lec2
DESCRIPTION
TRANSCRIPT
Membrane Potential (Vm): - charge difference across the membrane -
K+
Na+
K+
Na+
inside outside…how can passive diffusion of potassium and sodium lead to development of negative membrane potential?
Simplest Case
If a membrane were permeable to only K+ then…
inside outside
K+ K+
K+ would diffuse down its concentration gradient until the electrical potential across the membrane countered diffusion.
Simplest Case
K+ K+
If a membrane were permeable to only K+ then…
The electrical potential that counters net diffusion of K+ is called the K+ equilibrium potential (EK).
inside outside
The Potassium Nernst Potential
Example: If Ko = 5 mM and Ki = 140 mM
EK = -61 log(140/4)
EK = -61 log(35)
EK = -94 mV
EK = 61 log
Ki
Ko
So, if the membrane were permeable only to K+, Vm would be -94 mV
…also called the equilibrium potential
Simplest Case
Na+Na+
If a membrane were permeable to only Na+ then…
The electrical potential that counters net diffusion of Na+ is called the Na+ equilibrium potential (ENa).
inside outside
Na+ would diffuse down its concentration gradient until potential across the membrane countered diffusion.
The Sodium Nernst Potential
Example: If Nao = 142 mM and Nai = 14 mM
EK = -61 log(14/142)
EK = -61 log(0.1)
EK = +61 mV
EK = 61 log
Nai
Nao
So, if the membrane were permeable only to Na+, Vm would be +61 mV
Resting Membrane Potential
0 mV
EK -94 ENa +61
Vm -90 to -70
Why is Vm so close to EK?Ans. The membrane is far more permeable to K than Na..
The Goldman-Hodgkin-Katz Equation (also called the Goldman Field Equation)
Calculates Vm when more than one ion is involved.
oCliNaiK
iCloNaoKm
ClpNapKp
ClpNapKpV
]['][']['
]['][']['log. -++
-++
++++
=61
NOTE:P’ = permeability
iCloNaoK
oCliNaiKm
ClpNapKp
ClpNapKpV
]['][']['
]['][']['log. -++
-++
++++
= -61
or
The Goldman-Hodgkin-Katz Equation
The resting membrane potential is closest to the equilibrium potential for the ion with the highest permeability!
ATP
3 Na+
2 K+
ADP
Active Transport
K+ Na+
Na+ K+
inside outside
Remember: sodium is pumped out of the cell, potassium is pumped in...
Resting Membrane Potential Summary
Cells: contain high a K+ concentration have membranes that are essentially
permeable to K+ at rest
Membrane electrical potential difference (membrane potential) is generated by diffusion of K+ ions and charge separation measured in mV (=1/1000th of 1V) typically resting membrane potentials in
neurons are -70 to 90 mV
Resting and action potentials
++
+
+
+ +
+
+
+
++
–
–
–– –
–
–
–––
–
Voltmeter
– +0 mV-80 mV +
Nerve Action Potential
Nerve signals are transmitted by action potentials, which are rapid changes in the membrane potential that spread rapidly along the nerve fiber membrane
Action potential begins with a sudden change from the normal resting negative membrane potential to a positive potential and then ends with an almost equally rapid change back to the negative potential
Changes that occur at the membrane during the action potential Transfer positive
charges to the interior of the fiber at the onset and return positive charges to the exterior at its end
Nerve Action Potential
Stages of action potential
Resting Stage. This is the resting membrane potential before the action potential begins. The membrane is said to be "polarized" during this stage because of the -90 millivolts negative membrane potential that is present
Depolarization Stage
The membrane suddenly becomes very permeable to sodium ions, allowing tremendous numbers of positively charged sodium ions to diffuse to the interior of the axon.
The normal "polarized" state is neutralized by the inflowing positively charged sodium ions, with the potential rising rapidly in the positive direction
This is called depolarization
Repolarization Stage
After the membrane becomes highly permeable to sodium ions, the sodium channels begin to close and the potassium channels open more than normal
Rapid diffusion of potassium ions to the exterior re-establishes the normal negative resting membrane potential
This is called repolarization of the membrane
The AP - membrane permeability
• During the upstroke of an action potential: Na permeability increases
due to opening of Na+ channels memb. potential approaches
ENa
Num
ber
of o
pen
chan
nel s
Na+ channels
upst
roke
K permeability increases due to opening of K+ channels
mem. potential approaches EK
downstroke
• After hyperpolarization of membrane following an action potential:
Membranehyperpolarized
resting potential
K+ channels
There is increased K+ conductance due to delayed closure of K+
channels
• During the downstroke of an action potential: Na permeability decreases
due to inactivation of Na+ channels
1 ms
+61
0
(mV)
-90
ENa
EK
Properties of action potentials Action potentials: are all-or-none events
threshold voltage (sudden increase in the membrane potential) threshold
-70
+60
mV
Stim
ulus
0
non- myelinated
0 800400
have constant conduction velocity Fibers with large diameter conduct
faster than small fibers
Fiber diameter (mm)
Vel
ocity
(m
/s)
0 3 6 9
Myelinated
12
75
15
50
25
0
are initiated by depolarization action potentials can be induced in nerve
and muscle by extrinsic stimulation
Propagation:
Rest
Opening of Na+ channels generates local current circuit that depolarizes adjacent membrane, opening more Na+ channels…
Stimulated(local depolarization)
Propagation(current spread)
Signal Transmission:
Myelination• Schwann cells surround the nerve
axon forming a myelin sheath
• Sphingomyelin decreases membrane capacitance and ion flow 5,000-fold
• Sheath is interrupted every 1-3 mm : node of Ranvier
Saltatory Conduction• AP’s only occur at the nodes (Na
channels concentrated here!)• increased velocity• energy conservation
Conduction velocity
non-myelinated
myelinated
- non-myelinated vs myelinated -