2023
DOI: 10.1007/978-3-031-39109-5_19
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A Simulation Study on Characterizing Transfer Functions of Railway Tracks Using Train-Borne Laser Doppler Vibrometer

Abstract: Due to train load and aging, the dynamic properties of railway tracks degrade over time and deviate over space, which should be monitored to facilitate track maintenance decisions. A train-borne laser Doppler vibrometer (LDV) can directly measure track vibrations in response to the moving train load, which can be potentially applied to large-scale rail infrastructure monitoring. This paper characterizes track structures as a distributed system by estimating transfer functions between the wheel-rail force and t… Show more

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Cited by 1 publication
(4 citation statements)
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“…Therefore, the measured sleeper vibrations can be used to monitor the dynamic properties of track structures. To tackle the challenge induced by the amplitude and frequency variation of the excitation from the vehicle to the track, wheel‐rail force or vehicle vibration signals can be incorporated to normalize the train‐borne LDV signals and estimate the transfer functions of track structures (Zeng, Núñez, et al., 2023). The deviation in the estimated transfer functions can reflect the difference in track stiffness and damping, which can be further used for anomaly detection in railway tracks.…”
Section: Discussionmentioning
confidence: 99%
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“…Therefore, the measured sleeper vibrations can be used to monitor the dynamic properties of track structures. To tackle the challenge induced by the amplitude and frequency variation of the excitation from the vehicle to the track, wheel‐rail force or vehicle vibration signals can be incorporated to normalize the train‐borne LDV signals and estimate the transfer functions of track structures (Zeng, Núñez, et al., 2023). The deviation in the estimated transfer functions can reflect the difference in track stiffness and damping, which can be further used for anomaly detection in railway tracks.…”
Section: Discussionmentioning
confidence: 99%
“…This research first uses modeling and simulation to characterize train‐borne LDV measurement and generate signals of sleeper vibration and speckle noise. A vertical train‐track model is built to simulate sleeper vibration measurement using a train‐borne LDV (Zeng, Núñez, et al., 2023), as shown in Figure 2. The train is modeled as a quarter vehicle as follows, mvz̈v(t)badbreak+kv[]zv(t)zw(t)goodbreak+cv[]żv(t)żw(t)goodbreak=0$$\begin{equation}{m}_{\mathrm{v}}{\ddot{z}}_{\mathrm{v}}(t) + {k}_{\mathrm{v}}\left[ {{z}_{\mathrm{v}}(t) - {z}_{\mathrm{w}}(t)} \right] + {c}_{\mathrm{v}}\left[ {{{\dot{z}}}_{\mathrm{v}}(t) - {{\dot{z}}}_{\mathrm{w}}(t)} \right] = 0\end{equation}$$ mnormalwtruez̈normalwknormalvznormalvfalse(tfalse)znormalwfalse(tfalse)cnormalvtrueżnormalvfalse(tfalse)trueżnormalwfalse(tfalse)+Fnormalcfalse(tfalse)=0$$\begin{eqnarray} && {m}_{\mathrm{w}}{\ddot{z}}_{\mathrm{w}} - {k}_{\mathrm{v}}\left[ {{z}_{\mathrm{v}}(t) - {z}_{\mathrm{w}}(t)} \right] - {c}_{\mathrm{v}}\left[ {{{\dot{z}}}_{\mathrm{v}}(t) - {{\dot{z}}}_{\mathrm{w}}(t)} \right]\nonumber\\ &&\quad +\, {F}_{\mathrm{c}}(t) = 0 \end{eqnarray}$$where m v and m w are the masses of the vehicle and the wheel, respectively, z v and z w are their vertical displacements, respectively, k v and c v are the stiffness and damping of the suspension, respectively, and F c is the wheel‐r...…”
Section: Simulation and Validationmentioning
confidence: 99%
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