Behaviour of ballasted track during high speed train passage William Powrie and Jeffrey Priest University of Southampton High Speed Track Railways Day - 15 February 2011 Outline of talk • Background and Aims • Sub-base issues: effect of train speed on vertical track movements during train passage - numerical analysis - field monitoring • Ballast issues - ballast migration - flying ballast • Conclusions High Speed Track Railways Day - 15 February 2011 Background and Aims High Speed Track Railways Day - 15 February 2011 Background • Increased train speeds on both new and classic railway lines • Lack of detailed analytical understanding of track system / sub-soil behaviour, even for traditional speed railways • Not sure how well past experience and observation (empiricism) will extrapolate to higher speed lines • Application of recent advances in soil mechanics and instrumentation ⇒ improved understanding of ballast and sub-base performance ⇒ better whole life cost modelling • Is ballasted track the best choice for high speed rail? High Speed Track Railways Day - 15 February 2011 Aims • To assess the effects of train speed on the load/deformation response of the track foundation, by analysis and field measurements • To investigate some additional problems associated with the use of ballasted track for high speed railway lines High Speed Track Railways Day - 15 February 2011 Numerical modelling of track-bed displacements Effect of train speed High Speed Track Railways Day - 15 February 2011 Method • Dynamic, 2D finite element analysis using ABAQUS • Elastic, undrained response • Interpretation in terms of total stresses • Loading magnitude and geometry based on Spoornet COALlink line (“Cape” gauge, 1067 mm) • 130 kN maximum wheel load • Analysis modelled the vertical centre plane along the track, and passage of a three-wagon train • Model validated with reference to field data High Speed Track Railways Day - 15 February 2011 2D dynamic FE mesh Pad (0.01m thick) Rail 0.38 Sleeper 0.27 0.2 V1 Ballast 0.3 SSB 0.2 V2 V3 V4 E1 0.2 A 0.2 B 0.2 E2 31.51 SB E3 Natural ground 109.2 High Speed Track Railways Day - 15 February 2011 Typical results: deflections High Speed Track Railways Day - 15 February 2011 Variation of maximum displacement with speed High Speed Track Railways Day - 15 February 2011 Field monitoring: methods High Speed Track Railways Day - 15 February 2011 Measurement techniques: remote video monitoring Webcam captures digital video images of a target, from which displacement is calculated using computer algorithm. Digital camera frame rate up to 170fps High Speed Track Railways Day - 15 February 2011 Measurement techniques: geophones Geophones: LF24, 1 Hz natural frequency, logged at 500Hz Mounted on sleeper or positioned in borehole at different depths in the ground High Speed Track Railways Day - 15 February 2011 Geophone data a b c d Geophone produces a voltage proportional to velocity of the sensor (a). Knowing the response characteristics of the geophone the velocity can be computed (b). Integration of data leads to calculated displacement (c). Dominant axle and bogie frequencies can be obtained (d). High Speed Track Railways Day - 15 February 2011 Comparison: PIV and geophone data Geophones and PIV data are in agreement. 0.1 Geophone Video 0 Displacement (mm) -0.1 -0.2 -0.3 -0.4 -0.5 -0.6 6 6.5 7 7.5 High Speed Track Railways Day - 15 February 2011 8 Time (s) 8.5 9 9.5 10 Video frame rate of 30fps gives an image every 880mm of travel compared with 53mm for 500 Hz geophones. Both methods capture displacements due to individual axles. Field monitoring: results What happens in reality? High Speed Track Railways Day - 15 February 2011 Effect of train speed: HS1 • Standard gauge (1435 mm) • Same trains (Class 390 Eurostar sets) • Static axle load 15.36 tonne (wheel load ~ 75.3 kN) • Speeds ~ 120 km/hr and 270 km/hr High Speed Track Railways Day - 15 February 2011 Vertical displacement vs speed for similar trains on HS1 High Speed Track Railways Day - 15 February 2011 Calculate subgrade modulus from Beam on Elastic Foundation (BOEF) model High Speed Track Railways Day - 15 February 2011 Track modulus from sleeper displacements assuming a constant (static) axle load High Speed Track Railways Day - 15 February 2011 Track modulus vs displacement for all sleepers; track modulus assumed constant for an individual sleeper High Speed Track Railways Day - 15 February 2011 Trend lines for different speeds at constant modulus High Speed Track Railways Day - 15 February 2011 Increase in dynamic load with speed • Dynamic FE analysis suggest that at o.5Vc (train speed = 400km/h) dynamic load increases by less than 10% of static, so at 260km/h dynamic load ≈ static load • Field monitoring suggests dynamic load at 260km/h is around 1.2 – 1.3 × static • At 260km/h, Li and Selig (1998) suggest dynamic load increases to around 2.45 × static High Speed Track Railways Day - 15 February 2011 Ballast issues (1) Ballast migration (ballast circles) High Speed Track Railways Day - 15 February 2011 Ballast migration High Speed Track Railways Day - 15 February 2011 Ballast migration investigation: instrument layout Vertical, lateral and longitudinal sleeper velocities measured using geophones High Speed Track Railways Day - 15 February 2011 Measured sleeper displacements Vertical displacement of high rail end of sleeper is about 2.2 times that of low rail end High Speed Track Railways Day - 15 February 2011 2 mv /R mgsinα mg Ye α h Qe hc Yi s High Speed Track Railways Day - 15 February 2011 Qi For a Pendolino traversing a curve of radius 1230m radius at 180km/h, quasi static analysis gives Qe = 85.0 kN and Qi = 49.2 kN, i.e. a ratio of loads of 1.73 Train Run Inner rail δ mm Outer rail δ mm Ratio δinner /δouter Ratio kouter /kinner 1 0.390 0.853 2.19 1.27 2 0.414 0.900 2.17 1.25 3 0.402 0.903 2.25 1.30 4 0.387 0.908 2.35 1.36 Ratio of deflections is greater than the ratio of quasi‐ static loads implying difference in support stiffnesses High Speed Track Railways Day - 15 February 2011 Dynamic analysis using Vampire gives a maximum value of Qe of >100kN and a load ratio of up to at least ~2.5 High Speed Track Railways Day - 15 February 2011 Proposed mechanism Idealised movement of sleeper During loading sleeper rotates about the low rail end and moves towards the high rail end. Due to shape of sleeper ballast falls vertically during loading and is pushed up (down slope) during unloading. High Speed Track Railways Day - 15 February 2011 WCML: vertical movements due to loco + coaches vs Pendolino trainset Class 87 locomotive produces displacements comparable with the Class 390 Pendolino train; displacements for Mk3 coaches are considerably less. High Speed Track Railways Day - 15 February 2011 Ballast issues (2) Ballast flight (flying ballast) High Speed Track Railways Day - 15 February 2011 Flying ballast • Geotechnical and aerodynamic investigation in collaboration with University of Birmingham (aerodynamics: Professor Chris Baker, Dr Andrew Quinn) and Network Rail HS1 (David Hutchinson, Mick Hayward) High Speed Track Railways Day - 15 February 2011 Background • During passage of a high speed train, ballast particles become detached from the ballast bed (“flying ballast”) • Cause rail defects which require grinding to repair • Causes damage to undercarriages and exposed equipment unless protection is provided • At present the cause is not understood • Is it mechanical, aerodynamic or a combination? High Speed Track Railways Day - 15 February 2011 High Speed Track Railways Day - 15 February 2011 Measurements • Geophones to measure velocities of sleepers during train passage • Accelerometers to measure accelerations of the ballast • High speed camera to observe air turbulence near sleeper (Professor Chris Baker, University of Birmingham) High Speed Track Railways Day - 15 February 2011 Instrumentation layout Aerodynamic equipment installed in between sleeper Accelerometer position in ballast High Speed Track Railways Day - 15 February 2011 Instrumentation view High Speed Track Railways Day - 15 February 2011 Sleeper velocity – vertical At the site monitored, sleeper vertical velocity was typically around 20mm/s High Speed Track Railways Day - 15 February 2011 Sleeper displacements - vertical High Speed Track Railways Day - 15 February 2011 Accelerations Filtered accelerations from ballast are similar in magnitude to accelerations of sleeper obtained by differentiating sleeper velocity High Speed Track Railways Day - 15 February 2011 Air turbulence: visual observation High Speed Track Railways Day - 15 February 2011 Does the track see this turbulence? Slight increase in voltage is observed just before train arrives (4.2 m ahead of first wheel). Is this caused by the turbulence? High Speed Track Railways Day - 15 February 2011 Ballast flight: findings • Sleeper velocity was reasonably consistent for all train passages and sleepers ~ 20 mm/s • Maximum ballast accelerations were ~ 3 m/s • Geotechnical effects (ground accelerations) alone are insufficient to cause ballast flight: the cause is probably a combination of aerodynamic and ballast acceleration effects • Video recording showed pulse of air, which is quite turbulent, travelling in front of train, which may give rise to downward force into ballast High Speed Track Railways Day - 15 February 2011 Conclusions High Speed Track Railways Day - 15 February 2011 Conclusions • Stresses and deflections increase with train speed perhaps more than analysis of “perfect” track would suggest, but less than current empirical rules allow • Differential forces on rails when curving at high cant deficiency together with sleeper geometry and trainset operation (⇒ 10 × the number of high load events per train pass) can cause ballast migration • Combined aerodynamic and ground vibrational effects can lead to ballast flight High Speed Track Railways Day - 15 February 2011 Journal papers (1) • Monitoring the dynamic displacements of railway track. D Bowness, W Powrie, A C Lock, J A Priest and D J Richards. Proc I Mech E Part F, J Rail and Rapid Transit 221 (F1), 13-22, March 2007. Awarded IMechE John F Alcock Memorial Prize and Thomas Hawksley Gold Medal • Stress changes in the ground below ballasted railway track during train passage. W Powrie, L A Yang and C R I Clayton. Proc I Mech E, Part F, J Rail and Rapid Transit 221 (F2), 247-261, May 2007 • Dynamic stress analysis of a ballasted railway track bed during train passage. L Yang. W Powrie and J A Priest. J ASCE Geotechnical and Geoenvironmental Engineering 135(5), 680-689, May 2009 • Determination of dynamic track modulus from measurement of track velocity during train passage. J A Priest and W Powrie. J ASCE Geotechnical and Geoenvironmental Engineering 135(11), 1732-1740, November 2009 High Speed Track Railways Day - 15 February 2011 Journal papers (2) • A full-scale experimental and modelling study of ballast flight under high-speed trains. A D Quinn, M Hayward, C J Baker, F Schmid, J A Priest and W Powrie. Proc I Mech E, Part F, J Rail and Rapid Transit 224 (F2), 61-74, 2010 • Measurements of transient ground movements below a ballasted railway line. J A Priest, W Powrie, L Yang, P J Gräbe and C R I Clayton. Géotechnique 60(9), 667-677, September 2010 • Contribution of base, crib, and shoulder ballast to the lateral sliding resistance of railway track: a geotechnical perspective. L M Le Pen and W Powrie. Proc I Mech E, Part F, J Rail and Rapid Transit 225(F2), 113128, 2011 • An assessment of transition zone performance. B Coelho, P Hölscher, J A Priest, W Powrie and F Barends. Proc I Mech E, Part F, J Rail and Rapid Transit 225(F2), 129-139, 2011 High Speed Track Railways Day - 15 February 2011 Acknowledgements • EPSRC • Daren Bowness, Chris Clayton, Tony Lock, Louis le Pen, David Richards, Liang Yang; University of Southampton • David Hutchinson, Mick Hayward; Network Rail CTRL • Chris Baker, Andrew Quinn; University of Birmingham • Patric Mak, Mark Burstow, James Dean; Network Rail High Speed Track Railways Day - 15 February 2011 Thank you for listening High Speed Track Railways Day - 15 February 2011