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1
Study of Crossflow in Total Cavopulmonary
Connectionby
Sandesh RajputGuide:
Prof. S.D.Sharma
Department of Aerospace EngineeringIIT Bombay
26 June 201326 June 2013
2
Topics to be covered
IntroductionFontan OperationTotal Cavopulmonary ConnectionComputational Models MethodologyResultsConclusionReference
26 June 2013
3
Introduction
Congenital Heart diseases (CHD)
o defects in the structure of the heart at the time of birth
o 8 out of 1000 live births
o 2,00,000 children born with such defects and accounts for 10%
infant mortality rate in
Single ventricular deficiencies
o refers to defect where the heart has only one effective or
functional pumping chamber e.g. Tricuspid atresia, Hypoplastic
left heart syndrome etc.26 June 2013
4
Fontan operation
In 1971, Fontan and Baude successfully by-passed right heart
Tricuspid atresia ( complete absence of tricuspid valve )
Development of hypoplastic (undersized) or absent right ventricle
Purpose was to drain the whole vena cava
blood to the pulmonary arteries.
Connection between superior vena cava
(SVC) and right pulmonary artery (RPA)
Atriopulmonary connection (APC)
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SVC connected directly to right pulmonary artery (RPA)IVC can be connected to PA through right atrium or outside the
heart
Total cavopulmonary Connection
Intra-atrial conduit Fonta Extra-cardiac conduit Fonta
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Computational Models
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LPA
IVC
SVC
RPA
SVC- Superior Vena CavaIVC - Inferior Vena CavaRPA- Right Pulmonary ArteryLPA- Left Pulmonary Artery
Base Model
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Computational 2D Models
a) Model 1, straight zero offset b) Model 2, Flared zero offset26 June 2013
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Computational 2D Models continued…
c) Model 3, Flared 0.5 diameter offset
d) Model 4, Flared 1 diameter offset (2D)26 June 2013
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Computational Models
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offset
2 cm Offset Model
• Offset model prepared for offset value of 1 cm, 1.5 cm and 2 cm
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Computational 3D Models
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22% Blockage Plate
Blockage Model Control case
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Computational 3D Models
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Optiflo ModeHalf( SVC) Optiflo
Half( IVC) Optiflo
• Bifurcation of SVC or IVC or both
• Avoid head-on collision• Growth problem
12
Methodology
Ansys WorkbenchPre-processing
1. DesignModeler
2. MeshingTetrahedral and Triangular
elements180,000-200,000 nodesMesh Quality
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Methodology continued…
Ansys FLUENT 2D Model Simulation
1. Flow split RPA:LPA (30:70, 40:60, 50:50, 60:40 and 70:30)
2. Flow rate , SVC : IVC = 40:60
3. Boundary Condition- Velocity at inlet and Outflow at Outlet3D Model Simulation
1. Flow rate and
2. SVC : IVC =
3. Boundary Condition- Velocity at inlet and Outflow at pressureAssumptions (Flow, Fluid and Vessel walls)
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Methodology
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• Convergence Criteria- Residual• 1200 iteration• RMS =0.00001
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The total pressure and volume flow was calculated using area-weighted average at the boundaries
Hydraulic dissipated power,
It is difference between the total energy rate at the inlet and at the outlet of the model.
Total Energy-loss coefficient
It is the ratio of the hydraulic dissipated power and the inlet
kinetic energy.
26 June 2013
Methodology
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Results- 2D Models
power loss in the flared model was on an average 20% less than in model with straight connection
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Effect of flaring (equal flow split)
Effect of offset (at equal flow split )
Flared zero offset Flared 0.5 diameter offset1726 June 2013
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power losses decreases with increase in the offset valueshead-on collision in zero offset models results inaccurate
Effect of offset (at equal flow split ) continued…
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Comparison with previous studies for flared 1 dia. model
similar patterns in the trends of energy loss as a function of RPA flow split ratio
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3D Model Results
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Power loss through offset models for Q =3 Lit/min
• the power loss goes on decreasing with increasing offset values• Power losses are reduced by almost 9 % when the model is offset
by 2 cm.
21
Power loss comparison of various TCPC models
Application of turbulent modeling on zero offset shows maximum power loss while Optiflo [7] is found to most energy efficient
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Velocity Contours for Blockage and Control Model
The velocity magnitude increased tremendously at the blockage due to least cross sectional
The plate kept at the center does not allow the head-on collision of flows from IVC and SVC
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Velocity contour for Optiflo Model
Due to inertia of the caval flow entering the bifurcation, the majority of the follow could not follow the outer curved of the model.
This caused large low flow regions and flow separation region contributing to the power loss
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Turbulence ModelingSimulation on Control model and Base model using turbulence
modeling
Realizable k-epsilon model was used with 5% of turbulence intensity
The Turbulent kinetic energy variable determines the scale of the
turbulence while epsilon variable determines the energy in the
turbulence
The power losses relatively higher than the laminar model
vortex main source of turbulence in the central region
the plate does not allow head-on collision, hence no vortex is formed
causing less turbulence.
As a result of this, the power loss in control model is 30% lesser than
in Base model26 June 2013
25
Conclusion
Flaring at the connection site reduced power losses by 20%
when compared to model with straight connections
The energy losses are minimum in all the models for equal flow
split to both the pulmonary arteries
The offset enhances the hemodynamics of the connection and
power losses reduce with increasing offset values
The power loss in Control model is 30% lesser than in Base
model
26 June 2013
References
[1] A. Saxena, “Congenital heart disease in India: a status report,” Indian journal of pediatrics,
vol. 72, no. 7, pp. 595–8, Jul. 2005.
[2] F. Fontan and E. Baudet, “Surgical repair of tricuspid atresia,” Thorax, vol. 26, no. 3, pp.
240–8, May 1971.
[3] M. R. de Leval et al. “Total cavopulmonary connection: a logical alternative to
atriopulmonary connection for complex Fontan operation. Experimental studies and early
clinical experience,” The Journal of thoracic and cardiovascular surgery, vol. 96, no. 5, pp.
682–95, Nov. 1988.
[4]H. D. Puga et al. “Modifications of the Fontan operation applicable to patients with left
atrioventricular valve atresia or single a atrioventricular valve,” Circulation, vol. 76, no. (3 Pt 2),
pp. III53–60, 1987.
2626 June 2013
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References
[5] Ann E. Ensley et al. “Toward designing the optimal total cavopulmonary
connection: an in vitro study,” The Annals of thoracic surgery, vol. 68, no. 4, pp.
1384–90, Oct. 1999
[6] K. Ryu, et al. “Importance of Accurate Geometry in the Study of the Total
Cavopulmonary Connection: Computational Simulations and In Vitro Experiments,”
Annals of Biomedical Engineering, vol. 29, no. 10, pp. 844–853, Oct. 2001.
[7] D. D. Soerensen, K. Pekkan, D. de Zélicourt, S. Sharma, K. Kanter, M. Fogel,
and A. P. Yoganathan, “Introduction of a new optimized total cavopulmonary
connection.,” The Annals of thoracic surgery, vol. 83, no. 6, pp. 2182–90, Jun. 2007.
26 June 2013
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Thank You
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29
Energy Indices
1. Hydraulic dissipated power,
It is calculated using following expression:
where,
2. Total Energy-loss coefficient It is the ratio of the hydraulic dissipated power and the inlet kinetic energy.
It is calculated using following expression:26 June 2013
and as a function of the offset
et al., “Use of computational fluid dynamics in the design of surgical procedures : application to the study of competitive flows in cavopulmonary connections,” Journal of Thoracic Cardiovascular Surgery, vol. 111, pp. 502–13, 1996.
3026 June 2013
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Pulmonary Flow distributions among offset models
26 June 2013