Membrane proteins as ion channels. Selective and non-selective channels
Ion channels represented by integral membrane proteins. These proteins are capable, under certain influences, of changing their conformation (shape and properties) in such a way that the pore through which any ion can pass opens or closes. Sodium, potassium, calcium, and chlorine channels are known; sometimes a channel can pass two ions, for example, sodium-calcium channels are known. Only passive transport of ions occurs through ion channels. This means that for an ion to move, not only an open channel is required, but also a concentration gradient for that ion. In this case, the ion will move along a concentration gradient - from an area with a higher concentration to an area with a lower concentration. It must be remembered that we are talking about ions - charged particles, the transport of which is also determined by charge. Situations are possible when movement along the concentration gradient can be directed in one direction, and existing charges counteract this transfer.
Ion channels have two important properties: 1) selectivity (selectivity) towards certain ions and 2) ability to open (activate) and close. When activated, the channel opens and allows ions to pass through (Fig. 8). Thus, the complex of integral proteins that form the channel must necessarily include two elements: structures that recognize “their” ion and are able to let it through, and structures that allow you to know when to let this ion through. The selectivity of the channel is determined by the proteins that form it; the “own” ion is recognized by its size and charge.
Channel activation possible in several ways. First, channels can open and close as the membrane potential changes. The change in charge leads to a change in the conformation of protein molecules, and the channel becomes permeable to the ion. To change the properties of the channel, a slight fluctuation in the membrane potential is sufficient. Such channels are called voltage dependent(or electrically controlled). Second, the channels may be part of a complex protein complex called a membrane receptor. In this case, the change in the properties of the channel is caused by a conformational rearrangement of proteins, which occurs as a result of the interaction of the receptor with a biologically active substance (hormone, mediator). Such channels are called chemodependent(or receptor-gated ) . In addition, the channels can open under mechanical influence - pressure, stretching (Fig. 9). The mechanism that provides activation is called channel gating. Based on the speed at which the channels open and close, they can be divided into fast and slow.
Most channels (potassium, calcium, chloride) can be in two states: open and closed. There are some peculiarities in the operation of sodium channels. These channels, like potassium, calcium, and chloride, tend to be either in an open or closed state, however, the sodium channel can also be inactivated, this is a state in which the channel is closed and cannot be opened by any influence (Fig. 10).
Figure 8. Ion channel states
Figure 9. Example of a receptor-gated channel. ACh – acetylcholine. The interaction of the ACh molecule with the membrane receptor changes the conformation of the gate protein in such a way that the channel begins to allow ions to pass through.
Figure 10 Example of a potential-dependent channel
The voltage-gated sodium channel has activation and inactivation gates (gates). Activation and inactivation gates change conformation at different membrane potentials.
When considering the mechanisms of excitation, we will be mainly interested in the work of sodium and potassium channels, however, let us briefly dwell on the features of calcium channels, we will need them in the future. Sodium and calcium channels differ in their properties. Sodium channels are fast and slow, while calcium channels are only slow. Activation of sodium channels only leads to depolarization and the occurrence of either LO or AP; activation of calcium channels can additionally cause metabolic changes in the cell. These changes are due to the fact that calcium binds to special proteins that are sensitive to this ion. The calcium-bound protein changes its properties in such a way that it becomes capable of changing the properties of other proteins, for example, activating enzymes, triggering muscle contraction, and releasing mediators.
According to modern concepts, biological membranes form the outer shell of all animal cells and form numerous intracellular organelles. The most characteristic structural feature is that membranes always form closed spaces, and this microstructural organization of membranes allows them to perform essential functions.
Structure and functions of cell membranes.
1. The barrier function is expressed in the fact that the membrane, using appropriate mechanisms, participates in the creation of concentration gradients, preventing free diffusion. In this case, the membrane takes part in the mechanisms of electrogenesis. These include mechanisms for creating a resting potential, generation of an action potential, mechanisms for the propagation of bioelectric impulses across homogeneous and heterogeneous excitable structures.
2. The regulatory function of the cell membrane is the fine regulation of intracellular contents and intracellular reactions due to the reception of extracellular biologically active substances, which leads to changes in the activity of enzyme systems of the membrane and the launch of mechanisms of secondary “messengers” (“intermediaries”).
3. Conversion of external stimuli of a non-electrical nature into electrical signals (in receptors).
4. Release of neurotransmitters in synaptic endings.
Modern methods of electron microscopy determined the thickness of cell membranes (6-12 nm). Chemical analysis showed that the membranes are mainly composed of lipids and proteins, the amount of which varies among different cell types. The difficulty of studying the molecular mechanisms of the functioning of cell membranes is due to the fact that when isolating and purifying cell membranes, their normal functioning is disrupted. Currently, we can talk about several types of cell membrane models, among which the liquid mosaic model is the most widespread.
According to this model, the membrane is represented by a bilayer of phospholipid molecules, oriented in such a way that the hydrophobic ends of the molecules are located inside the bilayer, and the hydrophilic ends are directed into the aqueous phase. This structure is ideal for the formation of a separation between two phases: extra- and intracellular.
Globular proteins are integrated into the phospholipid bilayer, the polar regions of which form a hydrophilic surface in the aqueous phase. These integrated proteins perform various functions, including receptor, enzymatic, form ion channels, are membrane pumps and transporters of ions and molecules.
Some protein molecules diffuse freely in the plane of the lipid layer; in the normal state, parts of protein molecules emerging on different sides of the cell membrane do not change their position.
Electrical characteristics of membranes:
Capacitive properties are mainly determined by the phospholipid bilayer, which is impermeable to hydrated ions and at the same time thin enough (about 5 nm) to allow efficient separation and accumulation of charges and electrostatic interaction of cations and anions. In addition, the capacitive properties of cell membranes are one of the reasons that determine the time characteristics of electrical processes occurring on cell membranes.
Conductivity (g) is the reciprocal of electrical resistance and is equal to the ratio of the total transmembrane current for a given ion to the value that determined its transmembrane potential difference.
Various substances can diffuse through the phospholipid bilayer, and the degree of permeability (P), i.e., the ability of the cell membrane to pass these substances, depends on the difference in concentrations of the diffusing substance on both sides of the membrane, its solubility in lipids and the properties of the cell membrane.
The conductivity of a membrane is a measure of its ionic permeability. An increase in conductivity indicates an increase in the number of ions passing through the membrane.
Structure and functions of ion channels. Na+, K+, Ca2+, Cl- ions penetrate into the cell and exit through special fluid-filled channels. The channel size is quite small.
All ion channels are divided into the following groups:
- By selectivity:
a) Selective, i.e. specific. These channels are permeable to strictly defined ions.
b) Low-selective, non-specific, without specific ion selectivity. There are a small number of them in the membrane.
- According to the nature of the ions passed through:
a) potassium
b) sodium
c) calcium
d) chlorine
- According to the rate of inactivation, i.e. closing:
a) quickly inactivating, i.e. quickly turning into a closed state. They provide a rapidly increasing reduction in MP and an equally rapid recovery.
b) slow-acting. Their opening causes a slow decrease in MP and its slow recovery.
4. According to opening mechanisms:
a) potential-dependent, i.e. those that open at a certain level of membrane potential.
b) chemo-dependent, opening when the cell membrane chemoreceptors are exposed to physiologically active substances (neurotransmitters, hormones, etc.).
It has now been established that ion channels have the following structure:
1. Selective filter located at the mouth of the channel. It ensures the passage of strictly defined ions through the channel.
2. Activation gates that open at a certain level of membrane potential or the action of the corresponding PAS. The activation gates of potential-dependent channels have a sensor that opens them at a certain MP level.
3. Inactivation gate, ensuring the closure of the channel and the cessation of ion flow through the channel at a certain MP level (Fig).
Nonspecific ion channels do not have a gate.
Selective ion channels can exist in three states, which are determined by the position of the activation (m) and inactivation (h) gates:
1.Closed when the activation ones are closed and the inactivation ones are open.
2. Activated, both gates are open.
3. Inactivated, the activation gate is open and the inactivation gate is closed
Functions of ion channels:
1. Potassium (at rest) – generation of resting potential
2. Sodium – generation of action potential
3. Calcium - slow action generation
4. Potassium (delayed rectification) – ensuring repolarization
5. Potassium calcium-activated – limiting depolarization caused by Ca+2 current
The function of ion channels is studied in various ways. The most common method is voltage clamp, or “voltage-clamp”. The essence of the method is that, with the help of special electronic systems, the membrane potential is changed and fixed at a certain level during the experiment. In this case, the magnitude of the ionic current flowing through the membrane is measured. If the potential difference is constant, then, in accordance with Ohm's law, the current magnitude is proportional to the conductivity of the ion channels. In response to stepwise depolarization, certain channels open and the corresponding ions enter the cell along an electrochemical gradient, i.e., an ion current arises that depolarizes the cell. This change is detected by a control amplifier and an electric current is passed through the membrane, equal in magnitude but opposite in direction to the membrane ion current. In this case, the transmembrane potential difference does not change.
Studying the function of individual channels is possible using the method of local fixation of the “path-clamp” potential. A glass microelectrode (micropipette) is filled with saline solution, pressed against the surface of the membrane and a slight vacuum is created. In this case, part of the membrane is sucked to the microelectrode. If an ion channel appears in the suction zone, then the activity of a single channel is recorded. The system of irritation and recording of channel activity differs little from the voltage recording system.
The current through a single ion channel has a rectangular shape and is the same in amplitude for channels of different types. The duration of the channel's stay in the open state is probabilistic, but depends on the value of the membrane potential. The total ion current is determined by the probability of a certain number of channels being in the open state in each specific period of time.
The outer part of the canal is relatively accessible for study; studying the inner part presents significant difficulties. P. G. Kostyuk developed a method of intracellular dialysis, which allows one to study the function of the input and output structures of ion channels without the use of microelectrodes. It turned out that the part of the ion channel open to the extracellular space differs in its functional properties from the part of the channel facing the intracellular environment.
It is ion channels that provide two important properties of the membrane: selectivity and conductivity.
The selectivity, or selectivity, of the channel is ensured by its special protein structure. Most channels are electrically controlled, that is, their ability to conduct ions depends on the magnitude of the membrane potential. The channel is heterogeneous in its functional characteristics, especially with regard to the protein structures located at the entrance to the channel and at its exit (the so-called gate mechanisms).
Let's consider the principle of operation of ion channels using the sodium channel as an example. It is believed that the sodium channel is closed at rest. When the cell membrane is depolarized to a certain level, the m-activation gate opens (activation) and the flow of Na+ ions into the cell increases. A few milliseconds after the m-gate opens, the h-gate located at the exit of the sodium channels closes (inactivation). Inactivation develops very quickly in the cell membrane and the degree of inactivation depends on the magnitude and time of action of the depolarizing stimulus.
When a single action potential is generated in a thick nerve fiber, the change in the concentration of Na+ ions in the internal environment is only 1/100,000 of the internal Na+ ion content of the squid giant axon.
In addition to sodium, other types of channels are installed in cell membranes that are selectively permeable to individual ions: K+, Ca2+, and there are varieties of channels for these ions.
Hodgkin and Huxley formulated the principle of “independence” of channels, according to which the flow of sodium and potassium across the membrane is independent of each other.
The conductivity properties of different channels are not the same. In particular, for potassium channels, the inactivation process does not exist, as for sodium channels. There are special potassium channels that are activated when the intracellular calcium concentration increases and the cell membrane depolarizes. Activation of potassium-calcium-dependent channels accelerates repolarization, thereby restoring the original value of the resting potential.
Calcium channels are of particular interest. The incoming calcium current is usually not large enough to normally depolarize the cell membrane. Most often, calcium entering the cell acts as a “messenger”, or secondary messenger. Activation of calcium channels is achieved by depolarization of the cell membrane, for example by an incoming sodium current.
The process of inactivation of calcium channels is quite complex. On the one hand, an increase in the intracellular concentration of free calcium leads to inactivation of calcium channels. On the other hand, proteins in the cytoplasm of cells bind calcium, which makes it possible to maintain a stable calcium current for a long time, albeit at a low level; in this case, the sodium current is completely suppressed. Calcium channels play an essential role in heart cells. Electrogenesis of cardiomyocytes is discussed in Chapter 7. The electrophysiological characteristics of cell membranes are studied using special methods.
All channels present in living tissues, and now we know several hundred types of channels, can be divided into two main types. The first type is rest channels, which spontaneously open and close without any external influences. They are important for generating the resting membrane potential. The second type is the so-called gate channels, or portal channels(from the word "gate") . At rest, these channels are closed and can open under the influence of certain stimuli. Some types of such channels are involved in the generation of action potentials.
Most ion channels are characterized selectivity(selectivity), that is, only certain ions pass through a certain type of channel. Based on this feature, sodium, potassium, calcium, and chloride channels are distinguished. The selectivity of channels is determined by the size of the pore, the size of the ion and its hydration shell, the charge of the ion, as well as the charge of the inner surface of the channel. However, there are also non-selective channels that can pass two types of ions at once: for example, potassium and sodium. There are channels through which all ions and even larger molecules can pass.
There is a classification of ion channels according to activation method(Fig. 9). Some channels specifically respond to physical changes in the neuron's cell membrane. The most prominent representatives of this group are voltage-activated channels. Examples include voltage-sensitive sodium, potassium, and calcium ion channels on the membrane, which are responsible for the formation of the action potential. These channels open at a certain membrane potential. Thus, sodium and potassium channels open at a potential of about -60 mV (the inner surface of the membrane is negatively charged compared to the outer surface). Calcium channels open at a potential of -30 mV. The group of channels activated by physical changes includes
Figure 9. Methods for activating ion channels
(A) Ion channels activated by changes in membrane potential or membrane stretch. (B) Ion channels activated by chemical agents (ligands) from the extracellular or intracellular side.
Also mechanosensitive channels that respond to mechanical stress (stretching or deformation of the cell membrane). Another group of ion channels open when chemicals activate special receptor binding sites on the channel molecule. Such ligand-activated channels are divided into two subgroups, depending on whether their receptor centers are intracellular or extracellular. Ligand-activated channels that respond to extracellular stimuli are also called ionotropic receptors. Such channels are sensitive to transmitters and are directly involved in the transmission of information in synaptic structures. Ligand-activated channels, activated from the cytoplasmic side, include channels that are sensitive to changes in the concentration of specific ions. For example, calcium-activated potassium channels are activated by local increases in intracellular calcium concentration. Such channels play an important role in repolarizing the cell membrane during the termination of an action potential. In addition to calcium ions, typical representatives of intracellular ligands are cyclic nucleotides. Cyclic GMP, for example, is responsible for the activation of sodium channels in the retinal rods. This type of channel plays a fundamental role in the operation of the visual analyzer. A separate type of modulation of channel operation by binding an intracellular ligand is the phosphorylation/dephosphorylation of certain sections of its protein molecule under the action of intracellular enzymes - protein kinases and protein phosphatases.
The presented classification of channels by activation method is largely arbitrary. Some ion channels can only be activated by a few stimuli. For example, calcium-activated potassium channels are also sensitive to changes in potential, and some voltage-activated ion channels are sensitive to intracellular ligands.
The excitable membrane model according to the Hodgkin-Huxley theory assumes the controlled transport of ions across the membrane. However, the direct transition of an ion through the lipid bilayer is very difficult, and therefore the ion flow would be small.
This and a number of other considerations gave reason to believe that the membrane must contain some special structures - conducting ions. Such structures were found and called ion channels. Similar channels have been isolated from various objects: the plasma membrane of cells, the postsynaptic membrane of muscle cells and other objects. Ion channels formed by antibiotics are also known.
Basic properties of ion channels:
1) selectivity;
2) independence of operation of individual channels;
3) discrete nature of conductivity;
4) dependence of channel parameters on membrane potential.
Let's look at them in order.
1. Selectivity is the ability of ion channels to selectively allow ions of one type to pass through.
Even in the first experiments on the squid axon, it was discovered that Na+ and Kt ions have different effects on the membrane potential. K+ ions change the resting potential, and Na+ ions change the action potential. The Hodgkin-Huxley model describes this by introducing independent potassium and sodium ion channels. It was assumed that the former allow only K+ ions to pass through, and the latter only pass through Na+ ions.
Measurements have shown that ion channels have absolute selectivity towards cations (cation-selective channels) or anions (anion-selective channels). At the same time, various cations of various chemical elements can pass through cation-selective channels, but the conductivity of the membrane for the minor ion, and therefore the current through it, will be significantly lower, for example, for the Na + channel, the potassium current through it will be 20 times less. The ability of an ion channel to pass different ions is called relative selectivity and is characterized by a selectivity series - the ratio of channel conductivities for different ions taken at the same concentration. In this case, for the main ion, selectivity is taken as 1. For example, for the Na+ channel this series has the form:
Na + : K + = 1: 0.05.
2. Independence of the operation of individual channels. The flow of current through an individual ion channel is independent of whether current flows through other channels. For example, K + channels can be turned on or off, but the current through the Na + channels does not change. The influence of channels on each other occurs indirectly: a change in the permeability of some channels (for example, sodium) changes the membrane potential, and this already affects the conductivity of other ion channels.
3. Discrete nature of the conductivity of ion channels. Ion channels are a subunit complex of proteins that span the membrane. In its center there is a tube through which ions can pass. The number of ion channels per 1 μm 2 membrane surface was determined using a radioactively labeled sodium channel blocker - tetrodotoxin. It is known that one TTX molecule binds to only one channel. Then measuring the radioactivity of a sample with a known area made it possible to show that there are about 500 sodium channels per 1 µm2 squid axon.
Those transmembrane currents that are measured in conventional experiments, for example, on a squid axon 1 cm long and 1 mm in diameter, that is, an area of 3 * 10 7 μm 2, are due to the total response (change in conductivity) of 500 3 10 7 -10 10 ion channels. This response is characterized by a smooth change in conductivity over time. The response of a single ion channel changes over time in a fundamentally different way: discretely for Na+ channels, and for K+-, and for Ca 2+ channels.
This was first discovered in 1962 in studies of the conductivity of lipid bilayer membranes (BLMs) when microquantities of a certain excitation-inducing substance were added to the solution surrounding the membrane. A constant voltage was applied to the BLM and the current I(t) was recorded. The current was recorded over time in the form of jumps between two conducting states.
One of the effective methods for experimental study of ion channels was the method of local fixation of membrane potential (“Patch Clamp”), developed in the 80s (Fig. 10).
Rice. 10. Method of local fixation of membrane potential. ME - microelectrode, IR - ion channel, M - cell membrane, SFP - potential clamp circuit, I - single channel current
The essence of the method is that the ME microelectrode (Fig. 10), with a thin end having a diameter of 0.5-1 μm, is suctioned to the membrane so that the ion channel enters its inner diameter. Then, using a potential-clamp circuit, it is possible to measure currents that pass only through a single channel of the membrane, and not through all channels simultaneously, as happens when using the standard potential-clamp method.
The results of experiments performed on various ion channels showed that the conductivity of an ion channel is discrete and it can be in two states: open or closed. Transitions between states occur at random times and obey statistical laws. It cannot be said that a given ion channel will open at exactly this moment in time. You can only make a statement about the probability of opening a channel in a certain time interval.
4. Dependence of channel parameters on membrane potential. Nerve fiber ion channels are sensitive to membrane potential, such as the sodium and potassium channels of the squid axon. This is manifested in the fact that after the start of membrane depolarization, the corresponding currents begin to change with one or another kinetics. This process occurs as follows: The ion-selective channel has a sensor - some element of its design that is sensitive to the action of the electric field (Fig. 11). When the membrane potential changes, the magnitude of the force acting on it changes, as a result, this part of the ion channel moves and changes the probability of opening or closing the gate - a kind of damper that operates according to the “all or nothing” law. It has been experimentally shown that under the influence of membrane depolarization, the probability of the sodium channel transitioning to the conducting state increases. The voltage surge across the membrane created during potential clamp measurements causes a large number of channels to open. More charges pass through them, which means, on average, more current flows. It is important that the process of increasing channel conductivity is determined by an increase in the probability of the channel transitioning to an open state, and not by an increase in the diameter of the open channel. This is the modern understanding of the mechanism of current passage through a single channel.
Smooth kinetic curves of currents recorded during electrical measurements on large membranes are obtained due to the summation of many stepwise currents flowing through individual channels. Their summation, as shown above, sharply reduces fluctuations and gives fairly smooth time dependences of the transmembrane current.
Ion channels can also be sensitive to other physical influences: mechanical deformation, binding of chemicals, etc. In this case, they are the structural basis, respectively, of mechanoreceptors, chemo-receptors, etc.
The study of ion channels in membranes is one of the important tasks of modern biophysics.
Structure of the ion channel.
The ion-selective channel consists of the following parts (Fig. 11): immersed in the bilayer of the protein part, which has a subunit structure; a selective filter formed by negatively charged oxygen atoms, which are rigidly located at a certain distance from each other and allow ions of a certain diameter to pass through; gate part.
The gate of the ion channel is controlled by the membrane potential and can be in either a closed state (dashed line) or an open state (solid line). The normal position of the sodium channel gate is closed. Under the influence of an electric field, the probability of an open state increases, the gate opens and the flow of hydrated ions is able to pass through the selective filter.
If the ion fits in diameter, it sheds its hydration shell and jumps to the other side of the ion channel. If the ion is too large in diameter, such as tetraethylammonium, it is not able to fit through the filter and cannot cross the membrane. If, on the contrary, the ion is too small, then it has difficulties in the selective filter, this time associated with the difficulty of shedding the hydration shell of the ion.
Ion channel blockers either cannot pass through it, getting stuck in the filter, or, if they are large molecules like TTX, they sterically match some entrance to the channel. Since blockers carry a positive charge, their charged part is drawn into the channel to the selective filter as an ordinary cation, and the macromolecule clogs it.
Thus, changes in the electrical properties of excitable biomembranes are carried out using ion channels. These are protein macromolecules that penetrate the lipid bilayer and can exist in several discrete states. The properties of channels selective for K + , Na + and Ca 2+ ions may depend differently on the membrane potential, which determines the dynamics of the action potential in the membrane, as well as the differences in such potentials in the membranes of different cells.
Rice. 11. Cross-sectional diagram of the structure of the sodium ion channel of the membrane
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