BME 6938 Neurodynamics

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BME 6938 Neurodynamics Instructor: Dr Sachin S. Talathi

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BME 6938 Neurodynamics. Instructor: Dr Sachin S. Talathi. Recap. XPPAUTO introduction Linear cable theory Cable equation Boundary and Initial Conditions Steady State Analysis Transient Analysis Rall model-Equivalent cylinder. Nonlinear membrane. Linear cable properties - PowerPoint PPT Presentation

Transcript of BME 6938 Neurodynamics

Page 1: BME 6938 Neurodynamics

BME 6938Neurodynamics

Instructor: Dr Sachin S. Talathi

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Recap

• XPPAUTO introduction• Linear cable theory

– Cable equation– Boundary and Initial Conditions– Steady State Analysis– Transient Analysis

• Rall model-Equivalent cylinder

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Nonlinear membrane

Linear cable propertiessatisfying Ohms law

Nonlinear membrane

Ions: Na+,K+,Ca2+,Cl-

In general a nonlinear function in voltage and time

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Revisiting Goldman Eq.

Permeability of the membrane changes as function of voltage and time

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Gate Model

• HH proposed the gate model to provide a quantitative framework for determining the time and membrane potential dependent properties of ion channel conductance

• The Assumptions in the Gate Model:– Membrane comprise of aqueous pores through which the ions

flow down their concentration gradient– These pores contain voltage sensitive gates that close and

open dependent on trans membrane potential– The transition from closed to open state and vice-versa follow

first order kinetics with rate constants: and

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Kinetics of gate transition

• Let p represent the fraction of gates within the ion channel that are in open state at any given instant in time

• 1-p represents the remaining fraction of the gates that are in closed state

• If represents the transition rate for gate to go from closed to open state and represents the transition rate for gate to go from open to closed stat, we have

Open p

Closed 1-p

Steady state

The transient solution can then be obtained as:

OR

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Multiple gates

• If a ion channel is comprised of multiple gates; then each and every gate must be open for the channel to conduct ion flow.

• The probability of gate opening then is given by:

• Gate Classification– Activation Gate: p(t,V) increases with membrane

depolarization– Inactivation Gate: p(t,V) decreases with membrane

depolarization

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The unknowns

• In order to use the gate model to determine the ion channel dynamics, HH had to estimate the following 3 quantities– Macro characteristics of channel type – The number and type of gates on a given ion channel– The transition rate constants &

Macro characteristics include: Reversal potential, maximum conductance and ion specificy

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The experiments

• Two important factors permitted HH analysis as they set about to design experiments to find the unknowns– Giant Squid Axon (Diameter approx 0.5 mm), allowed for

the use of crude electronics of 1950’s (Squid axon’s utility for of nerve properties is credited to J.Z Young (1936) )

– Development of feed back control device called the voltage clamp capable of holding the membrane potential to a desired value

Before we look into the experiments; lets have a look at

the model proposed by HH to describe the dynamics of squid axon cell membrane

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HH model

• HH proposed the parallel conductance model wherein the membrane current is divided up into four separate contributions– Current carried by sodium ions– Current carried by potassium ions– Current carried by other ions (mainly chloride and

designated as leak currents)– The capacitive current

We have already seen this idea being utilized in GHK equations

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The equivalent circuit

Goal: Find &

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Results

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The Experiments

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Space clamp: Eliminate axial dependence of membrane voltage

• Stimulate along the entire length of the axon• Can be done using a pair

of electrodes as shown• Provides complete axial symmetry Result:

Eliminate the axial component inThe cable equation

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Voltage Clamp: Eliminate capacitive current

http://www.sinauer.com/neuroscience4e/animations3.1.html

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Example of Voltage Clamp Recording

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Sum of parts

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Series of Voltage clamp expts

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Selectively blocking specific currents

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H-H experiments to test Ohms law

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HH measurement of Na and K conductance

Gating variables

Maximum conductance

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Functional fitting to gate variable

• We see from last slide• Na comprise of activation and inactivation• K comprise of only activation term• HH fit the the time dependent components of the

conductance such that

Activation gate Inactivation gate

m,n and h are gate variables and follow first order kinetics of the gate model

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Gate model for m,n and h

Activation: Inactivation:

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• Determine and• Use the following relationship

• Do empirical curve fitting to obtain

Estimating gate model parameters

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Profiles of fitted transition functions

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Summary of HH experiments

• Determine the contributions to cell membrane current from constituent ionic components

• Determine whether Ohms law can be applied to determine conductances

• Determine time and voltage dependence of sodium and potassium conductances

• Use gate model to fit gating variables• Use equations from gate model to determine the

voltage dependent transition rates

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The complete HH model

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Success of HH model

• 150 years of animal electricity problem solved; in terms of a quantitative description of the process of generation of an action potential

• Correct form of experimentally observed action potential shape (on average 8 hours per 5 ms of the solution)

• Predicted the speed of action potential propagation correctly (we haven’t talked about this in the class)

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Process of action potential generation