In-Silico Modeling of Glycosylation Modulation Dynamics in K+ Ion Channels and Cardiac Signaling
|
|
- Edmund Stephens
- 5 years ago
- Views:
Transcription
1 In-Silico Modeling of Glycosylation Modulation Dynamics in K+ Ion Channels and Cardiac Signaling Dongping Du, Hui Yang Industrial and Management Systems Engineering Andrew R. Ednie, Eric S. Bennett Molecular Pharmacology and Physiology University of South Florida July 29,
2 Research Background Action Potential (AP): Net changes of transmembrane potentials Cardiac Contraction Ventricular cell K+ Schematic diagram of a cardiac cell AP 2
3 Cardiac Action Potential Cardiac arrhythmias and sudden cardiac death K+ Channels Stimulated 20 mv AP of ventricular cells 100 ms 3
4 Research Background Glycosylation: The enzymatic process that attaches glycans to proteins, lipids, or other organic molecules 4
5 Motivations Congenital Disorders of Glycosylation (CDG): High infant mortality rate Multi-system effects, e.g., diabetes, cardiac diseases Prevalence of cardiac involvement Unknown etiology of cardiomyopathy among young CDG patients Goals Understand the pathology of cardiac disease among CDG patients Develop pertinent therapeutic solutions 5
6 Gaps Gaps Little is known on how reduced glycosylation affects cardiac electrical signaling I K1 Joint K+ current I Kslow I Kur myocyte Limitations Study the changes at molecular levels, i.e., channel level Connect changes at one organizational level, e.g., ion channels, to another organizational level, cardiac cells. Objectives: Couple in-silico studies with the wealth of data from our electrophysiological experiments to model, mechanistically, how reduced sialylation affects K+ activity and cardiac electrical signaling. 6
7 Challenges Kv channels share similar gating kinetics Experimental decomposition is challenging Patch Clamp Experiment Joint AP K+ Current 0 Currents Nerbonne et. Al
8 K+ Channel Currents Current density of K+ currents at different clamp voltages (Bondarenko et. al. model) 50 Current Density (pa/pf) ik1 iks ikur ikss ikr ito Small Voltage (mv) 8
9 K+ Current Decomposition Bi-exponential decomposition of the K+ currents f t = A 1 e t/τ 1 + A 2 e t/τ 2 + A 3 30 K+ current (pa/pf) Membrane Potential = 30mV I K,sum I to I Kslow I Kss iksum ik1 iks ikur ikss ikr ito Time (ms) 9
10 Data K+ Channel Gating Kinetics K+ Closed K+ Channel K+ Open K+ Channel Inactivated K+ Channel Refractory Period Steady State Activation Steady State Inactivation 1 Activation Probability Activation Probability Voltage (mv) Voltage (mv) 10
11 Research Methodology Transient Outward K+ Current, I to I to = G Kto a 3 toi to (V E K ) where G Kto is the maximum whole cell conductance (ms/uf), a to and i to are the activation and inactivation. a to t = a to 0 a ss,to e τ ato + a ss,to i to t = i to 0 i ss,to e t τ ito + i ss,to t K+ current Time (ms) 11
12 Research Methodology Transient Outward K+ Current, I Kslow I Kslow = G Kslow a ur i ur (V E K ), where G Kslow is the maximum whole cell conductance (ms/uf), a ur and i ur are the activation and inactivation. a ur t = a ur 0 a ss e τ aur + a ur i ur t = i ur 0 i ss e t τ iur + i ur Transient Outward K+ Current, I Kss I Kss = G Kss a Kss V E K where G Kss is the maximum whole cell conductance (ms/uf), a ur are the activation and inactivation. a Kss t = a Kss 0 a ks e τ Kss + a ks t t 12
13 Results IKslow- Steady State Activation & Steady State Inactivation IKslow SS IKto SS Silico WT In-vitro WT Silico ST3Gal4 -/ In-vitro ST3Gal4 -/- IKslow SS Voltage (mv) Silico WT In-vitro WT Silico ST3Gal4 -/- In-vitro ST3Gal4 -/ Voltage (mv) 13
14 Results IKto- Steady State Activation & Steady State Inactivation IKto SS SS Silico WT In-vitro WT Silico ST3Gal4 -/- In-vitro ST3Gal4 -/- IKto SS Voltage (mv) Voltage (mv) 14
15 Results IKslow (pa/pf) In-silico WT In-silico ST3Gal4 -/- IKto (pa/pf) In-silico WT In-silico ST3Gal4 -/ Time (ms) In-silico WT In-silico ST3Gal4 -/ Time (ms) 20 0 In-silico WT In-silico ST3Gal4 -/- IKss 4 2 AP (mv) Time (ms) Time (ms) 15
16 Conclusions Challenges Similar gating kinetics Multiple K+ currents vs a joint K+ current Decomposition of K+ currents Methodological and Biomedical Merits Glycosylation models of K+ currents Integrated glycosylation model of K+ channels and the ventricular cells. Improve fundamental knowledge about the functional role of sialylation in cardiac electrical signaling New pharmaceutical designs to correct aberrant glycosylation 16
17 Acknowledges CMMI IIP IOS Publications 1. D. Du, H. Yang, A. R. Ednie, and E. S. Bennett, Statistical Metamodeling and Sequential Design of Computer Experiments to Model Glyco-altered Gating of Sodium Channels in Cardiac Myocytes IEEE Journal of Biomedical and Health Informatics, second round review. 2. D. Du, H. Yang, S. Norring, and E. S. Bennett, In-silico modeling of glycosylation modulation dynamics in herg channels and cardiac electrical signaling, IEEE Journal of Biomedical and Health Informatics, vol. 18, issue 1, p , (Feature article by IEEE Journal of Biomedical and Health Informatics) 3. D. Du, H. Yang, S. Norring, and E. Bennett, "Multiscale modeling of glycosylation modulation dynamics in cardiac electrical signaling," Proceedings of 2011 IEEE Engineering in Medicine and Biology Society Conference (EMBC), pp , Aug Sept , Boston, MA. (Placed first in IBM Best Student Paper competition) 17
18 Thank you! Questions? 18
Physical-Statistical Modeling and Optimization of Cardiovascular Systems
University of South Florida Scholar Commons Graduate Theses and Dissertations Graduate School 1-1-22 Physical-Statistical Modeling and Optimization of Cardiovascular Systems Dongping Du University of South
More informationElectrophysiological Modeling of Membranes and Cells
Bioeng 6460 Electrophysiology and Bioelectricity Electrophysiological Modeling of Membranes and Cells Frank B. Sachse fs@cvrti.utah.edu Overview Recapitulation Electrical Modeling of Membranes Cardiac
More informationParameters for Minimal Model of Cardiac Cell from Two Different Methods: Voltage-Clamp and MSE Method
Parameters for Minimal Model of Cardiac Cell from Two Different Methods: oltage-clamp and MSE Method Soheila Esmaeili 1, * and Bahareh beheshti 1 Department of Biomedical engineering, ran University of
More informationMathematical Foundations of Neuroscience - Lecture 3. Electrophysiology of neurons - continued
Mathematical Foundations of Neuroscience - Lecture 3. Electrophysiology of neurons - continued Filip Piękniewski Faculty of Mathematics and Computer Science, Nicolaus Copernicus University, Toruń, Poland
More informationChapter 2 Basic Cardiac Electrophysiology: Excitable Membranes
Chapter Basic Cardiac Electrophysiology: Excitable Membranes Deborah A. Jaye, Yong-Fu Xiao, and Daniel C. Sigg Abstract Cardiomyocytes are excitable cells that have the ability to contract after excitation;
More informationQuestions: Properties of excitable tissues Transport across cell membrane Resting potential Action potential Excitability change at excitation
Questions: Properties of excitable tissues Transport across cell membrane Resting potential Action potential Excitability change at excitation EXCITABLE TISSUES The tissues can change the properties under
More informationPhysiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES
Physiology Unit 2 MEMBRANE POTENTIALS and SYNAPSES In Physiology Today Ohm s Law I = V/R Ohm s law: the current through a conductor between two points is directly proportional to the voltage across the
More information... Cardiac Gap Junctions Physiology, Regulation, Pathophysiology and Pharmacology
... Cardiac Gap Junctions Physiology, Regulation, Pathophysiology and Pharmacology S. Dhein, Cologne 23 figures and 3 tables, 1998 StefanDhein InstituteofPharmacology UniversityofCologne (Germany) All
More informationCSD-TR R. Samade, B. Kogan
The properties of the cardiac cell mathematical model with a Markovian representation of potassium channel gating processes under high pacing rate (Computer simulation study) CSD-TR040007 R. Samade, B.
More informationChannels can be activated by ligand-binding (chemical), voltage change, or mechanical changes such as stretch.
1. Describe the basic structure of an ion channel. Name 3 ways a channel can be "activated," and describe what occurs upon activation. What are some ways a channel can decide what is allowed to pass through?
More informationProblem Set No. 4 Due: Monday, 11/18/10 at the start of class
Department of Chemical Engineering ChE 170 University of California, Santa Barbara Fall 2010 Problem Set No. 4 Due: Monday, 11/18/10 at the start of class Objective: To understand the thermodynamic and
More informationTransport of ions across plasma membranes
Transport of ions across plasma membranes Plasma Membranes of Excitable tissues Ref: Guyton, 13 th ed: pp: 61-71. 12 th ed: pp: 57-69. 11th ed: p57-71, Electrical properties of plasma membranes Part A:
More informationQuantitative Electrophysiology
ECE 795: Quantitative Electrophysiology Notes for Lecture #1 Wednesday, September 13, 2006 1. INTRODUCTION TO EXCITABLE CELLS Historical perspective: Bioelectricity first discovered by Luigi Galvani in
More informationLecture Notes 8C120 Inleiding Meten en Modelleren. Cellular electrophysiology: modeling and simulation. Nico Kuijpers
Lecture Notes 8C2 Inleiding Meten en Modelleren Cellular electrophysiology: modeling and simulation Nico Kuijpers nico.kuijpers@bf.unimaas.nl February 9, 2 2 8C2 Inleiding Meten en Modelleren Extracellular
More information2013 NSF-CMACS Workshop on Atrial Fibrillation
2013 NSF-CMACS Workshop on A Atrial Fibrillation Flavio H. Fenton School of Physics Georgia Institute of Technology, Atlanta, GA and Max Planck Institute for Dynamics and Self-organization, Goettingen,
More informationNeural Modeling and Computational Neuroscience. Claudio Gallicchio
Neural Modeling and Computational Neuroscience Claudio Gallicchio 1 Neuroscience modeling 2 Introduction to basic aspects of brain computation Introduction to neurophysiology Neural modeling: Elements
More informationCellular Electrophysiology. Cardiac Electrophysiology
Part 1: Resting and Action Potentials Cardiac Electrophysiology Theory Simulation Experiment Scale The membrane: structure, channels and gates The cell: resting potential, whole cell currents, cardiac
More informationBasic mechanisms of arrhythmogenesis and antiarrhythmia
EHRA EDUCATIONAL REVIEW AND PREPARATORY COURSE ON INVASIVE CARDIAC ELECTROPHYSIOLOGY EUROPEAN HEART HOUSE, February 2011 Basic mechanisms of arrhythmogenesis and antiarrhythmia Antonio Zaza Università
More informationQuantitative Electrophysiology
ECE 795: Quantitative Electrophysiology Notes for Lecture #1 Tuesday, September 18, 2012 1. INTRODUCTION TO EXCITABLE CELLS Historical perspective: Bioelectricity first discovered by Luigi Galvani in 1780s
More informationSimulation of Cardiac Action Potentials Background Information
Simulation of Cardiac Action Potentials Background Information Rob MacLeod and Quan Ni February 7, 2 Introduction The goal of assignments related to this document is to experiment with a numerical simulation
More informationMembrane Potentials, Action Potentials, and Synaptic Transmission. Membrane Potential
Cl Cl - - + K + K+ K + K Cl - 2/2/15 Membrane Potentials, Action Potentials, and Synaptic Transmission Core Curriculum II Spring 2015 Membrane Potential Example 1: K +, Cl - equally permeant no charge
More informationIntroduction to electrophysiology. Dr. Tóth András
Introduction to electrophysiology Dr. Tóth András Topics Transmembran transport Donnan equilibrium Resting potential Ion channels Local and action potentials Intra- and extracellular propagation of the
More informationلجنة الطب البشري رؤية تنير دروب تميزكم
1) Hyperpolarization phase of the action potential: a. is due to the opening of voltage-gated Cl channels. b. is due to prolonged opening of voltage-gated K + channels. c. is due to closure of the Na +
More informationCharacterizing rate-dependent effects of state-specific sodium channel blockers using idealized models
Characterizing rate-dependent effects of state-specific sodium channel blockers using idealized models Abstract Increased propensity for arrhythmias is a well-documented but not well understood side-effect
More information6 Mechanotransduction. rotation
rotation inflow outflow Figure 6.3: Circumferential and uniaxial flow devices applying shear stress to the cell culture. They are stimulated through a circumferential fluid flow generating by a rotating
More informationMaster Thesis. Modelling the Effects of Dofetilide on I Kr Channel Activation using a Markov Model Approach L. Ramekers
Master Thesis Modelling the Effects of Dofetilide on I Kr Channel Activation using a Markov Model Approach L. Ramekers Supervisors: Dr. R.L. Westra J. Heijman MSc Maastricht University Faculty of Humanities
More informationIon Channels. 6 th December, Touqeer Ahmed PhD Atta-ur-Rahman School of Applied Biosciences National University of Sciences and Technology
Ion Channels 6 th December, 2016 Touqeer Ahmed PhD Atta-ur-Rahman School of Applied Biosciences National University of Sciences and Technology Introduction The ion channels of nerve cells are optimally
More informationLESSON 2.2 WORKBOOK How do our axons transmit electrical signals?
LESSON 2.2 WORKBOOK How do our axons transmit electrical signals? This lesson introduces you to the action potential, which is the process by which axons signal electrically. In this lesson you will learn
More informationEffects of Betaxolol on Hodgkin-Huxley Model of Tiger Salamander Retinal Ganglion Cell
Effects of Betaxolol on Hodgkin-Huxley Model of Tiger Salamander Retinal Ganglion Cell 1. Abstract Matthew Dunlevie Clement Lee Indrani Mikkilineni mdunlevi@ucsd.edu cll008@ucsd.edu imikkili@ucsd.edu Isolated
More informationIntroduction and the Hodgkin-Huxley Model
1 Introduction and the Hodgkin-Huxley Model Richard Bertram Department of Mathematics and Programs in Neuroscience and Molecular Biophysics Florida State University Tallahassee, Florida 32306 Reference:
More informationInvariant Manifold Reductions for Markovian Ion Channel Dynamics
Invariant Manifold Reductions for Markovian Ion Channel Dynamics James P. Keener Department of Mathematics, University of Utah, Salt Lake City, UT 84112 June 4, 2008 Abstract We show that many Markov models
More informationBiol2174 Cell Physiology in Health & Disease
Biol2174 Cell Physiology in Health & Disease Lecture 4: Membrane Transport Proteins Kiaran Kirk Research School of Biology Learning objectives To understand: The need for membrane transport proteins in
More informationMembrane Physiology. Dr. Hiwa Shafiq Oct-18 1
Membrane Physiology Dr. Hiwa Shafiq 22-10-2018 29-Oct-18 1 Chemical compositions of extracellular and intracellular fluids. 29-Oct-18 2 Transport through the cell membrane occurs by one of two basic processes:
More informationIonic mechanisms underlying human atrial action potential properties: insights from a mathematical model
Ionic mechanisms underlying human atrial action potential properties: insights from a mathematical model MARC COURTEMANCHE, 1,2 RAFAEL J. RAMIREZ, 1 AND STANLEY NATTEL 1,3,4 1 Research Center, Montreal
More informationIntroduction to electrophysiology 1. Dr. Tóth András
Introduction to electrophysiology 1. Dr. Tóth András Topics Transmembran transport Donnan equilibrium Resting potential Ion channels Local and action potentials Intra- and extracellular propagation of
More informationΝευροφυσιολογία και Αισθήσεις
Biomedical Imaging & Applied Optics University of Cyprus Νευροφυσιολογία και Αισθήσεις Διάλεξη 5 Μοντέλο Hodgkin-Huxley (Hodgkin-Huxley Model) Response to Current Injection 2 Hodgin & Huxley Sir Alan Lloyd
More informationVoltage-clamp and Hodgkin-Huxley models
Voltage-clamp and Hodgkin-Huxley models Read: Hille, Chapters 2-5 (best) Koch, Chapters 6, 8, 9 See also Clay, J. Neurophysiol. 80:903-913 (1998) (for a recent version of the HH squid axon model) Rothman
More informationA note on discontinuous rate functions for the gate variables in mathematical models of cardiac cells
Procedia Computer Science (2) (22) 6 945 95 Procedia Computer Science www.elsevier.com/locate/procedia International Conference on Computational Science ICCS 2 A note on discontinuous rate functions for
More informationPhysiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES
Physiology Unit 2 MEMBRANE POTENTIALS and SYNAPSES Neuron Communication Neurons are stimulated by receptors on dendrites and cell bodies (soma) Ligand gated ion channels GPCR s Neurons stimulate cells
More information6.3.4 Action potential
I ion C m C m dφ dt Figure 6.8: Electrical circuit model of the cell membrane. Normally, cells are net negative inside the cell which results in a non-zero resting membrane potential. The membrane potential
More informationCardiac cell-cell Communication Part 1 Alonso P. Moreno D.Sc. CVRTI, Cardiology
Bioengineering 6003 Cellular Electrophysiology and Biophysics Cardiac cell-cell Communication Part 1 Alonso P. Moreno D.Sc. CVRTI, Cardiology moreno@cvrti.utah.edu November 2010 poster Physiological Relevance
More informationChapter 2 Cellular Homeostasis and Membrane Potential
Chapter 2 Cellular Homeostasis and Membrane Potential 2.1 Membrane Structure and Composition The human cell can be considered to consist of a bag of fluid with a wall that separates the internal, or intracellular,
More informationSingle-Compartment Neural Models
Single-Compartment Neural Models BENG/BGGN 260 Neurodynamics University of California, San Diego Week 2 BENG/BGGN 260 Neurodynamics (UCSD) Single-Compartment Neural Models Week 2 1 / 18 Reading Materials
More information4. Active Behavior of the Cell Membrane 4.1 INTRODUCTION
1 of 50 10/17/2014 10:48 PM 4.1 INTRODUCTION When a stimulus current pulse is arranged to depolarize the resting membrane of a cell to or beyond the threshold voltage, then the membrane will respond with
More informationPhysiology Coloring Book: Panels 29, 32, 33,
ELEC4623/ELEC9734: Semester 2, 2009 Dr Stephen Redmond School of Electrical Engineering & Telecommunications Email: s.redmond@unsw.edu.au Ph: 9385 6101 Rm: 458, ELECENG (G17) Physiology Coloring Book:
More informationResting membrane potential,
Resting membrane potential Inside of each cell is negative as compared with outer surface: negative resting membrane potential (between -30 and -90 mv) Examination with microelectrode (Filled with KCl
More informationPeripheral Nerve II. Amelyn Ramos Rafael, MD. Anatomical considerations
Peripheral Nerve II Amelyn Ramos Rafael, MD Anatomical considerations 1 Physiologic properties of the nerve Irritability of the nerve A stimulus applied on the nerve causes the production of a nerve impulse,
More informationMEMBRANE POTENTIALS AND ACTION POTENTIALS:
University of Jordan Faculty of Medicine Department of Physiology & Biochemistry Medical students, 2017/2018 +++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ Review: Membrane physiology
More informationCELL BIOLOGY - CLUTCH CH. 9 - TRANSPORT ACROSS MEMBRANES.
!! www.clutchprep.com K + K + K + K + CELL BIOLOGY - CLUTCH CONCEPT: PRINCIPLES OF TRANSMEMBRANE TRANSPORT Membranes and Gradients Cells must be able to communicate across their membrane barriers to materials
More informationComputational Neuroscience Summer School Neural Spike Train Analysis. An introduction to biophysical models (Part 2)
Computational Neuroscience Summer School Neural Spike Train Analysis Instructor: Mark Kramer Boston University An introduction to biophysical models (Part 2 SAMSI Short Course 2015 1 Goal: Model this,
More informationMEMBRANE STRUCTURE. Lecture 9. Biology Department Concordia University. Dr. S. Azam BIOL 266/
MEMBRANE STRUCTURE Lecture 9 BIOL 266/4 2014-15 Dr. S. Azam Biology Department Concordia University RED BLOOD CELL MEMBRANE PROTEINS The Dynamic Nature of the Plasma Membrane SEM of human erythrocytes
More informationVoltage-clamp and Hodgkin-Huxley models
Voltage-clamp and Hodgkin-Huxley models Read: Hille, Chapters 2-5 (best Koch, Chapters 6, 8, 9 See also Hodgkin and Huxley, J. Physiol. 117:500-544 (1952. (the source Clay, J. Neurophysiol. 80:903-913
More informationme239 mechanics of the cell me239 mechanics of the cell - final projects 4 6 mechanotransduction downloadable layout file from coursework
6 mechanotransduction downloadable layout file from coursework wong, goktepe, kuhl [2010] me239 mechanics of the cell 1 me239 mechanics of the cell - final projects 2 downloadable sample project downloadable
More informationLecture 2. Excitability and ionic transport
Lecture 2 Excitability and ionic transport Selective membrane permeability: The lipid barrier of the cell membrane and cell membrane transport proteins Chemical compositions of extracellular and intracellular
More informationRahaf Nasser mohammad khatatbeh
7 7... Hiba Abu Hayyeh... Rahaf Nasser mohammad khatatbeh Mohammad khatatbeh Brief introduction about membrane potential The term membrane potential refers to a separation of opposite charges across the
More informationA Model Based Analysis of Steady-State versus Dynamic Elements in the Relationship between Calcium and Force
A Model Based Analysis of Steady-State versus Dynamic Elements in the Relationship between Calcium and Force Casey L. Overby, Sanjeev G. Shroff BACKGROUND Cardiac contraction and calcium. Intracellular
More informationMembrane Currents in Mammalian Ventricular Heart Muscle Fibers Using a Voltage-Clamp Technique
Membrane Currents in Mammalian Ventricular Heart Muscle Fibers Using a Voltage-Clamp Technique GERHARD GIEBISCH and SILVIO WEIDMANN From the Department of Physiology, University of Berne, Berne, Switzerland.
More informationScience Course Descriptions
BIOLOGY I (L) 3024 (BIO I) Biology I is a course based on the following core topics: cellular chemistry, structure and reproduction; matter cycles and energy transfer; interdependence of organisms; molecular
More information9 Generation of Action Potential Hodgkin-Huxley Model
9 Generation of Action Potential Hodgkin-Huxley Model (based on chapter 12, W.W. Lytton, Hodgkin-Huxley Model) 9.1 Passive and active membrane models In the previous lecture we have considered a passive
More informationNerve Signal Conduction. Resting Potential Action Potential Conduction of Action Potentials
Nerve Signal Conduction Resting Potential Action Potential Conduction of Action Potentials Resting Potential Resting neurons are always prepared to send a nerve signal. Neuron possesses potential energy
More informationSynaptic dynamics. John D. Murray. Synaptic currents. Simple model of the synaptic gating variable. First-order kinetics
Synaptic dynamics John D. Murray A dynamical model for synaptic gating variables is presented. We use this to study the saturation of synaptic gating at high firing rate. Shunting inhibition and the voltage
More informationMultiple Mechanisms of Spiral Wave Breakup in a Model of Cardiac Electrical Activity
Multiple Mechanisms of Spiral Wave Breakup in a Model of Cardiac Electrical Activity Flavio H. Fenton and Elizabeth M. Cherry Center for Arrhythmia Research at Hofstra University and The Heart Institute,
More information3.3 Simulating action potentials
6 THE HODGKIN HUXLEY MODEL OF THE ACTION POTENTIAL Fig. 3.1 Voltage dependence of rate coefficients and limiting values and time constants for the Hodgkin Huxley gating variables. (a) Graphs of forward
More informationCOGNITIVE SCIENCE 107A
COGNITIVE SCIENCE 107A Electrophysiology: Electrotonic Properties 2 Jaime A. Pineda, Ph.D. The Model Neuron Lab Your PC/CSB115 http://cogsci.ucsd.edu/~pineda/cogs107a/index.html Labs - Electrophysiology
More informationBo Deng University of Nebraska-Lincoln UNL Math Biology Seminar
Mathematical Model of Neuron Bo Deng University of Nebraska-Lincoln UNL Math Biology Seminar 09-10-2015 Review -- One Basic Circuit By Kirchhoff's Current Law 0 = I C + I R + I L I ext By Kirchhoff s Voltage
More informationModel-Order Reduction of Ion Channel Dynamics Using Approximate Bisimulation
Manuscript (PDF) Model-Order Reduction of Ion Channel Dynamics Using Approximate Bisimulation Md. Ariful Islam a,, Abhishek Murthy a,, Ezio Bartocci b, Elizabeth M. Cherry e, Flavio H. Fenton c, James
More informationVertebrate Physiology 437 EXAM I 26 September 2002 NAME
437 EXAM1.DOC Vertebrate Physiology 437 EXAM I 26 September 2002 NAME 0. When you gaze at the stars, why do you have to look slightly away from the really faint ones in order to be able to see them? (1
More informationCELLULAR NEUROPHYSIOLOGY CONSTANCE HAMMOND
CELLULAR NEUROPHYSIOLOGY CONSTANCE HAMMOND Chapter 1 Zoom in on Patch configurations In the jargon of electrophysiologists, a patch is a piece of neuronal membrane. Researchers invented a technique known
More informationThe Department of Electrical Engineering. nkrol Mentors: Dr. Mohammad Imtiaz, Dr. Jing Wang & Dr. In Soo Ahn
Bradley University The Department of Electrical Engineering nkrol Mentors: Dr. Mohammad Imtiaz, Dr. Jing Wang & Dr. In Soo Ahn AN ELECTRICAL ENGINEERING PERSPECTIVE OF THE HUMAN HEART This research project
More informationINVESTIGATING THE FUNCTION OF KCNE4 IN CARDIAC PHYSIOLOGY. Erin Julia Ciampa. Dissertation. Submitted to the Faculty of the
INVESTIGATING THE FUNCTION OF KCNE4 IN CARDIAC PHYSIOLOGY By Erin Julia Ciampa Dissertation Submitted to the Faculty of the Graduate School of Vanderbilt University in partial fulfillment of the requirements
More informationOrigins of Spiral Wave Meander and Breakup in a Two-Dimensional Cardiac Tissue Model
Annals of Biomedical Engineering, Vol. 28, pp. 755 771, 2000 Printed in the USA. All rights reserved. 0090-6964/2000/28 7 /755/17/$15.00 Copyright 2000 Biomedical Engineering Society Origins of Spiral
More informationQUESTION? Communication between neurons depends on the cell membrane. Why is this so?? Consider the structure of the membrane.
QUESTION? Communication between neurons depends on the cell membrane Why is this so?? Consider the structure of the membrane. ECF ICF Possible ANSWERS?? Membrane Ion Channels and Receptors: neuron membranes
More informationAction potentials. Conductances channels
Action potentials Conductances channels Cole and Curtis AC Wheatstone bridge resistance decreased during action potential R1 & R2 divide one path, Rv (variable) and Ru divide the other Galvanometer between
More informationAll-or-None Principle and Weakness of Hodgkin-Huxley Mathematical Model
All-or-None Principle and Weakness of Hodgkin-Huxley Mathematical Model S. A. Sadegh Zadeh, C. Kambhampati International Science Index, Mathematical and Computational Sciences waset.org/publication/10008281
More informationSupplementary information. A proposal for a novel impact factor as an alternative to the JCR impact factor
Supplementary information A proposal for a novel impact factor as an alternative to the JCR impact factor Zu-Guo Yang a and Chun-Ting Zhang b, * a Library, Tianjin University, Tianjin 300072, China b Department
More informationGPU-Enabled Spatiotemporal Model of Stochastic Cardiac Calcium Dynamics and Arrhythmias
GPU-Enabled Spatiotemporal Model of Stochastic Cardiac Calcium Dynamics and Arrhythmias M. Saleet Jafri Hoang Trong Minh Tuan Department of Bioinformatics and Computational Biology George Mason University
More informationSupplementary Figure 1
Supplementary Figure 1 Activation of P2X2 receptor channels in symmetric Na + solutions only modestly alters the intracellular ion concentration. a,b) ATP (30 µm) activated P2X2 receptor channel currents
More informationSlide 1. Slide 2. Membrane Transport Mechanisms II and the Nerve Action Potential. Epithelia
Slide 1 Membrane Transport Mechanisms II and the Nerve Action Potential Slide 2 Apical Basolateral Epithelia Microvilli Tight junction Basal Lamina Lie on a sheet of connective tissue (basal lamina) Tight
More informationParticles with opposite charges (positives and negatives) attract each other, while particles with the same charge repel each other.
III. NEUROPHYSIOLOGY A) REVIEW - 3 basic ideas that the student must remember from chemistry and physics: (i) CONCENTRATION measure of relative amounts of solutes in a solution. * Measured in units called
More informationModule Membrane Biogenesis and Transport Lecture 15 Ion Channels Dale Sanders
Module 0220502 Membrane Biogenesis and Transport Lecture 15 Ion Channels Dale Sanders 9 March 2009 Aims: By the end of the lecture you should understand The principles behind the patch clamp technique;
More informationEEE105 Teori Litar I Chapter 7 Lecture #3. Dr. Shahrel Azmin Suandi Emel:
EEE105 Teori Litar I Chapter 7 Lecture #3 Dr. Shahrel Azmin Suandi Emel: shahrel@eng.usm.my What we have learnt so far? Chapter 7 introduced us to first-order circuit From the last lecture, we have learnt
More informationDecoding. How well can we learn what the stimulus is by looking at the neural responses?
Decoding How well can we learn what the stimulus is by looking at the neural responses? Two approaches: devise explicit algorithms for extracting a stimulus estimate directly quantify the relationship
More informationme239 mechanics of the cell - syllabus me239 mechanics of the cell me239 mechanics of the cell - grading me239 mechanics of the cell - overview
6 mechanotransduction wong, goktepe, kuhl [2010] me239 mechanics of the cell add l information http://biomechanics.stanford.edu and coursework 1 me239 mechanics of the cell - syllabus favorite topics in
More informationResting Membrane Potential
Resting Membrane Potential Fig. 12.09a,b Recording of Resting and It is recorded by cathode ray oscilloscope action potentials -70 0 mv + it is negative in polarized (resting, the membrane can be excited)
More informationQuantitative Electrophysiology
ECE 795: Quantitative Electrophysiology Notes for Lecture #4 Wednesday, October 4, 2006 7. CHEMICAL SYNAPSES AND GAP JUNCTIONS We will look at: Chemical synapses in the nervous system Gap junctions in
More informationMuscle tissue. Types. Functions. Cardiac, Smooth, and Skeletal
Types Cardiac, Smooth, and Skeletal Functions movements posture and body position Support soft tissues Guard openings body temperature nutrient reserves Muscle tissue Special Characteristics of Muscle
More informationModeling action potential generation and propagation in NRK fibroblasts
Am J Physiol Cell Physiol 287: C851 C865, 2004. First published May 12, 2004; 10.1152/ajpcell.00220.2003. Modeling action potential generation and propagation in NRK fibroblasts J. J. Torres, 1,2 L. N.
More information(Na++ K +)-ATPase in artificial lipid vesicles: influence of the concentration of mono- and divalent cations on the pumping rate
254 Biochimica et Biophysica Acta 862 (1986) 254-264 Elsevier BBA 72961 (Na++ K +)-ATPase in artificial lipid vesicles: influence of the concentration of mono- and divalent cations on the pumping rate
More informationElectrophysiological Modeling of Membranes and Cells
Bioeng 6460 Electrophysiology and Bioelectricity Electrophysiological Modeling of Membranes and Cells Frank B. Sachse fs@cvrti.utah.edu Overview Motivation and Principles Electrical Modeling of Membranes
More informationGeneral Physics. Nerve Conduction. Newton s laws of Motion Work, Energy and Power. Fluids. Direct Current (DC)
Newton s laws of Motion Work, Energy and Power Fluids Direct Current (DC) Nerve Conduction Wave properties of light Ionizing Radiation General Physics Prepared by: Sujood Alazzam 2017/2018 CHAPTER OUTLINE
More informationCoupled dynamics of voltage and calcium in paced cardiac cells
Coupled dynamics of voltage and calcium in paced cardiac cells Yohannes Shiferaw, 1,2 Daisuke Sato, 1 and Alain Karma 1 1 Department of Physics and Center for Interdisciplinary Research on Complex Systems,
More informationBA, BSc, and MSc Degree Examinations
Examination Candidate Number: Desk Number: BA, BSc, and MSc Degree Examinations 2017-8 Department : BIOLOGY Title of Exam: Molecular Biology and Biochemistry Part I Time Allowed: 1 hour and 30 minutes
More informationSignal processing in nervous system - Hodgkin-Huxley model
Signal processing in nervous system - Hodgkin-Huxley model Ulrike Haase 19.06.2007 Seminar "Gute Ideen in der theoretischen Biologie / Systembiologie" Signal processing in nervous system Nerve cell and
More informationNerves and their impulses. Biology 12 C-11
Nerves and their impulses Biology 12 C-11 Nerves and their impulses Nerves are designed to transmit electrical impulses from the dendrites, over the cell body and through the axon. The impulse will then
More informationMembrane Protein Channels
Membrane Protein Channels Potassium ions queuing up in the potassium channel Pumps: 1000 s -1 Channels: 1000000 s -1 Pumps & Channels The lipid bilayer of biological membranes is intrinsically impermeable
More informationVoltage-dependent gating of ion channels Prof. Keith S. Elmslie
Voltage-Dependent Gating of Ion Channels Department of Pharmacology A.T. Still University Kirksville College of Osteopathic Medicine 1 The action potential (AP) E Na Threshold The N eur onal AP Sensory
More informationReproducing Cardiac Restitution Properties Using the Fenton Karma Membrane Model
Annals of Biomedical Engineering, Vol. 33, No. 7, July 2005 ( 2005) pp. 907 911 DOI: 10.1007/s10439-005-3948-3 Reproducing Cardiac Restitution Properties Using the Fenton Karma Membrane Model ROBERT A.
More informationR7.3 Receptor Kinetics
Chapter 7 9/30/04 R7.3 Receptor Kinetics Professional Reference Shelf Just as enzymes are fundamental to life, so is the living cell s ability to receive and process signals from beyond the cell membrane.
More informationIon Channel Structure and Function (part 1)
Ion Channel Structure and Function (part 1) The most important properties of an ion channel Intrinsic properties of the channel (Selectivity and Mode of Gating) + Location Physiological Function Types
More informationSECOND PUBLIC EXAMINATION. Honour School of Physics Part C: 4 Year Course. Honour School of Physics and Philosophy Part C C7: BIOLOGICAL PHYSICS
2757 SECOND PUBLIC EXAMINATION Honour School of Physics Part C: 4 Year Course Honour School of Physics and Philosophy Part C C7: BIOLOGICAL PHYSICS TRINITY TERM 2011 Monday, 27 June, 9.30 am 12.30 pm Answer
More information