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

Similar documents
Membrane Potential Fox Chapter 6 pt 2

Action Potential Propagation

The Membrane Potential

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

The Membrane Potential

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

NeuroPhysiology and Membrane Potentials. The Electrochemical Gradient

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

Resting membrane potential,

Neuroscience: Exploring the Brain

Lojayn Salah. Zaid R Al Najdawi. Mohammad-Khatatbeh

2002NSC Human Physiology Semester Summary

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

Chapter 1 subtitles Ion gradients

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

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

Electrical Properties of the Membrane

Cell membrane resistance and capacitance

Universality of sensory-response systems

NEURONS, SENSE ORGANS, AND NERVOUS SYSTEMS CHAPTER 34

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

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

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

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

Chapter 2 Cellular Homeostasis and Membrane Potential

Introduction to cardiac electrophysiology 1. Dr. Tóth András 2018

9 Generation of Action Potential Hodgkin-Huxley Model

Computational Neuroscience. Session 2-1

Cellular Electrophysiology. Cardiac Electrophysiology

LESSON 2.2 WORKBOOK How do our axons transmit electrical signals?

Alaa' Alajrami. Hussam Twaissi. Mohammad khatatbeh

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

Chapter 7-3 Cells and Their Environment

Biological membranes and bioelectric phenomena

Neurons and Nervous Systems

Ch. 5. Membrane Potentials and Action Potentials

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

Main idea of this lecture:

Physiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES

9.01 Introduction to Neuroscience Fall 2007

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

Physiology Unit 2. MEMBRANE POTENTIALS and SYNAPSES

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

Housekeeping, 26 January 2009

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

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

Passive Membrane Properties

BIOELECTRIC PHENOMENA

Electrophysiology of the neuron

What are neurons for?

Lecture 10 : Neuronal Dynamics. Eileen Nugent

Neurons. The Molecular Basis of their Electrical Excitability

The Nervous System and the Sodium-Potassium Pump

TRANSPORT ACROSS MEMBRANE

Transport of ions across plasma membranes

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

2.6 The Membrane Potential

Introduction to electrophysiology 1. Dr. Tóth András

Quantitative Electrophysiology

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

ACTION POTENTIAL. Dr. Ayisha Qureshi Professor MBBS, MPhil

Equivalent Circuit Model of the Neuron

Quantitative Electrophysiology

The Neuron - F. Fig. 45.3

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

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

Rahaf Nasser mohammad khatatbeh

Chapt. 12, Movement Across Membranes. Chapt. 12, Movement through lipid bilayer. Chapt. 12, Movement through lipid bilayer

Membrane Protein Channels

Resting Membrane Potential

Balance of Electric and Diffusion Forces

Introduction to electrophysiology. Dr. Tóth András

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

Physiology Coloring Book: Panels 29, 32, 33,

Nernst Equilibrium Potential. p. 1

لجنة الطب البشري رؤية تنير دروب تميزكم

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

Neuron Structure. Why? Model 1 Parts of a Neuron. What are the essential structures that make up a neuron?

CELLULAR NEUROPHYSIOLOGY CONSTANCE HAMMOND

Membrane transport 1. Summary

Lecture 3 13/11/2018

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

Supplementary Material. Model Details

Ionic gradients, membrane potential and ionic currents Constance Hammond

Fundamentals of the Nervous System and Nervous Tissue

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

MEMBRANE STRUCTURE. Lecture 9. Biology Department Concordia University. Dr. S. Azam BIOL 266/

Introduction to electrophysiology 1. Dr. Tóth András

Chapter 48 Neurons, Synapses, and Signaling

Neural Conduction. biologyaspoetry.com

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

3 Detector vs. Computer

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

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

one day Time t past deadline (hours)

Biomedical Instrumentation

2401 : Anatomy/Physiology

Questions: Properties of excitable tissues Transport across cell membrane Resting potential Action potential Excitability change at excitation

Membranes 2: Transportation

Converting energy into nerve impulses, resting potentials and action potentials Sensory receptors

Transcription:

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.

http://www.youtube.com/watch?v=k48jxzfgmc8

http://www.youtube.com/watch?v=aey-t9hynbi

Ion Channels & Membrane Potential Neurons need to send signals quickly over long distances. They utilize waves of electrical current across their membranes. This requires that they maintain a differential distribution of charge between the inside and outside of the neuron, and that they can switch a cross-membrane current on and off to make the signal.

Major ions in neuroscience: Na+, K+, Cl-, Ca++, & protein anions (A-)

outside [Na+][K+] [Na+][K+] inside

Na+/K+ Transporter Ion Outside (mm) Inside (mm) K + 5 100 Na + 150 15 Na ions slowly leak into cell down concentration gradient and attracted by negative charges of the cytoplasm. Neuron actively maintains Na and K concentrations by exchanging: 3 Na ions out for 2 K ions in for every 1 ATP molecule.

[Na+][K+] [Na+][K+]

Unequal charges across the cell membrane

Membrane potential (V m ) V m = resting membrane potential = electrical potential generated by separation of charges = voltage across the membrane = V inside - V outside

Membrane potential (V m ) V m = V in - V out (V out = 0 mv by definition) V m = V in - 0 (more negative ions inside) V m = -60 to -70 mv V out = 0 V in = -60 mv

Membrane potential is caused by small number of total ions

Membrane potential is caused by small number of total ions

Measuring Vm

How to establish the membrane potential?

Ion Channels: proteins that span the membrane and allow ions to diffuse across the phospholipid bilayer

Equilibrium Potential for an ion Each ion species feels two forces pulling on it: chemical driving force: depends on concentration gradient across membrane electrical driving force: depends on electrical potential difference across membrane

Force on ions: Diffusion down concentration gradient

Force on ions: Pulled toward opposite charge

Equilibrium Potential for an ion Each ion species feels two forces pulling on it: chemical driving force: depends on concentration gradient across membrane electrical driving force: depends on electrical potential difference across membrane these forces can act in same direction or opposite directions across the membrane

For potassium, chemical and electrical forces are in opposite directions

For potassium, chemical and electrical forces are in opposite directions Electrical gradient for K+ pulls K+ into the cell

Electrochemical Forces on Potassium K + Ion outside neuron chemical electrical inside neuron

Electrochemical Forces on Sodium Na + Ion outside neuron chemical Na+ electrical inside neuron Na+

Equilibrium Potential for an ion Each ion species feels two forces pulling on it: chemical driving force: depends on concentration gradient across membrane electrical driving force: depends on electrical potential difference across membrane these forces can act in same direction or opposite directions across the membrane the electrical potential that balances the concentration gradient is called the equilibrium potential.

Equilibrium Potential for an ion 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.

Equilibrium Potential for one ion across the membrane https://www.youtube.com/watch?v=4kx9_0ywshe

Distribution of Ions in Mammalian Neurons Ion Outside (mm) Inside (mm) Ratio Out : In E ion K + 5 100 1:20? Na + 150 15 10:1? Ca ++ 2 0.0002 10,000:1? Cl - 150 15 10:1?

Calculating the Equilibrium Potential Given the concentrations of ions inside and outside of a neuron, we can calculate its Equilibrium Potential using the Nernst Equation

Nernst Equation E ion is the equilibrium potential for a single permeant ion E ion (mv) = RT / zf log ([ion] out / [ion] in ) R = gas constant T = temperature (kelvin) z = valence F = Faraday constant E ion (mv) = 62 / charge log ([ion] out / [ion] in ) at 37 C

Distribution of Ions in Mammalian Neurons Ion Outside (mm) Inside (mm) Ratio Out : In E ion K + 5 100 1:20? Na + 150 15 10:1? Ca ++ 2 0.0002 10,000:1? Cl - 150 15 10:1?

Nernst Equation for K + E ion (mv) = 62 / charge log ([ion] out / [ion] in ) E K + (mv) = 62 / +1 log (5 mm / 100 mm) = 62 / +1 log (.05) = 62 / +1-1.3 = 80 mv

Nernst Equation for Na + E ion = 62 / charge log ([ion] out / [ion] in ) E Na + = 62 / +1 log (150 mm / 15 mm) = 62 / +1 log (10) = 62 / +1 log (1) = +62 mv

Nernst Equation for Cl - E ion = 62 / charge log ([ion] out / [ion] in ) E Cl = 62 / 1 log ( 100 mm / 10 mm) = 62 / 1 log ( 10 ) = 62 / 1 1 = 62 mv

Nernst Equation for Ca++ E ion = 62 / charge log ([ion] out / [ion] in ) E Ca++ = 62 / +2 log ( 2 mm /.0002 mm) = 62 / +2 log ( 10,000) = 62 / +2 4 = 123 mv

Nernst Equation E + K = 62 / +1 log (5 mm = 80 mv / 125 mm) E + Na = 62 / +1 log (150 mm = +62 mv / 15 mm) E Cl = 62 / 1 log ( 100 mm = 62 mv / 10 mm) E Ca++ = 62 / 2 log ( 2 mm = 123 mv /.0002 mm) But how to calculate overall membrane potential?

Membrane Potential (Vm) for a cell: Each ion contributes to overall membrane potential Equilibrium Potentials +62 mv -80 mv -62 mv +123 mv Fox Figure 6.26

Distribution of Ions in Mammalian Neurons Ion Outside (mm) Inside (mm) Ratio Out : In E ion (mv) K + 5 100 1:20-80 Na + 150 15 10:1 +62 Ca ++ 2 0.0002 10,000:1 123 Cl - 150 15 10:1-62 But how to calculate overall membrane potential?

Equilibrium Potential for an ion 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. Because the cell is selectively permeable to ions, some ions can move across the membrane, while ions with closed ion channels cannot move across the membrane.

Protein structure of K+ channel makes it selective for K+ (i.e. Na+, Cl-, Ca++ can t get through)

Pore Loop

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 neuron, Lots of open K + channels, so K + flux can be large. Very few open Na + channels, so Na + flux is low. Neuron actively controls concentrations of Na + & K + So, V m lies in between Equilibrium Potentials of K + and Na +

Permeability of Ions in Mammalian Neurons Outside Inside (mm) E ion Permeab. K + 5 125-81 1.0 Na + 150 15 +62 0.04 Cl - 100 10-62 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 is the compromise potential reached accounting for each permeant ion. P K [K + ] o + P Na [Na + ] o + P Cl [Cl - ] i V membrane = 62 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 1[5] o +.04[150] o +.05[10] i V m = 62 log 1[125] I +.04[15] i +.05[100] o V m = -65 mv V m approaches the Equilibrium Potential of the most permeable ion.

Distribution of Ions in Mammalian Neurons Outside Inside (mm) E ion Permab. K + 5 125-80 1.0 Na + 150 15-62 0.04 Cl - 100 10-62 0.045 V m = -65 mv

Change of Concentration leads to change of V m Outside Inside (mm) E ion Permab. K + 150 150 0 1.0 Na + 150 15 +62 0.04 Cl - 100 10-62 0.045 V m = +0 mv

Change of Permeability leads to change of V m Outside Inside (mm) E ion Permab. K + 5 125-80 1.0 Na + 150 15-62 20 Cl - 100 10-62 0.045 V m = +49 mv

Changing the Membrane Potential https://www.youtube.com/watch?v=qnvtlw8lprw