What is the contribution of Ca2 to the membrane potential?

12.5 The Activeness Potential

Learning Objectives

By the terminate of this section, you will be able to:

Draw how move of ions across the neuron membrane leads to an activity potential

  • Describe the components of the membrane that found the resting membrane potential
  • Describe the changes that occur to the membrane that result in the action potential

The functions of the nervous system—sensation, integration, and response—depend on the functions of the neurons underlying these pathways. To understand how neurons are able to communicate, information technology is necessary to describe the office of an excitable membrane in generating these signals. The basis of this procedure is the action potential.An action potential is a predictable modify in membrane potential that occurs due to the open up and endmost of voltage gated ion channels on the cell membrane.

Electrically Active Cell Membranes

Nearly cells in the body make employ of charged particles (ions) to create electrochemical charge across the cell membrane. In a prior chapter, nosotros described how musculus cells contract based on the motility of ions across the jail cell membrane. For skeletal muscles to contract, due to excitation–contraction coupling, they require input from a neuron. Both musculus and nerve cells make use of a cell membrane that is specialized for betoken conduction to regulate ion motility betwixt the extracellular fluid and cytosol.

As you learned in the affiliate on cells, the cell membrane is primarily responsible for regulating what can cross the membrane. The cell membrane is a phospholipid bilayer, then only substances that can pass straight through the hydrophobic core tin can diffuse through unaided. Charged particles, which are hydrophilic, cannot laissez passer through the cell membrane without aid (Figure 12.5.1). Specific transmembrane channel proteins allow charged ions to motility across the membrane. Several passive ship channels, too equally active ship pumps, are necessary to generate a transmembrane potential, and an action potential. Of special interest is the carrier protein referred to as the sodium/potassium pump that uses energy to motion sodium ions (Na+) out of a cell and potassium ions (Chiliad+) into a jail cell, thus regulating ion concentration on both sides of the cell membrane.

This diagram shows a cross section of a cell membrane. The cell membrane proteins are large, blocky, objects. Peripheral proteins are not embedded in the phospholipid bilayer. The peripheral protein shown here is attached to the outside surface of another protein on the extracellular fluid side. Integral proteins are embedded between the phospholipids of the cell membrane. The transmembrane integral protein extends through both phospholipids layers. The opposite ends of this protein project into the cytosol and the extracellular fluid. A second, smaller integral protein only extends into the inner phospholipid layer. Its opposite end projects into the cytosol. This second protein is, therefore, not a transmembrane protein. The channel protein is cylinder shaped with a hollow internal tube labeled the pore. The sides of the channel protein can bulge inward to close the pore.
Figure 12.5.1 – Cell Membrane and Transmembrane Proteins: The cell membrane is equanimous of a phospholipid bilayer and has many transmembrane proteins, including different types of channel proteins that serve as ion channels.

The sodium/potassium pump requires energy in the form of adenosine triphosphate (ATP), so it is likewise referred to as an ATPase pump. As was explained in the cell chapter, the concentration of Na+ is higher exterior the prison cell than inside, and the concentration of K+ is higher inside the cell than outside. Therefore, this pump is working confronting the concentration gradients for sodium and potassium ions, which is why it requires energy. The Na+/Chiliad+ ATPase pump maintains these of import ion concentration gradients.

Ion channels are pores that allow specific charged particles to cross the membrane in response to an existing electrochemical slope. Proteins are capable of spanning the prison cell membrane, including its hydrophobic cadre, and can interact with charged ions because of the varied properties of amino acids found within specific regions of the protein channel. Hydrophobic amino acids are found in the regions that are adjacent to the hydrocarbon tails of the phospholipids, where as hydrophilic amino acids are exposed to the fluid environments of the extracellular fluid and cytosol. Additionally, ions will interact with the hydrophilic amino acids, which will be selective for the accuse of the ion. Channels for cations (positive ions) will take negatively charged side chains in the pore. Channels for anions (negative ions) will have positively charged side chains in the pore. The diameter of the channel's pore also impacts the specific ions that can pass through.  Some ion channels are selective for charge but not necessarily for size. These nonspecific channels let cations—peculiarly Na+, K+, and Caii+—to cross the membrane, simply exclude anions.

Some ion channels do not allow ions to freely diffuse across the membrane, only are gated instead. A ligand-gated channel opens because a molecule, or ligand, binds to the extracellular region of the channel (Effigy 12.5.2).

These two diagrams each show a channel protein embedded in the cell membrane. In the left diagram, there is a large number of sodium ions (NA plus) and calcium ions (CA two plus) in the extracellular fluid. Within the cytosol, there is a large number of potassium ions (K plus) but only a few sodium ions. In this diagram, the channel is closed. Two ACH molecules are floating in the extracellular fluid. Their label indicates that a neurotransmitter, a ligand, is required to open the ion channel. The neurotransmitter receptor site on the extracellular fluid side of the channel protein matches the shape of the ACH molecules. In the right diagram, the two ACH molecules attach to the neurotransmitter receptor sites on the channel protein. This opens the channel and the sodium and calcium ions diffuse through the channel and into the cytosol, down their concentration gradient. The potassium ions also diffuse through the channel in the opposite direction down their concentration gradient (out of the cell and into the extracellular fluid).
Figure 12.5.2 – Ligand-Gated Channels: When the ligand, in this instance the neurotransmitter acetylcholine, binds to a specific location on the extracellular surface of the aqueduct protein, the pore opens to permit select ions through. The ions, in this case, are cations of sodium, calcium, and potassium.

A mechanically-gated aqueduct opens considering of a physical distortion of the prison cell membrane. Many channels associated with the sense of touch are mechanically-gated. For instance, equally pressure level is applied to the peel, mechanically-gated channels on the subcutaneous receptors open up and allow ions to enter (Figure 12.5.3).

These two diagrams each show a channel protein embedded in the cell membrane. In the left diagram, there are a large number of sodium ions in the extracellular fluid, but only a few sodium ions in the cytosol. There is a large number of calcium ions in the cytosol but only a few calcium ions in the extracellular fluid. In this diagram, the channel is closed, as the extracellular side has a lid, somewhat resembling that on a trash can, that is closed over the channel opening. In the right diagram, the mechanically gated channel is open. This allows the sodium ions to flow from the extracellular fluid into the cell, down their concentration gradient. At the same time, the calcium ions are moving from the cytosol into the extracellular fluid, down their concentration gradient.
Effigy 12.5.3 – Mechanically-Gated Channels: When a mechanical change occurs in the surrounding tissue (such as pressure or stretch) the channel is physically opened, and ions can motility through the channel, down their concentration gradient.

A voltage-gated aqueduct is a aqueduct that responds to changes in the electrical properties of the membrane in which it is embedded. Normally, the inner portion of the membrane is at a negative voltage. When that voltage becomes less negative and reaches a value specific to the channel, it opens and allows ions to cross the membrane (Figure 12.v.4).

This is a two part diagram. Both diagrams show a voltage gated channel embedded in the lipid membrane bilayer. The channel contains a sphere shaped gate that is attached to a filament. In the first diagram there are several ions in the cytosol but only one ion in the extracellular fluid. The voltage across the membrane is currently minus seventy millivolts and the voltage gated channel is closed. In the second diagram, the voltage in the cytosol is minus fifty millivolts. This voltage change has caused the voltage gated channel to open, as the small sphere is no longer occluding the channel. One of the ions is moving through the channel, down its concentration gradient, and out into the extracellular fluid.
Figure 12.5.4 – Voltage-Gated Channels: Voltage-gated channels open when the transmembrane voltage changes around them. Amino acids in the structure of the protein are sensitive to accuse and crusade the pore to open up to the selected ion.

A leak channel is randomly gated, significant that information technology opens and closes at random, hence the reference to leaking. There is no actual event that opens the channel; instead, it has an intrinsic charge per unit of switching between the open and closed states. Leak channels contribute to the resting transmembrane voltage of the excitable membrane (Figure 12.5.five).

This is a two part diagram. Both diagrams show a leakage channel embedded in the lipid membrane bilayer. The leakage channel is cylindrical with a large, central opening. In the first diagram there are several ions in the cytosol but only one ion in the extracellular fluid. No ions are moving through the leakage channel because the channel is closed. In the second diagram, the leakage channel randomly opens, allowing two ions to travel through the channel, down their concentration gradient, and out into the extracellular fluid.
Figure 12.five.5 – Leak Channels: These channels open and close at random, allowing ions to laissez passer through when they are open up.

The Membrane Potential

The membrane potential is a distribution of charge across the cell membrane, measured in millivolts (mV). The standard is to compare the within of the cell relative to the exterior, then the membrane potential is a value representing the charge on the intracellular side of the membrane (based on the outside being naught, relatively speaking; Figure 12.5.6).

This diagram shows a cross section of a cell membrane. The extracellular fluid side of the cell membrane is positively charged while the cytosol side of the membrane is negatively charged. There is a microelectrode embedded in the cell membrane. The microelectrode is attached to a voltmeter, which also has a reference electrode on the extracellular fluid side. The readout of the voltmeter is negative 70 millivolts.
Figure 12.5.6 – Measuring Charge across a Membrane with a Voltmeter: A recording electrode is inserted into the cell and a reference electrode is outside the cell. By comparing the charge measured by these two electrodes, the transmembrane voltage is determined. It is conventional to express that value for the cytosol relative to the exterior.

There is typically an overall net neutral accuse between the extracellular and intracellular environments of the neuron. However, a slight departure in accuse occurs right at the membrane surface, both internally and externally. It is the departure in this very limited region that holds the power to generate electrical signals, including action potentials, in neurons and muscle cells.

When the prison cell is at rest, ions are distributed across the membrane in a very predictable way. The concentration of Na+ exterior the prison cell is x times greater than the concentration within. Likewise, the concentration of Grand+ inside the cell is greater than outside. The cytosol contains a loftier concentration of anions, in the class of phosphate ions and negatively charged proteins. With the ions distributed across the membrane at these concentrations, the difference in charge is described as the resting membrane potential. The exact value measured for the resting membrane potential varies between cells, only -70 mV is a commonly reported value. This voltage would actually be much lower except for the contributions of some important proteins in the membrane. Leak channels allow Na+ to slowly move into the cell or K+ to slowly move out, and the Na+/K+ pump restores their concentration gradients across the membrane. This may appear to be a waste of free energy, but each has a role in maintaining the membrane potential.

The Activity Potential

Resting membrane potential describes the steady state of the prison cell, which is a dynamic process balancing ions leaking downwards their concentration slope and ions being pumped back upward their concentration gradient. Without any outside influence, the resting membrane potential will exist maintained. To become an electrical point started, the membrane potential has to get more positive.

This starts with the opening of voltage-gated Na+ channels in the neuron membrane. Because the concentration of Na+ is higher outside the prison cell than inside the cell by a gene of 10, ions will rush into the cell, driven by both the chemical and electric gradients. Because sodium is a positively charged ion, equally it enters the cell it volition change the relative voltage immediately inside the jail cell membrane. The resting membrane potential is approximately -seventy mV, and so the sodium cation entering the cell will cause the membrane to become less negative. This is known every bit depolarization, significant the membrane potential moves toward nada (becomes less polarized). The concentration gradient for Na+ is so potent that information technology will proceed to enter the cell even afterward the membrane potential has get zero, so that the voltage immediately around the pore and then begins to become positive.

As the membrane potential reaches +xxx mV, slower to open voltage-gated potassium channels are now opening in the membrane. An electrochemical gradient acts on K+, likewise. As Thou+ starts to leave the cell, taking a positive charge with it, the membrane potential begins to move back toward its resting voltage. This is called repolarization, significant that the membrane voltage moves back toward the -70 mV value of the resting membrane potential.

Repolarization returns the membrane potential to the -seventy mV value of the resting potential, simply overshoots that value. Potassium ions accomplish equilibrium when the membrane voltage is below -70 mV, and then a menstruation of hyperpolarization occurs while the K+ channels are open. Those K+ channels are slightly delayed in closing, accounting for this short overshoot.

What has been described here is the action potential, which is presented as a graph of voltage over time in Figure 12.5.7. Information technology is the electrical signal that nervous tissue generates for communication. The change in the membrane voltage from -lxx mV at rest to +30 mV at the finish of depolarization is a 100-mV change.

This graph has membrane potential, in millivolts, on the X axis, ranging from negative 70 to positive thirty. Time is on the X axis. The plot line starts steadily at negative seventy and then increases to negative 55 millivolts. The plot line then increases quickly, peaking at positive thirty. This is the depolarization phase. The plot line then quickly drops back to negative seventy millivolts. This is the repolarization phase. The plot line continues to drop but then gradually increases back to negative seventy millivolts. The area where the plot line is below negative seventy millivolts is the hyperpolarization phase.
Figure 12.5.7 – Graph of Activeness Potential: Plotting voltage measured across the cell membrane against fourth dimension, the action potential begins with depolarization, followed past repolarization, which goes by the resting potential into hyperpolarization, and finally the membrane returns to rest.

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What happens across the membrane of an electrically active cell is a dynamic process that is hard to visualize with static images or through text descriptions. View this animation to larn more than about this process. What is the difference betwixt the driving forcefulness for Na+ and K+? And what is similar about the motility of these two ions?

The membrane potential will stay at the resting voltage until something changes. To brainstorm an action potential, the membrane potential must change from the resting potential of approximately -70mV to the threshold voltage of -55mV. Once the jail cell reaches threshold, voltage-gated sodium channels open and beingness the predictable membrane potential changes describe in a higher place as an activity potential.  Any sub-threshold depolarization that does not change the membrane potential to -55 mV or higher will non achieve threshold and thus will non outcome in an activity potential. Likewise, any stimulus that depolarizes the membrane to -55 mV or beyond will cause a large number of channels to open and an action potential will exist initiated.

Because of the anticipated changes that occur once threshold is reached, the activity potential is referred to as "all or none". This ways that either the action potential occurs and is repeated along the entire length of the neuron or no action potential occurs. A stronger stimulus, which might depolarize the membrane well past threshold, will not make a "bigger" activeness potential. Either the membrane reaches the threshold and everything occurs as described higher up, or the membrane does not achieve the threshold and nothing else happens. All action potentials top at the same voltage (+xxx mV), and then ane action potential is not bigger than another. Stronger stimuli will initiate multiple action potentials more rapidly, but the private signals are not bigger.

As we have seen, the depolarization and repolarization of an action potential are dependent on two types of channels (the voltage-gated Na+ channel and the voltage-gated Thousand+ channel). The voltage-gated Na+ channel actually has two gates. One is the activation gate, which opens when the membrane potential crosses -55 mV. The other gate is the inactivation gate, which closes later on a specific period of time—on the lodge of a fraction of a millisecond. When a prison cell is at residual, the activation gate is closed and the inactivation gate is open up. However, when the threshold is reached, the activation gate opens, assuasive Na+ to rush into the cell. Timed with the peak of depolarization, the inactivation gate closes. During repolarization, no more sodium tin enter the cell. When the membrane potential passes -55 mV once again, the activation gate closes. After that, the inactivation gate re-opens, making the channel ready to start the whole process over again.

The voltage-gated Chiliad+ channel has only 1 gate, which is sensitive to a membrane voltage of -fifty mV. However, it does not open as quickly as the voltage-gated Na+ aqueduct does. It takes a fraction of a millisecond for the K+ channel to open up once that voltage has been reached, which coincides exactly with when the Na+ flow peaks. So voltage-gated K+ channels open only equally the voltage-gated Na+ channels are being inactivated. Every bit the membrane potential repolarizes and the voltage passes -50 mV over again, the K+ channels brainstorm to shut. Potassium continues to leave the cell for a short while and the membrane potential becomes more negative, resulting in the hyperpolarization overshoot. Then the K+ channels are closed and the membrane returns to the resting potential because of the ongoing action of the leak channels and the Na+/One thousand+ ATPase pump.

All of this takes identify within approximately 2 milliseconds (Figure 12.five.8). While an action potential is in progress, another 1 cannot be initiated. That upshot is referred to as the refractory flow. There are two phases of the refractory menses: the accented refractory period and the relative refractory period. During the absolute refractory catamenia, another activeness potential will not start. This is considering of the inactivation gate of the voltage-gated Na+ channel. In one case the Na+ channel is back to its resting conformation, a new action potential could be started during the hyperpolarization phase, only only by a stronger stimulus than the one that initiated the current action potential.

This graph has membrane potential, in millivolts, on the X axis, ranging from negative 70 to positive thirty. Time is on the X axis. In step one, which is labeled at rest, the plot line is steady at negative seventy millivolts. In step 2, a stimulus is applied, causing the plot line to increase to positive 30 millivolts. The curve sharply increases at step three, labeled voltage rises. After peaking at positive thirty, the plot line then quickly drops back to negative 70. This is the fourth step, labeled voltage falls. The plot line continues to drop below negative 70 and this is step 5, labeled end of action potential. Finally, the plot line gradually increases back to negative seventy millivolts, which is step 6, labeled return to rest.
Figure 12.5.8 – Stages of an Activeness Potential: Plotting voltage measured across the cell membrane against time, the events of the action potential can be related to specific changes in the membrane voltage. (1) At rest, the membrane voltage is -seventy mV. (2) The membrane begins to depolarize when an external stimulus is applied. (three) The membrane voltage begins a rapid rise toward +30 mV. (4) The membrane voltage starts to return to a negative value. (five) Repolarization continues past the resting membrane voltage, resulting in hyperpolarization. (half dozen) The membrane voltage returns to the resting value shortly after hyperpolarization.

Propagation of the Action Potential

The action potential is initiated at the beginning of the axon, at what is called the initial segment (trigger zone). Rapid depolarization can take place here due to a high density of voltage-gated Na+ channels. Going down the length of the axon, the action potential is propagated because more voltage-gated Na+ channels are opened as the depolarization spreads. This spreading occurs because Na+ enters through the channel and moves along the within of the cell membrane. Every bit the Na+ moves, or flows, a curt distance along the cell membrane, its positive accuse depolarizes a trivial more of the jail cell membrane. Equally that depolarization spreads, new voltage-gated Na+ channels open and more ions blitz into the cell, spreading the depolarization a petty further.

Because voltage-gated Na+ channels are inactivated at the acme of the depolarization, they cannot be opened over again for a brief time (absolute refractory period). Because of this, positive ions spreading dorsum toward previously opened channels has no upshot. The activeness potential must propagate from the trigger zone toward the axon terminals.

Propagation, equally described above, applies to unmyelinated axons. When myelination is present, the activeness potential propagates differently, and is optimized for the speed of signal conduction. Sodium ions that enter the cell at the trigger zone kickoff to spread forth the length of the axon segment, but at that place are no voltage-gated Na+ channels until the get-go node of Ranvier. Considering in that location is non abiding opening of these channels along the axon segment, the depolarization spreads at an optimal speed. The distance betwixt nodes is the optimal altitude to go on the membrane even so depolarized in a higher place threshold at the next node. As Na+ spreads along the within of the membrane of the axon segment, the accuse starts to misemploy. If the node were any farther downwardly the axon, that depolarization would have fallen off too much for voltage-gated Na+ channels to be activated at the side by side node of Ranvier. If the nodes were any closer together, the speed of propagation would be slower.

Propagation along an unmyelinated axon is referred to as continuous conduction; forth the length of a myelinated axon it is referred to as saltatory conduction. Continuous conduction is slow considering there are always voltage-gated Na+ channels opening, and more than and more Na+ is rushing into the cell. Saltatory conduction is faster because the activity potential "jumps" from one node to the next (saltare = "to jump"), and the new influx of Na+ renews the depolarized membrane. Along with the myelination of the axon, the diameter of the axon tin influence the speed of conduction. Much as h2o runs faster in a wide river than in a narrow creek, Na+-based depolarization spreads faster down a wide axon than down a narrow one. This concept is known as resistance and is generally true for electrical wires or plumbing, simply as it is true for axons, although the specific conditions are different at the scales of electrons or ions versus water in a river.

Homeostatic Imbalances – Potassium Concentration

Glial cells, especially astrocytes, are responsible for maintaining the chemical environment of the CNS tissue. The concentrations of ions in the extracellular fluid are the ground for how the membrane potential is established and changes in electrochemical signaling. If the balance of ions is upset, drastic outcomes are possible.

Unremarkably the concentration of G+ is college inside the neuron than outside. Afterward the repolarizing phase of the activeness potential, Chiliad+ leak channels and Na+/K+ pumps ensure that the ions return to their original locations. Following a stroke or other ischemic event, extracellular Thou+ levels are elevated. The astrocytes in the area are equipped to articulate backlog G+ to aid the pump. But when the level is far out of balance, the effects can be irreversible.

Astrocytes can become reactive in cases such equally these, which impairs their ability to maintain the local chemic environment. The glial cells enlarge and their processes swell. They lose their K+ buffering ability and the function of the pump is afflicted, or even reversed. I of the early signs of cell disease is this "leaking" of sodium ions into the body cells. This sodium/potassium imbalance negatively affects the internal chemistry of cells, preventing them from functioning ordinarily.

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Visit this site to see a virtual neurophysiology lab, and to detect electrophysiological processes in the nervous system, where scientists directly mensurate the electrical signals produced past neurons. Oftentimes, the activeness potentials occur so rapidly that watching a screen to see them occur is not helpful. A speaker is powered by the signals recorded from a neuron and it "pops" each time the neuron fires an action potential. These action potentials are firing then fast that it sounds like static on the radio. Electrophysiologists can recognize the patterns within that static to understand what is happening. Why is the leech model used for measuring the electrical action of neurons instead of using humans?

Affiliate Review

The nervous system is characterized past electrical signals that are sent from i area to some other. Whether those areas are close or very far apart, the signal must travel along an axon. The basis of the electrical indicate is the controlled distribution of ions across the membrane. Transmembrane ion channels regulate when ions can movement in or out of the cell, so that a precise signal is generated. This signal is the activity potential which has a very characteristic shape based on voltage changes across the membrane in a given time catamenia.

The membrane is normally at rest with established Na+ and Grand+ concentrations on either side. A stimulus will start the depolarization of the membrane, and voltage-gated channels will outcome in further depolarization followed past repolarization of the membrane. A slight overshoot of hyperpolarization marks the end of the action potential. While an action potential is in progress, another cannot exist generated under the same conditions. While the voltage-gated Na+ aqueduct is inactivated, absolutely no action potentials can be generated. Once that aqueduct has returned to its resting state, a new action potential is possible, merely it must be started by a relatively stronger stimulus to overcome the state of hyperpolarization.

The action potential travels down the axon as voltage-gated ion channels are opened by the spreading depolarization. In unmyelinated axons, this happens in a continuous fashion because at that place are voltage-gated channels throughout the membrane. In myelinated axons, propagation is described every bit saltatory considering voltage-gated channels are only constitute at the nodes of Ranvier and the electrical events seem to "jump" from one node to the adjacent. Saltatory conduction is faster than continuous conduction, meaning that myelinated axons propagate their signals faster. The diameter of the axon also makes a deviation equally ions diffusing within the cell have less resistance in a wider space.

Interactive Link Questions

What happens across the membrane of an electrically active cell is a dynamic process that is hard to visualize with static images or through text descriptions. View this animation to really empathize the process. What is the divergence between the driving strength for Na+ and K+? And what is similar about the movement of these two ions?

Sodium is moving into the jail cell because of the immense concentration gradient, whereas potassium is moving out because of the depolarization that sodium causes. However, they both move down their respective gradients, toward equilibrium.

Visit this site to see a virtual neurophysiology lab, and to observe electrophysiological processes in the nervous system, where scientists directly measure the electrical signals produced by neurons. Often, the action potentials occur and so rapidly that watching a screen to see them occur is not helpful. A speaker is powered by the signals recorded from a neuron and it "pops" each fourth dimension the neuron fires an action potential. These action potentials are firing so fast that information technology sounds like static on the radio. Electrophysiologists can recognize the patterns inside that static to sympathize what is happening. Why is the leech model used for measuring the electric activity of neurons instead of using humans?

The backdrop of electrophysiology are common to all animals, then using the leech is an easier approach to studying the properties of these cells. There are differences between the nervous systems of invertebrates (such as a leech) and vertebrates, but not for the sake of what these experiments study.

Review Questions

Critical Thinking Questions

1. What does it hateful for an action potential to be an "all or none" result?

ii. The conscious perception of pain is often delayed because of the time it takes for the sensations to accomplish the cerebral cortex. Why would this be the instance based on propagation of the axon potential?

Glossary

absolute refractory period
time during an action period when another action potential cannot exist generated because the voltage-gated Na+ channel is inactivated
activation gate
part of the voltage-gated Na+ aqueduct that opens when the membrane voltage reaches threshold
continuous conduction
wearisome propagation of an activeness potential along an unmyelinated axon attributable to voltage-gated Na+ channels located along the entire length of the prison cell membrane
depolarization
change in a cell membrane potential from rest toward zero
electrochemical exclusion
principle of selectively allowing ions through a channel on the footing of their charge
excitable membrane
cell membrane that regulates the movement of ions so that an electric bespeak can be generated
gated
property of a channel that determines how information technology opens under specific conditions, such as voltage change or physical deformation
inactivation gate
office of a voltage-gated Na+ channel that closes when the membrane potential reaches +xxx mV
ionotropic receptor
neurotransmitter receptor that acts as an ion aqueduct gate, and opens past the binding of the neurotransmitter
leakage channel
ion channel that opens randomly and is not gated to a specific event, also known equally a non-gated channel
ligand-gated channels
another proper name for an ionotropic receptor for which a neurotransmitter is the ligand
mechanically gated channel
ion aqueduct that opens when a physical event directly affects the structure of the protein
membrane potential
distribution of charge across the prison cell membrane, based on the charges of ions
nonspecific channel
aqueduct that is not specific to ane ion over another, such as a nonspecific cation channel that allows any positively charged ion beyond the membrane
refractory period
time afterward the initiation of an action potential when another action potential cannot exist generated
relative refractory menstruation
fourth dimension during the refractory menses when a new action potential can only exist initiated by a stronger stimulus than the current action potential because voltage-gated Grand+ channels are non closed
repolarization
return of the membrane potential to its normally negative voltage at the end of the activity potential
resistance
belongings of an axon that relates to the ability of particles to diffuse through the cytoplasm; this is inversely proportional to the fiber diameter
resting membrane potential
the difference in voltage measured across a cell membrane under steady-state conditions, typically -70 mV
saltatory conduction
quick propagation of the action potential along a myelinated axon attributable to voltage-gated Na+ channels existence present only at the nodes of Ranvier
size exclusion
principle of selectively assuasive ions through a channel on the ground of their relative size
voltage-gated channel
ion channel that opens because of a change in the charge distributed across the membrane where it is located

Solutions

Answers for Critical Thinking Questions

  1. The cell membrane must reach threshold before voltage-gated Na+ channels open. If threshold is not reached, those channels do not open up, and the depolarizing phase of the action potential does not occur, the cell membrane will just become back to its resting state.
  2. Axons of pain sensing sensory neurons are sparse and unmyelinated and so that it takes longer for that sensation to reach the brain than other sensations.

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