01 Neuronal Function
Transcript of 01 Neuronal Function
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The Physiology of Neuronal
Functionsneuronal morphologyneuronal circuits
membrane potentials
passive electrical properties of
membranes
electrochemical potentials
the generation of the membrane
resting potential
stimulation of the action potential
ionic basis of the action potential
the voltage-gated Na+channel
References: p. 113-128; 131-137
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Central nervous system (CNS): neurons of the brainand
the nerve cord(the spinal cord in vertebrates)Peripheral nervous system (PNS): neurons that connect
the CNS to all target tissues
Nervous systems
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Morphology
of neurons
All neurons have the
soma, one axon, and
numerous dendrites. Thecomplexity of structure
is related to function,
not phylogeny.
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Neuronal morphology
Soma
cell body
site of metabolism and cell
maintenance
may receive stimuli from
other neuronsDendrites
extensions of the soma
receive stimuli
receive signals form otherneurons
typical neuron can have
100s-1000s
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Axonconducts signals away from the cell body and toward the
axon terminal
only one per neuron
may branch at the axon terminalduring the development of the nervous system: the axon
extends from the soma toward the target cell(s) following
migratory cues
when the target is reached, specific junctions are formed
Neuronal morphology
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Cell body extensions and their interactions with other cells
establish a cell polarity:
dendrites: toward somaaxon: away from soma
Neuronal polarity
Example: skin mechanoreceptors (touch receptors) signals
travel from dendrites near skin to soma, then from soma
to axon terminals near the spinal cord (next illustration)
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Transmission of signals
between neurons in a
simple neuronal circuit
Sensory neurons (afferent neurons):
receive external stimuli and
transmit them to the CNS.
Interneurons: connections withinthe CNS.
Motor neurons (efferent neurons):
relays the signal to the tissue
that will elicit the response.
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A simple neuronal circuit
The ref lex arch in the cockroach:
afferent neuron: wind receptor
a giant interneuron
within the CNS
efferent neuron: leg
motor neuron
Note: locations
of the soma.
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In any neural connection there
is a presynaptic cell (the neuron
that transmits the signal) and a
postsynaptic cell (thetarget,
which may be another neuron ora different cell type).
Transmission of electrical
signalsbetweenneurons
Synapses: the junctions between
both cells.
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Graded signals: through thesomavary in amplitude
the strength of the signal depends
on the strength of the stimulus
lose intensity as they propagateAll-or-none signals:through the
axon
invariant amplitude
initiate in response to graded signals
once initiated, they propagate down
the axon without loss of signal
intensity
Transmission of electrical
signalswithin neurons
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The dendrites and the soma receive neurotransmitters
(chemicalsignals)from presynaptic terminals (the axon
terminals from presynaptic neurons).
chemical signals are then converted into electrical signals
when ion currents in the synapse region flow into the cell
these ion currents (graded signals) travel through the somaand are integrated at the spike initiation zone
the neuron then initiates its own electrical signal: the action
potential (AP, an all-or-none signal)
the action potential then travels down the axon and away
from the soma without losing its intensity
the signal reaches the axon terminal
the signal is converted back into a chemical signal when a
neurotransmitter is secreted into the next synapse
Transmission of electrical signalswithinthe neuron
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Transmission of electrical
signalswithin neurons
The neurons ability to transmit
a graded signal depends on the
passive electrical properties of
its membrane. The neurons
ability to initiatean all-or-nonesignal, and its ability to transmit
it withoutsignal loss, depend
on the active electrical properties
of its membrane.
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The nature of electrical signals in neurons
Electric potential:
the concentration of ions on one side of the membrane
electrostatic force:potential energy(why?)
Membrane potential:
the difference in ionic electric potentials between the two
sides of a membrane
Result: a voltage across the membrane (Vm), measured in
millivolts (mV)
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The ion gradients across the membrane
of a typical mammalian cell
The ion gradients across the membrane maintains osmotic
balance and are also necessary for many physiological
functions.
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Membrane-targeted antibiotics transport ions across the cell
membrane and destroy ionic gradients that are essential to
the life of the cells
Ionophores:
Valinomycin is a small ring molecule that binds K+in its
hydrophilic interior, shielding its charge from the
surrounding environmentthe outside region of the molecule is nonpolar, thus
facilitating its crossing of the hydrophobic interior of the
lipid membrane
Channel formers:Gramicidins are dimers of linear peptides that insert
themselves into lipid bilayers and allow the free passage
of H+, K+, and Na+ions
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Cystic fibrosis
Cystic fibrosis is caused by a mutation in an ATP-dependent
Cl
-
transport, which alters the normal ionic gradients inseveral types of epithelial cells.
this results in the abnormal production of thick, sticky
mucous secretions by epithelial cells lining the
respiratory and intestinal tracts (Why?)treatment may extend the survival of affected individuals to
about 30 years, but the disease is ultimately fatal, with
lung disease being responsible for 95% of mortality
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The ATP-dependent Cl-
transport
70% of the point mutations
that cause cystic fibrosis
disrupt the folding of the
protein, resulting in
defective Cl-
transport.
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Na+,K+,Ca2+, and Cl-gradients maintain membrane
voltages in all living cells, but:
only two types of cells are able to respond to changes in
membrane voltage: neurons and muscle cells
only neurons and muscle cells areexcitable cells
The voltage across a membrane
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Luigi Galvani
(1737-1798)
Italian physicist
i i l i i ( )
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Luigi Galvani was looking for the animal electr ici tythat
activated the muscles of his dissected frog specimens.
he devised an electrical circuit: a muscle cell touched by a
nerve and a zinc rod, and a different metal rod (cooper)
that linked the nerve and the zinc rod (a)
he then observed that muscle cells contracted when the twodissimilar rods touched (circuit completed)
Alessandro Volta (1792) suggested that the metal rods
provided an outside energy source that excited the cells
Carlo Matteucci demonstrated that excitable tissues produce
electric currents (b)
Luigi Galvanis experiments (1791)
i i G l i i (1 91)
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Luigi Galvanis experiments (1791)
C l M i i
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Carlo Matteuccis experiments
M i b i l
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Vmcan be recorded as the difference in electric potentials
detected by a recording glass microelectrode and a
reference electrode.
no difference when both electrodes are in the saline bath
Measuring membrane potential
M i b t ti l
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when the recording electrode penetrates cell, the difference
in electric potentials between the two sides of themembrane is recorded as a voltage (Vm)
Vm(membrane voltage) of living cells have negative values:
higher concentration of negative ions on the cytosolicside
of the membrane (inside the cell)
Measuring membrane potential
M b t ti l
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Membrane potential
The membrane potential of living cells is defined as the
cytosolic potential relative to the extracellular potential
(extracellular potential is conventionally defined as zero).
steady inside-negative potential: resting potential (Vrest)
all cells have a Vrestbetween -20 mV and -100 mV
due to the passive electrical properties of the membran
P i l t i l ti f th ll b
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Electrical Resistance (R): impermeability to ions.
Electrical Conductance (g): permeability to ions due to open
ion channels.
Passive electrical properties of the cell membrane
the resistive current (Ir) will be higher if R is low (when ion
channels open)
R=1/g
P i l t i l ti f th ll b
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Capacitance: the ability to store electric charges (Cm).
the lipid bilayer is impermeable to ions but is very thin,
therefore:
ionic charges on both sides of the membrane can interact
if there is an excess of positive charges on the extracellular
side: they will be displaced toward the membrane, theywill attract anions on the other side, and cations on the
cytoplasm will be repelled from the membrane
effect: a capacitative current (Ic)
Passive electrical properties of the cell membrane
Th ll b it
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Capacitance: CmCapacitative
current: Ic
The cell membrane as a capacitor
Membrane oltage changes in response to
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Membrane voltage changes in response to
stimulating currents
Stimulus current: an ion flow through the cell membrane that
can change its resting potential.
this current can be experimentally applied using a current
electrode
Membrane voltage
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Membrane voltage
changes in response to
stimulating currents
Deviations from the resting
potential in response
to applied currents:
small negative stimuluscurrent: a small
hyperpolarization of
the membrane (1 & 2)
smallpositive stimulus
current: a small
depolarization of
the membrane (3)
Membrane voltage
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But:
if Vmreaches the
threshold potential:
an action potential(AP) is fired(4)
Membrane voltage
changes in response to
stimulating currents
(this happens only
in excitable cells)
Membrane voltage
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Whats wrong with
this figure?
The DVmresulting from
a subthreshold stimulusshould be sustained for
as long as the stimulus
current is applied.
Membrane voltage
changes in response to
stimulating currents
Passive electrical properties of the membrane
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capacitance and conductance/resistance are the passive
electrical properties of the membrane
they give the membrane its ability for time-dependent
responses to stimulation and voltage changes
they depend on the membrane potential (Vm)
Summary
How is the membrane potential generated?
Passive electrical properties of the membrane
Electrochemical potential
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Electrochemical potential defines the potential difference
across the plasma membrane. It is dependent on two
features of cells:
1. the concentrations of certain ions on the cytosolicside
of the membrane are different from the extracellular
side of the membrane2. membranes are selectively permeable to ions due to
the presence of selective ion channels
Electrochemical potential
A chamber filled with KCl with two compartments separated
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A chamber filled with KCl, with two compartments separated
by a membrane that is permeable to K+but notto Cl-
equal movement of K+in both directions but no net
changes in K+concentration
equal distribution of charges: no potential difference (Vm=0)
If KCL concentration in compartment I is increased
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If KCL concentration in compartment I is increased
K+will tend to move to compartment II (due to the K+
concentrationgradient)
this will generate a K+gradient and a voltage across the
membrane
the resulting electromotive force (emf) will tend to drive K+
back to compartment I
when no more net K+flow occurs: electrochemical
equilibrium, due to both driving forces, which occurs
at the equilibrium potential
If KCL concentration
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If KCL concentration
in compartment I
is increased
Summary of definitions
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Summary of definitions
Electrochemical equilibrium:
the state at which the concentration gradient of an ion acrossa membrane is precisely balanced by the electromotive
force across the membrane in the opposite direction
not netflow of the ion occurs
it is notthe state in which the concentrations of the ion onboth sides of the membrane are equal
Equilibrium potential (Ex):
the Vmat which an ionic species that can diffuse across the
membrane is in electrochemical equilibrium
example: the equilibrium potential for K+isEK
The generation of the membrane potential
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The resting membrane potential (Vrest) in cells is
maintained at the expense of metabolic energy.
because of this, Vrestis a steady state potential (not an
equilibrium potential)
Vrestgives the membrane itspassiveelectrical properties(capacitance and conductance/resistance)
The generation of the membrane potential
in biological membranes
Generation of the membrane resting potential
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Generation of the membrane resting potential
The ions channels responsible for the steady state potential
are the Na+/K+pump(requires energy) and the
K+leak channel(does notrequire energy).
The Na+/K+pump
hydrolyzes ATP to transport 3 Na+s out of the cell
and 2 K+s to the cytoplasmresult: unequal ionic distribution (an electrochemichal
gradient)
The K+
leak channelallowssomeK+to flow back through the membrane
determined by:
1. concentration gradient (K+inside)
2. electrical gradient (Na+emf from outside)
The Na+/K+
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The Na /K
pump generates
the membrane
resting potential
Active electrical properties of the membrane
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Active electrical properties of the membrane
The action potential
The action potential(AP) is a sudden and transient changein the cell membrane potential: Vmbecomes positive.
occurs when voltage gated Na+ channels on the excitable
membraneopen, allowing the flow of Na+into the cell
these channels are not the same as the Na+/K+pump thatgenerate the electrochemichal gradient
the AP is an all-or-none signal: its amplitude is invariable*
APs can only occur in excitable cells: neurons and muscle
cells
the repolarization of the membrane following an AP
depends on voltage-gated K+ channels
Ionic basis of the action potential
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Sequence of events:
at rest, all voltage-gated channels are closed
when Na+voltage-gated channels open: depolarization
(rising phase)
Na+channels then become inactive and K+voltage-gated
channels (not pictured) open: return(falling phase)after hyperpolarization, K+channels close and Na+channels
return to the closed conformation
Ionic basis of the action potential
Voltage gated Na+ channels & the action potential
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Voltage gated Na channels & the action potential
Changes in V and ionic conductances
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Vrest~ -70 mV
Rising phase:
Na+conductance (gNa) increases
Na+flows in(depolarization)
Falling phase:
gNadecreases
K+conductance (gK) increases
as the inwardNa+current decreases, an outwardflow of K+
occurs, resulting in hyperpolarizationAfter the AP:
gKdecreases
as the K+current decreases, the membrane returns to Vrest
Changes in Vmand ionic conductances
during an action potential
Changes in Vm and
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Changes in Vmand
ionic conductances during
an action potential
Ion cunductances (g)
Membrane polarity (V)
(not the direction of
ion currents)
Threshold potential
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The threshold potential is defined as the Vmat which an AP is
triggered 50% of the times.
Threshold potential
if a stimulating current is not intense enough to fire an AP
(1& 2,subthreshold stimuli), the resulting Vmis only
sustained for as long as the stimulus current is applied but
will return to Vrest
as soon as the stimulus ends
an AP response will continue without the stimulus current
overshoot: the period during which the membrane polarity is
reversed and the interior is more positive
membrane will quickly return directly to Vrest, or:it may go below Vrest: hyperpolarization (undershoot), then
slowly return to Vrest
a threshold current (3) triggers APs but can sometimes result
in a local response (an abortive AP)
The action potential is fired when the membrane reaches the
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e c o po e s ed w e e e b e e c es e
threshold potential in response to a stimulating current
The refractory periods after an action potential
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y p p
Immediately following an AP, a second AP is not possible
during the absolute refractory per iod(ARP).
the first stimulus current triggers an AP, buta second stimulus will not trigger an AP if applied within
the absolute refractory period
during the relative refractory period (RRP), an AP may be
triggered but only if the stimulus is more intense
the amplitude of any AP triggered during the relative
refractory period will be smaller
The refractory periods
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y p
after an action potential
Excitability of the
membrane:
zero during ARP
increases during RRP
(textbook toilet!)
The neuron threshold potential can increase in response
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p p
to slowly increasing subthreshold stimuli
Accommodation
Accommodation to sustained stimulation
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Phasic accommodation is a rapid accommodation to a
sustainedstimuluscurrent.
only 1-2 APs will occur, and only when the stimulus begins
Lowered accommodation response
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p
Tonic accommodation is slow accommodation.
APs will be fired repeatedly during stimulation, but with
decreasing frequency
Transmission of electrical
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In thesomaand the dendrites,
a stimulus current elicited bya presynaptic cell induces a
voltage change (agraded
signal) that propagates until it
reaches thespike initiation
zone. If the current is still
strong enough when it reaches
the spike initiation zone, it willinduce APs (all-or- nothing
signals) that will propagate
down the axon.
signalswithinneurons
Propagation of the action potential
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p g p
The opening and closing of voltage-gated Na+channels
along the axon is sequential.
the current that flows through one Na+channel (or througha local group of Na+channels) provides the stimulus
(voltage change) to open the next channels
electrodes can measure membrane voltage at different
points along an axon
Propagation of the action potential
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p g p
Propagation of an action potential along an axon
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orange arrows: Na+
flowblue box: depolarized region
Propagation of an action potential along an axon
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orange arrows: Na+
flowblue box: depolarized region
The refractory periods after an action potential
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absolute: alllocal voltage-gated Na+channels are inactive
relative: local voltage-gated Na+channels are returning tothe closed conformation andsome voltage-gated K+
channels remain open
in an excitable membrane (a membrane that can elicit an
all-or-none response): all voltage-gated Na+and K+
channels are closed