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Towards Curvature-Based Prediction of Spiral Breakup in Cardiac Tissue Abhishek Murthy Stony Brook University (SBU) amurthy@cs.sunysb.edu Joint Work with Ezio Bartocci, Prof. Radu Grosu and Prof. Scott Smolka April 28, 2011 Abhishek Murthy


  1. Towards Curvature-Based Prediction of Spiral Breakup in Cardiac Tissue Abhishek Murthy Stony Brook University (SBU) amurthy@cs.sunysb.edu Joint Work with Ezio Bartocci, Prof. Radu Grosu and Prof. Scott Smolka April 28, 2011 Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 1 / 22

  2. Outline Introduction 1 Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 2 / 22

  3. Outline Introduction 1 Wave Breaks and Atrial Fibrillation 2 Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 2 / 22

  4. Outline Introduction 1 Wave Breaks and Atrial Fibrillation 2 Curvature of Cardiac Excitation Waves 3 Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 2 / 22

  5. Outline Introduction 1 Wave Breaks and Atrial Fibrillation 2 Curvature of Cardiac Excitation Waves 3 Case Studies 4 Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 2 / 22

  6. Outline Introduction 1 Wave Breaks and Atrial Fibrillation 2 Curvature of Cardiac Excitation Waves 3 Case Studies 4 Future Work 5 Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 2 / 22

  7. Why Atrial Fibrillation Matters Atrial Fibrillation (AF) - the quivering of heart muscles of atrial chambers, is the most common cardiac arrhythmia. Prevalent in 2.66 Million Americans, AF responsible for 14,490 deaths in 2010. As an independent risk factor for ischemic strokes, responsible for at least 15% to 20% cases. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 3 / 22

  8. Cardiac Excitation Waves Modelling electrical excitation of cardiac tissue as a reaction-diffusion system - Minimal Model Simulating model under Isotropic Diffusion (ID) Figure: One time step of simulating cardiac electrical conduction under ID Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 4 / 22

  9. Wave Breaks and AF Spatio-temporal description of the fibrillating cardiac tissue involves wave breaks or phase singularities. Curved waves break up near regions of high curvature. (Loading breakupExample.avi) Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 5 / 22

  10. Wave Breaks and AF Spatio-temporal description of the fibrillating cardiac tissue involves wave breaks or phase singularities. Curved waves break up near regions of high curvature. (Loading breakupExample.avi) Predicting wave break-ups will help predict the onset of AF. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 5 / 22

  11. Wave Breaks and AF - A closer look Wave propagation speed and curvature are related. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 6 / 22

  12. Wave Breaks and AF - A closer look Wave propagation speed and curvature are related. If V is propagation speed and K , the curvature, then V ( K ) = V 0 − DK V 0 = speed of a planar wave D = diffusion co-efficient Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 6 / 22

  13. Wave Breaks and AF - A closer look Wave propagation speed and curvature are related. If V is propagation speed and K , the curvature, then V ( K ) = V 0 − DK V 0 = speed of a planar wave D = diffusion co-efficient Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 6 / 22

  14. Wave Breaks and AF - A closer look Wave propagation speed and curvature are related. If V is propagation speed and K , the curvature, then V ( K ) = V 0 − DK V 0 = speed of a planar wave D = diffusion co-efficient Curved waves break near regions of high curvature - wave propagation velocity decreases with increasing convexity. Thus wave breaks up at critical curvature K cr = V 0 / D Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 6 / 22

  15. Curvature of Cardiac Excitation Waves Requirements for estimating and analysing the curvature of excitation waves (for prediction purposes): Curvature estimation must be accurate. 1 Curvature should be estimated continuously along the length of 2 the wave. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 7 / 22

  16. Curvature of Cardiac Excitation Waves Requirements for estimating and analysing the curvature of excitation waves (for prediction purposes): Curvature estimation must be accurate. 1 Curvature should be estimated continuously along the length of 2 the wave. Figure: Curvature Estimation of Cardiac Excitation Waves Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 7 / 22

  17. Curvature - Estimating Excitation Waves Given a simulation of a grid G of m × n cells, wave W ( c , t ) can be written as W ( c , t ) = { ( x , y ) | x , y ∈ R F ( x , y ) = c at time t } Where F ( x , y ) = interpolation of the simulation results onto R 2 Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 8 / 22

  18. Curvature - Estimating Excitation Waves Given a simulation of a grid G of m × n cells, wave W ( c , t ) can be written as W ( c , t ) = { ( x , y ) | x , y ∈ R F ( x , y ) = c at time t } Where F ( x , y ) = interpolation of the simulation results onto R 2 Check for intersection of wave and an edge of the grid. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 8 / 22

  19. Curvature - Estimating Excitation Waves Given a simulation of a grid G of m × n cells, wave W ( c , t ) can be written as W ( c , t ) = { ( x , y ) | x , y ∈ R F ( x , y ) = c at time t } Where F ( x , y ) = interpolation of the simulation results onto R 2 Check for intersection of wave and an edge of the grid. Intersection point is obtained by linear interpolation. Implemented using contour function of Matlab Figure: Contour estimation on grid Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 8 / 22

  20. Curvature - Estimating Excitation Waves Given a simulation of a grid G of m × n cells, wave W ( c , t ) can be written as W ( c , t ) = { ( x , y ) | x , y ∈ R F ( x , y ) = c at time t } Where F ( x , y ) = interpolation of the simulation results onto R 2 Check for intersection of wave and an edge of the grid. Intersection point is obtained by linear interpolation. Implemented using contour function of Matlab Figure: Contour estimation on grid Track the same wave across different time steps of the simulation. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 8 / 22

  21. Curvature - Cubic Bézier Fits of Waves Obtain C2 continuous Bézier fit that can be used for symbolic curvature estimation. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 9 / 22

  22. Curvature - Cubic Bézier Fits of Waves Obtain C2 continuous Bézier fit that can be used for symbolic curvature estimation. Fit each of the overlapping strip with cubic Bézier curves of the form: X j ( t ) = ( 1 − t ) 3 P 0 j + 3 t ( 1 − t ) 2 P 1 j + 3 t 2 ( 1 − t ) P 2 j + t 3 P 3 j . t ∈ [ 0 , 1 ] (1) Y j ( t ) = ( 1 − t ) 3 Q 0 j + 3 t ( 1 − t ) 2 Q 1 j + 3 t 2 ( 1 − t ) Q 2 j + t 3 Q 3 j . t ∈ [ 0 , 1 ] (2) where j is the strip index. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 9 / 22

  23. Curvature - Cubic Bézier Fits of Waves Obtain C2 continuous Bézier fit that can be used for symbolic curvature estimation. Fit each of the overlapping strip with cubic Bézier curves of the form: X j ( t ) = ( 1 − t ) 3 P 0 j + 3 t ( 1 − t ) 2 P 1 j + 3 t 2 ( 1 − t ) P 2 j + t 3 P 3 j . t ∈ [ 0 , 1 ] (1) Y j ( t ) = ( 1 − t ) 3 Q 0 j + 3 t ( 1 − t ) 2 Q 1 j + 3 t 2 ( 1 − t ) Q 2 j + t 3 Q 3 j . t ∈ [ 0 , 1 ] (2) where j is the strip index. In the region of overlap take weighted average of the two curves. Figure: Weighted average based Bézier curve fitting Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 9 / 22

  24. Curvature - Symbolic Curvature Estimation Closed form expressions corresponding to C2 smooth Bézier fit can be processed symbolically in MATLAB’s symbolic computation toolbox. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 10 / 22

  25. Curvature - Symbolic Curvature Estimation Closed form expressions corresponding to C2 smooth Bézier fit can be processed symbolically in MATLAB’s symbolic computation toolbox. If X j ( t ) and Y j ( t ) denote the fit for a strip, then curvature is calculated as | r ′ j ( t ) × r ′′ j ( t ) | κ j ( t ) = (3) j ( t ) | 3 | r ′ where r j ( t ) = [ X j ( t ) , Y j ( t )] is the position vector described by the Bézier curve. Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 10 / 22

  26. Curvature - Symbolic Curvature Estimation Closed form expressions corresponding to C2 smooth Bézier fit can be processed symbolically in MATLAB’s symbolic computation toolbox. If X j ( t ) and Y j ( t ) denote the fit for a strip, then curvature is calculated as | r ′ j ( t ) × r ′′ j ( t ) | κ j ( t ) = (3) j ( t ) | 3 | r ′ where r j ( t ) = [ X j ( t ) , Y j ( t )] is the position vector described by the Bézier curve. Continuous closed form of κ j ( t ) = > continuous curvature estimate along wavefront Abhishek Murthy (SBU) Towards Curvature based Breakup Prediction April 28, 2011 10 / 22

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