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Personal experiences
at the boundary of
physics and mathematics
E. Jurjen Kranenborg,
ABB Corporate Research,
Västerås, Sweden
Career Path
 Childhood Hobbies
 Education at Twente University:
o Start of Computer Science, Start of Applied Mathematics
o M.Sc. In Applied Maths., Fluid Dynamics, Grid generation
 Ph.D at Utrecht University, Physics & Astronomy
o Density driven Convection (“Double-Diffusive Convection”)
 PostDoc, Free University of Amsterdam (Earth Sciences)
 Research/Consultancy at Delft Hydraulics
 Research at Philips Research (Software Architectures)
 Currently: ABB Corp. Research (Thermal modeling of Power
Transformers using CFD), Västerås, Sweden
Childhood Hobbies
Astronomy …
… Analog Electronics
16/32-bit Processor
Architecture …
M.Sc. In Applied Mathematics
 Topic: “Control Functions for Numerical Orthogonal Grid
generation in Curved Geometries”
Final grid in
physical domain
Computational grid
Main Part
Ph.D. Research
(1991-1996)
Utrecht University,
Physics & Astronomy
Promotores:
Prof. W.P.M. de Ruijter,
Prof. H.A. Dijkstra
Oceanic layered structures near polar ice
Melting Icebergs ...
… Lateral mixing
of meltwater
Influence of layers
on iceberg melting ...
Layer Development
Heating up of left sidewall at t > 0.
Shown: Perturbation of initial stable salt gradient.
Layer thickness h scales with a.DT / b.fS
Layer properties, Problem parameters
Ra (Rayleigh) = measure of thermal & saline forcing intensity
R (Buoyancy Ratio) = b.DS / a.DT
Ph.D. Research Issues
 Flow dynamics & pattern selection
o Video suggests: transitions between steady states!
o Continuation and stability analysis to map out
solution behaviour in parameter space
 Physical mechanisms?
o Layer merging
o Layer self-propagation
 Scaling up towards oceanographic conditions:
o determination of effective diffusivities
Patterns & Pattern selection: “Attractor Analysis”
 Flow Model as a Dynamical System
o Main steady states?
o Stability of steady states?
o Transitions between steady states?
 Result: Qualitative picture of dynamics as a
function of combined thermal/saline forcing
(Ra) and buoyancy ratio (R)
 Model: Sidewall heating of a stable salinity
gradient, using Ra as bifurcation parameter, R
fixed at R = 3
T=0
S=0
T=1
S=1
AGU Geophysical Monograph 94, 89–96, 1995,
Phys. Fluids 7(3), 680–682, 1995,
Int. J. Heat Mass Transfer 39, 2699–2710, 1996
R=3
S.S. patterns, function of buoy. forcing
A: weak forcing regime
S.S. patterns, function of buoy. forcing
B: strong forcing regime
Heat, salt transport
Heat
(Nu)
Salt
(Sh)
Transitions between flow patterns
Interface migration
Perturbation
causing this ...
Unstable states may be physically relevant!
Layer merging
Int. J. Heat Mass Transfer 41, 2743–2756, 1998
Self-propagation of layers
Int. J. Heat Mass Transfer 41, 2113–2124, 1998
Propagation after forcing stopped …
Kinetic energy increase ...
... does not happen if
initial vertical temperature
gradient is absent
Convection near an ice plate geometry
Int. J. Heat Mass Transfer 41, 1873–1884, 1998.
Global transport: effective diffusivities
 Vertical salt fluxes determined for several simulations:
o Ra = [5*104 - 1*106]
o R = [2.5 - 10]
 Results satisfy a published Flux law for vertical salt
transport validated by laboratory experiments
 After analysis of our case: vertical salt diffusivity takes
extremely simple form:
o KS = cS * Ra1/3 (dim. less, cS = 1.15*10-3 from simulations)
o independent of diffusive interface stability
 KS in fair agreement with oceanographic measurements
o Ra is much larger ( O(109), i.e. 104 times)
o Fails only for diffusive interfaces with very low stability
Time-Dependent Nonlinear Convection (Advances in Fluid Mechanics), 1998
Final Part
Recent employment activities
PostDoc at Free University of Amsterdam
 Domain: Sedimentary Geology
 Context: Climate reconstruction from sediment
analysis of calcium carbonate
 Project: Model Implementation of CaCO3
Dissolution due to Organic Carbon Degradation
Tectonophysics, 320, 347–374, 2000
Research/Consultancy at Delft Hydraulics
 Project leader: drill slib deposition in the Scheldt
Estuary;
o numerical modeling and visualisation of hydrodynamics + slib
transport,
 Hong Kong power plant water inlet: water quality
scenario study,
 Project leader: software module for nutrient
regeneration due to organic carbon degradation in
North Sea sediments,
 Feasibility study for fresh water retrieval, Indonesia;
o data retrieval & checking
o analytical modeling of lake desalination.
Research at Philips Research the Netherlands
 2000 - 2002: Cluster Domain Modelling,
 2003 - 2004: Cluster Internet Connected
Consumer Systems,
o Gatewayed Services Architecture for internet-
enabled consumer electronics devices (project
2003),
o Home Networking Security (project 2004).
… [ Experiment ] make your own private
layered structure [ Experiment ] …
 Ocean Model: Cup of HOT coffee
 Ice-edge model: Use a Transparent, Glass Cup
 Add Salt Stratification: GENTLY pour some coffee milk
 Wait for a few minutes and …
 Your private oceanic staircase is ready for consumption !
The End
WEB publications:
 Ph.D. work: www.kranenborg.org/jurjen
 (Analog) electronics: www.kranenborg.org/ee

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Presentation_Jurjen_ABB

  • 1. Personal experiences at the boundary of physics and mathematics E. Jurjen Kranenborg, ABB Corporate Research, Västerås, Sweden
  • 2. Career Path  Childhood Hobbies  Education at Twente University: o Start of Computer Science, Start of Applied Mathematics o M.Sc. In Applied Maths., Fluid Dynamics, Grid generation  Ph.D at Utrecht University, Physics & Astronomy o Density driven Convection (“Double-Diffusive Convection”)  PostDoc, Free University of Amsterdam (Earth Sciences)  Research/Consultancy at Delft Hydraulics  Research at Philips Research (Software Architectures)  Currently: ABB Corp. Research (Thermal modeling of Power Transformers using CFD), Västerås, Sweden
  • 3. Childhood Hobbies Astronomy … … Analog Electronics 16/32-bit Processor Architecture …
  • 4. M.Sc. In Applied Mathematics  Topic: “Control Functions for Numerical Orthogonal Grid generation in Curved Geometries” Final grid in physical domain Computational grid
  • 5. Main Part Ph.D. Research (1991-1996) Utrecht University, Physics & Astronomy Promotores: Prof. W.P.M. de Ruijter, Prof. H.A. Dijkstra
  • 6. Oceanic layered structures near polar ice
  • 7. Melting Icebergs ... … Lateral mixing of meltwater Influence of layers on iceberg melting ...
  • 8. Layer Development Heating up of left sidewall at t > 0. Shown: Perturbation of initial stable salt gradient. Layer thickness h scales with a.DT / b.fS
  • 9.
  • 10. Layer properties, Problem parameters Ra (Rayleigh) = measure of thermal & saline forcing intensity R (Buoyancy Ratio) = b.DS / a.DT
  • 11. Ph.D. Research Issues  Flow dynamics & pattern selection o Video suggests: transitions between steady states! o Continuation and stability analysis to map out solution behaviour in parameter space  Physical mechanisms? o Layer merging o Layer self-propagation  Scaling up towards oceanographic conditions: o determination of effective diffusivities
  • 12. Patterns & Pattern selection: “Attractor Analysis”  Flow Model as a Dynamical System o Main steady states? o Stability of steady states? o Transitions between steady states?  Result: Qualitative picture of dynamics as a function of combined thermal/saline forcing (Ra) and buoyancy ratio (R)  Model: Sidewall heating of a stable salinity gradient, using Ra as bifurcation parameter, R fixed at R = 3 T=0 S=0 T=1 S=1 AGU Geophysical Monograph 94, 89–96, 1995, Phys. Fluids 7(3), 680–682, 1995, Int. J. Heat Mass Transfer 39, 2699–2710, 1996 R=3
  • 13. S.S. patterns, function of buoy. forcing A: weak forcing regime
  • 14. S.S. patterns, function of buoy. forcing B: strong forcing regime
  • 16. Transitions between flow patterns Interface migration Perturbation causing this ... Unstable states may be physically relevant!
  • 17. Layer merging Int. J. Heat Mass Transfer 41, 2743–2756, 1998
  • 18. Self-propagation of layers Int. J. Heat Mass Transfer 41, 2113–2124, 1998 Propagation after forcing stopped … Kinetic energy increase ... ... does not happen if initial vertical temperature gradient is absent
  • 19. Convection near an ice plate geometry Int. J. Heat Mass Transfer 41, 1873–1884, 1998.
  • 20. Global transport: effective diffusivities  Vertical salt fluxes determined for several simulations: o Ra = [5*104 - 1*106] o R = [2.5 - 10]  Results satisfy a published Flux law for vertical salt transport validated by laboratory experiments  After analysis of our case: vertical salt diffusivity takes extremely simple form: o KS = cS * Ra1/3 (dim. less, cS = 1.15*10-3 from simulations) o independent of diffusive interface stability  KS in fair agreement with oceanographic measurements o Ra is much larger ( O(109), i.e. 104 times) o Fails only for diffusive interfaces with very low stability Time-Dependent Nonlinear Convection (Advances in Fluid Mechanics), 1998
  • 22. PostDoc at Free University of Amsterdam  Domain: Sedimentary Geology  Context: Climate reconstruction from sediment analysis of calcium carbonate  Project: Model Implementation of CaCO3 Dissolution due to Organic Carbon Degradation Tectonophysics, 320, 347–374, 2000
  • 23. Research/Consultancy at Delft Hydraulics  Project leader: drill slib deposition in the Scheldt Estuary; o numerical modeling and visualisation of hydrodynamics + slib transport,  Hong Kong power plant water inlet: water quality scenario study,  Project leader: software module for nutrient regeneration due to organic carbon degradation in North Sea sediments,  Feasibility study for fresh water retrieval, Indonesia; o data retrieval & checking o analytical modeling of lake desalination.
  • 24. Research at Philips Research the Netherlands  2000 - 2002: Cluster Domain Modelling,  2003 - 2004: Cluster Internet Connected Consumer Systems, o Gatewayed Services Architecture for internet- enabled consumer electronics devices (project 2003), o Home Networking Security (project 2004).
  • 25. … [ Experiment ] make your own private layered structure [ Experiment ] …  Ocean Model: Cup of HOT coffee  Ice-edge model: Use a Transparent, Glass Cup  Add Salt Stratification: GENTLY pour some coffee milk  Wait for a few minutes and …  Your private oceanic staircase is ready for consumption !
  • 26. The End WEB publications:  Ph.D. work: www.kranenborg.org/jurjen  (Analog) electronics: www.kranenborg.org/ee