tested to assess the range of variations in the in situ birefrin-
gence (B0). The in situ birefringence was assessed with four
measurements along the 4 ft rail length, one measurement per
foot of rail. The results are presented in Figure 6, which shows
a box enclosing the four measurements made along each rail
section, with the standard deviation for the four measurements
shown as error bars. The data illustrate the variation in the in
situ birefringence between different rail specimens, with the
lower-weight rail specimen generally showing increased in
situ birefringence compared to higher-weight rails. It was also
found that there was variation in the birefringence along the
length of the rail specimens, and this variation was generally
more considerable for the lower-weight rails.
The third testing phase was conducted to assess the vari-
ations in the stress-acoustic constant (m1) on the different
rail materials after they were cut to 1 ft lengths and the ends
of each specimen were machined to be perfectly parallel.
Producing parallel ends of the specimen allowed for end
loading of the specimen in bearing using a compression
machine with the test setup shown in Figure 2. Compression
loading was applied on each specimen at the incremental load
of 50 kips up to about 50% of the yield strength of the section,
and the ultrasonic measurements were made through the rail
web at each loading step. The results of the stress-birefringence
behavior of all the rail types are shown in Figure 7. As shown
in the figure, each rail type indicates a similar acoustoelastic
constant (m1) as illustrated by a comparable rate of change in
the birefringence with the change of stress, as seen in Table 1.
The only noticeable difference between the rail types is the in
situ birefringence (B0), which was found to be very comparable
to the values obtained in the in situ birefringence study of the
different rails explained earlier and shown in Figure 6.
Conclusion
This paper presented experimental work to investigate the
ability to evaluate longitudinal thermal stresses in rails using
the acoustic birefringence technique. The research objec-
tives were establishing the stress-birefringence relationship in
common rail materials and then assessing the potential varia-
tion of fundamental acoustoelastic properties between differ-
ent weight rail sections. Three different phases of laboratory
work were conducted to explore the applicability of the tech-
nique and to study the effect of different rail materials on the
key acoustoelastic properties of B0, the in situ birefringence,
and m1 that characterize the birefringence-stress relationship.
Two rail specimens machined out of 136RE and 141RE were
loaded under tensile and compressive stresses using a 220 kip
hydraulic machine. The birefringence measurement obtained
during the loading of this phase showed a very linear depen-
dency on the stresses applied, with correlation factors of 99%
for the stress-birefringence relationship for both specimens.
The second and third parts of the testing were dedicated to
studying the variations in rail materials on the technique
parameters, which are the in situ birefringence (B0) and the
0.40%
0.35%
0.30%
0.25%
0.20%
0.15%
0.10%
0.05%
0.00%
115RE 119RE 136RE (A) 136RE (B) 141RE
Rail type
Figure 6. In situ birefringence measurements on four different rail
specimens.
T A B L E 1
Stress-birefringence parameters for different 1 ft rails
Rail type
Linear regression data for stress-birefringence
Correlation
coefficient Acoustoelastic constant In situ
birefringence
R2 m1 (1/MPa [1/ksi]) B0
115RE 0.997 8.96 × 10–6 (6.18 × 10–5) 2.25 × 10–3
119RE 0.998 8.44 × 10–6 (5.82 × 10–5) 2.59 × 10–3
136RE (A) 0.997 9.44 × 10–6 (6.51 × 10–5) 1.50 × 10–3
136RE (B) 0.998 9.27 × 10–6 (6.39 × 10–5) 1.01 × 10–3
141RE 0.996 8.96 × 10–6 (6.17 × 10–5) 1.74 × 10–3
Average 9.01 × 10–6 (6.22 × 10–5) 1.82 × 10–3
Standard deviation 3.83 × 10–7 (2.64 × 10–6) 6.21 × 10-4
45 40 30 35 20 25 10 15 0
0 34 69 103 138 172 207 241 276 310
5
Stress (ksi)
Stress (MPa)
0.00%
0.10%
0.20%
0.30%
0.40%
0.50%
0.60%
115RE
Linear (115RE)
119RE
Linear (119RE)
136RE (A)
Linear (136RE [A])
136RE (B)
Linear (136RE [B])
141RE
Linear (141RE)
Figure 7. Plot showing the relationship between stress and
birefringence for five different sections of rail.
J A N U A R Y 2 0 2 4 M A T E R I A L S E V A L U A T I O N 85
2401 ME January.indd 85 12/20/23 8:01 AM
Birefringence
(B%)
Birefringence
(B%)
acoustic-stress constant (m1). Five different rails were used
in the second and third testing sets: 115RE rail, 119RE rail, two
different 136RE rails, and 141RE rails. The rails used for these
phases were full-size rail sections in their original surface
conditions to reflect the actual behavior of rails. Testing indi-
cated variation in the in situ birefringence between different
rail specimens, with the lower-weight rail specimen generally
showing increased birefringence compared to higher-weight
rails. These values ranged from a low of 0.67 × 10–3 to a high
of 3.61 × 10–3. The testing in the third phase showed a similar
acoustoelastic constant (m1) by experiencing a comparable
rate of change in the birefringence with the change of stress.
These values ranged from 8.44 × 10–6/MPa (5.82 × 10–5/ksi) to
9.44 × 10–6/MPa (6.51 × 10–5/ksi).
The key findings of this research were that the
birefringence-based approach to USM shows tremendous
potential as a tool for stress measurement in rails. However,
variations exist in the in situ, stress-free birefringence values.
The effect of these variations will greatly reduce the accuracy
of the USM stress measurement unless the in situ birefrin-
gence can be characterized. Approaches to determining this
value in situ through multiple measurements captured at dif-
ferent times of the year, such that the tensile and compressive
stresses are measured, is a current research topic, which will
be presented in future publications.
ACKNOWLEDGMENTS
The authors of this paper acknowledge the support from MxV Rail through
the AAR University Program Grand Challenge 2020 under the Agreement
20-0701-007536.
REFERENCES
Alers, G. A., and A. Manzanares. 1990. “Use of Surface Skimming SH
Waves to Measure Thermal and Residual Stresses in Installed Railroad
Tracks.” In Review of Progress in Quantitative Nondestructive Evaluation,
ed. D. O. Thompson and D. E. Chimenti, 1757–1764. Springer US. https://
doi.org/10.1007/978-1-4684-5772-8_226.
Béliveau, J. G. 1997. “Resonant frequencies of lateral vibrations of rail in
compression.” Canadian Society for Civil Engineering 4:389–98.
Burkhardt, G. L., and H. Kwun. 1988. “Application of the Nonlinear
Harmonics Method to Continuous Measurement of Stress in Railroad
Rail.” In Review of Progress in Quantitative Nondestructive Evaluation:
Volume 7B, ed. D. O. Thompson and D. E. Chimenti, 1413–1420. Springer
US. https://doi.org/10.1007/978-1-4613-0979-6_64.
Enshaeian, A., and P. Rizzo. 2021. “Stability of continuous welded rails:
A state-of-the-art review of structural modeling and nondestructive
evaluation.” Proceedings of the Institution of Mechanical Engineers.
Part F, Journal of Rail and Rapid Transit 235 (10): 1291–311. https://doi.
org/10.1177/0954409720986661.
Gokhale, S., and S. Hurlebaus. 2008. “Monitoring of the stress free
temperature in rails using the acoustoelastic effect.” AIP Conference
Proceedings 975 (1). https://doi.org/10.1063/1.2902594.
Huang, C.-L., Y. Wu, X. He, M. Dersch, X. Zhu, and J. S. Popovics. 2023.
“A review of non-destructive evaluation techniques for axial thermal stress
and neutral temperature measurement in rail: Physical phenomena and
performance assessment.” NDT &E International 137:102832. https://doi.
org/10.1016/j.ndteint.2023.102832.
Hurlebaus, S. 2011. Determination of longitudinal stress in rails. Safety
IDEA Project 15. Transportation Research Board of the National Acade-
mies. https://onlinepubs.trb.org/onlinepubs/idea/finalreports/safety/
s15report.pdf.
Johnson, E. 2004. “Measurement of forces and neutral temperatures in
railway rails an introductory study.” SP Report. Swedish National Testing
and Research Institute. http://urn.kb.se/resolve?urn=urn:nbn:se:ri:
diva-4627.
Kelleher, J., M. B. Prime, D. Buttle, P. M. Mummery, P. J. Webster, J.
Shackleton, and P. J. Withers. 2003. “The Measurement of Residual Stress
in Railway Rails by Diffraction and other Methods.” Journal of Neutron
Research 11 (4): 187–93. https://doi.org/10.1080/10238160410001726602.
Kish, A., and G. Samavedam. 1987. Longitudinal force measurement in
continuous welded rail from beam-column deflection response. AREA
Bulletin 712.
Kish, A., G. Samavedam, and D. Y. Jeong. 1982. “Analysis of thermal
buckling tests on US railroads.” Technical Report. US Department of Trans-
portation. Federal Railroad Administration.
Kish, A., G. Samavedam, and L. Al-Nazer. 2013. “Track buckling preven-
tion: theory, safety concepts, and applications.” Technical Report.
US Department of Transportation. Federal Railroad Administration.
https://railroads.dot.gov/elibrary/track-buckling-prevention-theory
-safety-concepts-and-applications
Kish, A., S. Kalay, A. Hazell, J. Schoengart, and G. Samavedam. 1993. “Rail
longitudinal force measurement evaluation studies using the track loading
vehicle.” American Railway Engineering Association Bulletin 742:315–42.
Kjell, G., and E. Johnson. 2009. “Measuring axial forces in rail by forced
vibrations: Experiences from a full-scale laboratory experiment.” Proceed-
ings of the Institution of Mechanical Engineers. Part F, Journal of Rail and
Rapid Transit 223 (3): 241–54. https://doi.org/10.1243/09544097JRRT210.
Knopf, K., D. C. Rizos, Y. Qian, and M. Sutton. 2021. “A non-contacting
system for rail neutral temperature and stress measurements: Concept
development.” Structural Health Monitoring 20 (1): 84–100. https://doi.
org/10.1177/1475921720923116.
Kwun, H., G. L. Burkhardt, and M. E. Smith. 1990. “Measurement of Longi-
tudinal Stress in Railroad Rail Under Field Conditions Using Nonlinear
Harmonics.” In Review of Progress in Quantitative Nondestructive Evalu-
ation, ed. D. O. Thompson and D. E. Chimenti, 1895–1902. Springer US
https://doi.org/10.1007/978-1-4684-5772-8_243.
Liu, G., H. Liu, A. Wei, J. Xiao, P. Wang, and S. Li. 2018. “A new device for
stress monitoring in continuously welded rails using bi-directional strain
method.” Journal of Modern Transportation 26 (3): 179–88. https://doi.
org/10.1007/s40534-018-0164-z.
Liu, X., M. R. Saat, and C. P. L. Barkan. 2012. “Analysis of causes of major
train derailment and their effect on accident rates.” Transportation
Research Record: Journal of the Transportation Research Board 2289 (1):
154–63. https://doi.org/10.3141/2289-20.
Lonsdale, C. P., and M. Engineer. 1999. “Thermite rail welding: History,
process developments, current practices and outlook for the 21st century.”
AREMA 1999 Annual Conference, Chicago, IL.
Miri, A., M. Dhanasekar, D. Thambiratnam, B. Weston, and T. H. T.
Chan. 2021. “Analysis of buckling failure in continuously welded railway
tracks.” Engineering Failure Analysis 119:104989. https://doi.org/10.1016/j.
engfailanal.2020.104989.
Nasrollahi, A., and P. Rizzo. 2019. “Numerical analysis and experimental
validation of an nondestructive evaluation method to measure stress
in rails.” ASME J Nondestructive Evaluation 2 (3): 031002 https://doi.
org/10.1115/1.4043949.
Okada, K. 1980. “Stress-acoustic relations for stress measurement by
ultrasonic technique.” Journal of the Acoustical Society of Japan (E) 1 (3):
193–200. https://doi.org/10.1250/ast.1.193.
Phillips, R., F. Lanza di Scalea, C. Nucera, M. Fateh, and J. Choros. 2014.
“Field testing of prototype systems for the non-destructive measurement
of the neutral temperature of railroad tracks.” Proceedings of the 2014 Joint
Rail Conference. Colorado Springs, CO. 2–4 April. https://doi.org/10.1115/
JRC2014-3735.
Posgay, G., and P. Molnár, P. 2011. “SFT measurement of CWR by the
means of MBN.” 28th Danubia Adria Symposium on Advances in
Experimental Mechanics. 28 September–1 October. Siófok, Hungary.
ME
|
RAILROADS
86
M A T E R I A L S E V A L U A T I O N J A N U A R Y 2 0 2 4
2401 ME January.indd 86 12/20/23 8:01 AM
Previous Page Next Page