# Overview and outlook on railway track stiffness measurement

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## Abstract

Stiffness is one of the basic performance parameters for railway track. The efficient and accurate stiffness measurement has been considered as the foundation for further development of railway engineering, and therefore has great theoretical and practical significance. Based on a summary of the connotation and measurement of track stiffness, the state of the art of measurement methods for track stiffness was analyzed systematically. The standstill measurement of track stiffness can be performed with the traditional jack-loading method, impact hammer method, FWD (falling weight deflectometer) method, and track loading vehicle method. Although these methods can be adopted in stiffness measurement for a section of railway track, they are not desirable owning to small range and low efficiency. In the recent 20 years, researchers have proposed many methods like unbalanced-loading laser displacement method, deflection basin deformation rate method, and eccentricity excitation method to continuously measure track stiffness; however, these methods have drawbacks like poor accuracy, low speed, and insufficient data analysis. In this work, the merits and demerits of these methods were summarized, and optimization suggestions were presented. Based on the wave transmission mechanism and principle of vibration energy harvesting, an overall conception on continuous measurement of stiffness and long-term stiffness monitoring for special sections was proposed.

## Keywords

Railway Track structure Track stiffness Measurement Maintenance Vibration## 1 Introduction

Track structure, a load bearing and transmitting structure of railway system, has stiffness to provide necessary elasticity. Track structure comprises several layers and each layer has its own stiffness, namely the track component stiffness. The overall track stiffness is usually adopted to characterize the total stiffness of all layers and reflect the stiffness characteristics of the whole track structure [1, 2]. The stiffness measurement of a track, generally, refers to measuring the overall stiffness. In laboratory tests, the stiffness of certain track component can be measured, such as fastener stiffness and ballast stiffness [3, 4].

Discrete rail support model and continuous rail support model are two classical models for the traditional mechanical analysis of railway track [1, 2]. In the discrete rail support model, the stiffness of fastener supporting track is a spring constant, while in the continuous rail support model, it is denoted by track modulus, which is calculated with the spring constant divided by the spacing between centers of discrete supports. The stiffness measurement method based on the Winkler elastic foundation model uses track modulus to characterize the overall track stiffness.

The track stiffness can also be classified into dynamic stiffness and static stiffness [2, 5, 6]. The resistance of track structure to deformation under a static load is called as static stiffness, which, usually, is determined by the deformation degree of track structure under the static load. The dynamic stiffness refers to the resistance of track structure to deformation under certain dynamic excitation, which is determined by the natural frequencies of track structure. The track dynamic stiffness reflects the supporting performance of the vibrating track structure and therefore is an important factor influencing the wheel–rail interaction and train running performance. However, the static stiffness is always adopted instead for the traditional mechanical analysis of the wheel–rail system. The rapid development of high-speed railway passenger transportation, heavy-loaded train transportation, and railway engineering technologies makes the theoretical analysis and practical measurement of dynamic stiffness significant.

*P*the rail beam will deform. If the deformation amount is

*y,*the track static stiffness

*K*will be

*a*and

*b*can be defined according to the specific requirement. For example, define

*b*as the final loading state and

*a*as the exact release state of the fastener clamping force.

*P*=

*P*

_{0}e

^{jωt }is exerted on the rail. If the dynamic displacement at the force acting point is

*Z*=

*Z*

_{0}e

^{j(ωt+φ)}, the track dynamic stiffness can be defined as the ratio of the acting force amplitude to the dynamic displacement amplitude:

Under this definition, the track dynamic stiffness can be adopted to reflect the stiffness characteristics in steady forced vibration at a certain frequency.

Now, the track dynamic stiffness is a complex value, with the amplitude and phase [8, 12]. The track dynamic stiffness can also be measured and analyzed through its reciprocal, namely the track dynamic flexibility.

## 2 Significance of track stiffness measurement

Track stiffness is an important factor influencing the safety and stability of train operation and the vibration and deformation of track structure as well as the dynamic response of substructures like subgrades and bridges [13, 14, 15, 16, 17, 18, 19, 20, 21, 22].

Researches in relation to track stiffness mainly focus on three aspects: ① the analysis of the influence of track stiffness on the vehicle-track-substructure coupled dynamics; ② the nonlinear characteristics of track component stiffness, such as the nonlinearities of the rubber pad; and ③ the evaluation methods of track stiffness and the reasonable stiffness for track structure and its components.

### 2.1 Stiffness design of new railway lines

Stiffness design of new railway lines is to determine overall track stiffness and track component stiffness to meet the operation conditions of new railways. The measurement of track stiffness can help evaluate the stiffness design of new railways and present the relevant modification opinions.

### 2.2 Daily maintenance of railway lines

Track stiffness is also an important parameter for maintenance of railway lines in addition to the track geometric irregularity [23]. For most maintenance methods, the track geometric irregularity of railway lines is always adopted as the diagnostic parameter. The track geometry can be adjusted by ballast tamping to keep it within the limited range. However, the performance of ballasts, mostly, is dependent on the performance of bottom subgrade or other substructures. Ballast tamping cannot help improve the performance of substructures, such that track geometric irregularity repeatedly occurs.

- (1)
*Low track stiffness*The railways built in soft soil areas and bad soil zones tend to experience serious rail displacement and fast cracking of track components after a period of operation. These diseases are mainly caused by poor stiffness of soil subgrade and therefore it should be strengthened. It is very important for checking the railway lines in time to keep safe train operation. - (2)
*Variable track stiffness*The stiffness always changes abruptly at the railway–bridge, railway–tunnel, and bridge–tunnel sections, and therefore transition zones shall be set [24]. Besides, when track geometric irregularity is deteriorated, support for the track will be uneven. - (3)
*Virtual track stiffness*Diseases, such as dirty ballast, hanging sleepers, and loose fasteners, can cause deformation and holes, leading to virtual stiffness for the rail support. The virtual stiffness represents potential risk to safe train operation. - (4)
*Assortative stiffness*The unmatched supporting stiffness of the right and left rails will result in uneven rail displacement, which can cause center bending of sleepers as well as the other unreasonable stress and cracking problems of track components.

The measurement of track stiffness can help direct the routine maintenance of railway lines and provide a reliable basis for making optimal maintenance strategies.

## 3 Track stiffness measurement methods

### 3.1 Standstill measurement

The standstill measurement of overall track stiffness means that a measurement point is decided in advance, and then the overall track stiffness can be calculated by measuring displacement and vertical force exerted on this point.

The overall track stiffness, generally, can be measured based on four methods: (1) traditional hydraulic jack-loading method [1, 2], (2) impact hammer method [25, 26], (3) FWD method [9, 27], and (4) TLV method [2, 5, 28, 29, 30, 31].

In the FWD (falling weight deflectometer) method, a mass impacts a track and the vibration response is measured at the same time. Afterwards, the track stiffness characteristics can be explored through transfer function calculation or other methods. The FWD method, to a certain extent, can reflect the impact effect on a track when a train is running at a high speed. The standard FWD method uses a 125 kN free-falling mass to impact the track. The vibration response of track is generally measured with velocity transducers or geophones.

Queensland University of Technology in Australia improved a movable track stiffness measurement vehicle based on common TLV. This vehicle is composed of three cars. The front one is a six-axle towing locomotive (weight of 90 tons) to tow the vehicle to the specified measurement point. The middle one is a buffer car for buffering the influence of the front car on the rear one during the measurement. The rear car is equipped with measurement instruments and is the key part of the vehicle. The rear car weighs 57 tons totally (each part of 14.3 tons) and is equipped with hydraulic jacks and displacement transducers to exert vertical force and measure track deflection basin. When the vehicle reaches the specified measurement point, the hydraulic jacks extend from both sides of the rear car and act on the track separately. The deflection basin is recorded by 22 transducers to calculate the track modulus.

### 3.2 Continuous measurements

By the time of November 2015, there are 61 high-speed railway lines in China, and the total mileage has reached 12,000 km. The rapid development of high-speed railway lines has made the accurate and continuous measurement of track stiffness extremely important.

The above methods for standstill measurement of overall track stiffness are arduous, time consuming, and not suitable for a long-distance and multi-point measurement. The maintenance of railway lines requires continuous track stiffness measurement equipment. Therefore, many organizations have started to develop vehicles for continuous track stiffness measurement.

As early as in 1997, China Academy of Railway Sciences (CARS) put forward the conception of a vehicle for track elasticity measurement [33]. This vehicle comprises a heavy car in the front and a light car in the rear. The axle load of the heavy car can be varied by adjusting the number of concrete blocks in the range of 150–250 kN. Thus, the influence of different train axle loads on the measured results can be obtained. The light car weighs 40 kN and is used to eliminate the clearances between the rail and sleeper as well as between the sleeper and ballast bed. The measurement equipment on both heavy and light cars is the same except for the axle load.

*y*

_{ K }of tracks, as shown in Fig. 6.

*d*is measured according to the camera view analysis and

*L*

_{1},

*L*

_{2},

*θ*

_{1},

*θ*

_{2}, and

*H*are all known values. After

*y*

_{ r }is obtained, an equation is established based on the Winkler foundation model. Solving this equation, one can obtain the track modulus.

The ZOYON Technology Co., Ltd of Wuhan University (China), is now investigating a deformation rate-based track stiffness measurement method to be applied in the movable stiffness measurement vehicles [38]. This method was first introduced by scholars of Delft University of Technology in Holland; however, no prototype car has been made [2, 39, 40, 41].

*w*′(

*x*) refers to the vertical track deflection rate obtained based on the Winkler foundation beam model.

The European Research for an Optimised BALlasted Track (EUROBALT II) project indicates that track stiffness is another import parameter for optimal long-term maintenance strategies in addition to track geometric irregularity (Meissonnier 2000).

The static load, dynamic load, and maximum speed of this trolley are 60 kN, 20 kN, and 30 km/h, respectively. This trolley can only run on straight sections and not on narrow curves or switches. This trolley can be excited with different frequencies but only one frequency for each run. This trolley has been used for many on-site measurements, which shows good repeatability and reproducibility.

In order to compare the measurement results of the RSMV with that of the prototype trolley, a comparison test was performed, showing that, for those railway sections with the overall track stiffness less than 150 kN/mm, the results were almost the same, while for those hard sections, the results are quite different.

A camera with a linear CCD sensor is mounted under the technical carriage to record and monitor the measured track surface. All measurements are monitored by the portable computer placed in the locomotive.

*M*

_{1}refers to the total mass,

*M*

_{0}the unsprung mass,

*Г*

_{ b }the vertical acceleration of the vibrating wheel,

*Г*

_{ c }the vertical acceleration of the suspended mass,

*m·e*the eccentric moment of the unbalanced system,

*ω*the angular velocity of rotation, and

*φ*the angle of rotation.

*z*can be obtained by calculating the double integration of the vertical acceleration of the unsprung mass:

The overall track stiffness, over an average time period, can be obtained according to wheel–rail force and vertical displacement.

## 4 Analysis and discussion of measurement methods

Comparison of track stiffness measurement vehicles

No. | Measurement concept | Measurement accuracy | Measurement speed | Research progress |
---|---|---|---|---|

1 | Standstill measurement, static stiffness | High accuracy for vertical measurement; unable to know the stiffness change along the line | Very slow | Mainly applied for heavy haul railway lines |

2 | Continuous measurement, static stiffness under dynamic load | Improved measurement accuracy due to enhancing displacement measurement | Adjustable, below 60 km/h usually | Mature |

3 | Continuous measurement, static stiffness under dynamic load, high-speed deflectograph | Unsure | 130 km/h, even higher | Successfully applied to the road modulus measurement and the track modulus measurement is in progress |

4 | Continuous measurement, dynamic stiffness, eccentric wheel excitation, hysteresis curve measurement | High accuracy because of hysteresis curve fitting, stiffness and damping parameter identification | Slow, approximate 6 km/h | Data analysis and vehicle optimization |

5 | Continuous measurement, dynamic stiffness, eccentric wheel excitation | High accuracy and able to identify many railway line stiffness problems | 50 km/h | Multi-line measurements and database construction |

From Table 1, the existing continuous measurements of track stiffness have four problems.

### 4.1 Inconsistent measurement concepts

At present, the measurement methods target at different stiffness: static stiffness, dynamic stiffness, or the track component stiffness, which makes it rather difficult to compare the measurement results of these measurement methods.

For instance, the exciting frequency is unnecessary for static stiffness measurement, while for dynamic stiffness measurement, it is requisite. Likewise, when the deformation rate (TU Delft and ZONYON) is to be measured, the vehicle shall run as fast as possible; when the steady dynamic stiffness is to be measured (CETE-NC and SNCF), the vehicle speed cannot be too high. Hence, the measurement of track stiffness, firstly, requires a unanimous stiffness notion that can reflect the track stiffness characteristics completely.

Relatively speaking, the track stiffness notions of the RSMV (KTH, Sweden) and Portancemetre (CETE-NC and SNCF, France) are more advanced. The notions indicate that the track stiffness relates to the exciting frequency, which agrees with the conclusions of many literatures [52, 53, 54]. Other notions are based on the Winkler support model, which are not suitable for exploring deep information about track stiffness though they may solve some practical engineering problems.

### 4.2 Incapability for high-accuracy measurement

All the above-mentioned measurement methods are not suitable for high-accuracy measurement. The accuracy of the laboratory test results are acceptable; however, the accuracy of field test results is not satisfactory. The measurement accuracy mainly depends on the accuracy of force and displacement sensors or acceleration measurements. The force measurement includes strain measurement and pressure intensity measurement of hydraulic system. The strain measurement is more sensitive and accurate. Laser method is more suitable for displacement measurement, which provides high accuracy. Although acceleration transducers have high accuracy, in continuous track stiffness measurement, noise (especially low-frequency noise) can greatly affect the measurement. In addition, error cannot be eliminated when the displacement is calculated through the double integration. Hence, for the acceleration measurement method, appropriate data processing and signal analysis technologies are required to ensure high displacement accuracy. In fact, the continuous track stiffness measurement can be graded according to the desired accuracy (10, 1, 0.1 kN/mm and so on) to save cost and reasonably use the measurement sources.

### 4.3 Low measurement speed

Measurement speed is always very important for continuous track stiffness measurement. Theoretically, high measurement is likely to produce more accurate results. The track deformation rate measurement method (TU Delft and ZONYON) has the quickest measurement speed. However, it has two defects: the static stiffness notion takes no account of the influence of railway stiffness irregularity and geometric irregularity, and it is hard to deal with the dilemma between the measurement speed, transducer accuracy, and equipment operation reliability. These problems limit the application of this measurement method.

The measurement speeds of the methods designed by the University of Nebraska (USA) and CARS are moderate, which are limited by the accuracy of laser displacement transducers. The RSMV designed by the KTH (Sweden) has rather low measurement speed, which is limited by the reliability of the hydraulic system as well as the accuracy of transducers.

The measurement speed of Portancemetre (CETE-NC and SNCF, France) cannot be too high because the force–displacement hysteresis curve is to be measured.

### 4.4 Insufficient data analysis

From the perspective of the excitation-response measurement, the system transfer characteristics (the stiffness information) can be obtained regardless of the excitation type as long as there is sufficient response information. Hence, the track stiffness information, to a great extent, depends on the analysis technology of data.

KTH (Sweden) takes the leading position in the analysis technology of data, which has investigated the relation between track stiffness and time frequency/spatial frequency, the phase information of track stiffness, and amplitude information.

In fact, the laser measurement method (University of Nebraska, USA, and CARS, China) can also collect more data because the real-time track vibration can be reflected through the laser displacement data.

Up to now, no quantitative research on the relation between track stiffness and exciting frequency, exciting intensity as well as the running speed has emerged, which is the main reason for inadequate analysis of the measurement data of continuous track stiffness.

## 5 Conclusions and suggestions

- (1)
Track stiffness is an important factor influencing the safety and reliability of train operation, the vibration and deformation of track structures, and the dynamic response of substructures like subgrades and bridges. The track stiffness measurement is of great theoretical and practical significance to the design of new railway lines and especially the railway maintenance works. The measurement of track stiffness for maintenance relates to four stiffness problems: low stiffness, variable stiffness, virtual stiffness, and assortative stiffness problems.

- (2)
The standstill measurement of overall track stiffness is time consuming and hard to realize a long-distance and multi-point measurement for whole railway lines. The existing methods for continuous track stiffness measurement have four problems: a. inconsistent measurement concepts. A unified stiffness notion has not been proposed to reflect the track stiffness characteristics completely; b. poor ability for high-accuracy measurement. The measurement accuracy for force, displacement, or acceleration is hard to ensure, especially for high-speed measurement; c. low measurement speed. It is difficult to solve the dilemma between the measurement speed, transducer accuracy, and equipment operation reliability; and d. insufficient data analysis. Much more stiffness information is expected to explore using the advanced analysis technology of the measurement data.

- (1)
A definite stiffness notion should be established to completely reflect the track stiffness characteristics.

- (2)
A theoretical and systematic research should be performed on the quantitative relation between track stiffness and the factors like exciting frequency, running speed, and vehicle axle load, as well as the influences of track stiffness and track geometric irregularities on the vibration response of the vehicle-track-substructure coupled dynamics, respectively.

- (3)
In view of the accuracy requirement for stiffness measurement, the track stiffness measurement can be categorized based on three grades, namely low accuracy (10 kN/mm, substructure disease identification, for heavy haul railways mainly), medium accuracy (1 kN/mm, potential safety hazard checking), and high accuracy (0.1 kN/mm, evaluation of track regularity, for high-speed railways mainly). For example, for continuous measurement vehicle with low measurement accuracy, single-axle vehicle can be used. The axle load should be more than 150 kN to ensure the vertical measurement for subgrade, and one span length (sleeper pitch) along the railway line can be the measurement unit. For the continuous measurement with medium measurement accuracy, it is advised to use double-axle vehicle with axle loads of 20 and 100 kN, the vertical measurement range is limited to the track structure, and the measurement unit ranges from 1 to 4 span lengths. For continuous measurement vehicle with high measurement accuracy, it is advised to use double-axle vehicle with axle loads of 10 and 50 kN, the vertical measurement range is limited to the rail and fasteners, and 4–10 span lengths can be adopted as the measurement unit.

For transition zones (railway–bridge, railway–tunnel, and bridge–tunnel areas), turnouts, and small-radius curve sections, the track stiffness characteristics are more complicated than those of straight lines [2, 49]. Thus, apart from the measurements, the stiffness of special track sections can be monitored.

In recent years, the features of wave propagation in track structures have attracted a wide attention, and the wave theory is applied to the high-frequency vibration of rails [55]. Rail support conditions affect the transfer laws of track vibration waves, and thus continuous track stiffness measurement equipment can be developed based on the wave transfer mechanism.

In addition, the vibrations of track components and vehicle components can be collected for power generation [56, 57, 58]. Different track stiffness values cause different vibration intensities, affecting the collection of electric energy. When the stiffness measurement accuracy is undesirable because of poor noise reduction in vibration displacement and vibration acceleration signals, the vibration energy storage ability or real-time electrical signals (voltage, power, etc.) might be a good index for continuous track stiffness measurement or long-term stiffness monitoring of special sections.

## Notes

### Acknowledgments

This research was supported by the project (51425804) of the National Science Fund for Distinguished Young Scholars of China and the National Natural Science Foundation of China (NSFC) under grants U1234201, U1334203, and 51378439.

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