Verification of an experimental prediction method for railway - - PowerPoint PPT Presentation
Verification of an experimental prediction method for railway - - PowerPoint PPT Presentation
Subtitle January 2012 XX, Sweden Verification of an experimental prediction method for railway induced vibration Hans Verbraken, Geert Lombaert, Geert Degrande geert.degrande@bwk.kuleuven.be bwk.kuleuven.be/bwm Structural Mechanics,
Introduction
Introduction
- n
FRA procedure Verification Conclusion Left footer January 2012 – 2/19
Railway induced vibrations and re-radiated noise in build- ings
■ Excitation mechanisms: wheel/rail roughness, rail joints,... ■ Vehicle-track interaction: dynamic axle loads. ■ Dynamic interaction between the tunnel and the soil: transfer functions. ■ Wave propagation in the soil: dynamic reciprocity theorem. ■ Dynamic soil-structure interaction. ■ Vibrations in buildings (1 to 80 Hz). ■ Re-radiated noise in buildings (16 to 250 Hz).
Introduction
Introduction
- n
FRA procedure Verification Conclusion Left footer January 2012 – 3/19
Prediction methods
■ Numerical predictions [Lombaert et al., JSV, 2009][François et al., CMAME, 2010]
+ Great variety in numerical models − Need for accurate parameter characterization
■ Empirical predictions
+ Soil characteristics inherently taken into account − Accurate input data is not always available
■ Hybrid predictions ■ Experimental transfer function (red) and 95% confidence region (blue) between 2 points
in the free field [Schevenels, OPTEC, 2009]
x x′ 25 50 75 100 125 150 10
−12
10
−11
10
−10
10
−9
10
−8
Frequency [Hz] Displacement [m/N] Prior model 25 50 75 100 125 150 10
−12
10
−11
10
−10
10
−9
10
−8
Frequency [Hz] Displacement [m/N] Posterior model
The FRA procedure
Introduction FRA procedure
- Vibration velocity
level
- Line transfer
mobility
- Force density
Verification Conclusion Left footer January 2012 – 4/19
FRA procedure
■ Detailed Vibration Assessment
◆ Federal Railroad Administration (FRA) and Federal Transit Administration (FTA)
[Hanson et al., FRA, 2005; Hanson et al., FTA, 2006]
High-Speed Ground Transportation Noise and Vibration Impact Assessment
Office of Railroad Development
- U. S. Department
- f Transportation
Federal Railroad Administration October 2005
TRANSIT NOISE AND VIBRATION IMPACT ASSESSMENT
FTA-VA-90-1003-06 May 2006 Office of Planning and Environment Federal Transit Administration
The FRA procedure
Introduction FRA procedure
- Vibration velocity
level
- Line transfer
mobility
- Force density
Verification Conclusion Left footer January 2012 – 5/19
Vibration velocity level
■ Prediction of the ground vibration velocity level in one-third octave bands [Hanson et al.,
2005, 2006] Lv = LF + TML (1)
◆ Vibration velocity level Lv = 20 log10(vRMS) [dB ref 10−8 m/s] ◆ Force density LF [dB ref N/√m ] ◆ Line transfer mobility TML [dB ref 10−8
m/s N/√m ]
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
The FRA procedure
Introduction FRA procedure
- Vibration velocity
level
- Line transfer
mobility
- Force density
Verification Conclusion Left footer January 2012 – 6/19
Line transfer mobility TML
■ Characterization of the transfer of vibration TML = 10 log10
- hn
k=1 10
TMPk 10
- Measurement line
Rail alignment Impact locations x y z Measurement line Rail alignment Impact locations x y z
8 16 31.5 63 125 −60 −50 −40 −30 −20 −10
TML [dB ref 10−8 (m/s)/(N/m0.5)] One−third octave band center frequency [Hz]
The FRA procedure
Introduction FRA procedure
- Vibration velocity
level
- Line transfer
mobility
- Force density
Verification Conclusion Left footer January 2012 – 7/19
Force density LF
Vibration velocity level Lv
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
Transfer mobility TML
8 16 31.5 63 125 −60 −50 −40 −30 −20 −10
TML [dB ref 10−8 (m/s)/(N/m0.5)] One−third octave band center frequency [Hz]
Force density LF = Lv − TML
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] LF [dB ref 1 N/m0.5]
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 8/19
Moving dynamic loads
■ Analytical expressions for the vibration velocity level due to moving loads in a tunnel or
at grade [Sheng et al., 1999; Lombaert et al., 2000; Forrest and Hunt, 2006]. v(x, t) =
na
- k=1
t
−∞
HT(xk(τ), x, t − τ)gk(τ)dτ (2)
x y z xk(τ) x x y z xk(τ) x
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 9/19
Case
■ Bakerloo line tunnel [Gupta et al., JSV, 2009] x z 5 m 28 m 3.704 m
ρs = 1980 kg/m3 βs = 0.042 Cs = 325 m/s Cp = 1964 m/s ρs = 1980 kg/m3 βs = 0.039 Cs = 220 m/s Cp = 1571 m/s
5.5 m 60 m A B ■ Non-ballasted concrete slab track ■ Train with 28 axles (Lt = 108.33 m) ■ Unevenness FRA class 3
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 10/19
Numerical prediction: coupled periodic FE–BE model
■ Model [Degrande et al., JSV, 2006] x y z ˜ x ˜ x + Ley ˜ x + nyLey x′ ■ (a) Transfer function, (b) time history and (c) one-third octave band spectrum of the vi-
bration velocity in the free field in point A [Gupta et al., JSV, 2009]
20 40 60 80 100 120 −60 −50 −40 −30 −20 −10
Frequency [Hz] Mobility [dB ref 10−8 m/s/N]
−20 −15 −10 −5 5 10 15 20 −2 −1 1 2 x 10
−4
Time [s] Velocity [m/s]
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 11/19
Numerical prediction model
■ Transfer functions of the track-tunnel-soil system at (a) 10 Hz and (b) 40 Hz [Gupta, 2008]
(a) Animation (avi) and zoom (avi). (b) Animation (avi) and zoom (avi).
■ Response (avi) in the free field due to a carriage moving at constant speed on an uneven
rail with a single wavelength unevenness (excitation at 40 Hz).
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 12/19
Derivation of analytical expressions for LF and TML
■ Vibration velocity
v(x, t) =
na
- k=1
t
−∞
HT(xk(τ), x, t − τ)gk(τ)dτ (3)
■ Assumptions
◆ Fixed point loads ◆ Non-coherent and equal axle loads ◆ Frequency-averaged transfer function ◆ Equidistant point sources
■ Analytical expressions for LF and TML
Lv = 10 log10
- g2
RMS
La
- LF
+ 10 log10
- La
na
- k=1
ω2
ω1 |ˆ
hzz(xk, x, ω)|2dω ∆ω
- TML
(4)
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 13/19
Results
■ One-third octave band spectra of the velocity in (a) point A and (b) point B for a train
passage at a speed of 30 km/h calculated with the numerical method (grey line) and the FRA procedure (black line).
x y z A B
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
(a) (b)
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 14/19
Assumption 1: fixed point loads
■ One-thirds octave band RMS value of the vertical velocity in (a) point A and (b) point B
due to a moving train (grey line) and due to a fixed train (black line).
x y z A B
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
(a) (b)
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 15/19
Assumption 2: non-coherent and equal axle loads
■ One-third octave band RMS value of the vertical velocity in (a) point A and (b) point B
with coherent point loads (grey line) and non-coherent point loads (black line)
x y z A B
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
(a) (b) [Hunt, 1996; Wu and Thompson, 2001]
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 16/19
Assumption 3: average value of the transfer function
■ One-third octave band spectra of the velocity in (a) point A and (b) point B with narrow
band (grey line) and frequency-averaged (black line) transfer function.
x y z A B
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
8 16 31.5 63 125 10 20 30 40 50 60
One−third octave band center frequency [Hz] Lv [dB ref 10−8 m/s]
(a) (b)
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 17/19
Assumption 4: equidistant point sources
■ Transfer mobility
TML = 10 log10
- La
na
- k=1
ω2
ω1 |ˆ
hzz(xk, x, ω)|2dω ∆ω
- (5)
(a) (b) (c)
La La h/2 h
TML = 10 log10
- h
n
- k=1
10
TMPk 10
- (6)
Verification
Introduction FRA procedure Verification
- Analytical
- Case
- Numerical
- Derivation
- Results
Conclusion Left footer January 2012 – 18/19
Assumption 4: equidistant point sources
■ Transfer mobility in (a) point A and (b) point B calculated with the original axle positions
(light-grey line), with 28 equidistant axle positions (dark-grey line) and with 15 equidistant axle positions including two edge points (black line).
x y z A B
8 16 31.5 63 125 −60 −50 −40 −30 −20 −10
One−third octave band center frequency [Hz] TML [dB ref 10−8 (m/s)/(N/m0.5)]
8 16 31.5 63 125 −60 −50 −40 −30 −20 −10
One−third octave band center frequency [Hz] TML [dB ref 10−8 (m/s)/(N/m0.5)]
(a) (b)
Conclusion
Introduction FRA procedure Verification Conclusion
- Conclusion
Left footer January 2012 – 19/19
Conclusion
■ Separate characterization of force density and line transfer mobility leads to a good ap-
proximation of the one-third octave band vibration velocity level
■ Analytical expressions of force density and line transfer mobility are obtained based on
four assumptions
◆ Fixed train position ◆ Non-coherent axle loads ◆ Averaged transfer function ◆ Equidistant point loads
■ The results for tunnels are also validated for the case of railway traffic at grade