CHAPTER 5 Flashcards

1
Q

Within a millisecond or so, the
potential difference between the inside and outside, called
the

A

Diffusion potential

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2
Q

becomes great enough to block further net potassium diffusion to the exterior, despite the high
potassium ion concentration gradient.

A

Diffusion potential,

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3
Q

becomes great enough to block further net potassium diffusion to the exterior, despite the high potassium ion concentration gradient. In the normal mammalian nerve fiber,
-the potential difference required is about 94 millivolts, with negativity inside the fiber membrane.

A
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4
Q

Diffusion of the positively charged sodium
ions to the inside creates a membrane potential of opposite polarity to that in, with negativity outside
and positivity inside.

A
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5
Q

The diffusion potential level across a membrane that exactly opposes the net diffusion of a particular ion through the membrane is called the

A

Nernst potential

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6
Q

The magnitude of this Nernst potential is determined by
the –
of the concentrations of that specific ion on the two sides of the membrane.

A

ratio

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6
Q

The greater this ratio, the
greater the tendency for the ion to diffuse in one direction, and therefore the greater the Nernst potential required
to prevent additional net diffusion.

A
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6
Q

Can be used to calculate
the Nernst potential for any univalent ion at normal body temperature of 98.6°F (37°C):

A

Nernst equation

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7
Q

When a membrane is permeable to several different ions, the diffusion potential that develops depends on three factors:

A

(1) the polarity of the electrical charge of each ion,
(2) the permeability of the membrane (P) to each ion, and
(3) the concentrations (C) of the respective ions on the inside (i) and
outside (o) of the membrane.

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8
Q

Formula, gives the calculated membrane potential on the inside of the membrane when two univalent positive
ions, sodium (Na+) and potassium (K+), and one univalent negative ion, chloride (Cl−), are involved.

A

Goldman equation, or the Goldman-HodgkinKatz equation,

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9
Q

Is placed in the extracellular fluid,
and the potential difference between the inside and outside of the fiber is measured using an appropriate voltmeter

A

“indifferent electrode,”

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10
Q

is a highly sophisticated electronic apparatus that is capable of measuring small voltages despite extremely high resistance to electrical flow through the tip of the micropipette, which has a lumen diameter usually less than 1 micrometer and a resistance more than a million ohms.

A

voltmeter

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11
Q

Then, as the recording electrode passes through the voltage change area at the
cell membrane (called the

A

Electrical dipole layer

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12
Q

Note that this is an electrogenic pump because more positive charges are pumped to the outside than to the inside(three Na+ ions to the outside for each two K+ ions to the inside), leaving a net deficit of positive ions on the inside; this causes a negative potential inside the cell membrane.

A
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12
Q

in the nerve membrane through which potassium can leak even in a resting cell.

A

“tandem pore domain,”
potassium channel, or
potassium (K+) “leak” channel,

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13
Q

Nerve signals are transmitted by

A

Action potentials

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14
Q

Which are rapid changes in the membrane potential that spread rapidly along the nerve fiber membrane.

A

action potentials

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15
Q

This is the resting membrane potential before the action potential begins. The membrane is said to be “polarized” during this stage because of the −90
millivolts negative membrane potential that is present.

A

Resting Stage

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16
Q

At this time, the membrane suddenly becomes permeable to sodium ions, allowing tremendous numbers of positively charged sodium ions to diffuse to the interior of the axon.

A

Depolarization Stage

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17
Q

immediately neutralized
by the inflowing positively charged sodium ions, with the potential rising rapidly in the positive direction

A

depolarization

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18
Q

after the membrane becomes highly permeable to sodium ions, the sodium channels begin to close and the
potassium channels open more than normal

A

Repolarization Stage.

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19
Q

Then, rapid diffusion of potassium ions to the exterior re-establishes the normal negative resting membrane potential

A

repolarization

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20
Q

The necessary actor in causing both depolarization and
repolarization of the nerve membrane during the action
potential is the

A

voltage-gated sodium channel

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21
Q

also plays an important role in
increasing the rapidity of repolarization of the membrane

A

voltage-gated potassium channel

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22
Q

This channel
has two gates—one near the outside of the channel called

A

activation gate

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23
Q

during this state, sodium ions can pour inward through
the channel, increasing the sodium permeability of the
membrane as much as 500- to 5000-fold

A

activated state

23
Q

and another near the inside called the

A

inactivation gate

24
Q

which is used to measure flow of ions through the
different channels.

A

voltage clamp

24
Q

-For instance, the sodium channels can be blocked by a toxin called
-by applying it to the outside
of the cell membrane where the sodium activation gates
are located.

A

tetrodotoxin

25
Q

Therefore, a sudden increase
in the membrane potential in a large nerve fiber from −90 millivolts up to about −65 millivolts usually causes the explosive development of an action potential. This level of −65 millivolts is said to be the

A

threshold for stimulation

25
Q

In fact, the calcium ion
concentration needs to fall only 50 percent below normal before spontaneous discharge occurs in some peripheral
nerves, often causing muscle

A

muscle “tetany

25
Q

tetraethylammonium ion

A

Blocks the potassium channels when it is applied to the interior of the nerve fiber.

26
Q

This transmission of the depolarization process along a nerve or muscle fiber is

A

nerve or muscle impulse

27
Q

Once an action potential has been elicited at any point on the membrane of a normal fiber, the depolarization process travels over the entire membrane if conditions are right, or it does not travel at all if conditions are not right. This is called the

A

all-or-nothing principle

28
Q

when the spread of depolarization stops?

A

action potential reaches a
point on the membrane at which it does not generate sufficient voltage to stimulate the next area of the membrane.

28
Q

Therefore, for continued propagation of an impulse to occur, the ratio of action potential to threshold for excitation must at all times be greater than 1. This “greater than 1” requirement is called the

A

“safety factor” for propagation

28
Q

This type of action potential occurs in

A

heart muscle fibers

29
Q

The cause of the plateau is a combination of several factors. First, in heart muscle, two types of channels enter into the depolarization process:

A

(1) the usual
voltage-activated sodium channels, called fast channels, and
(2) voltage-activated calcium-sodium channels, which are slow to open and therefore are called
slow channels.

30
Q

These rhythmical discharges cause:

A

These rhythmical
discharges cause

31
Q

This is not enough negative voltage to keep the sodium and calcium channels totally closed. Therefore, the following sequence occurs:

A

(1) some sodium and
calcium ions flow inward;
(2) this increases the membrane
voltage in the positive direction, which further increases
membrane permeability;
(3) still more ions flow inward
(4) the permeability increases more, and so on, until an action potential is generated.

32
Q

This continues for nearly a second after the preceding action potential is over, thus drawing the membrane potential nearer to the potassium Nernst potential. This is a state called

A

Hyperpolarization

33
Q

But the increased potassium conductance (and the state of hyperpolarization) gradually disappears, as shown after
each action potential is completed in the figure, thereby allowing the membrane potential again to increase up to the

A

threshold

34
Q

The large fibers are

A

myelinated

35
Q

and the small ones are

A

unmyelinated

36
Q

A typical myelinated fiber. The central
core of the fiber is the

A

axon

36
Q

The axon is filled in its center with a
-which is a viscid intracellular fluid.

A

axoplasm

36
Q

Surrounding the axon is a

A

myelin sheath

36
Q

About once every 1 to 3 millimeters along the length of the myelin sheath is a

A

node of Ranvier

37
Q

The myelin sheath is deposited around the axon by

A

Schwann cells

38
Q

Then the Schwann cell rotates around the axon many times, laying down multiple layers of Schwann cell membrane containing the lipid subtance

A

sphingomyelin

39
Q

Yet the action potentials
are conducted from node to node, as
this is called

A

saltatory conduction

40
Q

Thus, the nerve impulse jumps along the fiber, which is the origin of the term

A

“saltatory.”

40
Q

mechanical pressure to excite

A

nerve endings in the skin

41
Q

chemical neurotransmitters to

A

transmit signals from one neuron to the next in the brain

41
Q

Electrical current to transmit signals between

A

successive muscle cells in the heart and intestine.

41
Q

These local potential changes are called

A

Acute local potentials

42
Q

and when they fail to elicit an action potential, they are called

A

acute subthreshold potentials

42
Q

Now the local potential has barely reached the level required to elicit an action potential, called the

A

threshold level

43
Q

The period during which a second action potential cannot be elicited, even with a strong stimulus, is called the

A

Absolute refractory period

44
Q

In contrast to the factors that increase nerve excitability, still others, called

A

membrane-stabilizing factors, can
decrease excitability

44
Q

decreases membrane permeability to sodium ions and simultaneously reduces excitability

A

high extracellular fluid calcium ion concentration

45
Q

Among the most important stabilizers are the many substances used clinically as local anesthetics, including p

A

procaine and tetracaine

46
Q

The cathode ray tube itself is composed
basically of an

A

electron gun and a fluorescent screen

46
Q

When excitability has been reduced so low that the ratio of action potential
strength to excitability threshold (called the

A

“safety factor”