dinâmica estrutural ii_pontes_01
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Universidade do Estado do Rio de Janeiro, UERJ
Centro de Tecnologia e Ciências, CTC
Faculdade de Engenharia, FEN
Análise Dinâmica de Tabuleiros Rodoviários Análise no Domínio do Tempo
Efeito do Peso dos VeículosEfeito das Irregularidades da Pista
Prof. José Guilherme Santos da Silva, DSc.Coordenador da Área de Concentração de EstruturasPrograma de Pós-graduação em Engenharia Civil, PGECIV
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ÍNDICE
1. Introdução2. Modelagem da carga móvel
3. Modelagem do sistema veículo-ponte
4. Exemplos: efeito do peso dos veículos5. Conclusões
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1. INTRODUCTION
Number of vehicles on the bridge is an important point in the evaluationof their dynamical actions;
Effect of the interaction of their masses with the bridge deck mass;
Crossing frequency of the moving load which can produce a steady-state response situation;
The moving load is taken as an infinite series of vehicles, regularlyspaced and moving at constant velocity, to allow the observation of thesteady state response of the structure.
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2. INFINITE TRAIN OF VEHICLES
3. MODEL OF THE VEHICLE-BRIDGE SYSTEM
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4. EXAMPLES
4.1. Vehicles Properties
Two classes: 450kN and 120kN;Regularly spaced: l=5.0m;
Frequencies: 3Hz and 20Hz;Damping factor: =0.1.
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The moving load is modelled by an infinite series of equal vehicles, regularly spaced, and running
at constant velocity, . Each vehicle is considered by a two, three or four masses model,respectively, with in plane degrees of freedom (translational and rotational) and one, two or even
three axles. If l is the distance between two successive vehicles and as these cars enter one byone into the bridge deck, it is created a time repeated movement variation governed by the
frequency, f t = /l (traversing frequency), associated with the movement of the vehicles on thebridge. After a certain time period, t1 (crossing period), the first vehicle in the train reaches the farend of the bridge and from this instant, on the total mass of the vehicles on the bridge remains
practically constant. Under these conditions the bridge will soon reach a steady-state responsesituation, which includes repetition of maximum values directly related to the fatigue strength.
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4.2. Simple Supported Beam Deck
Inertia moment: I=3.98m
4
;Young’s modulus: E=3x107kN/m
2;
Distributed mass: m=9200kg/m;Frequency (unloaded deck): 6.3Hz;Frequency (loaded deck: vehicles 120kN and 450kN): 6.6Hz and 7.2Hz;
Damping factor: =0.03;Finite Element Model.
0,12m
2,50m
10,00m
0,30m
0,12m
2,26m
9,20m 0,40m0,40m
...
17
13
L
m1 m2 m10 m11...
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Time Response: displacement.
0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5
t/t1
0.00
0.20
0.40
0.60
0.80
1.00
1.20
v/vest
Displacement: load mobility effectSimple supported beam: L=30mInfinite train of vehicles: V=125km/h e P=450kNSteady-state phase: t/t1 > 0,80
Time Response: bending moment.
0.80
1.00
1.20
Bending moment: load mobility effectSimple supported beam: L=30mInifinite train of vehicles: V=125km/h e P=450kNSetady-state phase: t/t1 > 0,80
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Time Response: reaction force.
0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5
t/t1
0.00
0.20
0.40
0.60
0.80
1.00
1.20
R/Rest
Reaction force: load mobility effectSimple supported beam: L=30mInfinite train of vehicles: V=125km/h e P=450kNSteady-state phase: t/t1 > 0,80
Response Spectra: displacement.
1.08
1.10
1.12
Load mobility effect
Weight of the vehicles: 450kN
Weight of the vehicles: 120kN
Response spectraLoad mobility effectDisplacement
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Response Spectra: bending moment.
0.0 1.0 2.0 3.0
Beta=v/l.f01
1.00
1.02
1.04
1.06
1.08
1.10
1.12
FA=M/Mest
Response spectraLoad mobility effect
Bending moment
Load mobility effect
Weight of the vehicles: 450kN
Weight of the vehicles: 120kN
Response Spectra: reaction force.
1.08
1.10
1.12
Response spectraLoad mobility effectReaction force
Load mobility effect
Weight of the vehicles: 450kN
Weight of the vehicles: 120kN
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4.3. Continuous Beam Deck
Finite Element Model
m1 m34 m35m2 ......
L Le = 0.83LLb = 0.25L Le = 0.83L Lb = 0.25L
1 2 34 2614 36
399 3120
Variations of Beam Fundamental Frequency with Bridge Geometry
MiddleSpan
End Span OverhangsSectionSpacing
Unloaded Deck Loaded Deck
L(m) Le(m) Lb(m) Ls(m)Lowest Mode
Frequency (Hz)Lowest Mode
Frequency (Hz)
24.00 20.00 6.00 2.00 9.12 9.22
30.00 25.00 7.50 2.50 7.43 7.78
36.00 30.00 9.00 3.00 5.20 5.86
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Maximum Displacements: FA= v/vest.
BRIDGE: Continuous beams deck with overhangs. Spans 24m, 30m e 36m.CRITICAL VELOCITY (km/h): 130, 140 e 125, respectively.SECTIONS: S1 and S20.
Middle SpanL(m)
Maximum amplification factor: FA = v/vest
Section S1 Section S20
24.0m 2.68 1.54
30.0m 2.42 1.77
36.0m 1.98 1.54
Maximum Bending Moments: FA= M/Mest.
BRIDGE: Continuous beams deck with overhangs. Spans 24m, 30m e 36m.CRITICAL VELOCITY (km/h): 130, 140 e 125, respectively.SECTIONS: S4, S14 and S20.
Middle SpanL(m)
Maximum amplification factor: FA = M/MestSection S4 Section S14 Section S20
24.0m 1.15 1.29 1.42
30.0m 1.15 1.33 1.62
36.0m 1.12 1.30 1.44
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Maximum Reaction Forces: FA= R/Rest.
BRIDGE: Continuous beams deck with overhangs. Spans 24m, 30m e 36m.
CRITICAL VELOCITY (km/h): 130, 140 e 125, respectively.SECTIONS: S4 and S14.
Middle SpanL(m)
Maximum amplification factor: FA = R/Rest
Section S4 Section S14
24.0m 1.23 1.2130.0m 1.25 1.20
36.0m 1.22 1.19
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5. CONCLUSIONS
Infinite Train of Vehicles suitable solution to the computation ofmoving load response values for highwaybridge decks where the steady-stateresponse can be a major concern as in the
case of the bridge fatigue behaviour;
Response Values dynamic amplification factors (DAF), due to theload mobility, more than twice of those obtained
with only one moving vehicle;Irregular Pavement Surface the amplifications can be still much
larger than those due to the load
mobility;The Redundant Beam Problem deserves more attention to widely
be verified the DAF, when the staticvalues obtained according todesign codes are considered.