Fine, Ch. 2 Flashcards

1
Q

resting membrane potential

A

x

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2
Q

receptor potential

A

x

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3
Q

pacinian corpuscles

A

x

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4
Q

synaptic potentials

A

x

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5
Q

hyperpolarization

A

x

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6
Q

passive electrical responses

A

x

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7
Q

depolarization

A

x

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8
Q

Threshold potential

A

x

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9
Q

action potential

A

x

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10
Q

active transporters

A

x

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11
Q

ion channels

A

x

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12
Q

electrochemical equilibrium

A

x

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13
Q

Best way to observe electrical signals in neurons is by

A

using an intracellular electrode

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14
Q

resting membrane potential is the

A

negative signal reads upon entering neuron

RMP typically -40 to -90 mV

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15
Q

typical resting membrane potential

A

-40 to -90 mV

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16
Q

change in resting membrane potential is a

A

receptor potential

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17
Q

receptor potentials are due to

A

activation of sensory neurons by external stimuli

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18
Q

XY are for communication between neurons at synaptic contacts

A

synaptic potentials

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19
Q

potentials that travel along the nerve axon

A

action potentials

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20
Q

action potentials are used for

A

LONG RANGE transmission of information

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21
Q

If the potential goes more negative it has

A

hyperpolarized

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22
Q

hyperpolarizations are xxx responses

A

passive electrical responses

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23
Q

membrane potential becomes more positive

A

depolarization

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24
Q

xxx must be met for Action Potential to occur

A

threshold potential

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25
intensity of a stimulus is encoded by
frequency of APs
26
receptor potentials amplitude are graded by
magnitude of the stimulus
27
action potentials amplitude are graded by
they are not graded; the amplitude is of the same level independent of strength of stimulus, provided the threshold is met.
28
Synaptic potentials amplitude is graded by
number of synapses activated & previous synaptic activity
29
fundamental problem with neurons
axons are not good conductors
30
if current pulse is below threshold it will
decay as it moves away from the site of current injection as it leaks from axonal membrane
31
serve as a booster system to send info over long distances
action potentials at nodes of ranvier
32
xxx circumvent the leakiness of neurons
action potentials
33
neuronal signals rely upon
movement of ions across the membrane
34
cell membranes transmit electrical signals because they (2)
a. are selectively permeable B. differences in ion concentration across the membrane
35
ion concentration gradients are established by
active transporters (proteins)
36
selective permeability of membranes is due to
ion channels
37
ion channels and transporters work...
against each other to generate the various potentials
38
an electrical potential will be generated when K+
K+ is not the same on the two sides
39
difference in electrical potential across the membrane results from
potassium ions flow down their concentration gradient
40
resting membrane potential is maintained by
continual resting efflux of K+
41
electrochemical equilibrium is
an exact balance between a) concentration gradient of K+ from in > out, b) an opposing electrical gradient that prevents K+ moving across membrane
42
K+ stops flowing at
electrochemical equilibrium
43
tiny fluxes in ions do not disrupt chemical electroneutrality because
each ion has a counter-ion of opposite charge
44
in opposite compartments, Cl:Na is
equal
45
passive membrane decrement of current flow with distance formula
Vx = Vo e^-x / /\
46
Vx
voltage response at position x
47
Vo
voltage change at point where current is injected
48
e
base of natural logarithms
49
/\
length constant of the axon
50
length constant of the axon (/\)
where initial voltage Vo decays to 1/e (37%) of its value
51
/\ length constant formula
(sqrt) (rm / ro + ri)
52
rm
relative resistance of plasma membrane
53
ri
relative resistance of intracellular axoplasm
54
ro
relative resistance of extracellular axoplasm
55
for optimal passive flow, rm should be x and ri and ro should be x
high; low; low
56
delays in change in membrane potential upon injection is due to
plasma membrane behaving as a capacitor, storing initial charge.
57
change in membrane potential at any time formula =
t = V(infinity)(1-e^-t/T)
58
V(infinity)
steady state value of membrane potential change
59
small t =
time after current pulse begins
60
big T
membrane time constant = time when Vt rises to 1-(1/e) or 63% of V(inf).
61
membrane time constant
time when Vt rises to 1-(1/e) or 63% of V(inf).
62
formula to calculate Potential decline after current pulse ends
Vt = V(inf) e^-t/T
63
Equilibrium potential -
potential generated across the membrane at electrochemical equilibrium
64
nernst equation predicts what
equilibrium potential
65
nernst equation formula
Ex = (RT/zF) In(Xout)/(Xin)
66
simplified nernst at room temp
Ex = 58/z log (Xout)/(Xin)
67
ex
equilibrium potential
68
R
GAS CONSTANT
69
T
absolute temp
70
Z
valence (charge) permeant ion
71
F
faraday constant (amount of electrical charge contained in one mole of univalent ion)
72
faraday constant
amount of electrical charge contained in one mole of univalent ion)
73
what does the nernst equation predict exactly
linear slope of 58 mV per tenfold change in the K+ gradient
74
K+ conc. higher inside =
negative inside