive Forces Arising from Flying Head/Disk Collision in Magnetic Disk Storage Systems , 1990 .

[11]  N. Yen,et al.  Time and frequency representation of acoustic signals by means of the Wigner distribution function: Implementation and interpretation , 1987 .

[12]  Frank E. Talke,et al.  The dynamics of slider bearings during contacts between slider and disk , 1989 .

[13]  Y. S. Shin,et al.  Pseudo Wigner–Ville Time-Frequency Distribution and Its Application to Machinery Condition Monitoring , 1993 .

[14]  D. Bogy,et al.  Dynamics of Gas-Lubricated Slider Bearings in Magnetic Recording Disk Files—Part II: Numerical Simulation , 1986 .