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• Acceptable relative displacement between rail/deck and deck/span to pre-
clude damage to deck and/or fasteners. Occurs due to excessive longi-
tudinal movements (lower longitudinal stiffness) at either rail-to-deck or
deck-to-superstructure.
• Avoidance of bearing component damage.
4.4.3.1
Safe Rail Separation Criteria
If the steel bridge is modeled as a series of spans with a distributed longitudinal
force due to thermal expansion of rails transferred through an elastic deck system,
the magnitude of the axial force in the CWR, N(x) ,is
EA r d x(x)
d x − αΔ t c ,
N(x) =
(4.41)
where EA r is the axial stiffness of the CWR; A r is the cross-sectional area of the CWR
(about 13 in. 2 on typical heavy freight railroads); α is the coefficient of thermal expan-
sion of the CWR and is
10 6 / F;
Δ t c is the cold weather rail temperature
change (with respect to neutral temperature).
Assuming zero displacement far from the rail break, x(
6.5
×
)
=
0, and zero force at
the rail break, N( 0 )
=
0, Equations 4.39 and 4.40 yield
= −αΔ
t c
e −λ x ,
x(x)
(4.42)
λ
e −λ x ) ,
N(x)
=−
EA r αΔ
t c ( 1
(4.43)
λ = k 1 / EA r , k 1 is the longitudinal stiffness associated with a high strain rate
event such as a rail breaking. It is generally about 1/2 of normal strain rate event (such
as rail thermal expansion and contraction) stiffness.
The separation of the CWR at fracture (assumed to occur over the expansion
bearings) is
where
t c 1
,
1
λ t
Δ
x s =−αΔ
λ d +
(4.44)
λ d = k d / EA,
where
k t
EA ,
λ t =
k d is the equivalent high strain rate event horizontal spring constant for the bridge
deck, and k t is the equivalent high strain rate event horizontal spring constant for
the track ap proach. Figure 4.21 outlines the relationship of Equation 4.44, where
F k =
+ (k d /k t ) .
1
From Association of American Railrods, Transportation Technology Center, Inc. (AAR/TTCI) testing
related to draft report of “Thermal Forces on Open Deck Steel Bridges,” January, 2009.
 
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