ME01 - Membrane Electrophysiology Flashcards

1
Q

Characteristics of Ion Channels

A

Ion Channel Selectivity
Ion Channel Gating
Conductance of Ion Channel

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2
Q

Ion channels permit the passage of some ions, but not other

A

Ion Channel Selectivity

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3
Q

Ion Channel Selectivity is based on:

A

Channel size
Distribution of charges that line it
Size and charge of ions
How much water the ion attracts and holds around it

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4
Q

Ion channels are either GATED or NON-GATED

A

Ion Channel Gating

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5
Q

What are Gated ion channels and it’s types

A

Gated ion channels have gates that can open or close the channel
Voltage-gated - gates are controlled by voltage (difference in membrane potential)
Ligand-gated - open or closed by hormones, second messengers or neurotransmitters

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6
Q

Ion channels that are always open

Also called as leakage channels

A

Non-Gated Ion Channels

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7
Q

Conductance of Ion Channels depend on ______

A

If the channel is OPEN

The higher the probability that a channel is open, the higher the conductance or permeability

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8
Q

Location of ION CHANNELS

A

Non-Gated: Cell membrane on dendrites, Cell Body and Axon
Ligand-Gated: dendrites, cell body
Voltage-Gated: Axon hillock, unmyelinated axons, along the nodes of Ranvier in myelinated axons

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9
Q

Functions of ION CHANNELS

A

Non-Gated : RMP
Ligand-Gated: Synaptic potentials (incoming signals to neurons)
Voltage-Gated: Generation and Propagation of action potential (outgoing signals from neurons)

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10
Q

Types of Membrane Potentials

A

Diffusion Potential

Equilibrium Potential

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11
Q

Potential difference generated across a membrane because of a concentration difference of an ion

A

DIFFUSION POTENTIAL

Can be generated only if the membrane is permeable to the ion

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12
Q

Factors related to the Diffusion Potential
Size
Sign

A

Size depends on the size of the concentration gradient

Sign depends on whether the diffusing ion is positively or negatively charged

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13
Q

Diffusion Potential do not result in changes in concentration of the diffusing ions

A

TRUE.

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14
Q

Diffusion potential that exactly balances (opposes) the tendency for diffusion caused by a concentration difference

A

Equilibrium Potential

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15
Q

Chemical and Electrical Driving forces that act on an ion are equal and opposite
No net diffusion of the ion occurs

A

Electrochemical Equilibrium

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16
Q

In the presence of a nondiffusable ion, diffusable ions distribute themselves so that at equilibrium their concentration ratios are equal
For any pair of cation/anion

A

Gibbs-Donnan Equilibrium

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17
Q

Formula for Gibbs-Donnan Equilibrium

A

[K+]in x [Cl-]in = [K+]out x [Cl-]out

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18
Q

Implications and Consequence of Gibbs-Donnan Equilibrium

A

(1) Presence of charged proteins in cells, there are more osmotically active particles in cells than in IF
C: Animal cells have flexible walls; Osmosis make cells swell and rupture; Prevented by Na/K ATPase

(2) At equilibrium, distribution of ions across membrane is assymetric
C: Electrical potential difference exists across membrane (MP)
Magnitude can be determined by Nernst equation

(3) There are more proteins in the plasma than in the IF
C: Gibbs-Donnan equilibrium will affect ion movement across capillary walls

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19
Q

Calculates the equilibrium potential at a given concentration difference of a permeable ion across cell membrane

A

Nernst equation

EMF = 61+log concentration inside/conc. outside

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20
Q

Signs to remember in Nernst equation

A

sign of potential is (+) if diffusing ion is a negative ion

sign of potential is (-) if diffusing ion is a positive ion

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21
Q

Calculates the membrane potential in the inside of a membrane when a membrane is permeable to several different ions

A

Goldman-Hodgkin-Katz Equation

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22
Q

Measured potential difference across the cell membrane in millivolts (mV)

A

RMP

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23
Q

Intracellular potential relative to the extracellular potential

A

RMP

RMP of -70 means 70mV cell negative

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24
Q

Characteristics of EMP

A

Established by diffusion potentials that result from concentration differences of permeable ions
Each permeable ion attempts to drive the membrane potential toward its equilibrium potential

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25
ORIGIN OF RMP
Contribution of K+ Diffusion Potential Contribution of Na+ Diffusion Contribution of Na/K ATPase
26
If potassium ions were the only factor causing the resting potential, the resting potential INSIDE THE FIBER would be equal to ________
-94 millivolts
27
Potassium vs Sodium in Diffusion and Permeability
Diffusion of K contributes far more to membrane potential than diffusion of Na Permeability to K is about 100 times as great as its permeability to Na
28
Contribution of Na/K ATPase to the Original RMP
Direct electrogenic contribution of the pump (3Na2K) is small This creates an additional degree of -4mV
29
Short range change in voltage Incoming Na ions diffuse for short distances inside the plasma membrane Produce a current that travels from the point of stimulation toward the cell's trigger zone
LOCAL POTENTIALS
30
Any change in which membrane voltage shifts to a less negative value
Depolarization
31
Two possible effects of Depolarization
Local potential - generation of a nonpropagated response | Action potential - generation of a propagated response
32
Characteristics of LOCAL POTENTIAL
Graded. (Stronger the stimulus, stronger the response) Decremental. (Gets weaker as they spread from point of stimulation) Reversible. (If stimulation ceases, K diffusion out of cell to return membrane voltage to its resting potential) Either Excitatory or Inhibitory. Excitatory - produce an action potential Inhibitory - less likely to produce an action potential
33
Types of Local Potential
Synaptic Local Potentials Generator/Receptor Potentials Electrotonic Potentials
34
Alteration in the Membrane Potential of cell resulting from activation at the synapse
Synaptic Potential
35
Types of Synaptic Potential
Excitatory Post-Synaptic Potential - Intracellular voltage increases Inhibitory Post-Synaptic Potential - Intracellular voltage decreases
36
Transmembrane potential difference produced in sensory receptor Occurs as depolarization resulting from inward current flow
Generator/Receptor Potential
37
Influx of current will often bring the membrane potential of the sensory receptor towards the threshold for triggering an action potential
Generator/Receptor Potential
38
Passive spread of charge inside a neuron due to local changes in ionic conductance Ionic charge enters in one location and dissipates to others, losing intensity as it spreads (graded response)
Electrotonic Potential
39
Rapid changes in the membrane potential that spread along the nerve fiber
Action Potential
40
How do you conduct a nerve signal
The action potential moves along the nerve fiber until it comes to the fiber's end
41
Characteristics of Action Potential
Follow All-or-None Law. If stimulus depolarizes neuron to threshold, neuron fires at its maximum voltage. Above threshold, stronger stimuli do not produce stronger action potential. Nondecremental. AP do not get weaker with distance Irreversible. AP goes to completion. AP cannot be stopped once it begins.
42
``` Fill the table. Parameter LOCAL POTENTIAL ACTION POTENTIAL Mediator Voltage Change Intensity Reversibility Distance of Effect Progression ```
Parameter LOCAL POTENTIAL ACTION POTENTIAL Mediator Ligand-gated ion channels Voltage-gated ion channel Voltage Change Depolarizing/Hyperpolarizing Depolarizing Intensity GRADED ALL-OR-NONE Reversibility Reversible Irreversible Distance of Effect Short (Local) Long (distant) Progression Decremental Non-decremental
43
Steps in the Generation of Action Potential
Resting Stage - RMP, before AP begins, -90mV Depolarization - Threshold potential is reached (-65mV) Voltage-gated Na overwhelm K+, permeable to Na ions Overshoot - great excess of positive Na ions causes MP to overshoot beyond the zero level
44
Ionic Basis of Depolarization | Necessary factor in both depolarization and repolarization of the nerve membrane
Voltage-Gated Sodium Channel
45
Feedback Control of Depolarization
Positive Feedback
46
Sodium channels begin to close and the K channels open more than normal Rapid diffusion of K ions to the exterior reestablishes resting membrane potential
Repolarization
47
Ionic Basis of Repolarization | Also plays an important role in increasing the rapidity of repolarization of the membrane
Voltage-Gated Potassium Channel
48
Feedback Control of Hyperpolarization
Negative Feedback
49
Afterhypolarization K+ conductance remains higher than at rest after closure of the Na+ channels Membrane potential is driven very close to the K+ equilibrium potential
Undershoot
50
Effects of Ion Fluxes on Action Potential Structure Contribution K+ leak channel Na+/K+ ATPase pump Voltage-gated Na+channels Voltage-gated K+ channels
Structure Contribution K+ leak channel Resting Membrane Potential Na+/K+ ATPase pump Maintenance of the Concentration gradient Voltage-gated Na+channels Depolarization and Hyperpolarization Voltage-gated K+ channels Hyperpolarization
51
Effect on | DECREASE extracellular Na+ concentration
Reduce the size of AP | No effect on RMP
52
Effect on: | INCREASE extracellular K+ concentration
Decrease RMP
53
Effect on: | DECREASE extracellular Ca2+ concentration
INCREASE excitability | DECREASE threshold
54
Effect on: | INCREASE extracellular Ca2+ concentration
DECREASE excitability | INCREASE threshold
55
Effect on: INCREASE intracellular Cl- concentration INCREASE intracellular Protein concentration
DECREASE RMP
56
How are AP propagated?
By the spread of local currents to ADJACENT areas of membrane, which are then depolarized to threshold and generate action potentials
57
Direction of AP Propagation
No single direction of propagation | An AP travels in both directions away from the stimulus until the entire membrane has become depolarized
58
Depolarization process travels over the entire membrane if conditions are right, or it does not travel at all if conditions are not right
All-Or-Nothing Principle
59
Factors Affecting Conduction Velocity
Fiber Size - Increase diameter, faster | Myelination - myelin acts insulator; saltatory conduction (5-50 fold)
60
Action potentials can be generated only at gaps in the myelin sheath called as
Nodes of Ranvier
61
Importance of Saltatory conduction
It conserves energy for the axon | Only the nodes depolarize, allowing 100 times less loss of ions than would otherwise be necessary
62
Time periods after an action potential during which new stimulus cannot be readily elicited
Refractory Period
63
Another AP cannot elicited, no matter how large the stimulus is Coincides with almost the entire duration of the action potential
Absolute Refractory Period
64
Ionic basis of Absolute Refractory Period
Inactivated gates of Na+ channel are closed when membrane potential is depolarized and remain closed until repolarization occurs No AP can occur until the inactivations gates open
65
Begins at the end of the Absolute refractory period and continues until the membrane potential returns to the resting level AP ca be elicited only if a larger than usual inward current is provided
Relative Refractory period
66
Ionic Basis of Relative Refractory Period
K+ conductance is higher than the rest MP is closer to the K+ equilibrium potential and farther from the threshold More inward current is required to bring the membrane to threshold
67
Integral proteins that span the cell membrane | When open, permit the passage of certain ions
Ion Channels