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Computational Biology, Part 20 Neuronal Modeling Robert F. Murphy Copyright  1996, 1999, 2001. All rights reserved.

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Presentation on theme: "Computational Biology, Part 20 Neuronal Modeling Robert F. Murphy Copyright  1996, 1999, 2001. All rights reserved."— Presentation transcript:

1 Computational Biology, Part 20 Neuronal Modeling Robert F. Murphy Copyright  1996, 1999, 2001. All rights reserved.

2 Basic Neurophysiology An imbalance of charge across a membrane is called a membrane potential An imbalance of charge across a membrane is called a membrane potential The major contribution to membrane potential in animal cells comes from imbalances in small ions (e.g., Na, K) The major contribution to membrane potential in animal cells comes from imbalances in small ions (e.g., Na, K) The maintainance of this imbalance is an active process carried out by ion pumps The maintainance of this imbalance is an active process carried out by ion pumps

3 Basic Neurophysiology The cytoplasm of most cells (including neurons) has an excess of negative ions over positive ions (due to active pumping of sodium ions out of the cell) The cytoplasm of most cells (including neurons) has an excess of negative ions over positive ions (due to active pumping of sodium ions out of the cell) By convention this is referred to as a negative membrane potential (inside minus outside) By convention this is referred to as a negative membrane potential (inside minus outside) Typical resting potential is -50 mV Typical resting potential is -50 mV

4 Basic Neurophysiology Ion pumps require energy (ATP) to carry ions across a membrane up a concentration gradient (they generate a potential) Ion pumps require energy (ATP) to carry ions across a membrane up a concentration gradient (they generate a potential) Ion channels allow ions to flow across a membrane down a concentration gradient (they dissipate a potential) Ion channels allow ions to flow across a membrane down a concentration gradient (they dissipate a potential)

5 Basic Neurophysiology A cell is said to be electrically polarized when it has a non-zero membrane potential A cell is said to be electrically polarized when it has a non-zero membrane potential A dissipation (partial or total) of the membrane potential is referred to as a depolarization, while restoration of the resting potential is termed repolarization A dissipation (partial or total) of the membrane potential is referred to as a depolarization, while restoration of the resting potential is termed repolarization

6 Basic Neurophysiology Ion channels can switch between open and closed states Ion channels can switch between open and closed states If an ion channel can switch its state due to changes in membrane potential, it is said to be voltage-sensitive If an ion channel can switch its state due to changes in membrane potential, it is said to be voltage-sensitive A membrane containing voltage-sensitive ion channels and/or ion pumps is said to be an excitable membrane A membrane containing voltage-sensitive ion channels and/or ion pumps is said to be an excitable membrane

7 Basic Neurophysiology An idealized neuron consists of An idealized neuron consists of  soma or cell body  contains nucleus and performs metabolic functions  dendrites  receive signals from other neurons through synapses  axon  propagates signal away from soma  terminal branches  form synapses with other neurons

8 Basic Neurophysiology The junction between the soma and the axon is called the axon hillock The junction between the soma and the axon is called the axon hillock The soma sums (“integrates”) currents (“inputs”) from the dendrites The soma sums (“integrates”) currents (“inputs”) from the dendrites When the received currents result in a sufficient change in the membrane potential, a rapid depolarization is initiated in the axon hillock When the received currents result in a sufficient change in the membrane potential, a rapid depolarization is initiated in the axon hillock

9 Basic Neurophysiology The depolarization is caused by opening of voltage-sensitive sodium channels that allow sodium ions to flow into the cell The depolarization is caused by opening of voltage-sensitive sodium channels that allow sodium ions to flow into the cell The sodium channels only open in response to a partial depolarization, such that a threshold voltage is exceeded The sodium channels only open in response to a partial depolarization, such that a threshold voltage is exceeded

10 Basic Neurophysiology As sodium floods in, the membrane potential reverses, such that the interior is now positive relative to the outside As sodium floods in, the membrane potential reverses, such that the interior is now positive relative to the outside This positive potential causes voltage- sensitive potassium channels to open, allowing K + ions to flow out This positive potential causes voltage- sensitive potassium channels to open, allowing K + ions to flow out The potential overshoots (becomes more negative than) the resting potential The potential overshoots (becomes more negative than) the resting potential

11 Basic Neurophysiology The fall in potential triggers the sodium channels to close, setting the stage for restoration of the resting potential by sodium pumps The fall in potential triggers the sodium channels to close, setting the stage for restoration of the resting potential by sodium pumps This sequential depolarization, polarity reversal, potential overshoot and repolarization is called an action potential This sequential depolarization, polarity reversal, potential overshoot and repolarization is called an action potential

12 Action Potential

13 Basic Neurophysiology The depolarization in the axon hillock causes a depolarization in the region of the axon immediately adjacent to the hillock The depolarization in the axon hillock causes a depolarization in the region of the axon immediately adjacent to the hillock Depolarization (and repolarization) proceeds down the axon until it reaches the terminal branches, which release neurotransmitters to stimulate neurons with which they form synapses Depolarization (and repolarization) proceeds down the axon until it reaches the terminal branches, which release neurotransmitters to stimulate neurons with which they form synapses

14 Basic Neurophysiology These sequential depolarizations form a traveling wave passing down the axon These sequential depolarizations form a traveling wave passing down the axon Note that while a signal is passed down the axon, it is not comparable to an electrical signal traveling down a cable Note that while a signal is passed down the axon, it is not comparable to an electrical signal traveling down a cable

15 Basic Neurophysiology Current flows in an electrical cable Current flows in an electrical cable  are in the direction that the signal is propagating  consist of electrons Current flows in a neuron Current flows in a neuron  are transverse to the signal propagation  consist of positively-charged ions

16 The Hodgkin-Huxley Model Based on electrophysiological measurements of giant squid axon Based on electrophysiological measurements of giant squid axon Empirical model that predicts experimental data with very high degree of accuracy Empirical model that predicts experimental data with very high degree of accuracy Provides insight into mechanism of action potential Provides insight into mechanism of action potential

17 The Hodgkin-Huxley Model Define Define  v(t)  voltage across the membrane at time t  q(t)  net charge inside the neuron at t  I(t)  current of positive ions into neuron at t  g(v)  conductance of membrane at voltage v  C  capacitance of the membrane  Subscripts Na, K and L used to denote specific currents or conductances (L=“other”)

18 The Hodgkin-Huxley Model Start with equation for capacitor Start with equation for capacitor

19 The Hodgkin-Huxley Model Consider each ion separately and sum currents to get rate of change in charge and hence voltage Consider each ion separately and sum currents to get rate of change in charge and hence voltage

20 The Hodgkin-Huxley Model Central concept of model: Define three state variables that represent (or “control”) the opening and closing of ion channels Central concept of model: Define three state variables that represent (or “control”) the opening and closing of ion channels  m controls Na channel opening  h controls Na channel closing  n controls K channel opening

21 The Hodgkin-Huxley Model Define relationship of state variables to conductances of Na and K Define relationship of state variables to conductances of Na and K

22 The Hodgkin-Huxley Model Can write differentials for m,n,h with respect to t Can write differentials for m,n,h with respect to t Gives set of four coupled, non-linear, ordinary differential equations Gives set of four coupled, non-linear, ordinary differential equations Must be integrated numerically Must be integrated numerically

23 Hodgkin-Huxley Gates

24 Interactive demonstration (Integration of Hodgin-Huxley equations using Maple) (Integration of Hodgin-Huxley equations using Maple)


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