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1 Tao Xin 1,2 , Uday Kumar 1 & Liang Gao 2 1 Division of Operation and Maintenance, Luleå University of Technology 2 School of Civil Engineering, Beijing Jiaotong University [email protected] Dynamic design of track transition between two different slab tracks
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Dynamic design of track transition between two different .../Me… · Dynamic design of track transition between two different slab tracks. 2 2012-Postdoc in Operation and Maintenance

Oct 18, 2020

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Page 1: Dynamic design of track transition between two different .../Me… · Dynamic design of track transition between two different slab tracks. 2 2012-Postdoc in Operation and Maintenance

1

Tao Xin1,2, Uday Kumar1 & Liang Gao2

1 Division of Operation and Maintenance, Luleå University of Technology2 School of Civil Engineering, Beijing Jiaotong University

[email protected]

Dynamic design of track transition between two different slab tracks

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2012- Postdoc in Operation and Maintenance EngineeringLuleå University of Technology

2006-2011Ph.D. in Highway and Railway EngineeringSchool of Civil Engineering, Beijing Jiaotong University

2002-2006B.S. in Civil EngineeringSchool of Civil Engineering, Beijing Jiaotong University

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Outline

Introduction

Simulation Model

Transition Problems

Transition Remedies

Transition Design

Future Work

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Introduction

With the development of high-speed rail system, various types of slab track were put into service in Europe, China and Japan.

China Railway Track System (CRTS)

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Generally speaking, it has been substantiated that the noise level on slab track was 5dB higher than that on the ballast track. (Quarterly report of RTRI, 1997)Rail vibration levels on the slab track are 5db higher that those on the ballasted track, particularly for frequencies above 1kHz. (Wang 2010)

Introduction

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Introduction

In order to reduce track vibration into surrounding structures, new slab track is specially designed for vibration sensitive areas like railway stations by inserting soft rubber mats under slabs. The newly designed track is referred to as floating slab track.

Slab mat

Slab base

Slab

Slab

Slab base

Fixed slab track

Floating slab track

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Introduction

At the transition point between fixed slab track and floating slab track, a moving wheel experiences a rapid change in elevation and dynamic problems occur because of the abrupt change in the vertical track stiffness.Transition regions require frequent maintenance. When neglected, the track geometry will deteriorate at an accelerated rate. (Lei & Zhang, 2011)A vehicle-track dynamic analysis model is established based on self-developed simulation package FORSYS to study the dynamic behaviours of track transition between fixed slab track and floating slab track.

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Outline

Introduction

Simulation Model

Transition Problems

Transition Remedies

Transition Design

Future Work

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Vehicle-Track Model

The vehicle-track system model is composed of vehicle model, track model and wheel/rail interaction model. Vehicle model

• MBS• FORTRAN code

Track model • FEM• ANSYS software

WRI model • rigid-flexible coupled• FORSYS platform

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Vehicle Model

The vehicle is composed of car body, bogies and wheel-sets. • Car body, bogies and wheel/sets

Rigid bodies

• Primary and secondary suspensions spring-dampers

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Track Model

The slab track is composed of rail, fastener, slab and slab mat.• Rail

point supporting beam element

• Fastener spring-damping element

• Slab solid element

• Slab mat spring-damping element

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WRI Model

The wheel/rail contact force is calculated by Hertz nonliner elastic contact theory as following:

3 / 2ZPG

Where G is contact coefficient, ∆Z is elastic penetration between wheel and rail. The penetration is determined by the relative displacement of wheel and rail at the wheel/rail contact point.

w rZ Z Z R

Where Zw is the vertical displacement of wheel, Zr is the vertical displacement of rail and R refers to the irregularities of rail surface.

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Vibration Equation

The system vibration differential equation can be expressed as following:

0 0 00 0 0

m m m m mm m

f f f f ff f

M C K PM C K P

The subscripts m and f represent MBS (vehicle model) and FEM (track model). After the above system vibration equations obtained, Newmark-β method is applied to solve the equations in the time domain.

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Outline

Introduction

Simulation Model

Transition Problems

Transition Remedies

Transition Design

Future Work

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Transition Problems

At the transition point between fixed slab track and floating slab track, a moving wheel experiences a rapid change in elevation and dynamic problems occur because of the abrupt change in the vertical track stiffness.

• Track stiffness/modulus• Wheel/rail contact force• Rail deflection

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Transition Problems

Track stiffness (Kt) is the ratio of the applied wheel load (P) to rail deflection (y):

tPKy

50 100 150 2000

20

40

60

80

100

120

140

160

Floating slab track

Fixed slab track

46 kN/mm

Trac

k st

iffne

ss (k

N/m

m)

Distance(m)

136 kN/mm

136/36≈3

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Transition Problems

Track modulus is often used as a measure of vertical stiffness of the rail foundation and is defined as the supporting force per unit length of rail per unit vertical deflection under a vertical load, as determined by the following equation (Selig and Waters 1994):

50 100 150 2000

20

40

60

80

100

120

Floating slab track

Fixed slab track

22 MPaTrac

k m

odul

us (M

Pa)

Distance(m)

92 MPa

43

14

tKuEI

92/22≈4

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Transition Problems

50 100 150 200 2500

30

60

90

120

150

Fixed slab track

Floating slab track

Whe

el/ra

il fo

rce

(kN

)

Distance (m)

Fixed slab track

120.6 kN

v = 350 km/hDynamic amplification factor:Fd / F0 =120.6/68.6≈1.76

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Transition Problems

50 100 150 200 2500

30

60

90

120

150

Fixed slab track

Floating slab track

Whe

el/ra

il fo

rce

(kN

)

Distance (m)

Fixed slab track

120.6 kN

v = 350 km/hDynamic amplification factor:Fd / F0 =120.6/68.6≈1.76

The dynamic analysis results show that the wheel/rail interaction is larger when vehicle passes the transition from low-stiffness side to high-stiffness side, compared to the passing in the opposite direction. Even without any initial track irregularities, an abrupt track stiffness change alone would lead to 76% higher dynamic load than static load in the transition.

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Transition Problems

70 71 72 73 74 75 76

2.5

2.0

1.5

1.0

0.5

0.0

-0.5

slope = 1.11 mm/mm

v = 350 km/h

fixed slab track floating slab track

Rai

l def

lect

ion

(mm

)

Distance (m)180 182 184 186 188

2.5

2.0

1.5

1.0

0.5

0.0

-0.5

slope = 2.7 mm/m

v = 350 km/h

fixed slab trackfloating slab track

Distance (m)

Rai

l def

lect

ion

(mm

)

The rail deflection difference is 1.5mm occurring in about 2m. The maximum variation rate of rail deflection is 2.7mm/m, far more than expected.

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Transition Problems

At the transition point between fixed slab track and floating slab track, a moving wheel experiences a rapid change in elevation and dynamic problems occur because of the abrupt change in the vertical track stiffness.

• Track stiffness/modulus: 3, 4 times • wheel/rail contact force: 68.6→120.6kN, 1.76• Rail deflection: 1.5mm/2m, 2.7mm/m

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Outline

Introduction

Simulation Model

Transition Problems

Transition Remedies

Transition Design

Future Work

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Transition Remedies

Increase stiffness of low-stiffness side• Additional rail• Long/wide sleeper• Reducing sleeper spacing• Approach slab• Glued ballast

And/orDecrease stiffness of high-stiffness side

• Rail seat pad• Sleeper pad• Slab mat• Ballast mat

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Transition Remedies

Additional rail

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Transition Remedies

(Sasaoka & Davis 2005)

Glued ballast

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Transition Remedies

Additional rail

Glued ballast

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Transition Remedies

Increase stiffness of low-stiffness side• Additional rail• Long/wide sleeper• Reducing sleeper spacing• Approach slab• Glued ballast

And/orDecrease stiffness of high-stiffness side

• Rail seat pad• Sleeper pad• Slab mat• Ballast mat

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Outline

Introduction

Simulation Model

Transition Problems

Transition Remedies

Transition Design

Future Work

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Transition Design

50 100 150 200 2500

30

60

90

120

150

Floating slab trackW

heel

/rail

forc

e (k

N)

Distance (m)

Fixed slab track

v=350km/h 25m

Transition length: 25m < L < 50m, 6.54m×5=32.7m √

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Transition Design

Railway track Rail deflection(mm) Slab mat stiffness(MN/m3)Fixed slab track 0.5 -

Track transition

S1 0.75 150S2 1.0 70S3 1.25 40S4 1.5 30S5 1.75 24

Floating slab track 2.0 20

0 100 200 300 400 500 6000.5

1.0

1.5

2.0

S3

S3

Rai

l def

lect

ion

(mm

)

Slab mat stiffness (MN/m3)

S5

S2

S1

• Equalize the rail deflection • Provide a gradual stiffness increase

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Transition Design

50 100 150 200 2500

30

60

90

120

150W

heel

/rail

forc

e (k

N)

Distance (m)

transition absence transition existence

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Transition Design

180 190 200 210 220 230

3.0

2.5

2.0

1.5

1.0

0.5

0.0

-0.5

Rai

l def

lect

ion

(mm

)

Distance (m)

transition absence transition existence

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Transition DesignRailway track

Slab mat stiffness (MN/m3)

Track stiffness(MN/m)

Track modulus(MPa)

Fixed slab track - 136 92

Tracktransition

1 150 96 582 70 77 443 40 63 334 30 56 285 24 50 24

Floating slab track 20 46 22

0 50 100 150 200 2500

40

80

120

160

floating slab track

fixed slab trackfixed slab track

transition

Trac

k st

iffne

ss (k

N/m

m)

Distance (m)

transition absence transition existence

transition

0 50 100 150 200 2500

20

40

60

80

100

120

transitiontransition

floating slab track

fixed slab track

Trac

k m

odul

us (M

Pa)

Distance (m))

transition absence transition existence

fixed slab track

A ‘gradual’ increase in track stiffness and modulus dose not mean linear change.

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Outline

Introduction

Simulation Model

Transition Problems

Transition Remedies

Transition Design

Future Work

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Future Work

• Track faults Rail surface irregurlarities Long-term track deformation

• Integrated transition remedies Slab mat Additional rail Fastener stiffness ···

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Thank you for your kind attention!