Fatigue Safety in Concrete Bridges
Fatigue Safety in Concrete Bridges
Mário Pimentel
Joaquim Figueiras
Eugen Brühwiler
Index
1. Introduction
2. Mathematical model
3. Validation
4. Parametric study
5. Conclusions
1. Introduction
• Modern railway systems sustainability demands for larger traffic volumes, higher
traffic loads and higher trains speeds;
• These issues are already reflected in recent studies of the ERRI regarding the
formulation of a new load model, the LM2000;
• For the design of new railway bridges in European international lines, the Eurocode 1
already recommends the adoption of a classification factor of a=1.33 for the LM71 and
SW/0 load models;
• The existing bridge stock also needs to be checked against these demanding loading
conditions and decisions must be taken concerning their upgrade to withstand the new
loading scenario (axle loads up to 30ton);
• However, the economical impact of strengthening measures is much larger than the
additional cost due to a conservative design;
• It can be then understood that, in the case of existing bridges, besides new traffic
models, also the development of methodologies enabling the exploitation of
hidden reserves is mandatory.
1. Introduction
• In a scenario of increasing maximum axle loads the fatigue life of short span
reinforced concrete bridges is drastically reduced:
500 25
Fatigue life, FL (years)
10%
33t traffic mix
300 15
200 10
100 5
0 0
4 5 6 7 8 9 10 11 4 5 6 7 8 9 10 11
Span (m) Span (m)
Fatigue life of simply supported railway RC Ratio between the fatigue lives with the
short span bridges under different traffic 25ton and 33ton traffic scenarios
scenarios
1. Introduction
• Fatigue life is very sensitive to some underlying assumptions usually adopted in the
fatigue verification procedure:
250
x= Dss,real/Dss,calc 100
50
0
0.85 0.9 0.95 1 1.05 1.1 1.15
Precision factor, x
• Looking only to the “action side” of the problem, several aspects contribute to the
differences between the real and calculated stress amplitude spectra:
1. Continuous rails over the supports may provide significant partial fixity;
2. Load distribution through the rail/sleepers/ballast is relevant when analysing
short span bridges;
3. Real axle loads and axle spacing can provide significantly different stress
amplitude spectra than obtained with the load models;
4. Dynamic amplification of traffic effects can be different from the code DAF’s.
2. Mathematical model
• Bridge
2 w x, t w x, t
Lw x, t m x Cx pt vl*tl
Pl+1(t)
t 2
t dx,l
dy,l vl+1*tl+1
P t x vx tl y v y tl
Nl dx,l+1
pt l rect dx dy,l+1
l 1 d x ,l d y ,l
R d x ,l
rect
dy
,l
Nl
Pb,k t v t P t
med
k l l
l 1
P t
6.0E-04 1 Mode + Correct.
N mod e
Nl
w (m)
x, t A ,k x Yk t b,k 2 x, v t P t w(t)
4.0E-04 FEM - DIANA
k
l l
2.0E-04
k 1 l 1
0.0E+00
0 0.2 0.4 0.6 0.8 1
-2.0E-04
M (kN.m)
1 Mode + Correct.
600 FEM - DIANA
M(t)
A ,k x - contribution to x, t due to a unit
400
200
displacement in the kth mode 0
-200 0 0.2 0.4 0.6 0.8 1
250
-400
V(t)
x, v tl - static influence field (or influence
t (s)
200 Static
1 Mode
V (kN)
100 3 Modes + Correct.
FEM - DIANA
50
0
0 0.2 0.4 0.6 0.8 1
-50
t (s)
2. Mathematical model
• Vehicles – Freight wagons
d T T V WD
0
dt uv ,i uv ,i uv ,i uv ,i
2. Mathematical model
• Track
2. Mathematical model
Bridge equations of motion (NmodexNmode) Vehicle equations of motion (Nv,dofxNv,dof)
C Y
Mb Y K Y P t v Cv u v K v u v Pv t
Mv u
b b b
Can be expressed in terms of the system unknowns Yk, uv,l and its derivates
2. Mathematical model
• Computational implementation
Currently the model is implemented in Matlab;
The coupled system of differential equations is solved with the fourth order
Runge-Kutta method and an automatic adaptative time stepping scheme;
An event driven integration scheme is adopted to deal with situations where loss
of contact between the wheels and the bridge is detected. If contact is lost, the
integration is stopped, the contact parameters adjusted, the integration
restarted and vice-versa (automatic procedure).
The model needs the input of the bridge modal parameters and influence fields
(or influence lines). In simple cases these can be analytically derived. They can
also be most generally obtained from detailed (and eventually updated) finite
element models.
3. Validation
• Simple bridge travelled by a two axle system with a large wheel flat in the
rear axle
3 modes included in the response;
Rounded wheel flat modelled as a analytical sinusoidal function;
Axles excited before entering the bridge by imposing initial
conditions in the vehicle degrees of freedom;
Bridge, vehicle and wheel flat properties according to Fryba (1999)
The wheel flat “hits” the deck
The wheel flat in approximately at midspan
The first axle the rear axle “hits”
enters the bridge the deck
Proposed model
Fryba (1999)
Midspan displacement
mb=8.3t/m mb=7.0t/m
20t axle loads: mc=38t, mw=1t, Ic=7mc
x=2.2% x=2.55% 30t axle loads: mc=58t, mw=1t, Ic=7mc
2.2Hz
2.2
2.0Hz
2
1.8Hz kv = 80MN/m; 160MN/m.
Linearized spring stiffness: 1.8
1.6
fv1 = 1.8Hz-2.0Hz-2.2Hz 1.4
1.2
Body bounce frequency 1
100 150 200 250 300
Max. Axle Load [kN]
Body bounce frequencies for loaded
wagons
• Dynamic amplification
Max dyn
DAF 1
Max sta
1.4 1.4
20t - Irreg. Type 1 20t - Irreg. Type 3
1.3 30t 1.3 30t
Amplification (1 + )
Amplification (1 + )
1.4 1.4
20t - Irreg. Type 1 20t - Irreg. Type 3
30t 30t EC1 fatigue DAF
1.3 1.3
Amplification (1 + )
Amplification (1 + )
1.4
kt=160MN/m - Irreg.Type 4
EC1 fatigue DAF
1.3 •5m span bridge;
Amplification (1 + )
Max
1.2 • xv=10%;
1.1 Mean • fv1=2Hz;
1 • 30t axles
Min
0.9
40 60 80 100 120 140
Speed [km/h]
5. Conclusions
• The proposed algorithm proved highly efficient, requiring very low calculation times;
• The model is appropriate for performing statistical analyses and parametric studies
requiring a large number of calculations as well as for a detailed 3D dynamic analysis
of a specific bridge;
• The undertaken parametric study, although of limited extension, revealed that the
EC1 DAF for fatigue verifications might be conservative and revealed a trend for the
DAF to decrease with increasing axle loads;
END