A brief introduction to neuronal dynamics

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A brief introduction to neuronal dynamics Gemma Huguet Universitat Politècnica de Catalunya In Collaboration with David Terman Mathematical Bioscience Institute Ohio State University

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A brief introduction to neuronal dynamics. Gemma Huguet Universitat Politècnica de Catalunya In Collaboration with David Terman Mathematical Bioscience Institute Ohio State University. Outline Goal of mathematical neuroscience : develop and analyze models for neuronal activity patterns. - PowerPoint PPT Presentation

Transcript of A brief introduction to neuronal dynamics

Page 1: A brief introduction to neuronal dynamics

A brief introduction to neuronal dynamics

Gemma Huguet

Universitat Politècnica de Catalunya

In Collaboration with David Terman

Mathematical Bioscience Institute

Ohio State University

Page 2: A brief introduction to neuronal dynamics

OutlineGoal of mathematical neuroscience: develop and analyze

models for neuronal activity patterns.

1. Some biology

2. Modeling neuronal activity patterns

Single neuron models. Hodgkin-Huxley formalism.

Coupling between neurons. Chemical synapsis.

Network architecture.

3. Example. Numerical simulations of network activity patterns. Synchronization.

4. Conclusions.

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The brain

~ 1012 Neurons

~ 1015 Synapses

How do we model neuronal systems?

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The neuron

Electrical signal: Action potential that propagates along axon

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Nobel Prize, 1963

Hodgin-Huxley model (1952)

Describe the generation of

action potentials in the

squid giant axon

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Membrane potential The membrane cell separates two ionic solutions with different concentrations (ions are electrically charged atoms).

Membrane potential due to charge separation across the cell membrane.

V=Vin-Vout (by convention Vout=0)

Resting state V=-60 to -70 mV

Ionic channels embedded in the cell membrane (Na+ and K+ channels)

K +K +

K +

Na+

Na+ Na+

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Closed channelOpen channelDirection of propagation of nervous impulse

RestingActive state(action potential)

Resting and temporarily unable to fire

Repolarization (K+)

K+

K+Cellbody

Electrical signal

Travelling wave

Action potential

0 mV

-60 mV

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Action potential that propagates along the axon

xV

-60 mV

0 mV

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Electrical parameters: • Potential Difference V(x,t)=Vin -Vout

• Current I(t)• Conductance g(t), Resistance R(t)=1/g(t) • Capacitance C

Rules for electrical circuits• Capacitor (Two conducting plates separated by an insulating layer. It stores charge). C dV/dt = I • Ohm´s Law I=Vg, IR=V

Current balance equation for membrane

Electrical activity of cells

C∂V/∂t = D ∂2V/∂x2 - Iion + Iapp

= D ∂2V/∂x2 - Σi gi (V-Vi)+Iapp

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CdV/dt = - INa - IK – IL + Iapp

= – gNam3h(V-VNa) - gKn4(V-VK) - gL(V-VL) + Iapp

dm/dt = [m∞(V)-m]/m(V)dh/dt = [h∞(V) - h]/h(V)dn/dt = [n∞(V) – n]/n(V)

Hodgin-Huxley model (1952)

Model for electronically compact neurons V(x,t)=V(t).

V membrane potential

h,m,n channel state variables

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Other models…

The models for single neurons are based on HH formalism.

Models for describing some activity patterns: silent, bursting, spiking.

Reduced models to study networks consisting of a large number of coupled neurons.

C dv/dt = f(v,w) + I dw/dt = εg(v,n)

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Chemical synapsis

Synapsis can be:

Excitatory

Inhibitory

Presynaptic neuron

Postsynaptic neuron

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Reduced model for chemical synapsisModel for two mutually coupled neurons

Assume si= H(vj-), H Heaviside function

(vi – vsyn) <0 (>0) excitatory (inhibitory) synapsis

dv1/dt = f(v1,w1) – gsyns2(v1 – vsyn)

dw1/dt = g(v1,w1)

ds1/dt= (1-s1)H(v1-)-s1

dv2/dt = f(v2,w2) – gsyns1(v2 – vsyn)

dw2/dt = g(v2,w2)

ds2/dt = (1-s2)H(v2-)-s2

Cell 1

Cell 2

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Reduced model for chemical synapsisModel for two mutually coupled neurons

dv1/dt = f(v1,w1) – gsyns2(v1 – vsyn)

dw1/dt = g(v1,w1)

dv2/dt = f(v2,w2) – gsyns1(v2 – vsyn)

dw2/dt = g(v2,w2)

s1= H(v1-), s2 = H(v2-)

Cell 1

Cell 2

H Heaviside function ( H(x)=1 if x>0 and H(x)=0 if x<0 )

(vi – vsyn) <0 (>0) excitatory (inhibitory) synapsis

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Network Architecture

Which neurons communicate with each other.

How are the synapsis: excitatory or inhibitory.

Exemple. Architecture of the STN/GPe network (Basal Ganglia, involved in the control of movement )

GPe CELLS

STN CELLS

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Modeling neuronal activity patterns

Neuronal networks contain many parameters and time-scales:

• Intrinsic properties of individual neurons: Ionic channels.

• Synaptic properties: Excitatory/Inhibitory; Fast/Slow.

• Architecture of coupling.

Network activity patterns:

• Syncrhronized oscillations (all cell fires at the same time).

• Clustering (the population of cells breaks up into subpopulations; within each single block population fires synchronously and different blocks are desynchronized from each other).

• More complicated rythms

QUESTION: How do these properties interact to produce network behavior?

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Example. Numerical simulations of network activity.

Clustering and propagating activity patterns

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Synchronization

Why is synchronization important?

How do the brain know which neurons are firing according to the same reason?

Some diseases like Parkinson are associated to synchronization.

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Conclusions

Goal of neuroscience: unsderstand how the nervous system communicates and processes information.

Goal of mathematical neuroscience: Develop and analyze mathematical models for neuronal activity patterns.

Mathematical models • Help to understand how AP are generated and how they can change as parameters are modulated.

• Interpret data, test hypothesis and suggest new experiments.

• The model has to be chosen at an appropriate level: complex to include the relevant processes and “easy” to analyze.