Cathal's PhD 22.03.2010_ver1.06_2003

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    1. Introduction

    2. Literature review

    3. Wheel force represented as time varying nodal forces

    4. Sprung mass represented by time varying stiffnessmatrices

    5. Unsprung mass represented by time varying mass,damping, and stiffness matrices within a modal and

    finite element framework6. Wheel rail systems on irregularities

    7. Conclusions & recommendations

    8. Appendices

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    ANSYS Strengths Element Library

    Equation Solvers

    Post-processor tool

    APDL Code

    ANSYS Limitations No force between nodes

    Contact elements cant model

    irregularities or braking forces

    3D contacts need surface

    Dynamic effects of trains traversing railway bridges

    Centre span of Boyne Viaduct Railway bridgeCentre span of Boyne Viaduct Railway bridge

    Modelled using ANSYS finite element program

    Development own models

    Wheels modelled as moving forces

    Wheels modelled as sprung masses

    Wheels modelled as unsprung mass (modal & finite element)

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    Moti tions Moving Force odel s it le for long s n ridges

    Ti e of exec tionof odel re gener ll ver s ort

    ANSYS c nnot l force et eennodes of single ele ent Developments

    Simple andExact numericalmodels for single moving force

    Expandmodels for several moving forces

    es lts alidated singnumericalmodels from t e literature

    Simulate Dand D oyne ridge to several moving forces

    esonance canoccur due to closely spacedve icle loadings

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    Motivations ANSYS contact elements are unable tomodel irregularities

    Develop elements t at canmodel smoot rail and irregularities

    Developments ertical springunder eel i.e. Hertzian spring

    ongitudinal spring element capture braking effects

    ateral spring elements stabilize Dmodels

    esults alidatemodel results it results from t e literature as ell asANSYS contact elements

    Train eels as sprungmasses traversing oyne iaduct

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    Motivations Toaddress t e issue of omitting convective acceleration

    T e ability to compare it sprungmass models

    Developments Modalmet od for movingunsprungmass

    Finite element model for movingunsprungmass

    Expand to simulate several movingunsprungmasses

    esults alidatemodel results it results from t e literature

    AddressingAkin Mofids incorrectmodel results

    Sensitivityof internal forces

    Train eels as unsprungmasses traversing oyne iaduct

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    Motivations Simulate realistic eel-rail conditions

    ANSYS contact elements cannot model irregularities

    Developments Modify sprungmass model to simulate rail irregularities

    Modifyunsprungmassmodels to simulate rail irregularities

    esults

    alidatemodel results it results from t e literature Train traversing oyne iaduct it irregularities along rails

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    ANSYS limitation for modelling moving forces

    Simple or Exact numerical models can now be used

    ANSYS contacts cannot model irregularities

    Development of WRC element WRC element more accurate than ANSYS contact elements

    WRC element can model rail irregularities, braking, lateral

    stability, wheel separation as well as rigid rails

    Developed unsprung models Address the issue of Akin & Mofids results been inaccurate

    Comparable with sprung mass model (under certain circumstances)

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    Contains many fundamental equations used throughout

    the thesis as well as bridge and train properties

    Areas of interested include:

    Convention Elastic beam theory

    inite element method applied to equation of motion of a beam

    Natural frequencies and modal shapes for a beam

    Beam Damping

    Newmark time integration scheme

    Bridge dimensions, material and section properties

    Railway vehicle dynamics