Modeling. EC-Coupling and Contraction
|
|
- Rosemary Lynch
- 6 years ago
- Views:
Transcription
1 Bioeng 6460 Electrophysiology and Bioelectricity Modeling of EC-Coupling and Contraction Frank B. Sachse
2 Overview Recapitulation Group Work Excitation-Contraction Coupling Hill s Muscle Model Sarcomere Modeling Coupling to Electrophysiological Models 3D Simulations Summary Bioeng 6460: Electrophysiology and Bioelectricity - Page 2
3 Group Work: Most Important States of Force Model Work in pairs of 2 Time 5 min Several proteins are involved in force development changing their configuration depending on e.g. Ca concentration and other proteins configurations. Which states would you consider most important for modeling? Bioeng 6460: Electrophysiology and Bioelectricity - Page 3
4 Models of Force Development 1938 today Hill Skeletal muscle Frog Huxley Skeletal muscle - Wong Cardiac muscle - Panerai Papillary muscle Mammalian Peterson, Hunter, Berman Papillary muscle Rabbit Landesberg, Sideman Skinned cardiac - myocytes Hunter, Nash, Sands Cardiac muscle Mammalian Noble, Varghese, Kohl, Noble Ventricular muscle Guinea pig Rice, Winslow, Hunter Papillary muscle Guinea pig Rice, Jafri, Winslow Cardiac muscle Ferret Glänzel, Sachse, Seemann Ventricular myocytes Human Bioeng 6460: Electrophysiology and Bioelectricity - Page 4
5 Hill s Model of Muscle Contraction (1924/1938) Measurement Muscle is fixed at length l 0 Electrical stimulation Isometric, tetanus with max. mechanical tension P 0 Release of fixation Force F is applied with F=mg g: Gravitational constant m: Mass Measurement of time t, when muscle passes mark at length l Calculation of velocity Mark l M u s c l e l 0 Fixation v = l 0! l t m F Bioeng 6460: Electrophysiology and Bioelectricity - Page 5
6 Relationship between Mass and Contraction Velocity Contraction of frog skeletal muscle Contraction velocity v [m/s] measured value Mass [g] Bioeng 6460: Electrophysiology and Bioelectricity - Page 6
7 Modeling of Muscle Contraction ( v + b) ( P + a) = b( P 0 + a) P: Spannung Tension des of muscle Muskels " # $ N m 2 P 0 : Maximale Spannung tension of des muscle Muskels v: Kontraktionsgeschwindigkeit Contraction velocity % &' " m% # $ s &' " # $ N m 2 a,b: Konstanten Constants depending abhängig von l 0 l,, temperature, Temperatur, Ca Concentration -Ionenkonzentration, of Ca,... % & ' m Elastic Element Contractile Element Bioeng 6460: Electrophysiology and Bioelectricity - Page 7
8 Model Extension: Hill s 3-Element Model (1970) Limitations of Hill s Model only force-velocity relationship only tetanized muscle, no information of partial or not stimulated muscle only serial elastic element only quick responses Hills 3-Element Model Inclusion of parallel elastic element Elastic parallel element Elastic serial element Contractile element m Bioeng 6460: Electrophysiology and Bioelectricity - Page 8
9 Modeling of Cellular Force Development [Ca] i /µm F/F maxi t [s] Intracellular concentration of calcium Calculated with electrophysiological cell models t [s] Processes in myofilaments State of troponins, tropomyosins and cross bridges t [s] Force Development System of coupled ordinary differential equations System of coupled ordinary differential equations Bioeng 6460: Electrophysiology and Bioelectricity - Page 9
10 4-State Model of Force Development: State Diagram N0 g N1 Force k l (Ca i ) k -1 (Ca i ) k m (Ca i ) k m (Ca i ) T0 Ca bound f g T1 Ca bound Force Description by set of 1st order ODEs Transfer of states N0, N1, T0, and T1 is dependent of rate coefficients Rate coefficients are partly function of intracellular calcium [Ca 2+ ] i (Model 1 of Rice 1999 et al./ Landesberg et al.1994) Bioeng 6460: Electrophysiology and Bioelectricity - Page 10
11 4-State Model of Force Development Several states contribute to force development: F = " F : T1+ N1 F max Normalized force [N/N] F max : Maximal simulated force " : Myofilament overlap function Force is dependent on overlap of actin and myosin filaments. Frank-Starling Mechanism Force ~ initial length Diastolic volume ~ cardiac output! Bioeng 6460: Electrophysiology and Bioelectricity - Page 11
12 4-State Model of Force Development: Matrix Notation # " % % " t % $ N 0 T 0 T 1 N 1 & # ( % ( = % ( % ' $ )K l k l 0 g 0 + g 1 V K l )f ) k l g 0 + g 1 V 0 0 f )g 0 ) g 1 V ) k )l K l 0 0 k )l )g 0 ) g 1 V ) K l &# (% (% (% ' $ N 0 T 0 T 1 N 1 & ( ( ( ' Ca i " T0 T1 Transfer Rate constants: coefficients: K l,k l, f, g 0, g 1,k ) l und V States of Troponin Calcium Cross bridges N 0 unbound weak T 0 bound weak T 1 bound strong N 1 unbound strong t [s] Numerical solution e.g. with Euler- and Runge-Kutta-methods Bioeng 6460: Electrophysiology and Bioelectricity - Page 12
13 3rd Model of Rice 1999 et al.: State Diagram States of Troponin States of Tropomyosin and cross bridges (XB) T unbound N0 0 XB g N1 1 XB k on k off k 1 (TCa,SL) k -1 k -1 k 1 (TCa,SL) TCa bound P0 Permissive 0 XB f g P1 Permissive 1 XB Bioeng 6460: Electrophysiology and Bioelectricity - Page 13
14 3rd Model of Rice 1999 et al.: Matrix Notation y =! T $ # & " TCa% # y = "k on[ca] % $ k on [Ca] k off "k off & ( y ' States of Troponin Transitions x =! # # # " N 0 P 0 P 1 N 1 $ & & & % x = ( ) 0 g0 ( )! f g0 0 ( ) k 1 ( )!g! k 1 "!k 1 k!1 TCa,SL $ k 1 -k!1 TCa,SL $ $ $ # 0 f!g! k!1 TCa,SL 0 0 k!1 TCa,SL % ' ' x ' ' & States of Tropomyosin and cross bridges Transitions Rice et al. Model 3, 1999 Bioeng 6460: Electrophysiology and Bioelectricity - Page 14
15 Force Development for Different Static Sarcomere Lengths (SL) Force normalized with maximal force [N/N] time [s] Bioeng 6460: Electrophysiology and Bioelectricity - Page 15
16 Model of Glänzel et al. 2002: Activation [Ca] I, #, XB T TCa TCa, TM on TM off TM on T Troponin TCa Troponin with bound calcium TM off Tropomyosin in nonpermissive state TM on Tropomyosin in permissive state # Stretch XB Cross-bridges [Ca] I Free calcium in intracellular fluid Ca-binding to Troponin C Shifting of Tropomyosin (Glänzel, Diploma Thesis, IBT, Universität Karlsruhe (TH), 2002, Sachse, Glänzel, and Seemann, IJBC, 2003, Sachse, Glänzel, and Seemann, LNCS 2674, 2003) Cooperativity mechanisms XB-TN TM-TM Bioeng 6460: Electrophysiology and Bioelectricity - Page 16
17 Model of Glänzel et al. 2002: Crossbridge Cycling v M ATP A M ATP v M v A M v A M ADP A Actin M Myosin ATP Adenosine triphospate ADP Adenosine diphosphate P i Phosphate # Stretch v Velocity of filaments XB Cross-bridges weakly coupled strong binding M ADP P i v M ADP v A M ADP Cooperativity mechanism v A M ADP P i TM on, #, XB A M ADP P i XB-XB Bioeng 6460: Electrophysiology and Bioelectricity - Page 17
18 Reconstruction of Static Measurements Study Species: rat Ventricular myocytes Resting length ~ 2µm Protocol Intracellular calcium concentration [Ca 2+ ] i controlled Stretch varied Isometric measurement Normalized Force [N/N] Normalized Force [N/N] Calcium concentration [µm] Measurement ter Keurs et al. 00 Normalized Force [N/N] Normalized Force [N/N] Calcium concentration [µm] Model of Glänzel et al. 02 Calcium concentration [µm] Calcium concentration [µm] Model Peterson et al. 91 3rd model Rice et al. 99 Bioeng 6460: Electrophysiology and Bioelectricity - Page 18
19 Reconstruction of Length Switch Experiments Study Species: rabbit Ventricular myocytes Length Switch Experiment Stretch of 4.6% in 10 ms Return to original configuration in 10 ms Measurement Peterson et al. 91 Normalized Force [N/N] Normalized Force [N/N] Normalized Force [N/N] t [s] Model of Glänzel et al. 02 t [s] t [s] Model Peterson et al. 91 3rd model Rice et al. 99 Bioeng 6460: Electrophysiology and Bioelectricity - Page 19
20 Coupling of Force with Electrophysiological Models: Basics Noble-Varghese-Kohl-Noble model Rice-Winslow-Hunter model 1 Stimulus at t=35 ms Sarcomere stretch # Bioeng 6460: Electrophysiology and Bioelectricity - Page 20
21 Coupling of Force with Electrophysiological Models Luo-Rudy model (Guinea pig ventricular) Rice-Winslow-Hunter model 3 (rabbit ventricular) Stimulus at t=35 ms Sarcomere stretch # Species don t fit Bioeng 6460: Electrophysiology and Bioelectricity - Page 21
22 Coupling of Force with Electrophysiological Models Noble-Varghese-Kohl-Noble model (Guinea pig ventricular) Rice-Winslow-Hunter model 3rd (rabbit ventricular) Stimulus at t=35 ms Sarcomere stretch # Differences in force development due to differences of Ca transient Bioeng 6460: Electrophysiology and Bioelectricity - Page 22
23 Coupling of Force with Electrophysiological Model: Human Priebe-Beuckelmann model (human ventricular) Glänzel et al. model (human ventricular) Stimulus at t=35 ms with frequency Sarcomere stretch # Validation of hybrid models with measured data necessary! Bioeng 6460: Electrophysiology and Bioelectricity - Page 23
24 Modeling Force Development with Cellular Automaton Anatomical Model Physiological Parameters Cellular Automaton Force Transmembrane voltage Calcium concentration F/F maxi t [s] Bioeng 6460: Electrophysiology and Bioelectricity - Page 24
25 Parameters for Simulation: Lookup Tables Known per volume element dv and for time t dv Force (t S ) (instead of transmembrane voltage) Refractory period (t S ) Stimulus Time since activation t S Stimulus frequency f Tissue type Autorhythmicity (t S ) Conduction velocity (f) Excitable neighborhood (constant) Bioeng 6460: Electrophysiology and Bioelectricity - Page 25
26 Modeling of Force Development: Sinus Rhythm Bioeng 6460: Electrophysiology and Bioelectricity - Page 26
27 Modeling of Force Development: Coupling Normalized Force Transmembrane Voltage Bioeng 6460: Electrophysiology and Bioelectricity - Page 27
28 Summary Recapitulation Group Work Excitation-Contraction Coupling Hill Model Sarcomere Modeling Coupling to Electrophysiological Models 3D Simulations Bioeng 6460: Electrophysiology and Bioelectricity - Page 28
Computational Modeling of the Cardiovascular and Neuronal System
BIOEN 6900 Computational Modeling of the Cardiovascular and Neuronal System Modeling of Force Development in Myocytes Overview Recapitulation Modeling of Conduction Modeling of Force in Skeletal Muscle
More informationCellular Electrophysiology and Biophysics
BIOEN 6003 Cellular Electrophysiology and Biophysics Modeling of Force Development in Myocytes II Frank B. Sachse, University of Utah Overview Experimental Studies Sliding Filament Theory Group work Excitation-Contraction
More informationModeling. EC-Coupling and Contraction
Bioeng 6460 Electrophysiology and Bioelectricity Modeling of EC-Coupling and Contraction Frank B. Sachse fs@cvrti.utah.edu Overview Quiz Excitation-Contraction Coupling Anatomy Cross Bridge Binding Coupling
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 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 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 informationThe molecular basis of cardiac mechanics: Regulation of motor unit recruitment.
1of 4 The molecular basis of cardiac mechanics: Regulation of motor unit recruitment. C. Levy, A. Landesberg Department of Biomedical Engineering, Technion-Israel Institute of Technology, Haifa, Israel.
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 informationLecture 13, 05 October 2004 Chapter 10, Muscle. Vertebrate Physiology ECOL 437 University of Arizona Fall instr: Kevin Bonine t.a.
Lecture 13, 05 October 2004 Chapter 10, Muscle Vertebrate Physiology ECOL 437 University of Arizona Fall 2004 instr: Kevin Bonine t.a.: Nate Swenson Vertebrate Physiology 437 18 1. Muscle A. Sarcomere
More informationComputer Science Department Technical Report. University of California. Los Angeles, CA
Computer Science Department Technical Report University of California Los Angeles, CA 995-1596 COMPUTER SIMULATION OF THE JAFRI-WINSLOW ACTION POTENTIAL MODEL Sergey Y. Chernyavskiy November 1998 Boris
More informationActive contraction of cardiac cells: a reduced model for sarcomere dynamics with cooperative interactions
MOX-Report No. 48/217 Active contraction of cardiac cells: a reduced model for sarcomere dynamics with cooperative interactions Regazzoni, F.; Dedè, L.; Quarteroni, A. MOX, Dipartimento di Matematica Politecnico
More informationPHYSIOLOGY CHAPTER 9 MUSCLE TISSUE Fall 2016
PHYSIOLOGY CHAPTER 9 MUSCLE TISSUE Fall 2016 2 Chapter 9 Muscles and Muscle Tissue Overview of Muscle Tissue types of muscle: are all prefixes for muscle Contractility all muscles cells can Smooth & skeletal
More informationMembrane Potential. 1. Resting membrane potential (RMP): 2. Action Potential (AP):
Membrane Potential 1. Resting membrane potential (RMP): 2. Action Potential (AP): Resting Membrane Potential (RMP) It is the potential difference across the cell membrane. If an electrode of a voltmeter
More informationModelling Muscle Contraction a multiscale approach
Porto Ercole, M&MKT 2016 Multiscale Systems from Particles to Continuum: Modelling and Computation Modelling Muscle Contraction a multiscale approach Giovanni Naldi Dipartimento di Matematica ``F. Enriques
More informationSimulation Analysis of Cardiac Muscle Isotonic Contractions at Different Pre- and Afterloads
18 The Open Physiology Journal, 2009, 2, 18-37 Open Access Simulation Analysis of Cardiac Muscle Isotonic Contractions at Different Pre- and Afterloads Natalie S. Schneider*,1,2 and Akira Amano 2 1 Cell/Biodynamics
More informationCardiac mechanoenergetics replicated by cross-bridge model Vendelin, M.; Bovendeerd, P.H.M.; Arts, M.G.J.; Engelbrecht, J.; van Campen, D.H.
Cardiac mechanoenergetics replicated by cross-bridge model Vendelin, M.; Bovendeerd, P.H.M.; Arts, M.G.J.; Engelbrecht, J.; van Campen, D.H. Published in: Annals of Biomedical Engineering DOI: 10.1114/1.1305910
More informationIonic Charge Conservation and Long-Term Steady State in the Luo Rudy Dynamic Cell Model
3324 Biophysical Journal Volume 81 December 2001 3324 3331 Ionic Charge Conservation and Long-Term Steady State in the Luo Rudy Dynamic Cell Model Thomas J. Hund,* Jan P. Kucera,* Niels F. Otani,* and
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 informationA Mathematical Model for β1-adrenergic Regulation of the Mouse Ventricular Myocyte Contraction
Georgia State University ScholarWorks @ Georgia State University Mathematics Dissertations Department of Mathematics and Statistics 5-10-2017 A Mathematical Model for β1-adrenergic Regulation of the Mouse
More informationA Cross-Bridge Model Describing the Mechanoenergetics of Actomyosin Interaction
A Cross-Bridge Model Describing the Mechanoenergetics of Actomyosin Interaction Mari Kalda, Pearu Peterson, Jüri Engelbrecht, Marko Vendelin Abstract In order to study the mechanical contraction and energy
More informationthe axons of the nerve meet with the muscle cell.
Steps to Contraction 1. A nerve impulse travels to the neuromuscular junction on a muscle cell. The neuromuscular junction is the point where the axons of the nerve meet with the muscle cell. 2. Ach is
More informationA Metabolite-Sensitive, Thermodynamically Constrained Model of Cardiac Cross-Bridge Cycling: Implications for Force Development during Ischemia
Biophysical Journal Volume 98 January 2010 267 276 267 A Metabolite-Sensitive, Thermodynamically Constrained Model of Cardiac Cross-Bridge Cycling: Implications for Force Development during Ischemia Kenneth
More informationBIOMECHANICS 3 Origins and consequences of forces in biological systems
BIOMECHANICS 3 Origins and consequences of forces in biological systems MOLECULAR MECHANISMS OF BIOLOGICAL MOVEMENT AT THE LEVELOF ORGANISMS MOLECULAR BASIS OF MUSCLE CONTRACTION DR. BEÁTA BUGYI - BIOPHYSICS
More information(pca is -log [Ca2+]) relationships in rabbit skinned psoas muscle fibres at mean
Journal of Physiology (1991), 440, pp. 273-289 273 With 6 figures Printed in Great Britain SUBSTITUTION OF CARDIAC TROPONIN C INTO RABBIT MUSCLE DOES NOT ALTER THE LENGTH DEPENDENCE OF Ca2l SENSITIVITY
More informationStiffness-distortion sarcomere model for muscle simulation
Stiffness-distortion sarcomere model for muscle simulation MARIA V. RAZUMOVA, 1,3 ANNA E. BUKATINA, 1,4 AND KENNETH B. CAMPBELL 1,2 Departments of 1 Veterinary and Comparative Anatomy, Pharmacology and
More informationUNIT 6 THE MUSCULAR SYSTEM
UNIT 6 THE MUSCULAR SYSTEM I. Functions of Muscular System A. Produces Movement Internal vs. External «locomotion & manipulation «circulate blood & maintain blood pressure «move fluids, food, baby B. Maintaining
More informationSignificant Impact on Muscle Mechanics of Small Nonlinearities in Myofilament Elasticity
Biophysical Journal Volume 99 September 21 1869 1875 1869 Significant Impact on Muscle Mechanics of Small Nonlinearities in Myofilament Elasticity Alf Månsson* School of Natural Sciences, Linnaeus University,
More informationThe Molecules of Movement Musc 1 - Professor Michael Ferenczi
The Molecules of Movement Musc 1 - Professor Michael Ferenczi (m.ferenczi@imperial.ac.uk) 1. Appreciate that there are a large number of molecular motors, each with its assigned role. 2. Linear molecular
More informationAccording to the diagram, which of the following is NOT true?
Instructions: Review Chapter 44 on muscular-skeletal systems and locomotion, and then complete the following Blackboard activity. This activity will introduce topics that will be covered in the next few
More informationSpatially explicit, nano-mechanical models of the muscle half-sarcomere: Implications for biomechanical tuning in atrophy and fatigue
Acta Astronautica 6 (27) 8 www.elsevier.com/locate/actaastro Spatially explicit, nano-mechanical models of the muscle half-sarcomere: Implications for biomechanical tuning in atrophy and fatigue Aya Kataoka
More informationRelaxation Kinetics Following Sudden Ca 2 Reduction in Single Myofibrils from Skeletal Muscle
2142 Biophysical Journal Volume 83 October 2002 2142 2151 Relaxation Kinetics Following Sudden Ca 2 Reduction in Single Myofibrils from Skeletal Muscle Chiara Tesi, Nicoletta Piroddi, Francesco Colomo,
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 informationOur patient for the day...
Muscles Ch.12 Our patient for the day... Name: Eddy Age: Newborn Whole-body muscle contractions No relaxation Severe difficulty breathing due to inadequate relaxation of breathing muscles Diagnosed with
More informationChapter 16. Cellular Movement: Motility and Contractility. Lectures by Kathleen Fitzpatrick Simon Fraser University Pearson Education, Inc.
Chapter 16 Cellular Movement: Motility and Contractility Lectures by Kathleen Fitzpatrick Simon Fraser University Two eukaryotic motility systems 1. Interactions between motor proteins and microtubules
More informationsignificant quantities are also thought to be produced by ATP splitting by the (Received 4 May 1984) length decreases below 2-20,um.
J. Phy8iol. (1984), 357, pp. 495-504 495 With 3 text-fgurem Printed in Great Britain THE SARCOMERE LENGTH DEPENDENCE OF THE RATE OF HEAT PRODUCTION DURING ISOMETRIC TETANIC CONTRACTION OF FROG MUSCLES
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 informationTISSUE. A) Types. (i)
MUSCLES & MUSCLE TISSUE I. OVERVIEW - Muscle ( little mouse ) - tissue designed to cause movementt thru contraction ( shortening ). A) Types - There are some SIMILARITIES between muscle types: (i) All
More informationFundamentals of Neurosciences. Smooth Muscle. Dr. Kumar Sambamurti 613-SEI; ;
Fundamentals of Neurosciences Smooth Muscle Dr. Kumar Sambamurti 613-SEI; 792-4315; sambak@musc.edu 1 Smooth Muscle Structure Cells much smaller than skeletal muscle (2-5µM diam, 100-400µM long) Single
More informationSlide 1. Slide 2. Slide 3. Muscles general information. Muscles - introduction. Microtubule Function
Slide 1 Muscles general information Vertebrates and many invertebrates have three main classes of muscle Skeletal muscle connect bones are are used for complex coordianted activities. Smooth muscles surround
More informationA Simple Model with Myofilament Compliance Predicts Activation- Dependent Crossbridge Kinetics in Skinned Skeletal Fibers
Biophysical Journal Volume 83 December 2002 3425 3434 3425 A Simple Model with Myofilament Compliance Predicts Activation- Dependent Crossbridge Kinetics in Skinned Skeletal Fibers D. A. Martyn,* P. B.
More informationCalcium, Cross-Bridges, and the Frank-Starling Relationship
ATP. This methodology should help to elucidate the pathways involved in regulated release of nucleotide from intact cells. References 1. Anderson CM and Parkinson FE. Potential signaling roles for UTP
More informationSarcomere Lattice Geometry Influences Cooperative Myosin Binding in Muscle
Sarcomere Lattice Geometry Influences Cooperative Myosin Binding in Muscle Bertrand C. W. Tanner 1, Thomas L. Daniel 2, Michael Regnier 1* 1 Department of Bioengineering, University of Washington, Seattle,
More informationBioelectricity Prof. Mainak Das Department of Biological Sciences, and Bioengineering Indian Institute of Technology, Kanpur.
Bioelectricity Prof. Mainak Das Department of Biological Sciences, and Bioengineering Indian Institute of Technology, Kanpur Lecture 17 Welcome back to the bioelectricity lecture, series. So, in the last
More information(Be sure to clearly state the principles addressed in your discussion.)
CELL QUESTION 1992: AP BIOLOGY A laboratory assistant prepared solutions of 0.8 M, 0.6 M, 0.4 M, and 0.2 M sucrose, but forgot to label them. After realizing the error, the assistant randomly labeled the
More informationTheeffectofmusclefatigueonthebehaviorofsinglemusclefibre
Applied and Computational Mechanics 1 (2007) 401-410 Theeffectofmusclefatigueonthebehaviorofsinglemusclefibre L.Číhalová a, a Faculty of AppliedSciences, University of WestBohemiainPilsen, Univerzitní
More informationcycle of the isometrically contracting state); bridges; and in both cases, there was an additional
THE JOURNAL OF BIOLOGICAL CHEMlSTRY 0 1987 by The American Society for Biochemistq ' and Molecular Biology, Inc Vol. 262, No.28, Issue of October 5, PP. 13627-13635,1987 Printed in U. S. A. Effect of Rigor
More informationNavigation (Chapter 16)
Lecture 13, 04 Oct 2005 Chapter 16 & 17 Navigation & Muscle Function Vertebrate Physiology ECOL 437 (aka MCB 437, VetSci 437) University of Arizona Fall 2005 Vertebrate Physiology 437 Chapter 16 1. Navigation
More informationLecture 13, 04 Oct 2005 Chapter 16 & 17 Navigation & Muscle Function
Lecture 13, 04 Oct 2005 Chapter 16 & 17 Navigation & Muscle Function Vertebrate Physiology ECOL 437 (aka MCB 437, VetSci 437) University of Arizona Fall 2005 instr: Kevin Bonine t.a.: Kristen Potter 1
More informationLawrence Davis Yates*
Lawrence Davis Yates* Introduction provide a cornerstone to our understanding of a regulatory mechanism. A factor from muscle homogenates was found by Marsh (1952)to relax myofibrils previously contracted
More informationA Spatially Explicit Nanomechanical Model of the Half-Sarcomere: Myofilament Compliance Affects Ca 2+ -Activation
Annals of Biomedical Engineering, Vol. 32, No. 11, November 2004 ( 2004) pp. 1559 1568 A Spatially Explicit Nanomechanical Model of the Half-Sarcomere: Myofilament Compliance Affects Ca 2+ -Activation
More informationTHE PHYSIOLOGY OF STRIATED MUSCLE
fir. J. Anatsth. (1980), 52, 111 THE PHYSIOLOGY OF STRIATED MUSCLE K. FLOYD The purpose of this article is to present current views on the physiology of striated muscle, and in particular on the mechanism
More informationCoupling of Adjacent Tropomyosins Enhances Cross-Bridge-Mediated Cooperative Activation in a Markov Model of the Cardiac Thin Filament
224 iophysical Journal Volume 98 May 2 224 224 Coupling of Adjacent Tropomyosins Enhances Cross-ridge-Mediated Cooperative Activation in a Markov Model of the Cardiac Thin Filament Stuart G. Campbell,
More informationReview Article Poorly Understood Aspects of Striated Muscle Contraction
BioMed Research International Volume 2015, Article ID 245154, 28 pages http://dx.doi.org/10.1155/2015/245154 Review Article Poorly Understood Aspects of Striated Muscle Contraction Alf Månsson, 1 Dilson
More informationEvidence That the Velocity of Sarcomere Shortening in Single Frog Atrial Cardiac Cells is Load Dependent
200 CIRCULATION RESEARCH VOL. 48, No. 2, FEBRUARY 1981 during isometric contraction. J Physiol (Lond) 251: 627-643 Krueger JW, Wittenberg BA (1978) Dynamics of myofilament sliding in single intact cardiac
More informationMuscles and Muscle Tissue: Part A
PowerPoint Lecture Slides prepared by Janice Meeking, Mount Royal College CHAPTER 9 Muscles and Muscle Tissue: Part A Warm Up 12/12/16 Describe the major differences between cardiac, skeletal and smooth
More informationSome Properties of Linear Relaxation in Unfused Tetanus of Human Muscle
Physiol. Res. 41:437-443, 1992 Some Properties of Linear Relaxation in Unfused Tetanus of Human Muscle V.S. GURFINKEL, Yu.P. IVANENKO, Yu.S. LEVIK Institute o f Information Transmission Problems, Russian
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 informationHuman Motion Control Course (Wb 2407)
Part 1 Human Motion Control Course (Wb 2407) Lecture 4 Muscles physiology, morphology and models Muscle morphology and physiology Morphology: fiber arrangement force-velocity relation force-length relation
More informationBIOLOGICAL FRAMEWORKS FOR ENGINEERS Exam #2 [Due 12/9/11] by
BIOLOGICAL FRAMEWORKS FOR ENGINEERS Eam #2 [Due 12/9/11] by email Work on this on your own; do not discuss it with other members of the class. You can use any web or library resources to help, and you
More informationComputational biology of cardiac myocytes: proposed standards for the physiome
1576 The Journal of Experimental Biology 210, 1576-1583 Published by The Company of Biologists 2007 doi:10.1242/jeb.000133 Computational biology of cardiac myocytes: proposed standards for the physiome
More informationMuscle regulation and Actin Topics: Tropomyosin and Troponin, Actin Assembly, Actin-dependent Movement
1 Muscle regulation and Actin Topics: Tropomyosin and Troponin, Actin Assembly, Actin-dependent Movement In the last lecture, we saw that a repeating alternation between chemical (ATP hydrolysis) and vectorial
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 informationEFFECT OF Ca ION CONCENTRATION ON CROSS- BRIDGE KINETICS IN RABBIT PSOAS FIBERS
EFFECT OF Ca ION CONCENTRATION ON CROSS- BRIDGE KINETICS IN RABBIT PSOAS FIBERS EVIDENCE FOR THE PRESENCE OF Two Ca-ACTIVATED STATES OF THIN FILAMENT MASATAKA KAWAI, ROBERT N. COX, AND PHILIP W. BRANDT,
More informationBiomechanics. Soft Tissue Biomechanics
Biomechanics cross-bridges 3-D myocardium ventricles circulation Image Research Machines plc R* off k n k b Ca 2+ 0 R off Ca 2+ * k on R* on g f Ca 2+ R0 on Ca 2+ g Ca 2+ A* 1 A0 1 Ca 2+ Myofilament kinetic
More informationAutomatic Validation and Optimisation of Biological Models
Automatic Validation and Optimisation of Biological Models Jonathan Cooper St John s College Computational Biology Research Group Computing Laboratory University of Oxford Trinity Term 2008 This thesis
More informationCONTRACTION BANDS AT SHORT SARCOMERE LENGTH IN CHICK MUSCLE
CONTRACTION BANDS AT SHORT SARCOMERE LENGTH IN CHICK MUSCLE MARTIN HAGOPIAN. From the Department of Pathology, New York Medical College, New York 10029 INTRODUCTION The sliding filament model for contraction
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 informationCIE Biology A-level Topic 15: Control and coordination
CIE Biology A-level Topic 15: Control and coordination Notes Neuron structure The nerve cells called neurones play an important role in coordinating communication within the nervous system. The structure
More informationWoledge (1986). The time course of repriming of the labile heat was not affected by
Journal of Phy8ioloky (1988), 397, pp. 643-655 643 With 5 text-ftgurem Printed in Great Britain EFFECT OF CARBON DIOXIDE ON HEAT PRODUCTION OF FROG SKELETAL MUSCLES BY T. KITANO From the Department of
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 Modeling of the American Lobster Cardiac Muscle Cell: An Investigation of Calcium Ion Permeability and Force of Contractions
Bowdoin College Bowdoin Digital Commons Honors Projects Student Scholarship and Creative Work 5-2014 Mathematical Modeling of the American Lobster Cardiac Muscle Cell: An Investigation of Calcium Ion Permeability
More informationSENSITIVITY OF TENSION
ALTERATONS N THE CA2` SENSTVTY OF TENSON DEVELOPMENT Y SNGLE SKELETAL MUSCLE FERS AT STRETCHED LENGTHS RCHARD L. Moss, ANN E. SWNFORD, AND MARON L. GREASER Department ofphysiology, School of Medicine,
More informationLearning Cycle Linear Hybrid Automata for Excitable Cells
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
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 informationThe Myogenic Response in Isolated Rat Cerebrovascular Arteries: Smooth Muscle Cell Model
The Myogenic Response in Isolated Rat Cerebrovascular Arteries: Smooth Muscle Cell Model Jin Yang Department of Bioengineering, Rice University, Houston, TX 775 John W. Clark, Jr. Department of Electrical
More informationSupplementary Figures
Supplementary Figures Supplementary Figure 1. Sarcomere length-dependence of total fluorescence intensity in a relaxed muscle fibre containing BSR-RLC. a) Fluorescence intensity (I) relative to the value
More informationSensory-Motor Neuroscience, Department of Physiology, Queen's University, Kingston, ON, Canada, K7L 3N6
Journal of Muscle Research and Cell Motility 20: 443±456, 1999. 443 Ó 1999 Kluwer Academic Publishers. Printed in the Netherlands. Measured and modeled properties of mammalian skeletal muscle. I. The e
More informationBiology Slide 1 of 20
Biology 1 of 20 8-1 Energy and Life 2 of 20 8-1 Energy and Life Autotrophs and Heterotrophs Where do plants get the energy they need to produce food? Living things need energy to survive. This energy comes
More informationMovement & Muscle. 19 th Lecture Fri 27 Feb Chapter 18. Vertebrate Physiology ECOL 437 (MCB/VetSci 437) Univ. of Arizona, spring 2009
19 th Lecture Fri 27 Feb 2009 Vertebrate Physiology ECOL 437 (MCB/VetSci 437) Univ. of Arizona, spring 2009 Kevin Bonine & Kevin Oh Movement & Muscle Chapter 18 1 Housekeeping, Fri 27 February 2009 Readings
More informationMovement & Muscle Chapter 18
19 th Lecture Fri 27 Feb 2009 Vertebrate Physiology ECOL 437 (MCB/VetSci 437) Univ. of Arizona, spring 2009 Kevin Bonine & Kevin Oh Movement & Muscle Chapter 18 1 Housekeeping, Fri 27 February 2009 Readings
More informationUniversity of Warwick institutional repository: A Thesis Submitted for the Degree of PhD at the University of Warwick
University of Warwick institutional repository: http://go.warwick.ac.uk/wrap A Thesis Submitted for the Degree of PhD at the University of Warwick http://go.warwick.ac.uk/wrap/60665 This thesis is made
More informationRole of the Na -Ca 2 Exchanger as an Alternative Trigger of CICR in Mammalian Cardiac Myocytes
Biophysical Journal Volume 82 March 2002 1483 1496 1483 Role of the Na -Ca 2 Exchanger as an Alternative Trigger of CICR in Mammalian Cardiac Myocytes Chunlei Han, Pasi Tavi, and Matti Weckström Department
More informationFrontiers in CardioVascular Biology
Frontiers in CardioVascular Biology Young Investigator Award Mitofusin 2 controls calcium transmission between the SR and mitochondria and regulates the bioenergetic feedback response in cardiac myocytes
More informationrelationship between extent of overlap of thick and thin myofilaments and the rate
RELATION BETWEEN ADENOSINETRIPHOSPHA TE ACTIVITY AND SARCOMERE LENGTH IN STRETCHED GLYCEROL-EXTRACTED FROG SKELETAL MUSCZIE* BY PATRICK C. J. WARD,t CHARLES EDWARDS, AND E. S. BENSON DEPARTMENTS OF LABORATORY
More informationCompliant Realignment of Binding Sites in Muscle: Transient Behavior and Mechanical Tuning
Biophysical Journal Volume 74 April 1998 1611 1621 1611 Compliant Realignment of Binding Sites in Muscle: Transient Behavior and Mechanical Tuning Thomas L. Daniel,* Alan C. Trimble,* and P. Bryant Chase
More informationCopyright 2012 Charles David Williams
Copyright 2012 Charles David Williams A new view of the radial geometry in muscle: myofilament lattice spacing controls force production and energy storage. Charles David Williams A dissertation submitted
More informationThe Journal of Physiology
J Physiol 592.5 (2014) pp 1119 1137 1119 Sarcomere-length dependence of myosin filament structure in skeletal muscle fibres of the frog Massimo Reconditi 1,2, Elisabetta Brunello 1, Luca Fusi 3, Marco
More informationNumerical simulations of cardiac arrhythmias and defibrillation
Numerical simulations of cardiac arrhythmias and defibrillation M. Hanslien, J. Sundnes and G.T. Lines Simula Research Laboratory and Department of Informatics, University of Oslo Abstract This paper is
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 informationNOTE: LOOK ON MY WEBSITE FOR THE MUSCLE LABELING POWER POINT/PDF Part I. Identify the parts of the neuron that are labeled below.
Anatomy & Physiology Nervous System Part I 2/26/16 NOTE: LOOK ON MY WEBSITE FOR THE MUSCLE LABELING POWER POINT/PDF Part I. Identify the parts of the neuron that are labeled below. 1. 2. 3. 5. 4. 6. Part
More informationLESSON PLAN. B.Sc - SECOND YEAR ( REGULATION)
DEPARTMENT OF PHYSICS AND NANOTECHNOLOGY LESSON PLAN B.Sc - SECOND YEAR (2014-2015 REGULATION) THIRD SEMESTER. SRM UNIVERSITY SRM NAGAR, KATTANKULATHUR 603 203 SRM UNIVERSITY DEPARTMENT OF PHYSICS AND
More informationmeasure it, as it appears to be important. Glycerinated rabbit psoas fibers were used in the study. The stiffness was
STIFFNESS OF GLYCERINATED RABBIT PSOAS FIBERS IN THE RIGOR STATE Filament-Overlap Relation KATSUHISA TAWADA AND MICHIo KIMURA Department ofbiology, Faculty ofscience, Kyushu University, Fukuoka 812, Japan
More information1. True or false: at this moment, some of the muscle fibers in your gluteus maximus (a whole muscle) are contracting. a. True b.
Exam III ANP 213 Spring 2008 You only need to print out the last two pages. Please do not consult classmates once you have begun this exam. Multiple Choice- 1 point each (use a ScanTron) 1. True or false:
More informationA Dynamic Model of Excitation-Contraction Coupling during Acidosis in Cardiac Ventricular Myocytes
3074 Biophysical Journal Volume 90 May 2006 3074 3090 A Dynamic Model of Excitation-Contraction Coupling during Acidosis in Cardiac Ventricular Myocytes Edmund J. Crampin and Nicolas P. Smith Bioengineering
More informationComputational simulation of the heart Edmund Altman 2010/2011
Computational simulation of the heart Edmund Altman 2010/2011 The candidate confirms that the work submitted is their own and the appropriate credit has been given where reference has been made to the
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 informationTitin is a structural protein in muscle that
8 Journal of Undergraduate Research in Alberta Volume 2 212 The Mechanical Properties of Titin within a Sarcomere? Jens A. Herzog, Tim R. Leonard, Azim Jinha, Walter Herzog University of Calgary Titin
More informationEffect of Initial Sarcomere Length on Sarcomere Kinetics and Force Development in Single Frog Atrial Cardiac Cells
767 Effect of Initial Sarcomere Length on Sarcomere Kinetics and Force Development in Single Frog Atrial Cardiac Cells MERRILL TARR, JOHN W. TRANK, KENNETH K. GOERTZ, AND PAUL LEIFFER SUMMARY We studied
More informationDistribution of sarcomere length and intracellular calcium in mouse skeletal muscle following stretch-induced injury
Keywords: Stretch, Skeletal muscle fibre, Calcium imaging 6441 Journal of Physiology (1997), 502.3, pp. 649 659 649 Distribution of sarcomere length and intracellular calcium in mouse skeletal muscle following
More informationThis document is downloaded from DR-NTU, Nanyang Technological University Library, Singapore.
This document is downloaded from DR-NTU, Nanyang Technological University Library, Singapore. Title Author(s) Citation Revisiting Frank-Starling: regulatory light chain phosphorylation alters the rate
More information