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The Nerve Physiology




© 2008 Paul Billiet ODWS
HISTORY
Joseph Erlanger(1874-1965) and
Herbert Spencer Gasser (1888-
1963)




 1944 Joseph Erlanger and Herbert Spencer Gasser "for their discoveries
 relating to the highly differentiated functions of single nerve fibres
Joseph Erlanger and Herbert
 Spencer Gasser
 Joseph Erlanger was an American physiologist
 Herbert Spencer Gasser was an American physiologist, and
  recipient of the Nobel Prize for Physiology or Medicine in 1944 for
  his work with action potentials in nerve fibers while on the faculty of
  Washington University.
 Erlanger and his student Gasser were interested in developing
  tools that could measure impulses fired through nerve cells, and
  they turned to the cathode-ray oscilloscope – an instrument that
  allows electrical currents to be visualized as a moving two-
  dimensional graph on a phosphorescent screen.
 After its invention by Ferdinand Braun, the oscilloscope soon
  became the most effective tool for detecting rapid changes in
  electrical voltage, but still it was not sensitive enough to measure
  the weak and rapid electrical impulses that are fired along nerve
  cells
Eccles, Hodgkin and Huxley




The Nobel Prize in Physiology or Medicine 1963 was awarded jointly to Sir John Carew
Eccles, Alan Lloyd Hodgkin and Andrew Fielding Huxley "for their discoveries concerning the
ionic mechanisms involved in excitation and inhibition in the peripheral and central portions of
the nerve cell membrane".
Eccles, Hodgkin and Huxley
Sir Alan Lloyd Hodgkin British physiologist and biophysicist
Sir John Carew Eccles , Australian neurophysiologist
Sir Andrew Fielding Huxley English physiologist and biophysicist,
   Huxley evidenced the existence of saltatory conduction in myelinated nerve fibres.
 By showing how these impulses are generated and transmitted, the three scientists who received
an equal share of the 1963 Nobel Prize in Physiology or Medicine revealed the key triggers that
spark the nervous system's in-built electrical system into life.
Seeking ways of measuring electrical currents inside nerves, Alan Hodgkin and his student
Andrew Huxley turned to giant nerve fibres in the squid, which are almost a thousand times thicker
than their human counterparts.
 Using tiny electrodes to record the electrical difference between the inside and outside of these
nerves, they were surprised to find that the polarity did not drop from negative to zero during the
transmission of an impulse as predicted, but in fact reversed, becoming electrically positive.
 By carrying out a series of measurements and using complex mathematical models to interpret
the findings, Hodgkin and Huxley formulated a theory to propose how impulses are formed.
Changes in the permeability of the cell membrane allow charged atoms to flow in and out of a
nerve fibre, creating waves of electric charge that constitute the nerve impulse
Erwin Neher, Bert Sakmann




 The Nobel Prize in Physiology or Medicine 1991 was awarded jointly to
 Erwin Neher and Bert Sakmann "for their discoveries concerning the
 function of single ion channels in cells"
Erwin Neher, Bert Sakmann

 The two German cell physologisists Erwin Neher and Bert Sakmann
 have together developed a technique that allows the registration of
 the incredibly small electrical current (amounting to a picoampere-
 10-12A) that passes through a single ion channel.
 The technique is unique in that it records how a single channel
 molecule alters it's shape and in that way controls the flow of current
 within a time frame of a few millionths of a second.
 They have demonstrated what happens during the opening or
 closure of an ion channel with a diameter corresponding to that of a
 single sodium or chloride ion.
The neurone
                    Nodes of Ranvier
Dendrites
            Schwann cell               Nucleus of Schwann cell




            Myelin sheath      Axon            Terminal dendrites
Experiments on the neurone of a
 giant squid
                                Concentration /mmol kg-1 water

         Ion                  Axoplasm       Blood      Sea water
                           (the cytoplasm   plasma
                             in an axon)
          K+                    400           20            10
         Na+                    50            440          460

          Cl-                   120           560          540

     Organic
     anions                     360            -             -
    (-ve ions)

© 2008 Paul Billiet ODWS
Cells and membrane
 potentials
      All animal cells generate a small voltage across
      their membranes
      This is because there is a large amount of small
      organic molecules in the cytoplasm
      To balance this, animal cell pump Na+ out of the
      cells
      This regulates osmosis but it leaves a large
      number of organic molecules
      These are overall negatively changed (anions) in
      the cytoplasm
      Thus the cell has a potential difference (voltage)
      across its membrane
© 2008 Paul Billiet ODWS
Passive movement of ions across
 a cell membrane

      The concentration gradient:
      causing the ions to diffuse down their
      concentration gradient
      The electrical potential:
      causing ions to be attracted to the
      opposite charge to the one they carry



© 2008 Paul Billiet ODWS
Potassium & Sodium Ions
        The two important ions in a nerve cell (neurone
        or neuron) are K+ and Na+
        Both are cations (positively charged ions)
        Na+ ions move more slowly across the
        membrane than K+ or Cl- ions
        This is because although the Na+ ion is smaller
        than the K+ ion
        Na+ has a larger coating of water molecules
        giving it a bigger diameter
        This makes the plasma membrane 25 times
        more permeable to K+ than Na+

© 2008 Paul Billiet ODWS
Potassium & Sodium Ions
      In addition to this K+ ions leak out of K + ion pores
      when the nerve cell is at rest
      So to maintain the high concentration of K+ inside
      the cell, it has to be actively pumped inwards a bit
      when the cell is at rest
      The result is that the resting potential of the
      neurone is almost at the equilibrium for K+ ions
      K + leak out a bit and need pumping in
      Na + ions, however, are actively pumped
      out and kept out

© 2008 Paul Billiet ODWS
A coupled Na + -K + pump
                            plasma
        Cytoplasm
                           membrane     ECF


                    K+                K+
                           coupled
                             ion
                            pump
                    Na +              Na +




© 2008 Paul Billiet ODWS
Ionic basis of Em
                    NaK-
                    ATPase
                    pumps 3Na+
                    out for 2 K+
                    pumped in.
                    Some of the
                    K+ leaks
                    back out,
                    making the
                    interior of
                    the cell
Gated channels: ligand-gated
Gated channels: voltage-
gated
Characteristics of the Nerve
Impulse
  An electrochemical event that occurs in nerve
  cells following proper stimulation.
  An all-or-none process which is fast acting
  and quick to recover.
  An event that is described by a voltage curve
  that is called an action potential.
  The nerve impulse can be conducted the
  entire length of a nerve cell without
  diminishment (“domino effect”).
Characteristics of a Nerve
Impulse Continued:
  The nerve impulse serves as the primary
  information signal used by the nervous system
  to provide communication about stimuli, nerve
  cell activity, neurotransmitter release and to
  generate various output responses (motor
  action, glandular secretion, etc.).
  Typically initiated by graded or generator
  potentials from a stimulus.
Graded potential
A change in potential that decreases with
distance
   Localized depolarization or hyperpolarization
Graded Potentials
Graded Potentials
Graded potentials
vs
Action Potential
PSPs               vs        APs
 Graded                 All-or-none
  Summation

 longer duration
  *10-100 msec         short
 chemical-gated          1-2 msec
 passive spread
  instantaneous
                        voltage-gated
  decremental          propagated
                         slow

                         nondecremental
Resting Membrane Voltage
(RMV)
Nernst Equation

By the end of the 19th century, it was
known that the cytoplasm was high in K+
and that [Na+] was very low--and that this
relationship was reversed outside the cell.

The assumption was made that the cell
membrane was permiable to K+ but not to
Na+.
Goldman equation
was derived to solve
for transmembrane
potential using all ions
involved
simultaneously.
Resting
membrane potential(MP) resting potential(RP)

•nerve, muscle negative, constant, cell type
e.g.: warm-blooded animal: -55 to -100 mV; smooth muscle: -30 mV
Resting Potential
Outside of cell
                       Sodium/Potassium pump
                       continuously and actively pumps
                       (3) Na+ out of the cell and (2) K+
                       into the cell.
                       Na+ channels are closed so Na+
                       are not able to move into the cell.
                       K+ channels are open so K+ can
                       diffuse out of the cell.
                       This generates a separation of
                       charges so that the inside of the
                       cell is relatively – and the outside
                       is relatively +.
                       The cell will remain in this state (at
                       rest) until it is stimulated.


Inside of cell
Depolarisation
   Depolarising membranes may be
    achieved by:
    a stimulus arriving at a receptor cell
    (e.g. vibration of a hair cell in the ear)
    a chemical fitting into a receptor site
    (e.g. a neurotransmitter)
    a nerve impulse travelling down a
    neurone
© 2008 Paul Billiet ODWS
Action Potential
Appears when region of excitable
membrane depolarizes to threshold
Steps involved
   Membrane depolarization and sodium
    channel activation
   Sodium channel inactivation
   Potassium channel activation
   Return to normal permeability
The Action Potential
  Key Properties of the Action Potential
     Threshold
     Rising phase
     Overshoot
     Falling phase
     Undershoot
     Absolute refractory period
     Relative refractory period
Introduction
  Action Potential in the Nervous System
     Conveys information over distances
     Action potential
        Spike
        Nerve impulse
        Discharge
AP Characteristics
  Voltage-gated channels
  All or none
  Slow
  Non-decremental
  Self Propagated
The action potential
       The action potential is the state of the neurone
       membrane when a nerve impulse passes by
       A small change in the membrane voltage will
       depolarise the membrane enough to flip open Na+
       channels
       These are called voltage-gated Na + channels
       As Na+ moves into the cell more and more Na+
       channels open
       A small change in the membrane permeability to Na+
       results in a big change in membrane
       potential

© 2008 Paul Billiet ODWS
Properties of the Action
Potential
  The Ups and Downs of an Action
  Potential
     Oscilloscope to visualize an AP
        Rising phase, overshoot, falling phase, and
        undershoot
Properties of the Action
Potential
 The Generation of an Action Potential
    “All-or-none”: Cross threshold value for
     action potential
    Chain reaction
            Opens Na+-permeable channels Na+ influx
             depolarized membrane reaches threshold action
             potential
Properties of the Action
Potential
      Firing frequency reflects the magnitude of
       the depolarizing current
The Generation of an Action
Potential




                              Figure 2.16.1
Characteristics of action
potentials
 Generation of action potential follows all-or-none
 principle
 Refractory period lasts from time action potential
 begins until normal resting potential returns
 Continuous propagation
    spread of action potential across entire membrane in
     series of small steps
 Saltatory propagation
    action potential spreads from node to node, skipping
     internodal membrane
The Generation of an Action Potential
Induction of an action potential
Induction of an action potential
Action potential propagation
                     When the V-G Na+
                     channels open, they
                     cause a
                     depolarization of the
                     neighboring
                     membrane.
                     This causes the Na+
                     and K+ channels in
                     that piece of
                     membrane to be
                     activated
AP propagation cont.
 The V_G chanels in
 the neighboring
 membrane then
 open, causing that
 membrane to
 depolarize.
 That depolarizes
 the next piece of
 membrane, etc.
 It takes a while for
 the Na+ channels to
 return to their
 voltage-sensitive
 state. Until then,
 they won’t respond
 to a second
 depolarization.
Propagation of an Action Potential
along an Unmyelinated Axon
Saltatory Propagation along a
Myelinated Axon
Saltatory Propagation along a
Myelinated Axon
Action Potential Conduction
  Propagation of the action potential
     Down axon to the axon terminal
        Orthodromic: Action potential travels in one
         direction
        Antidromic (experimental): Backward
         propagation
     Typical conduction velocity: 10 m/sec
     Length of action potential: 2 msec
Action Potential Conduction
  Factors Influencing Conduction Velocity
     Spread of action potential along membrane
        Dependent upon axon structure
     Path of the positive charge
        Inside of the axon (faster)
        Across the axonal membrane (slower)
     Axonal excitability
        Axonal diameter (bigger = faster)
        Number of voltage-gated channels
Action Potential Conduction
  Factors Influencing Conduction Velocity
     Myelin: Facilitates current flow
     Layers of myelin sheath
        Myelinating cells
             Schwann cells in the PNS
             Oligodendroglia in CNS
Action Potential Conduction
  Factors Influencing Conduction Velocity
     Saltatory conduction
+35




                 0
                            More Na+
                            channels open
           mV               Na+ floods
                            into neurone

                           Na+ voltage-
                           gated
                           channels open
              -55                                              Threshold

              -70



                                                 Time

                     Resting potential      Action potential
© 2008 Paul Billiet ODWS
All-or-nothing
         As Na+ moves in the cell will become more
         positive with respect to the outside
         The ion pumps resist the change in the
         membrane potential but it only has to rise by
         15mV and the pumps cannot restore the
         equilibrium
         Na+ floods in
         Nerve impulses all look the same , there are
         not big ones and little ones
         This is the all-or-nothing law

© 2008 Paul Billiet ODWS
All-or-None Principle
Throughout depolarisation, the Na+ continues
   to rush inside until the action potential
   reaches its peak and the sodium gates close.
If the depolarisation is not great enough to
   reach threshold, then an action potential
   and hence an impulse are not produced.
This is called the All-or-None Principle.
The threshold

      –55mV represents the threshold
      potential
      Beyond this we get a full action potential
      The membrane potential rises to +35mV
      this is the peak of the action potential
      The cells are almost at the equilibrium
      for Na+ ions
© 2008 Paul Billiet ODWS
+35                                            Na+ channels close
                                                             and K+ channels
                                                             open, K+ floods out
                                                             of neurone
                  0


            mV



               -55                                                    Threshold

               -70


                                           Time

                      Resting potential   Action potential   Resting potential
© 2008 Paul Billiet ODWS
Potassium takes over
      After Na+ moves in passively until the Na+
      channels start to close
      At the same time K+ permeability increases as
      voltage-gated K + channels open – they are a
      bit slower to respond to the depolarisation than
      the Na+ channels
      The K+ ions move out
      This makes the cell negative inside with respect
      to outside again
      The membrane potential falls

© 2008 Paul Billiet ODWS
Hyperpolarisation
      The membrane potential falls below the
      resting potential of –70mV
      It is said to be hyperpolarised
      Gradually active pumping of the ions (K +
      in and Na+ out) restores the resting
      potential
      During this period no impulses can pass
      along that part of the membrane
      This is called the refractory period
© 2008 Paul Billiet ODWS
+35



                                                        Hyperpolarisation
                 0                                      of the membrane


         mV                                                 Active pumping
                                                            of Na+ out and K+
                                                            in during the
                                                            refractory period

               -55                                                 Threshold

               -70


                                          Time

                Resting potential   Action potential   Resting
© 2008 Paul Billiet ODWS                               potential
Repolarization
1. The sodium/potassium
pumps return the cell to a
resting state by actively
pumping (3) Na+ out of
the cell and (2) K+ into
the cell.
2. The K+ continues to
diffuse out of the cell.
Refractory Period
  after AP
      won’t fire again
      relative & absolute
  Relative
      during after hyperpolarization
      requires greater depolarization ~
Refractory Period
There are two types of
  refractory period:
Absolute Refractory
  Period – Na+ channels
  are inactivated and no
  matter what stimulus is
  applied they will not re-
  open to allow Na+ in &
  depolarise the membrane to the threshold of an action potential.


Relative Refractory Period - Some of the Na+ channels have re-opened but the
threshold is higher than normal making it more difficult for the activated Na+
channels to raise the membrane potential to the threshold of excitation.
Absolute refractory period
  Na+ channels deactivate
     will not trigger AP
     must reset
CLINICAL IMPLICATIONS
Cellular Electrophysiology
Membrane Potential
The Na+ / K+ Pump
SEIZURE
Anti-seizure Medications
  Seizures caused by hyperactive brain
  areas
  Multiple chemical classes of drugs
     All have same approach
     Decrease propagation of action potentials
        ⇓ Na+, Ca++ influx (delay depolarization/prolong
         repolarization)
        ⇑ Cl- influx (hyperpolarize membrane)
Anti-Seizure Medications
Benzodiazepines        Ion Channel Inhibitors
diazepam (Valium®)    carbamazepine
lorazepam (Ativan®)     (Tegretol®)
Barbiturates           phenytoin
phenobarbital           (Dilantin®)
  (Luminal®)           Misc. Agents
                       valproic acid
                         (Depakote®)
Clinical Correlation

  It is the rate of action potential propagation that
  determines neurologic function.
     Determined by frequency of action potentials.



                                            What is a seizure?
                                            What is a seizure?
         What would be the
          What would be the
      effect on the membrane
       effect on the membrane
            of ⇑ Cl- -influx
             of ⇑ Cl influx
          during a seizure?
           during a seizure?           Hyperpolarization & …
                                           ⇓ seizure
                                           activity!
Cl - -
Cl       Gamma Amino Butyric Acid
         Receptors
                           GABA
                           GABA
                          Receptor
                          Receptor



                                     Exterior

              Hyperpolarized!
              Hyperpolarized!


                                     Interior
Cl - -
 Cl

 GABA+Bz Complex
   Bz
  Bz                          GABA
                              GABA
Receptor
Receptor                     Receptor
                             Receptor



             Profoundly
             Profoundly                 Exterior

           Hyperpolarized!
           Hyperpolarized!


                                        Interior
THANK YOU

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Nerve physiology

  • 1. The Nerve Physiology © 2008 Paul Billiet ODWS
  • 3. Joseph Erlanger(1874-1965) and Herbert Spencer Gasser (1888- 1963) 1944 Joseph Erlanger and Herbert Spencer Gasser "for their discoveries relating to the highly differentiated functions of single nerve fibres
  • 4. Joseph Erlanger and Herbert Spencer Gasser  Joseph Erlanger was an American physiologist  Herbert Spencer Gasser was an American physiologist, and recipient of the Nobel Prize for Physiology or Medicine in 1944 for his work with action potentials in nerve fibers while on the faculty of Washington University.  Erlanger and his student Gasser were interested in developing tools that could measure impulses fired through nerve cells, and they turned to the cathode-ray oscilloscope – an instrument that allows electrical currents to be visualized as a moving two- dimensional graph on a phosphorescent screen.  After its invention by Ferdinand Braun, the oscilloscope soon became the most effective tool for detecting rapid changes in electrical voltage, but still it was not sensitive enough to measure the weak and rapid electrical impulses that are fired along nerve cells
  • 5. Eccles, Hodgkin and Huxley The Nobel Prize in Physiology or Medicine 1963 was awarded jointly to Sir John Carew Eccles, Alan Lloyd Hodgkin and Andrew Fielding Huxley "for their discoveries concerning the ionic mechanisms involved in excitation and inhibition in the peripheral and central portions of the nerve cell membrane".
  • 6. Eccles, Hodgkin and Huxley Sir Alan Lloyd Hodgkin British physiologist and biophysicist Sir John Carew Eccles , Australian neurophysiologist Sir Andrew Fielding Huxley English physiologist and biophysicist, Huxley evidenced the existence of saltatory conduction in myelinated nerve fibres. By showing how these impulses are generated and transmitted, the three scientists who received an equal share of the 1963 Nobel Prize in Physiology or Medicine revealed the key triggers that spark the nervous system's in-built electrical system into life. Seeking ways of measuring electrical currents inside nerves, Alan Hodgkin and his student Andrew Huxley turned to giant nerve fibres in the squid, which are almost a thousand times thicker than their human counterparts. Using tiny electrodes to record the electrical difference between the inside and outside of these nerves, they were surprised to find that the polarity did not drop from negative to zero during the transmission of an impulse as predicted, but in fact reversed, becoming electrically positive. By carrying out a series of measurements and using complex mathematical models to interpret the findings, Hodgkin and Huxley formulated a theory to propose how impulses are formed. Changes in the permeability of the cell membrane allow charged atoms to flow in and out of a nerve fibre, creating waves of electric charge that constitute the nerve impulse
  • 7. Erwin Neher, Bert Sakmann The Nobel Prize in Physiology or Medicine 1991 was awarded jointly to Erwin Neher and Bert Sakmann "for their discoveries concerning the function of single ion channels in cells"
  • 8. Erwin Neher, Bert Sakmann The two German cell physologisists Erwin Neher and Bert Sakmann have together developed a technique that allows the registration of the incredibly small electrical current (amounting to a picoampere- 10-12A) that passes through a single ion channel. The technique is unique in that it records how a single channel molecule alters it's shape and in that way controls the flow of current within a time frame of a few millionths of a second. They have demonstrated what happens during the opening or closure of an ion channel with a diameter corresponding to that of a single sodium or chloride ion.
  • 9. The neurone Nodes of Ranvier Dendrites Schwann cell Nucleus of Schwann cell Myelin sheath Axon Terminal dendrites
  • 10.
  • 11.
  • 12.
  • 13. Experiments on the neurone of a giant squid Concentration /mmol kg-1 water Ion Axoplasm Blood Sea water (the cytoplasm plasma in an axon) K+ 400 20 10 Na+ 50 440 460 Cl- 120 560 540 Organic anions 360 - - (-ve ions) © 2008 Paul Billiet ODWS
  • 14.
  • 15. Cells and membrane potentials All animal cells generate a small voltage across their membranes This is because there is a large amount of small organic molecules in the cytoplasm To balance this, animal cell pump Na+ out of the cells This regulates osmosis but it leaves a large number of organic molecules These are overall negatively changed (anions) in the cytoplasm Thus the cell has a potential difference (voltage) across its membrane © 2008 Paul Billiet ODWS
  • 16. Passive movement of ions across a cell membrane The concentration gradient: causing the ions to diffuse down their concentration gradient The electrical potential: causing ions to be attracted to the opposite charge to the one they carry © 2008 Paul Billiet ODWS
  • 17. Potassium & Sodium Ions The two important ions in a nerve cell (neurone or neuron) are K+ and Na+ Both are cations (positively charged ions) Na+ ions move more slowly across the membrane than K+ or Cl- ions This is because although the Na+ ion is smaller than the K+ ion Na+ has a larger coating of water molecules giving it a bigger diameter This makes the plasma membrane 25 times more permeable to K+ than Na+ © 2008 Paul Billiet ODWS
  • 18. Potassium & Sodium Ions In addition to this K+ ions leak out of K + ion pores when the nerve cell is at rest So to maintain the high concentration of K+ inside the cell, it has to be actively pumped inwards a bit when the cell is at rest The result is that the resting potential of the neurone is almost at the equilibrium for K+ ions K + leak out a bit and need pumping in Na + ions, however, are actively pumped out and kept out © 2008 Paul Billiet ODWS
  • 19. A coupled Na + -K + pump plasma Cytoplasm membrane ECF K+ K+ coupled ion pump Na + Na + © 2008 Paul Billiet ODWS
  • 20. Ionic basis of Em NaK- ATPase pumps 3Na+ out for 2 K+ pumped in. Some of the K+ leaks back out, making the interior of the cell
  • 23. Characteristics of the Nerve Impulse An electrochemical event that occurs in nerve cells following proper stimulation. An all-or-none process which is fast acting and quick to recover. An event that is described by a voltage curve that is called an action potential. The nerve impulse can be conducted the entire length of a nerve cell without diminishment (“domino effect”).
  • 24. Characteristics of a Nerve Impulse Continued: The nerve impulse serves as the primary information signal used by the nervous system to provide communication about stimuli, nerve cell activity, neurotransmitter release and to generate various output responses (motor action, glandular secretion, etc.). Typically initiated by graded or generator potentials from a stimulus.
  • 25. Graded potential A change in potential that decreases with distance  Localized depolarization or hyperpolarization
  • 29. PSPs vs APs Graded All-or-none Summation longer duration *10-100 msec short chemical-gated 1-2 msec passive spread instantaneous voltage-gated decremental propagated slow nondecremental
  • 31. Nernst Equation By the end of the 19th century, it was known that the cytoplasm was high in K+ and that [Na+] was very low--and that this relationship was reversed outside the cell. The assumption was made that the cell membrane was permiable to K+ but not to Na+.
  • 32. Goldman equation was derived to solve for transmembrane potential using all ions involved simultaneously.
  • 33. Resting membrane potential(MP) resting potential(RP) •nerve, muscle negative, constant, cell type e.g.: warm-blooded animal: -55 to -100 mV; smooth muscle: -30 mV
  • 34. Resting Potential Outside of cell Sodium/Potassium pump continuously and actively pumps (3) Na+ out of the cell and (2) K+ into the cell. Na+ channels are closed so Na+ are not able to move into the cell. K+ channels are open so K+ can diffuse out of the cell. This generates a separation of charges so that the inside of the cell is relatively – and the outside is relatively +. The cell will remain in this state (at rest) until it is stimulated. Inside of cell
  • 35. Depolarisation Depolarising membranes may be achieved by: a stimulus arriving at a receptor cell (e.g. vibration of a hair cell in the ear) a chemical fitting into a receptor site (e.g. a neurotransmitter) a nerve impulse travelling down a neurone © 2008 Paul Billiet ODWS
  • 36. Action Potential Appears when region of excitable membrane depolarizes to threshold Steps involved  Membrane depolarization and sodium channel activation  Sodium channel inactivation  Potassium channel activation  Return to normal permeability
  • 37. The Action Potential Key Properties of the Action Potential  Threshold  Rising phase  Overshoot  Falling phase  Undershoot  Absolute refractory period  Relative refractory period
  • 38. Introduction Action Potential in the Nervous System  Conveys information over distances  Action potential  Spike  Nerve impulse  Discharge
  • 39. AP Characteristics Voltage-gated channels All or none Slow Non-decremental Self Propagated
  • 40. The action potential The action potential is the state of the neurone membrane when a nerve impulse passes by A small change in the membrane voltage will depolarise the membrane enough to flip open Na+ channels These are called voltage-gated Na + channels As Na+ moves into the cell more and more Na+ channels open A small change in the membrane permeability to Na+ results in a big change in membrane potential © 2008 Paul Billiet ODWS
  • 41. Properties of the Action Potential The Ups and Downs of an Action Potential  Oscilloscope to visualize an AP  Rising phase, overshoot, falling phase, and undershoot
  • 42. Properties of the Action Potential The Generation of an Action Potential  “All-or-none”: Cross threshold value for action potential  Chain reaction  Opens Na+-permeable channels Na+ influx depolarized membrane reaches threshold action potential
  • 43. Properties of the Action Potential  Firing frequency reflects the magnitude of the depolarizing current
  • 44. The Generation of an Action Potential Figure 2.16.1
  • 45. Characteristics of action potentials Generation of action potential follows all-or-none principle Refractory period lasts from time action potential begins until normal resting potential returns Continuous propagation  spread of action potential across entire membrane in series of small steps Saltatory propagation  action potential spreads from node to node, skipping internodal membrane
  • 46. The Generation of an Action Potential
  • 47. Induction of an action potential
  • 48. Induction of an action potential
  • 49. Action potential propagation When the V-G Na+ channels open, they cause a depolarization of the neighboring membrane. This causes the Na+ and K+ channels in that piece of membrane to be activated
  • 50. AP propagation cont. The V_G chanels in the neighboring membrane then open, causing that membrane to depolarize. That depolarizes the next piece of membrane, etc. It takes a while for the Na+ channels to return to their voltage-sensitive state. Until then, they won’t respond to a second depolarization.
  • 51. Propagation of an Action Potential along an Unmyelinated Axon
  • 52. Saltatory Propagation along a Myelinated Axon
  • 53. Saltatory Propagation along a Myelinated Axon
  • 54. Action Potential Conduction Propagation of the action potential  Down axon to the axon terminal  Orthodromic: Action potential travels in one direction  Antidromic (experimental): Backward propagation  Typical conduction velocity: 10 m/sec  Length of action potential: 2 msec
  • 55. Action Potential Conduction Factors Influencing Conduction Velocity  Spread of action potential along membrane  Dependent upon axon structure  Path of the positive charge  Inside of the axon (faster)  Across the axonal membrane (slower)  Axonal excitability  Axonal diameter (bigger = faster)  Number of voltage-gated channels
  • 56. Action Potential Conduction Factors Influencing Conduction Velocity  Myelin: Facilitates current flow  Layers of myelin sheath  Myelinating cells  Schwann cells in the PNS  Oligodendroglia in CNS
  • 57. Action Potential Conduction Factors Influencing Conduction Velocity  Saltatory conduction
  • 58. +35 0 More Na+ channels open mV Na+ floods into neurone Na+ voltage- gated channels open -55 Threshold -70 Time Resting potential Action potential © 2008 Paul Billiet ODWS
  • 59. All-or-nothing As Na+ moves in the cell will become more positive with respect to the outside The ion pumps resist the change in the membrane potential but it only has to rise by 15mV and the pumps cannot restore the equilibrium Na+ floods in Nerve impulses all look the same , there are not big ones and little ones This is the all-or-nothing law © 2008 Paul Billiet ODWS
  • 60. All-or-None Principle Throughout depolarisation, the Na+ continues to rush inside until the action potential reaches its peak and the sodium gates close. If the depolarisation is not great enough to reach threshold, then an action potential and hence an impulse are not produced. This is called the All-or-None Principle.
  • 61. The threshold –55mV represents the threshold potential Beyond this we get a full action potential The membrane potential rises to +35mV this is the peak of the action potential The cells are almost at the equilibrium for Na+ ions © 2008 Paul Billiet ODWS
  • 62. +35 Na+ channels close and K+ channels open, K+ floods out of neurone 0 mV -55 Threshold -70 Time Resting potential Action potential Resting potential © 2008 Paul Billiet ODWS
  • 63. Potassium takes over After Na+ moves in passively until the Na+ channels start to close At the same time K+ permeability increases as voltage-gated K + channels open – they are a bit slower to respond to the depolarisation than the Na+ channels The K+ ions move out This makes the cell negative inside with respect to outside again The membrane potential falls © 2008 Paul Billiet ODWS
  • 64. Hyperpolarisation The membrane potential falls below the resting potential of –70mV It is said to be hyperpolarised Gradually active pumping of the ions (K + in and Na+ out) restores the resting potential During this period no impulses can pass along that part of the membrane This is called the refractory period © 2008 Paul Billiet ODWS
  • 65. +35 Hyperpolarisation 0 of the membrane mV Active pumping of Na+ out and K+ in during the refractory period -55 Threshold -70 Time Resting potential Action potential Resting © 2008 Paul Billiet ODWS potential
  • 66. Repolarization 1. The sodium/potassium pumps return the cell to a resting state by actively pumping (3) Na+ out of the cell and (2) K+ into the cell. 2. The K+ continues to diffuse out of the cell.
  • 67.
  • 68. Refractory Period after AP  won’t fire again  relative & absolute Relative  during after hyperpolarization  requires greater depolarization ~
  • 69. Refractory Period There are two types of refractory period: Absolute Refractory Period – Na+ channels are inactivated and no matter what stimulus is applied they will not re- open to allow Na+ in & depolarise the membrane to the threshold of an action potential. Relative Refractory Period - Some of the Na+ channels have re-opened but the threshold is higher than normal making it more difficult for the activated Na+ channels to raise the membrane potential to the threshold of excitation.
  • 70.
  • 71. Absolute refractory period Na+ channels deactivate  will not trigger AP  must reset
  • 72.
  • 73.
  • 77. Anti-seizure Medications Seizures caused by hyperactive brain areas Multiple chemical classes of drugs  All have same approach  Decrease propagation of action potentials  ⇓ Na+, Ca++ influx (delay depolarization/prolong repolarization)  ⇑ Cl- influx (hyperpolarize membrane)
  • 78. Anti-Seizure Medications Benzodiazepines Ion Channel Inhibitors diazepam (Valium®) carbamazepine lorazepam (Ativan®) (Tegretol®) Barbiturates phenytoin phenobarbital (Dilantin®) (Luminal®) Misc. Agents valproic acid (Depakote®)
  • 79. Clinical Correlation It is the rate of action potential propagation that determines neurologic function.  Determined by frequency of action potentials. What is a seizure? What is a seizure? What would be the What would be the effect on the membrane effect on the membrane of ⇑ Cl- -influx of ⇑ Cl influx during a seizure? during a seizure? Hyperpolarization & … ⇓ seizure activity!
  • 80. Cl - - Cl Gamma Amino Butyric Acid Receptors GABA GABA Receptor Receptor Exterior Hyperpolarized! Hyperpolarized! Interior
  • 81. Cl - - Cl GABA+Bz Complex Bz Bz GABA GABA Receptor Receptor Receptor Receptor Profoundly Profoundly Exterior Hyperpolarized! Hyperpolarized! Interior

Editor's Notes

  1. NOTE: I switched the position of slides 18 and 19