Designing for Longitudinal Force - AREMA · PDF fileDesign of Steel Bridges for Longitudinal Force Analytical Finite Element model for a single span bridge: Analytical model (SAP90)

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  • AREMA Annual Technical ConferenceStructures Session

    Tuesday, September 19, 2006KICC, Louisville, KY

    Designing for Longitudinal Force

    Design of Steel Bridges for Longitudinal Force

    John F. Unsworth, P.Eng.Manager, Structures Planning & DesignCANADIAN PACIFIC RAILWAYCalgary, Canada

  • Contents of Presentation

    Longitudinal Forces in Steel Bridges

    Development of Current AREMA Chapter 15 Longitudinal Force Provisions

    Design of Steel Bridges for Current AREMA Chapter 15 Longitudinal Forces

    Summary

    Design of Steel Bridges for Longitudinal Force

  • Longitudinal Forces in Steel Bridges

    Design of Steel Bridges for Longitudinal Force

    Longitudinal force due to rolling friction:

    Small at constant train speeds

    Large at variable train speeds due to adhesion between wheels and rails required for acceleration and braking

    New locomotives with adhesion of up to 50% of weight (175% increase over older locomotives with wheel slip)

    Dynamic braking forces large in new locomotives (up to 100% increase over older locomotives)

    Braking forces applied simultaneously throughout train and varied in accordance with car weight

  • t

    Traction

    Braking

    Time History of Longitudinal Force

    LF

    in s

    pan

    = N

    i

    Design of Steel Bridges for Longitudinal Force

  • Analytical model and equations of equilibrium for two span bridge:

    Design of Steel Bridges for Longitudinal Force

    Static state at maximum longitudinal force

    Independent of flexural deformations

    Bar elements (rails horizontally free at ends)

    Horizontal springs, k, for rail/deck/bridge connection (elastic fasteners)

  • Design of Steel Bridges for Longitudinal Force

    Rail boundary conditions:N1(0)=N4(L4)=0

    N1(L1)-LFL1=N2(0)

    N2(L2)-LFL2=N3(0)

    N3(L3)-LFL3=N4(0)

    u1(L1)=u2(0)

    u2(L2)=u3(0)

    u3(L3)=u4(0)

    Span boundary conditions:

    N5(L5)=N6(L6)=0

    u5(0)=u6(0)=0

    Particular boundary conditions:

    Expansion joints at end of bridge, L1=L4=0

    CWR across bridge, L1=L4

    No longitudinal rail restraint (free rails), k2=0

    Rails fixed (direct fixation to deck), k2

    dx

    xduAExN iiii

    )()( =

    Determine ui(x) and

  • Design of Steel Bridges for Longitudinal Force

    Analytical Finite Element model for a single span bridge:

    Analytical model (SAP90) developed at the University of Illinois in conjunction with AAR/TTCI testing in 1996/97:

    Girders modeled with bar & plate elements

    Track (rail/tie/ballast) with frame, plate, spring elements

    Reliable predictions of LF for single span open deck plate girder bridges

    after Report R-905, November 1987, TTCI, AAR

  • Design of Steel Bridges for Longitudinal Force

    Development of Current AREMA Chapter 15 Longitudinal Force Provisions

    AREA 1905: 20% of specified live load

    AREA 1920: Reduced longitudinal forces for ballasted deck and short spans

    AREA 1932: Tractive force of 25% Cooper driving axlesBraking Force of 15% of Cooper train load

    AREA 1968: 15% of Cooper train load x (L/1200)L=length of bridge in feet

  • Design of Steel Bridges for Longitudinal Force

    mid-1990s: Introduction of high adhesion locomotives

    1996: AAR test on 50 DPG shows longitudinal forces 25 times that in AREA

    1997 AREA: Tractive force of 25% Cooper axlesBraking Force of 15% of Cooper train load

    1997-2001: AAR research and testing of FAST and revenue service bridges

    2001 AREMA: New design equations for Tractive and Braking Forces

  • Design of Steel Bridges for Longitudinal Force

    Longitudinal Forces

    0

    100

    200

    300

    400

    500

    600

    0 50 100 150 200 250 300 350 400

    Length, L (ft)

    Longitudin

    al F

    orc

    e (

    kip

    s)

    Max LF 1996 AREAMax LF 1997 AREAMax LF 2001 AREMAAAR Traction Tests (E80)1997 AAR Test (E80)Traction LF 2001 AREMA Braking LF 2001 AREMA

  • Design of Steel Bridges for Longitudinal Force

    TTCI Traction Force Testing 1997-2000:

    from Technology Digest 00-018, Development of Design Guidelines for Longitudinal Forces in Bridges, Otter, Sweeney & Dick, August 2000, TTCI, AAR

  • Design of Steel Bridges for Longitudinal Force

    Observations from Testing of Steel Bridges for Longitudinal Forces due to Traction:

    Large for modern railway freight equipment

    Tractive effort greatest at low locomotive speeds

    Traction forces due to locomotives may affect a smaller length of bridge

  • Participation of rails is relatively small (due to relatively stiff elastic fastenings used in modern bridge deck construction)

    Grade related traction relatively insignificant for modern high adhesion locomotives

    Negligible difference in open deck and ballast deck behavior

    Ability of approach embankments to resist longitudinal forces reduced when bridge and approaches are loaded

    Design of Steel Bridges for Longitudinal Force

  • Design of Steel Bridges for Longitudinal Force

    Distribution between point of LF application and bridge supportsdepends on arrangement, orientation and relative stiffness of;

    Bridge members in the load path

    Bearings (type, fixed, expansion)

    Substructures

  • Longitudinal Braking Force (kips) = (acting 8 ft above top of rail)(approximately 15% of Cooper E80 train loan)

    LLFB

    2.145 +=

    LLFT

    25=

    Design of Steel Bridges for Longitudinal Force

    Longitudinal Traction Force (kips) = (acting 3 ft above top of rail)

    L= Length (feet) of portion of bridge under consideration(AREMA 15.1.3.12 & 15.9.1.3.12)

    Magnitude of Longitudinal Force: (AREMA 15.1.3.12)

    AREMA Longitudinal Force

    0

    100

    200

    300

    400

    500

    600

    0 20 40 60 80 100 120 140 160 180 200 220 240 260 280 300 320 340 360 380 400

    Length, L (ft)

    Long

    itudi

    nal F

    orce

    , LF

    (kip

    s)

    LF Traction LF Braking

  • Design of Steel Bridges for Longitudinal Force

    Magnitude of Longitudinal Force:

    L= Length (feet) of portion of bridge under consideration (loaded length)

    Distribution of Longitudinal Forces: (applied longitudinal force to supporting substructure)

    Superstructure Load Path (AREMA 15.1.3.12)Orientation & geometryRelative stiffness of members

    Design of Steel Bridges for Current AREMA Chapter 15 Longitudinal Forces

  • Design of Steel Bridges for Longitudinal Force

    Bearings and SubstructureTypeOrientation & geometryRelative stiffness of members

  • Span length loaded for braking and traction

    Orientation and relative stiffness of members

    Open and ballasted deck plate girder and truss spans without floor systems:

    Steel Bridge Superstructure

    Design of Steel Bridges for Longitudinal Force

    Longitudinal Force distributed through main girders or trusses

    Girders and trusses adequate to transfer LF to bearings and substructure

  • Open deck and through plate girder and truss spans with floor systems:

    Load path: stringers > lateral system > main girders or trusses to preclude transverse bending of floorbeams

    Girders and trusses adequate to transfer to bearings and substructure

    Design of Steel Bridges for Longitudinal Force

  • Traction Frames to Direct Single Track Longitudinal Loads in Stringers to Open-deck Main Trusses or

    Girders

    Main girder/truss

    Floorbeam

    Stringer

  • Traction Frames to Direct Double Track Longitudinal Loads in Stringers to Open-deck Main

    Trusses or Girders

    StringerFloorbeam

    Mai

    n gi

    rder

    /tru

    ss

  • Frame analysis shows very small web member loads and negligible transverse bending of floorbeams

  • Ballasted deck and through plate girder and truss spans with floor systems:

    Load path: deck > main girders or trussesLocalized traction at transverse floorbeam decks (direct fixation)Deck plate well fastened to closely spaced floorbeams may transmit LF through diaphragm or deep beam actionGirders and trusses adequate to transfer to bearings and substructure

    Design of Steel Bridges for Longitudinal Force

  • Traction Frames to Direct Single Track Longitudinal Loads in Stringers to Ballasted-deck Main Trusses

    or Girders

    LF

    Mai

    n gi

    rder

    Floorbeam

    Diaphragm

    ~ Deck plate ~

  • Entire length loaded for braking and traction Traction and dynamic braking forces distributed to many supports Braking (air-braking) occurs along entire train Continuous track structure across the bridge

    Orientation and relative stiffness of membersSubstructure type, geometry and spacing

    Bearings TypeFixedExpansionElastomeric

    Steel Bridge Substructure

    Design of Steel Bridges for Longitudinal Force

  • Design of Steel Bridges for Longitudinal Force

    Steel towers of trestle bridgesLongitudinal Force affects:

    Longitudinal bracing (affects optimum span lengths)Post dimensions

    8 0 4 0

    4 4 0

    T o w e r 1

    T o w e r 2

    T o w e r 3

    4 0

    1 0 0

    6 0

    1 0

    = f i x e d b e a r in g = e x p a n s i o n b e a r in g

    S p a n 1

    S p a n 7

    6 0

    1 0

    C r o s s S e c t io n T o w e r 3

    E le v a t io n o f B r id g e

    Example from AREMA Longitudinal Force Seminar