Membrane potentials Thermodynamic treatment: Nernst-Planck flux equation Nernst equationConstant...
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Transcript of Membrane potentials Thermodynamic treatment: Nernst-Planck flux equation Nernst equationConstant...
Membrane potentials
Thermodynamic treatment:
Nernst-Planck flux equation
Nernst equation Constant field equation
Equivalent electrical circuit:
Parallel conductance model
Active transport: pumps, carriers
Electrochemical potential
ui is the electrochemical potential (contribution of one mole of the ith constituent to free energy and is the drive for flux across the membrane)
Solute transport occurs from region of higher to lower electrochemical potential
For membrane transport: ui = ui
o + RTlnCi + ziFV + …
ziFV is the contribution of the electrical potential ie the work required to bring a mole of ions with charge z from zero potential to potential V (F = 9.65 x 104 coulombs/mole)
uio is the standard electrochemical potential at C= 1M,
V=0
Equilibrium
At equilibrium the electrochemical potential is the same on each side of membrane;
uio + RTlnC1 + ziFV1 = ui
o + RTlnC2 + ziFV2
V2-V1 = E = RT ln C1
ziF C2
Nernst potential
Z = valenceR = gas constant: 8.314 (volts x coulombs/KO x mol)T = absolute temperatureF = Faraday constant: 96,500 coulombs/mol
Nernst Equation: how it works
IN = 100 mM KCl OUT = 10 mM KCl
= K+
= Cl-
-
+
-
+
--
-
+```
(-)(+)
• A membrane separates solutions of 100 mM and 10 mM KCl:
• The membrane is permeable to K+, but not to Cl-
• K+ ions diffuse across the membrane from left to right
• The movement of K+ makes the inside negative with respect to outside - this membrane potential prevents further net movement of K+
• Equilibrium is quickly established; the magnitude of is computed from the Nernst equation
mvK
K
z in
out 60)1(*60100
10log*60
][
][log
60=−===
For a real cell
Area of cell membrane = 1000 µm2 ()Radius = 8.92 µmVolume = 2974 x 10-15 liters (4/3r3)
140 mM K+
5 mM Na+
145 mM Cl-
5 mM K+
140 mM Na+
145 mM Cl-
K+
Vm = 58.17 log [5]/[140] = -87 mV
Questions: 1) How many K+ ions did the cell lose? 2) Did the K+ concentration inside the cell change?
How many K+ ions did the cell lose?
Use Q= CV
Know Vm = -87 mV
Calculate C
A = 1000 µm2 = 10-5 cm2 (1 µm = 10-4 cm)
Cm = 1 µF/cm2 x A (cm2) = 10-6 F/cm2 x 10-5 cm2 = 10-11 F = 10 pF
Q = 0.087 V x 10-11 F = 8.7 x 10-13 coulombs
Using Faraday’s constant: 8.7 x 10-13 C / 96,500 C/mol = 8.7 x 10-18 moles
Using Avogadro’s #: 8.7 x 10-18 moles x 6 x 1023 molecules/mole =
5 x 106 K+ ions
A single K channel ~2 pA current passes 107 ions/sec
Did the K+ concentration inside the cell change?
140 mM K+ = 0.14 moles/liter
0.14 moles/l x 6 x 1023 molecules/mole
= 0.84 x 1023 molecules/liter
Cell volume is 2974 x 10-15 liters
0.84 x 1023 molecules/liters x 2974 x 10-15 liters
= 2.3 x 1011 K+ ions in the cell
So losing 5 x 106 ions is not much
Ki does not change (in some cases Ko can!)
Membrane potentials with more than one ion
In Out
100 mM KCl 10 mM KCl
10 mM NaCl 100 mM NaCl
• If membrane is permeable only to K+ - what is ?
-
-
-
-
+
+
+
+
-
-
-
-
+
+
+
+
mvEV Km 60100
10log60 −===
• If membrane is permeable only to Na+?
• What if the membrane is 10 times more permeable to K+ than to Na+?
mvVm 2.42−=
Vm in this case is somewhat more positive than Ek
mvEV Nam 6010
100log60 ===
-
-
-
-
+
+
+
+
can’t use Nernst equation in this situation – ions are not in equilibrium.
Ions are not in equilibriumNeed to calculate ion fluxes at steady-state
Nernst-Planck Flux Equation
J = L dµ/dxFlux (J) proportional to gradient of electrochemical potential
J = L d [RTlnC + zFV] dx
= L [RT dC + zF dV] C dx dx
For a neutral diffusing substance (z=0), flux given by Fick eqn
J = -D dC/dx = L RT dC C dx
so L = -DC/RT
Substituting and rearranging:
J = -D dC + C zF dV dx RT dx
Nernst-Planck Equation
V
d
µo
V(x) Constant field approximation:
dV = Vdx d
Integrate Nernst-Planck eqn from 0 to d across membrane:
J = -zF D V RT d
C(d)ezFV/RT - C(0)
ezFV/RT - 1
The concentration of an ion just inside the membrane is related toIts concentration in the bulk solution by a partition coefficient:
C (membrane) = k
C (bulk solution)
Permeability coefficient P= Dk/d
J = -zFV P RT
C(1)ezFV/RT - C(2)
ezFV/RT - 1
J -mol/cm2sD= cm2/sP= cm/s
What is the permeability constant?
Comes from flux equation: J = -DA dc/dx
J = flux (moles/second)A= areadc/dx = concentration gradient
x
Co
Ci
big
small
dc/dx ~ k (Co-Ci)/ x
So J = -DA k (Co-Ci)/ x
or J = -Dk/x A (Co-Ci)
= -P A (Co-Ci)
Permeability constant(can be measured)
k Is partition coefficient
For membrane permeable to Na+, K+, and Cl-:
INa+ = FzJNa+
IK+ = FzJK+
Icl-= FzJCl-
Itotal = INa+ + IK+ + Icl-
J = mol/cm2s F = 9.65 coul/molI = current density (coul/cm2 x sec-1)
When Itotal = 0
Vo = RT F
PNaNao + PKKo + PClCli
PNaNai + PKKi + PClClo
Vo = zero current potentialGoldman-Hodgkin-Katz equation
J = -zFV P RT
C(1)ezFV/RT - C(2)
ezFV/RT - 1
Rectification when C(1) < or > C(2)
J=0When C(1)ezFV/RT = C(2) or V=RTlnC(2)/C(1) zF
V∞, JzP C(1)FV RT
V-∞, J-z P C(2)FV RT
Limiting cases:
Fluxes depend on ion concentrations
What is Rectification?
Constant field: concentration asymmetry
Permeation mechanism: asymmetric barrier to ion entry or block
Gating
-100 -50
0.5
1000 mV
1.0G / Gmax
50
p
-100 -50 50 100
-15
-10
-5
5
10
15nA
I = N p i
K
Na
Resting Potential using the Goldman-Hodgkin-Katz eqn
iNaiK
oNaoKm NaPKP
NaPKPV
][][
][][log60
++
=
[Na]o = 145 mM [Na]i = ~12 mM
[K]o = 4 [K]i = 140 mM
K+
Na+
•In real cells there are many more open K+ channels than Na+ channels at rest
• Vm is somewhat more positive than EK
EK = -92.6 mv
ENa= +64.9 mv
Vm = -82 mv
• The Goldman-Hodgkin-Katz equation (constant field equation)
Where PK and PNa are the membrane permeability to K and Na, respectively
-
-
-
-
-
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-
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- - - -
The GHK Equation - continued
K
Na
P
P=α
• an equivalent formulation of the GHK equation is the following:
ii
oom NaK
NaKV
][][
][][log60
αα
++
= where
• The GHK equation is often expanded to include terms for Cl-
oCliNaiK
iCloNaoKm ClPNaPKP
ClPNaPKPV
][][][
][][][log60
++++
=
Note that internal [Cl] is in the numerator, external in the denominator
K+-Dependence of Resting Potential
• membrane potentials measured using microelectrodes
• depolarization – Vm becomes more positive (less negative) than resting potential • hyperpolarization – Vm becomes more negative than resting potential
• increasing the external [K+] depolarizes the membrane
⎟⎟⎠
⎞⎜⎜⎝
⎛
++
⋅= ++
++
ii
OOm NaK
NaK
F
RTV
][][
][][ln
α
α
Dependence of the resting membrane potential on [K+]o and on the PNa/PK ratio. The blue line shows the case with no Na+ permeability (i.e., PNa/PK = 0). Orange curves describe the Vm predicted by the GHK equation for α> 0. The deviation of these curves from linearity is greater at low [K+]o, where the Na+ contribution is relatively larger.
K+o increases K permeability
Ko = 4 mM
PNa PK
Ko = 10 mM
PNa/PK = 1 PNa/PK = 0.5
Na+ K+
Vm is halfway between Vna and VK
Vm closer to VK
PNa
PK
External K+ can modify K conductance of resting membrane
K+
K+
K+
K+
K+K+
K+ K+
K+
K+
K+
PNa
PK
Na+ K+
Hyperkalemia in a neuron with a large resting K conductance
PNa
PK
K+
EK
ENa
EK*
hyperkalemia
Mg2+
Ko = 4 mM
K+
K+
K+K+
Mg2+
Ko = 10 mM
K+
K+
K+ K+
K+
K+
Removal of Mg2+ block accounts for effects of Ko on PK
Inward K fluxclears Mg fromchannel
K+
K+K+
K+
K+
K+
K+K+
A case of too much K+
A 35 year old male with history of bipolar disorder, taking no medications,presented to the emergency department complaining of nausea, vomiting, lethargy, and abdominal pain 5 hours after ingesting an unknownnumber of digoxin tablets He was found partly conscious by a friend whocalled for emergency medical help. Paramedics found him to be agitatedwith a pulse of 30. Upon arrival to the ED, vital signs were blood pressure 162/87,pulse of 30 beats per minute, respiratory rate of 22 per minute and temperature of 97 oF. An ECG showed second degree AV block. The patient was intubated and digoxin antibody administered. The next day his digoxin level was reducedfrom 2.49 ng/ml to 0.69 ng/ml and he was transferred out of the ICU.
How does digoxin work?Can the GHK eqn explain the electrical effects of digoxin?