Membrane Potential Fox Chapter 6 pt 2

Similar documents
Cells have an unequal distribution of charge across their membrane: more postiive charges on the outside; more negative charges on the inside.

Action Potential Propagation

NeuroPhysiology and Membrane Potentials. The Electrochemical Gradient

- the flow of electrical charge from one point to the other is current.

PNS Chapter 7. Membrane Potential / Neural Signal Processing Spring 2017 Prof. Byron Yu

Lojayn Salah. Zaid R Al Najdawi. Mohammad-Khatatbeh

Resting membrane potential,

Neurons and the membrane potential. N500 John Beggs 23 Aug, 2016

Resting Distribution of Ions in Mammalian Neurons. Outside Inside (mm) E ion Permab. K Na Cl

Particles with opposite charges (positives and negatives) attract each other, while particles with the same charge repel each other.

General Physics. Nerve Conduction. Newton s laws of Motion Work, Energy and Power. Fluids. Direct Current (DC)

Electrical Properties of the Membrane

Physiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES

Chapter 1 subtitles Ion gradients

Cell membrane resistance and capacitance

Neuroscience: Exploring the Brain

Channels can be activated by ligand-binding (chemical), voltage change, or mechanical changes such as stretch.

Chapter 2 Cellular Homeostasis and Membrane Potential

Physiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES

The Membrane Potential

Main idea of this lecture:

Ionic basis of the resting membrane potential. Foundations in Neuroscience I, Oct

NEURONS, SENSE ORGANS, AND NERVOUS SYSTEMS CHAPTER 34

9.01 Introduction to Neuroscience Fall 2007

The Membrane Potential

Membrane Potentials, Action Potentials, and Synaptic Transmission. Membrane Potential

2002NSC Human Physiology Semester Summary

2.6 The Membrane Potential

Alaa' Alajrami. Hussam Twaissi. Mohammad khatatbeh

Lecture 04, 04 Sept 2003 Chapters 4 and 5. Vertebrate Physiology ECOL 437 University of Arizona Fall instr: Kevin Bonine t.a.

Introduction to cardiac electrophysiology 1. Dr. Tóth András 2018

CELLULAR NEUROPHYSIOLOGY CONSTANCE HAMMOND

Housekeeping, 26 January 2009

Neurons. 5 th & 6 th Lectures Mon 26 & Wed 28 Jan Finish Solutes + Water. 2. Neurons. Chapter 11

Phys498BIO; Prof. Paul Selvin Hw #9 Assigned Wed. 4/18/12: Due 4/25/08

What are neurons for?

Ch. 5. Membrane Potentials and Action Potentials

BIOELECTRIC PHENOMENA

Cellular Electrophysiology. Cardiac Electrophysiology

Introduction to electrophysiology 1. Dr. Tóth András

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

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

ACTION POTENTIAL. Dr. Ayisha Qureshi Professor MBBS, MPhil

Universality of sensory-response systems

Biological membranes and bioelectric phenomena

Passive Membrane Properties

Lecture 10 : Neuronal Dynamics. Eileen Nugent

Ch 8: Neurons: Cellular and Network Properties, Part 1

Resting Membrane Potential

7 Membrane Potential. The Resting Membrane Potential Results From the Separation of Charges Across the Cell Membrane. Back.

Introduction to electrophysiology. Dr. Tóth András

Introduction to Physiology II: Control of Cell Volume and Membrane Potential

Computational Neuroscience. Session 2-1

Chapter 7-3 Cells and Their Environment

لجنة الطب البشري رؤية تنير دروب تميزكم

Quantitative Electrophysiology

Overview Organization: Central Nervous System (CNS) Peripheral Nervous System (PNS) innervate Divisions: a. Afferent

Neurons and Nervous Systems

Transport of ions across plasma membranes

Quantitative Electrophysiology

Rahaf Nasser mohammad khatatbeh

Transmission of Nerve Impulses (see Fig , p. 403)

PROPERTY OF ELSEVIER SAMPLE CONTENT - NOT FINAL. The Nervous System and Muscle

Equivalent Circuit Model of the Neuron

Nernst Equation and Equilibrium Potentials

Properties of the living organism. Interaction between living organism and the environment. Processing informations. Definitions

SUMMARY OF THE EVENTS WHICH TRIGGER AN ELECTRICAL IMPUSLE IN NERVE CELLS (see figures on the following page)

Biomedical Instrumentation

Nernst Equilibrium Potential. p. 1

one day Time t past deadline (hours)

Biochemistry Prof. S. Dasgupta Department of Chemistry. Indian Institute of Technology Kharagpur. Lecture - 15 Nucleic Acids III

PETER PAZMANY CATHOLIC UNIVERSITY Consortium members SEMMELWEIS UNIVERSITY, DIALOG CAMPUS PUBLISHER

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

2401 : Anatomy/Physiology

Ionic gradients, membrane potential and ionic currents Constance Hammond

Advanced Higher Biology. Unit 1- Cells and Proteins 2c) Membrane Proteins

2401 : Anatomy/Physiology

Neurons. The Molecular Basis of their Electrical Excitability

9 Generation of Action Potential Hodgkin-Huxley Model

Balance of Electric and Diffusion Forces

Title: Membrane Potentials Subtitle: Ion Movement: Forces and Measurement Diomedes E. Logothetis, Ph.D. Lecture goals:

STUDIES OF CHANGING MEMBRANE POTENTIAL * : 1. BASIC ELECTRICAL THEORY, 2. GRADED AND ACTION POTENTIALS 3. THE VOLTAGE CLAMP AND MEMBRANE POTENTIALS

LESSON 2.2 WORKBOOK How do our axons transmit electrical signals?

The Nervous System and the Sodium-Potassium Pump

3/24/11. Introduction! Electrogenic cell

3 Detector vs. Computer

Physiology Coloring Book: Panels 29, 32, 33,

Neurophysiology. Danil Hammoudi.MD

FRTF01 L8 Electrophysiology

Chapter 48 Neurons, Synapses, and Signaling

CELL SIGNALLING and MEMBRANE TRANSPORT. Mark Louie D. Lopez Department of Biology College of Science Polytechnic University of the Philippines

Electrophysiology of the neuron

Biol2174 Cell Physiology in Health & Disease

PROPERTY OF ELSEVIER SAMPLE CONTENT - NOT FINAL

CELL BIOLOGY - CLUTCH CH. 9 - TRANSPORT ACROSS MEMBRANES.

Fundamentals of the Nervous System and Nervous Tissue

Membrane Potentials and Action Potentials

Introduction to electrophysiology 1. Dr. Tóth András

BIOL Week 5. Nervous System II. The Membrane Potential. Question : Is the Equilibrium Potential a set number or can it change?

Nervous & Endocrine System

Transcription:

Vert Phys PCB3743 Membrane Potential Fox Chapter 6 pt 2 T. Houpt, Ph.D. Resting Membrane potential (V m ) or RMP Many cells have a membrane potential (Vm) that can be measured from an electrode in the cell with a voltmeter. neurons, muscle cells, heart cells, endocrine cells... V m = resting membrane potential (RMP) = electrical potential generated by separation of charges = voltage across the membrane = V inside - V outside! Cells have an unequal distribution of charge across their membrane: more postiive charges on the outside; more negative charges on the inside. Charge separation is caused by movement of ions in and out the cell. Ions are moved by chemical diffusion down concentration gradients and by electrical attraction, and by active transport (e.g. Na+/K+ pump.) Concentration of ions inside and outside reaches equilibrium (stays constant) due to equilibrium potential. T Membrane potential (V m ) V m!= resting membrane potential = electrical potential generated by separation of charges! = voltage across the membrane! = V inside - V outside

Measuring Vm Unequal charges across the cell membrane more + charges on outside of membrane more - charges on inside of membrane Membrane potential (Vm) Vm! = Vin - Vout! (Vout = 0 mv by definition) Vm = Vin - 0! (more negative ions inside) Vm = -60 to -70 mv Vout = 0 Vin = -60 mv

Membrane potential is caused by small number of total ions ions that can move across the membrane thru ion channels Transport pump large charged proteins inside cell Fox Figure 6.24 Equilibrium Potential for an ion (Eion) Each ion species feels two forces pulling on it through open ion channels: 1. Chemical driving force depends on concentration gradient across membrane 2. Electrical driving force depends on electrical potential difference across membrane These forces can act in same direction or opposite directions across the membrane Example: K + has chemical driving force out of cell, but electrical driving force into cell. Example: Na+ ions has both chemical driving force and electrical driving force into cell. The electrical potential that balances the concentration gradient is called the equilibrium potential. If there are open channels for an ion, the electrical and chemical driving forces will try to force the ions to move across the membrane. The ion will move across the membrane until the change in electrical charge causes the cell s V m to reach the ion s equilibrium potential. T

Equilibrium Potential for an ion (Eion) Each ion species feels two forces pulling on it: 1. Chemical driving force depends on concentration gradient across membrane 2. Electrical driving force depends on electrical potential difference across membrane these forces can act in same direction or opposite directions across the membrane If there are open channels for an ion, the electrical and chemical driving forces will try to force the ions to move across the membrane. 2 Forces on ions: 1. Diffusion down concentration gradient 2 Forces on ions: 2. Electrical attraction toward opposite charge

For potassium K +, chemical and electrical forces are in opposite directions K + Extracellular side Selectively permeable membrane Cytoplasmic side Concentration gradient for K + moves K + out of cell Electrical gradient for K + pulls K + into the cell Electrochemical Forces on Potassium K + Ion outside neuron chemical electrical inside neuron Equilibrium Potential for an ion: Voltage at which electrical force balances chemical force Fox Figure 6.25

Equilibrium Potential for an ion: Voltage at which electrical force balances chemical force Fox Figure 6.25 Electrochemical Forces on Sodium Na + Ion outside neuron chemical Na+ electrical inside neuron Na+ Calculating the Equilibrium Potential Given the concentrations of ions inside and outside of a neuron, we can calculate its Equilibrium Potential (Eion) in mv using the Nernst Equation. E ion = 61 / charge log ([ion] out / [ion] in ) Multiple ions can move across the cell membrane, and each ion will have its own Equilibrium Potential, depending on the intracellular/extracellular concentations and the ion s charge. e.g. Na +, K +, Cl, Mg 2+ Ion Flux Because the cell is selectively permeable to ions, some ions can move easily across the membrane thru open ion channels (high flux), while ions with few channels or closed ion channels cannot move across the membrane (low flux). Membrane potential (Vm) or RMP The cell s overall membrane potential (Vm) is a combination of the Eion of all the ions that can permeate the membrane, with a greater contribution for the ions with the greatest permeability (i.e. with the most open ion channels). Need to know & apply Nernst Equation to find Eion for a simple case! T

Nernst Equation E ion is the equilibrium potential in mv for a single permeant ion E ion (mv) = RT / zf log ([ion] out / [ion] in ) R = gas constant T = temperature (kelvin) (assume 37 C) z = valence F = Faraday constant E ion = 61 / charge log ([ion] out / [ion] in ) Need to know & apply Nernst Equation to find Eion for a simple case! Nernst Equation for K + E ion (mv) = 61 / charge log ([ion] out / [ion] in ) E K + (mv) = 61 / +1 log (5 mm / 150 mm) = 61 / +1 log (.03) = 61 / +1-1.47 = 90 mv Equilibrium Potential for an ion: Voltage at which electrical force balances chemical force Fox Figure 6.25

Each ion has its own Equilibrium Potential: Depending on charge and concentrations of the ion Fox Figure 6.26 Distribution of Ions in Mammalian Neurons Each ion has a specific Equilibium potential Ion Outside Inside Ratio Out : In E ion (mv) chemical K + 5 150 1:30-90 inside electrical -90mV Na + 150 15 10:1? Cl - 150 15 10:1? Ca ++ 2.5 0.0001 10,000:1? Distribution of Ions in Mammalian Neurons Each ion has a specific Equilibium potential Ion Outside Inside Ratio Out : In E ion (mv) K + 5 150 1:30-90 chemical Na + 150 15 10:1 +61 electrical +60mV Cl - 150 15 10:1-61 Ca ++ 2.5 0.0002 10,000:1 136 But how to calculate overall membrane potential?

Nernst Equation for Na + E ion = 61 / charge log ([ion] out / [ion] in ) E Na + = 61 / +1 log (150 mm / 15 mm) = 61 / +1 log (10) = 61 / +1 1 = +61 mv Nernst Equation for Cl - E ion = 61 / charge log ([ion] out / [ion] in ) E Cl = 61 / 1 log ( 125 mm / 10 mm) = 61 / 1 log ( 12 ) = 61 / 1 1 = 61 mv Nernst Equation for Ca++ E ion = 61 / charge log ([ion] out / [ion] in ) E Ca++ = 61 / +2 log ( 2.5 mm /.0001 mm) = 61 / +2 log ( 25,000) = 61 / +2 4.5 = 136 mv

Nernst Equations for major ions E K + = 61 / +1 log (5 mm / 125 mm) = 90 mv E Na + = 61 / +1 log (150 mm / 15 mm) = +61 mv E Cl = 61 / 1 log ( 125 mm / 10 mm) = 61 mv E Ca++ = 61 / 2 log ( 25 mm /.0002 mm) = 136 mv But how to calculate overall membrane potential? Distribution of Ions in Mammalian Neurons Each ion has a specific Equilibium potential Ion Outside Inside Ratio Out : In E ion (mv) chemical K + 5 150 1:30-90 electrical -90mV Na + 150 15 10:1 +61 Cl - 150 15 10:1-61 Ca ++ 2.5 0.0002 10,000:1 136 But how to calculate overall membrane potential? Distribution of Ions in Mammalian Neurons Each ion has a specific Equilibium potential Ion Outside Inside Ratio Out : In E ion (mv) K + 5 150 1:30-90 chemical Na + 150 15 10:1 +61 electrical +60mV Cl - 150 15 10:1-61 Ca ++ 2.5 0.0002 10,000:1 136 But how to calculate overall membrane potential?

Membrane Potential (Vm) for a cell: Each ion contributes to overall membrane potential Equilibrium Potentials +61 mv -90 mv -61 mv +136 mv Fox Figure 6.26 Ion flux number of ions that are crossing the membrane ion flux = (electrical force + chemical force)! x membrane permeability for that ion In the resting nerve cell, Lots of open K + channels, so K + flux is large. Very few open Na + channels, so Na + flux is low. Rember: cell actively controls concentrations of Na + & K + Na+/K+ ATPase pumps keep high K +, low Na + inside the cell So, V m lies in between Equilibrium Potentials of K + and Na + Calculating the overall Membrane Potential (Vm) Membrane potential (Vm) or RMP The cell s overall membrane potential (Vm) is a combination of the Eion of all the ions that can permeate the membrane, with a greater contribution for the ions with the greatest permeability (i.e. with the most open ion channels). The Goldman Equation finds the compromise membrane potential accounting for each permeant ion. V m approaches the Equilibrium Potential of the most permeable ion. For neurons and most cells, the most permeable ion is K+. So, the membrane potential Vm at -70 mv is close to EK+ at -90 mv. Need to understand that Vm is dependent on most permeable ion, but don t need to memorize the Goldman equation. T

Permeability of Ions in Mammalian Neurons! Outside! Inside! E ion! Permeab. K +! 5! 150! -90! 1.0 Na +! 150! 15! +61! 0.04 Cl -! 125! 10! -61! 0.045 Because K + has the highest permeability, it has the highest flux and so contributes the most to the overall membrane potential. Goldman Equation Goldman Equation finds the compromise membrane potential accounting for each permeant ion.! P K [K + ] o + P Na [Na + ] o + P Cl [Cl - ] i V membrane = 61 log!! P K [K + ] i + P Na [Na + ] i + P Cl [Cl - ] o P X = relative permeability of ion X [X] i = concentration of X inside cell [X] o = concentration of X outside cell Goldman Equation K+ Na+ Cl-! 1[5] o! +.04[150] o! +.05[10] i V m = 62 log! 1[150] I! +.04[15] i! +.05[125] o V m = -70 mv V m approaches the Equilibrium Potential of the most permeable ion. Need to understand that Vm is dependent on most permeable ion, but don t need to memorize the Goldman equation.

Membrane Potential (Vm) for a cell: Voltage at which electrical forces balance chemical forces for all ions, depending on permeability of the ions. Equilibrium Potentials +61 mv -70 mv -90 mv -61 mv +136 mv Fox Figure 6.26 Membrane Potential (Vm) for a cell: Voltage at which electrical forces balance chemical forces for all ions -70 mv 0 mv Fox Figure 6.27 Contributions to Membrane Potential Fox Figure 6.28

Distribution of Ions in Mammalian Neurons! Outside! Inside! E ion! Permab. K +! 5! 150! -90! 1.0 Na +! 150! 15! +61! 0.04 Cl -! 125! 10! -61! 0.045 V m = -70 mv Change of Concentration leads to change of V m! Outside! Inside! E ion! Permab. K +! 150! 150! 0! 1.0 Na +! 150! 15! +61! 0.04 Cl -! 100! 10! -61! 0.045 V m = +0 mv