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Welcome to the 7 th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and after stenting

John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

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Page 1: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

Welcome to the 7th European Bifurcation Club

14-15 October 2011 - LISBON

John Doe LM flow dynamics before, during and after stenting

Page 2: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

Dr. Gabriele Dubini

Laboratory of Biological Structure Mechanics – LaBS

Dept. of Structural Engineering Politecnico di Milano

Milan, Italy

Page 3: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

3

STR

UC

TUR

AL

MO

DEL

(fr

om G

hent

Uni

vers

ity)

FLU

ID D

YNA

MIC

MO

DEL

î  Pre Expansion î  MB Expansion î  Pre Expansion î  MB Expansion î  Proximal Optimisation Technique (POT)

From structural to fluid dynamic model

(Xience Prime stent)

Page 4: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

î A tetrahedral mesh was created using ANSYS ICEM CFD 13.0

î  About 3.3 millions elements

Section S-S

4

S

S

Fluid dynamic model: mesh

Page 5: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

µ∞ = 0.0035 Pa·s λ = 25 s µ0 = 0.25 Pa·s n = 0.25

2/120 ])(1)[( −

∞∞ +++= nSλµµµµ

ρ = 1060 kg/m3

• Under relaxation factors: 0.3 for pressure and momentum 1 for density

• Convergence criterion: 10-7 for continuity and velocity residuals

î  Fluid model: non-Newtonian blood (Carreau model)

î  Solver: ANSYS FLUENT 13.0 coupled – steady state

(Seo et al. 2005)

• Momentum spatial discretization: second-order upwind scheme

5

• Courant number: 50

Fluid dynamic model: methods

Page 6: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

INLET

OUTLET SB (40 %)

OUTLET MB (60 %)

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î  Boundary conditions

• Inlet: paraboloid-shaped constant velocity profile

• Outlets: flow split (60% MB, 40% SB)

• Wall: no-slip condition

vmean = 0.13 m/s (Davies et al. 2006)

Fluid dynamic model: methods

Page 7: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

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î  Wall clock time for CFD a steady simulation: about 4 hours (with a mesh of 3.3 million elements)

î  CFD simulations were made on a desktop PC using 2 parallel cores. The computer is equipped with a 2,93 GHz quad-core processor with 16 GB RAM

î  Estimate wall clock time for a CFD transient simulation: 2 days (on a cluster)

Fluid dynamic model: methods

Page 8: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

î  Velocity stream lines

0 0.2 0.4

VELOCITY [m/s]

8

Fluid dynamic model: results

Page 9: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

î  Velocity streamlines 0 0.2 0.4

VELOCITY [m/s]

9

MB EXPANSION

PRE EXPANSION

Fluid dynamic model: results

Page 10: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

î  Velocity contours 0 0.2 0.4

VELOCITY [m/s]

10

MB EXPANSION POT PRE EXPANSION

Fluid dynamic results: comparison

Page 11: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

OSI = ⎟⎟

⎟⎟

⎜⎜⎜⎜

∫dt

dtT

w

T

w

0

0121

τ

τ

• Wall Shear Stress (WSS) and WSS gradients

Local fluid dynamics

Flow

Radius

• Oscillatory Shear Index (OSI)

T = duration of cardiac cycle and τw = instantaneous wall shear stress vector

OSI > 0.1 ÷ 0.2 associated with cellular proliferation, intimal thickening, and inflammation WSS < 0.5 Pa

OSI = ⎟⎟

⎟⎟

⎜⎜⎜⎜

∫dt

dtT

w

T

w

0

0121

τ

τ

T = duration of cardiac cycle and τw = instantaneous wall shear stress vector

11

Page 12: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

0 0.25 0.5

WSS [Pa]

12

î  Wall Shear Stress (WSS)

MB EXPANSION

WSS < 0.5 Pa risk of restenosis (Ku 1997, Malek et al. 1999)

Fluid dynamic results

Page 13: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

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î  Wall Shear Stress (WSS)

MB EXPANSION POT PRE EXPANSION

0 0.25 0.5

WSS [Pa]

Fluid dynamic results: comparison

Page 14: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

Conclusions (from EBC 2010)

Towards (patient-specific) virtual interventional planning - i.e. open problems for engineers:

•  How to smoothly fit in the clinical workflow?

•  Material properties of the arterial wall and plaque •  Detailed anatomy from routine visualisation techniques –

i.e. beyond fluoroscopy •  Inlet flow curve and outlet pressure/flow split •  Short term prediction

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Page 15: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

Dedicated vs standard devices

Dedicated device Standard device Dedicated device Standard device

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Page 16: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

Dedicated vs standard devices

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Page 17: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

0 0.2 0.4

Velocity [m/s]

0 0.25 0.5

Wall Shear Stress [Pa]

Dedicated vs standard devices

17

Page 18: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

0 0.2 0.4

Velocity [m/s]

0 0.6 1.2

PRT [s]

0 0.6 1.2

Particle residence Time [s]

Dedicated vs standard devices

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Page 19: John Doe LM flow dynamics before, during and after stenting · Welcome to the 7th European Bifurcation Club 14-15 October 2011 - LISBON John Doe LM flow dynamics before, during and

LABORATORY OF BIOLOGICAL STRUCTURE MECHANICS

www.labsmech.polimi.it

[email protected]

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Claudio Chiastra, PhD student

Stefano Morlacchi, PhD student

Francesco Migliavacca, Associate Professor

Acknowledgements