Boheler 2 Flashcards

1
Q

Where does Em(battery) of a cell originate?

A

two requirements: ion concentration gradient, ion-selective permeability of ion channels

by adding a charge difference (Q) across the lipid bilayer, a potential difference can be generated

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2
Q

Diffusion

A

a passive motion of molecules or ions from regions or higher concentration to regions of lower concentration

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3
Q

Rate of diffusion

A

depends on the concentration difference, the surface area, volume, and the permeability

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4
Q

Concentration gradient is

A

important for movement of molecules according to Fick’s Law

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5
Q

Electrical gradient

A

the electrical potential that acts on an ion to drive the movement of the ion in one or another direction

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6
Q

How does a cell establish concentration gradients?

A

Passive transport = the exergonic movement of substances across a membrane

Active transport = the endergonic movement of substances across a membrane that is couple to a exergonic reaction

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7
Q

The Na/K ATPase

A

maintains the electrochemical gradient in living cells

primary active transporter located on the plasma membrane

directly uses chemical energy in the form of ATP hydrolysis to move 3 ions of Na+ to the outside of a cell and 2 ions of K+ to the inside of the cell

it’s electrogenic because the charge movements and concentrations are not equal, and it establishes both a diffusion gradient and an electrical gradient across the membrane

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8
Q

ion channels

A

proteinaceous ‘holes’ in the membrane that ‘selectively’ allow ions to pass

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9
Q

Na and Ca channels

A

Four homologous domans (I-IV)

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10
Q

K channels

A

Most Vm-dependent K channels have the same overall structure except that each of the four domains is a separate protein, which assembles into a tetramer that is analogous to the Na and Ca channel

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11
Q

Permeation

A

the act of spreading through something, the movement of molecules through a membrane or interface

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12
Q

Conductivity

A

how well do ions pass through, it relates to the amount of current through a channel, given a specific transmembrane voltage and specific concentration of ions. Ion channels can pass ~10^6 ions/sec

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13
Q

Selectivity

A

how picky channels are for certain kinds of ions, is usually measured in a relative sense with PNa/PK for Na channels being 50-100:1

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14
Q

Gating

A

how the channels opens/closes

voltage-gated channels open in response to voltage with transitions at the single channel level that are very rapid («1 ms)

there are also ligand-gated channels that respond to ligands (not important to electrical signals)

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15
Q

Nernst Potential

A

the transmembrane voltage where there is no net current, the potential at which the electrical force acting on ion species X is equilibrated with the diffusional force

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16
Q

A master equation

A

Cm*dVm/dt = Icap = I1 + I2 +I3 + …

17
Q

G

A

stands for conductance and is always positive

18
Q

Goldman Hodgkin Katz equation

A

helps us calculate the Diffusion Potential when the membrane is permeable to multiple ions

19
Q

The resting potential

A

the weighted sum of the Nernst potentials for Na, K, and Cl channels, the weights are the values of the conductances Gx at rest

20
Q

In most cells

A

the dominant conductance at rest is GK

Vm, rest = GKVK/GK = Vk

21
Q

Voltage clamp

A

potentiostatic circuit where a feedback amplifier compares a command voltage to the actual voltage against ground and delivers current to cancel any deviation

22
Q

HH gating gates

A

independent, channel is open when all gates are open, probability that all n gates being open is the product of the probabilities that each individual gate is open, the gates are identical – thus the probability for each gate being open is the same

23
Q

For each given voltage, the change of n(t) represents

A

the opening of the gate (activation), with a time constant tau_n

24
Q

Total channel conductance is

A

GK = gKn^4

25
Q

The K current through the channel is

A

IK = gK(Vm-VK)

26
Q

gK is a function of

A

Vm, t

27
Q

The rates of opening and closing (alphas and betas)

A

determine the time constant of n gate opening and the n steady-state value. They are functions of voltage

28
Q

Na channel gating - like K channels but with a twist

A

superposition of activation and inactivation, Na channels activate much faster (open), Na channels inactivation (close) occurs with voltage and time, not a simple two-state model

29
Q

gNa

A

= gNam^3h

30
Q

m gates

A

similar to K channel activation gate (n gates)

31
Q

h fate

A

the inactivation gate – has a different votlage-dependence than m gate

32
Q

both m and h gates

A

have to be open to allow ion flux through the channel