Learning Cycle Linear Hybrid Automata for Excitable Cells

Similar documents
The Physics of the Heart. Sima Setayeshgar

Chimera states in networks of biological neurons and coupled damped pendulums

2013 NSF-CMACS Workshop on Atrial Fibrillation

Parameters for Minimal Model of Cardiac Cell from Two Different Methods: Voltage-Clamp and MSE Method

The Physics of the Heart. Sima Setayeshgar

6.3.4 Action potential

Systems Biology Review Copy

TAKING MATH TO THE HEART: Pulse Propagation in a Discrete Ring

Modelling excitable cells using cycle-linear hybrid automata

Lecture Notes 8C120 Inleiding Meten en Modelleren. Cellular electrophysiology: modeling and simulation. Nico Kuijpers

Spatial Networks of Hybrid I/O Automata for Modeling Excitable Tissue

From neuronal oscillations to complexity

All-or-None Principle and Weakness of Hodgkin-Huxley Mathematical Model

Peripheral Nerve II. Amelyn Ramos Rafael, MD. Anatomical considerations

Computer Science Department Technical Report. University of California. Los Angeles, CA

On Parameter Estimation for Neuron Models

Real-time computer simulations of excitable media: Java as a scientific language and as a wrapper for C and Fortran programs

Real-time computer simulations of excitable media:

Origins of Spiral Wave Meander and Breakup in a Two-Dimensional Cardiac Tissue Model

Saturation of Information Exchange in Locally Connected Pulse-Coupled Oscillators

Entrainment and Chaos in the Hodgkin-Huxley Oscillator

Asymptotic approximation of an ionic model for cardiac restitution

Lecture 10 : Neuronal Dynamics. Eileen Nugent

Systems Biology Across Scales: A Personal View XXVI. Waves in Biology: From cells & tissue to populations. Sitabhra Sinha IMSc Chennai

Conduction velocity restitution in models of electrical excitation in the heart

SUPPLEMENTARY INFORMATION

Single neuron models. L. Pezard Aix-Marseille University

CSD-TR R. Samade, B. Kogan

Systems Biology: Theoretical Biology. Kirsten ten Tusscher, Theoretical Biology, UU

Basic mechanisms of arrhythmogenesis and antiarrhythmia

Electrophysiology of the neuron

Chapter 24 BIFURCATIONS

Nervous Systems: Neuron Structure and Function

FRTF01 L8 Electrophysiology

Learning and Detecting Emergent Behavior in Networks of Cardiac Myocytes

Signal processing in nervous system - Hodgkin-Huxley model

لجنة الطب البشري رؤية تنير دروب تميزكم

Reproducing Cardiac Restitution Properties Using the Fenton Karma Membrane Model

Lecture 11 : Simple Neuron Models. Dr Eileen Nugent

Multiple Mechanisms of Spiral Wave Breakup in a Model of Cardiac Electrical Activity

STUDENT PAPER. Santiago Santana University of Illinois, Urbana-Champaign Blue Waters Education Program 736 S. Lombard Oak Park IL, 60304

Simulation of Cardiac Action Potentials Background Information

Neuronal Dynamics: Computational Neuroscience of Single Neurons

Periodic Behavior in Cardiac Tissue: Dynamics of Spatially Discordant Calcium Alternans

1. Synchronization Phenomena

Neural Modeling and Computational Neuroscience. Claudio Gallicchio

ACTION POTENTIAL. Dr. Ayisha Qureshi Professor MBBS, MPhil

Dynamical systems in neuroscience. Pacific Northwest Computational Neuroscience Connection October 1-2, 2010

Chapter 2 Basic Cardiac Electrophysiology: Excitable Membranes

Neural Coding: Integrate-and-Fire Models of Single and Multi-Neuron Responses

Voltage-clamp and Hodgkin-Huxley models

Introduction to Physiology V - Coupling and Propagation

9.01 Introduction to Neuroscience Fall 2007

arxiv: v1 [physics.bio-ph] 2 Jul 2008

Sean Escola. Center for Theoretical Neuroscience

Nonlinear systems, chaos and control in Engineering

Learning and Detecting Emergent Behavior in Networks of Cardiac Myocytes

Title. Author(s)Yanagita, T. CitationPhysical Review E, 76(5): Issue Date Doc URL. Rights. Type.

Firefly Synchronization. Morris Huang, Mark Kingsbury, Ben McInroe, Will Wagstaff

Physiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES

A note on discontinuous rate functions for the gate variables in mathematical models of cardiac cells

Mathematical analysis of a 3D model of cellular electrophysiology

Nervous Tissue. Neurons Electrochemical Gradient Propagation & Transduction Neurotransmitters Temporal & Spatial Summation

Voltage-clamp and Hodgkin-Huxley models

2401 : Anatomy/Physiology

Hopfield Neural Network and Associative Memory. Typical Myelinated Vertebrate Motoneuron (Wikipedia) Topic 3 Polymers and Neurons Lecture 5

Nonlinear Observer Design and Synchronization Analysis for Classical Models of Neural Oscillators

Computational Cell Biology

APPM 2360 Project 3 Mathematical Investigation of Cardiac Dynamics

ANALYSIS OF CELLULAR CARDIAC BIOELECTRICITY MODELS TOWARD COMPUTATIONALLY EFFICIENT WHOLE-HEART SIMULATION

BIOELECTRIC PHENOMENA

Ionic Charge Conservation and Long-Term Steady State in the Luo Rudy Dynamic Cell Model

Simulation-based Verification of Cardiac Pacemakers with Guaranteed Coverage

The Department of Electrical Engineering. nkrol Mentors: Dr. Mohammad Imtiaz, Dr. Jing Wang & Dr. In Soo Ahn

BME 5742 Biosystems Modeling and Control

Threshold dynamics and strength-duration curves

2011 NSF-CMACS Workshop on Atrial Fibrillation (5 th day )

The Spike Response Model: A Framework to Predict Neuronal Spike Trains

MEMBRANE POTENTIALS AND ACTION POTENTIALS:

Computational statistics

Electronics 101 Solving a differential equation Incorporating space. Numerical Methods. Accuracy, stability, speed. Robert A.

Classifying Mechanisms of Spiral Wave Breakup Underlying Cardiac Fibrillation Using Quantitative Metrics

MATH 3104: THE HODGKIN-HUXLEY EQUATIONS

Bounded Model Checking with SAT/SMT. Edmund M. Clarke School of Computer Science Carnegie Mellon University 1/39

UNIT 6 THE MUSCULAR SYSTEM

Compartmental Modelling

Math 345 Intro to Math Biology Lecture 20: Mathematical model of Neuron conduction

Introduction to Biomedical Engineering

Electrical Signaling. Lecture Outline. Using Ions as Messengers. Potentials in Electrical Signaling

Physics 178/278 - David Kleinfeld - Winter 2017

Dynamics and complexity of Hindmarsh-Rose neuronal systems

Analysis of Damped Oscillations during Reentry: A New Approach to Evaluate Cardiac Restitution

Control and Integration. Nervous System Organization: Bilateral Symmetric Animals. Nervous System Organization: Radial Symmetric Animals

Νευροφυσιολογία και Αισθήσεις

Physiology Coloring Book: Panels 29, 32, 33,

Nervous System Organization

Action Potentials & Nervous System. Bio 219 Napa Valley College Dr. Adam Ross

Computational Explorations in Cognitive Neuroscience Chapter 2

A realistic neocortical axonal plexus model has implications for neocortical processing and temporal lobe epilepsy

Bursting Oscillations of Neurons and Synchronization

Transcription:

Learning Cycle Linear Hybrid Automata for Excitable Cells Sayan Mitra Joint work with Radu Grosu, Pei Ye, Emilia Entcheva, I V Ramakrishnan, and Scott Smolka HSCC 2007 Pisa, Italy

Excitable Cells Outline Excitable cells Hybrid model for excitable cells Conclusions and future directions

Excitable Cells Excitable Cells An excitable cell generates electrical pulses or action potentials in response to electrical stimulation Examples: neurons, cardiac cells, smooth muscle cells Local regeneration allows electric signal propagation without damping Building block for electrical signaling in brain, heart, and muscles Neurons of a squirrel University College London Artificial cardiac tissue University of Washington

Excitable Cells Interaction of Excitable Cells Action Potential (AP) depends on stimulus, membrane voltage of neighboring cells, state of cell itself Normal: synchronous pulses, spiral waves Abnormal: incoherent pulses, wave breakup Leads to cardiac arrhythmia, epilepsy voltage Stimulus Schematic Action Potential Threshold failed initiation Resting potential time

Macro Models of Action Potentials Cellular automata Oscillators and uniform coupling between cells [Kuramoto`84] Small world network of coupled oscillators [Watts & Strogatz`98] θi = ωi + t i = 1... N K N N j= 1 sin( θ θ ) j i

Excitable Cells Micro Models for Action Potentials Membrane potential for squid giant axon [Hodgkin Huxley`52] Luo Rudy model (1991) for cardiac cells of guinea pig Neo Natal Rat (NNR) model for cardiac cells of rat Na + K+. CV = g m h ( V V ) + g n ( V V ) + g ( V V ) + I. h 3 4 Na Na K K L L st m = ( α + β ) m + α. α ( V ) = 007. e β h ( V ) = e m m m h = ( α + β ) h + α. h h h n = ( α + β ) n + α n n n 1 3 0. 1 V V 20 + 1 ( 25. 01. V ) α m ( V ) = 25. 01. V e 1 β ( V ) = 4e m ( 01. 001. V ) α n ( V ) = 1 0. 1 V e 1 β ( V ) = 0125. e n V 18 V 80 I Na I K I st Outside I L Na K L g Na g K g L C I C C V Large state space Nonlinear differential equations Multiple spatial and temporal scales V Na V K V L Inside

Excitable Cells Macro Analyzable but unrealistic Micro Realistic, but not analyzable. Simulation is slow.

Hybrid Automata Model for Excitable Cells Linear Hybrid Approximations for Action Potentials Suppose, AP can be partitioned into modes so that in mode M, v can be approximated by: x i = b Mi x i v = S i x i, M e {S,U,E,P,F,R} b Mi s can be found by Prony s method which fits sum of exponentials to data Mode switches at the beginning and end of stimulus when v crosses threshold voltages V M But, stimulus can appear at any M State of cell at the time of arrival of stimulus influences behavior of cell for the next AP b Mi s history dependent voltage (v) Upstroke (U) Stimulated (S) Early Repol (E) v V U U Plateau (P) E time v V E Final Repol (F) P v V F v V R Resting (R) F S R

Hybrid Automata Model for Excitable Cells History Dependence of APs Frequency of stimulation determines voltage (v 0 )at the time of appearance of stimulus, which influences shape of next AP voltage Lower frequency: longer resting time and v 0 closer to resting voltage results in longer AP time v 0 Higher frequency: shorter AP

Hybrid Automata Model for Excitable Cells History Dependence of APs Frequency of stimulation determines voltage (v 0 )at the time of appearance of stimulus, which influences shape of next AP voltage v 0 Even higher frequency: conjoined AP, bifurcation time 25 20 APD 15 10 50 100 150 200 stimulation frequency

Hybrid Automata Model for Excitable Cells History Dependence and Restitution Frequency of stimulation determines voltage (v 0 )at the time of appearance of stimulus, which influences shape of next AP voltage AP Duration (APD) Diastolic Interval (DI) Restitution curve: APD vs. DI Slope > 1 indicates breakup of spiral waves under high frequency stimulation Local to global behavior 10% of peak time v 0

Hybrid Automata Model for Excitable Cells Cycle Linear Hybrid Automata (CLHA) Uncountable family of modes = μ : Epoch and Regime (, <) is a total order Linear dynamics in each mode Unique ge that is visited infinitely many times M x i = b Mi (v 0 ) x i v = S i x i M e {S,U,E,P,F,R} There exists a snapshot function : Xö, such that for any switch (x 1, e 1, r 1 ) ö (x 2, e 2, r 2 ) (i) r 2 = g and e 2 = (x 1 ), or (ii) r 2 g, e 2 = e 1 and r 2 <r 1 = {S,U,E,P,F,R} determined by v 0 g v V T (v 0 ) U v 0 := v E S v V E (v 0 ) v 0 := v P v 0 := v v 0 := v R v V F (v 0 ) F v V R (v 0 )

Hybrid Automata Model for Excitable Cells Identifying CLHA Parameters for a single AP For each mode, we seek a solution for LTI: x& = bx, x(0) = a, b= diag( b,..., b ), a = [ a... a ] v = n i= 1 1 n 1 x i n T Observable solution is a sum of v = n i= 1 a e i bt i exponentials: Curve segments are Convex, concave or both Consequences: Solutions: might require at least two exponentials Coefficients a i and b i : positive/negative or real/complex Exponential fitting: Modified Prony s method [Osborne and Smyth `95]

Hybrid Automata Model for Excitable Cells Parameters as Functions of History Variable V TVE Parameters: Threshold voltages V S, V E, Coefficients of differential equations b S1, b S2, b E1, Coefficients in reset maps From each stimulation frequency in the training set, we get a corresponding value for b S1, b S2,, V S, V E, Apply Prony s method (a second time) to obtain b S1 as a function of v 0 : b M1 (v 0 ) = c M1 exp (v 0 d M1 ) + c M1 exp (v 0 d M1 ), for each M e {S,U,E,P,F,R} V T (v 0 ) = c T exp (v 0 d T ) + c T exp (v 0 d T ) v 0 V P V L

Conclusions: Results Contributions and Simulation Results CLHA as a model for almost periodic systems Iterative process to obtain excitable cell model with desired accuracy Simulation efficiency (> 8 times faster) [True, Entcheva, et al.] Biological interpretation of state variables x 1, x 2 ; restitution curve Spiral wave generation and breakup Spiral waves Breakup

Conclusions: Future Directions Future Directions CLHA for stimulation with different shapes CLHAs coupled through pulses or diffusion for analyzing synchronization conditions Specification of spatiotemporal voltage patterns Distributed control through targeted stimulation