Membrane Potentials and Action Potentials Flashcards

(35 cards)

1
Q

Voltage

A

Potential difference
Units: Volts
Generated by ions to produce a charge gradient

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2
Q

Current

A

Unit: Amps

Movement of ions due to a potential difference

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3
Q

Resistance

A

Units: Ohms

Barrier that prevents the movement of ions

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4
Q

How to measure membrane potential

A

A reference rod is placed outside the cell.
This is the zero-volt level

Another electrode is placed inside the cell . It measures a voltage difference that is negative compared with the outside

All cells have a membrane potential

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5
Q

How cell membrane maintains potential

A

Lipid (hydrophobic) cell membrane is a barrier to ion movement and separates ionic environment.

Cell membrane can selectively change its permeability to specific ions

Permeable pores in the membrane (ion channels) open and close depending on transmembrane voltage, presence of activating ligands or mechanical force

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6
Q

Ion channels

A

Ion channels can be selective for different types of ions

Movement across the membrane will occur when the concentration of the ion is different on one side of the membrane and ceases upon equilibration

Due to diffusion through a selectively permeable membrane

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7
Q

Nerst Equation

A

E = [(RT)/(zF)] * ln { [X2]/[X1] }

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8
Q

Concentration of ions

A

Na+ :
Extracellular 150 nM
Intracellular 10 nM

K+ :
Extracellular 5 nM
Intracellular 150 nM

Ca2+ :
Extracellular 2 nM
Intracellular 10^(-4) nM

Cl- :
Extracellular 110 nM
Intracellular 5 nM

Organic phosphates :
Extracellular 3 nM
Intracellular 130 nM

pH :
Extracellular 7.4
Intracellular 7.1

Osmolarity:
Extracellular = Intracellular = 285 mosmol/L

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9
Q

Why do membrane potentials not rest at E(K) or E(Na)?

A

E(K) = -90mV
E(Na) = +72mV
Typical E(Membrane) = -70mV

Because there are always some channels open at all times

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10
Q

Calculation for real membrane potential

A

K+, Na+ and Cl- concentrations all contribute to the real membrane potential

Size of each ion’s contribution is proportional to the real membrane potential

E = -61 log {P(K)[K in] +…} / {P(K)[K out] +…}

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11
Q

Depolarisation

A

Membrane potential moves towards 0mV

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12
Q

Repolarisation

A

Membrane potential decreases towards resting potential

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13
Q

Overshoot

A

When membrane potential becomes more positive

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14
Q

Hyperpolarisation

A

When membrane potential decreases beyond resting potential

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15
Q

Action potential

A

Occur in excitable cells (mainly neurons and muscle cells but also in some endocrine tissues)
In neurons they are also known as nerve impulses and allow the transmission of information reliably and quickly over long distances

Play a central role in cell-to-cell communication and can be used to activate intracellular processes

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16
Q

Ionic basis of action potentials

A

Permeability depends on conformational state of ion channels:

  • -Opened by membrane depolarisation
  • -Inactivated by sustained depolarisation
  • -Closed by membrane hyperpolarisation/repolarisation

When membrane permeability of an ion increases it crosses the membrane down its electrochemical gradient
Movement changes the membrane potential toward the equilibrium potential for that ion

Changes in membrane potential during the action potential are not due to ion pumps

17
Q

5 phases of the Action Potential

A

Phase 1. Resting membrane potential

Phase 2. Depolarising stimulus

Phase 3. Upstroke

Phase 4. Repolarisation

Phase 5. After-hyperpolarisation

18
Q

Phase 1. Resting membrane potential

A

Permeability for P(K) > P(Na)

Membrane potential nearer equilibrium potential for K+ (-90mV) than that for Na+ (+72mV)

19
Q

Phase 2. Depolarising stimulus

A

The stimulus depolarises the membrane potential

Moves it in the positive direction towards the threshold

20
Q

Phase 3. Upstroke

A

Starts at threshold potential

Increase in Na+ permeability because voltage-gated Na+ channels open quickly
[Na+ enters the cell down electrochemical gradient]

Followed by increase in K+ permeability as the voltage-gated K+ channels start to open slowly
[K+ leaves the cell down electrochemical gradient]

Less than Na+ entering
Membrane potential moves towards the Na+ equilibrium potential

21
Q

Phase 4. Repolarisation

A

P(Na) decreases because the voltage-gated Na+ channels close - Na+ stops entry

P(K) increases as more voltage-gated K+ channels open and remain open

K+ leaves the cell down the electrochemical gradient

Membrane potential moves towards the K+ equilibrium potential

22
Q

Absolute refractory period

A

Occurs at the start of repolarisation

Activation gate is open
Inactivation gate is closed

New action potential cannot be triggered even with very strong stimulus

Absolute refractory period continues later in repolarisation

Activation and inactivation gates closed

23
Q

Phase 5. After-hyperpolarisation

A

At rest voltage-gated K+ channels are still open

K+ continues to leave the cell down gradient

Membrane potential moves closer to the K+ equilibrium - some VGKC then close

Membrane potential returns to the resting potential

ATPase restores Na+ and K+ conc.

24
Q

Relative refractory period

A

Happens after-hyperpolarisation

Inactivation gate is open

Stronger than normal stimulus required to trigger an action potential

25
Regenerative relationship between P(Na) and E(m)
Once threshold potential reached, action potential triggered APs are 'all-or-nothing' events, once triggered a full-sized AP occurs Positive feedback causes the cycle of depolarisation, opening of VGSC, increase in P(Na), influx of Na+, to continue Cycle continues until VGSC inactivate Following AP there is a absolute refractory period where membrane is unresponsive to threshold depolarisation Membrane remains in the refractory period until VGSC recover from inactivation
26
Passive propagation of AP
Only K+ channels open Internal (or axial) membrane resistance alters propagation distance and velocity
27
Active propagation of AP
Local current flow depolarizes adjacent region toward threshold This happens due to passive propagation The adjacent region is the stimulated to form a new AP This cycle continues hence propagating the signal down the axon
28
Nodes of Ranvier
Gaps between myelin sheaths on an axon
29
Saltatory conduction
Voltage-gated channels are mostly located at nodes Myelin sheaths insulate the axons preventing leakage of the AP This means that an action potential generated at one node of Ranvier elicits current that flows passively within the myelinated segment until the next node is reached. Current flow then generates an action potential in the next Node of Ranvier. The cycle is repeated along the length of the axon. Current flows across the neuronal membrane only at the nodes. This is saltatory propagation, meaning that the action potential jumps from node to node.
30
Conduction velocity
Both axon diameter and myelination influence conduction velocity Action potential travels quickly Small diameter, non-myelinated axons : 1m/s Large diameter, myelinated axons : 120m/s
31
Factors affecting conduction velocity
Reduced axon diameter (i.e. regrowth after injury) Reduced myelination (i.e. multiple sclerosis, diphtheria) Cold Anoxia Compression and drugs (some anaesthetics)
32
What are the 3 main factors that influence movement of ions across the membrane
Concentration gradient of ions Charge on ions Voltage across the membrane
33
Which ion is important for the upstroke and which is important for the falling portion of the AP? In which direction do these ions flow
The upstroke mediated largely by Na+ ions moving down their conc. gradient into the cell. The falling portion dominated by K+ ions going down conc. gradient and therefore exiting the cell
34
Why is E(K) negative (-70mV) and E(Na) positive (+40mV) when both are positive ions.
There is more K+ inside the cell than outside, tend to flow out of the cell. More Na+ outside the cell, tend to flow in Potential to -70mV is needed to attract K+ and stop the net flow outwards while a positive charge of +40mV is needed to repel Na+ from entering the cell
35
What factors influence the speed of propagation of an action potential along an axon?
Larger axons have lower resistance, so ions move faster - conduction velocity is proportional to the square root of the axon diameter. There is a linear relationship between conduction velocity and myelin thickness