Cathal's PhD 22.03.2010_ver1.06_2003
-
Upload
cathalbowe -
Category
Documents
-
view
215 -
download
0
Transcript of Cathal's PhD 22.03.2010_ver1.06_2003
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
1/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
2/34
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
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
3/34
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)
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
4/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
5/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
6/34
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
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
7/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
8/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
9/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
10/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
11/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
12/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
13/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
14/34
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
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
15/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
16/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
17/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
18/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
19/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
20/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
21/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
22/34
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
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
23/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
24/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
25/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
26/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
27/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
28/34
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
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
29/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
30/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
31/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
32/34
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
33/34
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)
-
8/8/2019 Cathal's PhD 22.03.2010_ver1.06_2003
34/34
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