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11.3: Diffusion Across a Membrane - Channels

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  • If you punched a hole or pore in the membrane, depending on its size, multiple types of chemical species could flow through it simultaneously.  We'll talk about pores in the next section.  Let's focus on channels, which have much smaller openings which are gated open to allow ion flow through them.  They are often called ionotropic receptors.  Channels can be "gated" open by many mechanisms including ligand binding, change in membrane potential, lipid interactions, and mechanical stress.  Opening a channel to ion flow allows very quick passage of information (in this case an electrical signal) into the cell, leading to quick cellular responses.  This is an ideal signaling mechanism for neural cells which demand quick responses.

    We'll show examples of each type of gating mechanism. .

    Before we do, it is helpful to know typical extracellular and intracellular ion concentration in a mammalian neuron, for example.  They are listed in the table below.

    ion extracellular = [ion]out  (mM) intracellular = [ion]in (mM)
    Na+ 145 mM 5-10 mM
    K+ 5 mM 140 mM
    Cl- 110 mM 10 mM
    Ca2+ (free) 1.2 mM 100 nM

    When ion channels are opened in neural cell membranes, the direction of favorable thermodynamic flow is down a concentration (chemical potential) gradient but the direction is also affected by the transmembrane potential.  Typical resting potentials of neural cells are about -60 to -70 mV (negative inside).  If a nonspecific cation channel is gated open, the kinetic barriers to diffusion are relieved and  at that moment Na+ ions would flow in due to both the chemical and electrical potential, while Kions would flow out but with less driving forces since its efflux is hindered by the negative transmembrane potential.  How are such large gradients of these ions formed?  We'll answer that in the next section on active transport.

    Pentameric ligand-gated ion channels (pLGICs): 

    These channels play a key role in neuronal signaling.  They are ligand-gated channels.  In neural system, the ligands are neurotransmitters.  All are comprised of five monomers, which together form the functional channel with the pore formed in the center of the pentameric structure.  The subunits can be identical (homopentamer) or diffferent (heteropentamer).  All have "Cys-loop" motifs so they have been called Cys-loop receptors as well.  Examples include the mammalian nicotinic acetylcholine, serotonin (5-HT), γ-aminobutyric (GABA), glycine and glutamate receptors. 

    The figure below shows the generic structure of the pLGICs


    Allosteric modulation of pentameric ligand-gated ion channels.  Smelt, Charles L.C.; (2019) Allosteric modulation of pentameric ligand-gated ion channels. Doctoral thesis (Ph.D), UCL (University College London).  Original content in this thesis is licensed under the terms of the Creative Commons Attribution 4.0 International (CC BY 4.0) Licence ( 4.0/)  

    The monomeric structure is shown in the left.   Each contains four transmembrane helices (TM1-4).  A top-down view of the pentameric structure is shown to the right.  The pore surface forms at the interface of the central TM2 helices.   The ligand (neurotransmitter) binds to the extracellular domain with contributions from all the subunits.  On ligand binding, TM2 and TM3 rearrange to allow formation of a transient pore and passive diffusion of specific ions.  

    pLGICs are incredibly interesting and pharmacological relevant.  In general, they have two different types of binding sites.

    Orthosteric sites bind ligands in the extracellular domains.  When bound, a conformational change leads to rearrangement of helices opening the pore.  The natural ligand is also called the agonist as it promotes the function (either neuron excitation or inhibition) of the ion channel.  Binding of the natural ligand/agonist opens up the channel to ion flow.  This can lead to activation or excitation of the neural cell if positive cations flow into the cell, which depolarizes the cell as the transmembrane potential becomes more positive.  Neurotransmitters that lead to this response are excitatory. Alternatively, binding of inhibitor neurotransmitters in the orthosteric site can lead to inhibition of the neural cell activation if the channel is a ligand-gated anion channel.  This hyperpolarizes (makes the transmembrane potential more negative), leading to inhibition of neural cell activation.   Inhibitors or antagonists of channel function, whose structure typically resembles at least somewhat the structure of the endogenous ligand or agonist, also bind to the orthosteric site.  

    Allosteric sites are distal to the orthosteric site.  Ligands that bind to allosteric sites also lead to conformational changes that either augment or diminish the effect of normal ligand/agonist binding by modulating ion flow through the pore.

    pLGICs are interact with analgesics and anesthetics which makes them even more interesting.

    The figure below shows two excitatory pLGICs, the 5-hydroxytryptamine (5HT) (left) and nicotinic acetylcholine (right) receptors. The ligand binds in orthosteric site in the extracellular domain (ECD), which is composed mostly of beta secondary structure.  Allosteric site are often found in the transmembrane domain.  





    adapted from Lara César O., Burgos Carlos F., Moraga-Cid Gustavo, Carrasco Mónica A., Yévenes Gonzalo E. Pentameric Ligand-Gated Ion Channels as Pharmacological Targets Against Chronic Pain,  Frontiers in Pharmacology, 11 (2020), 167. ,   Creative Commons Attribution License (CC BY)


    Likewise, the figure below shows orthosteric binding sites for GABA and glycine, as well as the binding of modulators that can bind in the TMD or, in the case of benzodiazepines in the ECD as well.



    adapted from Lara César O., Burgos Carlos F., Moraga-Cid Gustavo, Carrasco Mónica A., Yévenes Gonzalo E. Pentameric Ligand-Gated Ion Channels as Pharmacological Targets Against Chronic Pain,  Frontiers in Pharmacology, 11 (2020), 167. ,   Creative Commons Attribution License (CC BY)

    The actual mechanisms of how anesthetics work are still unclear. One theory suggests that they exert their effects through bulk changes in the lipid bilayer, as the potency of anesthetics are genearlly related to their hydrophobicity.  Most modern theories suggest that they more directly affect specific target proteins and their proximal interacting lipids in neuromembrane bilayers. The main targets of anesthetics appear to be pLGICs.  Anesthetics reduce neuron excitability and firing.  Hence you could hypothesize that they inhibit excitatory pLGICs (such as the 5HT and acetycholine receptors) and/or activate inhibitory ones such as the GABA and glycine receptors. pLGICs are pharmacological targets of many general anesthetics.  However, cases anesthetic inhibition of certain GABA channels and potentiation of nicotinic acetylcholine channels have also been observed.   

    We will explore two pLGIC, the eukaryotic nicotinic acetylcholine channel, and a prokaryotic analog, GLIC.

    Nicotinic acetylcholine channel (6cnj)

    One very interesting channel is the one involved in the nicotine addiction.  It binds nicotine (an exogenous alkaloid) and the normal endogenous neurotransmitter, acetylcholine.  Both compete for the same orthosteric binding site.  Since the binding of nicotine gates open the channel, nicotine acts as an agonist.  The similarities in their structures are illustrated in the figure below.


    The membrane protein is a ligand (acetylcholine)-gated (open-close) positive ion (Na+ or K+) channel, involved in fast neural communication (such as at the neuromuscular junction). The quaternary structure of the pentameric receptor consists of two α4 and three β2 subunits - (α4)2(β2)3.  This isoform is the most abundant in the human brain and the one involved in nicotine addiction.  The iCn3D model (6CNJ) below has two bound nicotines (spacefill) in the extracellular domain and one Na+ ion (spacefill) in the transmembrane domain containing the pore. The Na+ or K+ ions flow across the membrane down a concentration gradient in a thermodynamically favored process.

    The gold, blue and brown β2 subunits are glycosylated on Asn 143 and are shown with a Man (β4) GlcNAc (β4) GlcNAc N-linked oliosaccharide.  Nicotine is bound between two alpha-beta interfaces. One is shown between the green (alpha) and gold (beta) subunits and the other between the magenta (alpha) and blue (beta) subunits. 


    GLIC: A prokaryotic pLGIC

    This protein is a proton-gated cation channel with specificity for both Na+ and K+, which diffuse down their electrochemical gradients.  In a sense, H+s in the extracellular side act as "ligands" as the channel is opened with increasing H+ concentration (decreasing pH) on the outside of prokaryotic cells.  The protein is homologous to eukaryotic pLGICs.  Structures of the protein from Gloeobacter violaceus bound to propofol, an anesthetic, are known.  GLICs also interacts with ethanol and barbiturates as well.  Hence they serve as models to elucidate binding and effects of anesthetics.

    In contrast to eukaroytic pLGICs, the "ligand - H+" does not bind in the orthosteric site in the extracelllular domain  occupied by traditional ligands.  Rather changes in protonation states of key proton acceptors and donors in the protein lead to conformational changes analogous to those found on binding ligands to orthosteric sites on classical pLGICs.  The external pH associated with half maximal inward current, pH50 is approximately 5.1 ± 0.2. 

    Evidence suggest that when pH is lowered from 7 to 4, Glu 35 (distant from the orthosteric site), with a pKa - 5.8, becomes protonated.  It connects through other H+ acceptors and donors in the open form through a hydrogen bond network.  These include two triads of amino acids found at the interface between the extracellular (ECD) and transmembrane (TMD) domains.  R192-D122-D32 comprise a conserved "electrostatic triad".  The second is Y197-Y119-K248.  The network allows a bridging of effects starting with Glu 35 in the ECD into the transmembrane region where allosteric effectors usually interact with the protein.

    Orient the iCn3D model below with the extracellular domain (mostly beta structure) to the top and the transmembrane domain (alpha-helical) to the bottom.  Key molecular players involved in the interactions described above, from top down:

    • Glu 35 (stick, color CPK)
    • R192-D122-D32 electrostatic triad (sphere, CPK color)
    • Y197-Y119-K248 triad (stick, color magenta)
    • propofol (sphere, color CPK)

    The open form of GLIC (3P50) with bound PFL

    Propofol and another anesthetic, desflurane, bind at the same site localized in the upper part of the transmembrane domain of each of the five subunits..

    The model below show the mostly nonpolar (induced dipole-induced dipole) interactions between one of bound propofol and side chains in the TMD.  Also shown is an interaction between phosphatidylcholine and the propofol.


    Voltage-Gated Ion Channels

    In contrast to pentameric ligand-gated ion channels, which require 5 monomeric subunits to aggregate into a quaternary structure to form a pentameric pore, voltage-gated ion channels can form a channel from an aggregate of monomeric proteins, each containing a single 6 transmembrane helical unit, or from a longer polypeptide containing multiple repeating 6 transmembrane helical units.  

    The figure below shows a cartoon of a common voltage-gated K+ channel.  The monomer (top), denoted as the α subunit, contains a transmembrane domain containing 6 helix segments.  Four of these monomers aggregate to form the actual homo- or heterotetrameric channel (bottom).


    The genes for the Kchannel family, which facilitate K+ diffusion across the membrane, encode α subunits of approximately 500 amino acids and a molecular weight of about 57,000.  Four these α subunits come together in the membrane to form the functional channel, a tetramer of α subunits, which together make one central pore.  The α subunit can from homo- or heterotetramers, since there are different α subunit encoding genes. In additional the functional channel has smaller, regulatory β subunits as well.

    A cartoon structure of a typical voltage-gated Na+ channel is shown in the figure below.  It is a single polypeptide (α) chain that contains 4 sequential repeats of the 6 transmembrane helical segments (I-IV).  The functional channel (bottom) has just one polypeptide chain.


    adapted from

    The Na+ channel has a molecular weight of around 229K and about 2000 amino acids (each 4x that of the K+ channel α subunit).  It is glycosylated and subjected to multiple post-translational modifications.  Usually the protein in the central nervous system is a complex of the the α subunit, and small additional regulatory β subunits, which modify the kinetics and voltage-dependency of the α subunit channel.

    Segment (helix) 4 of each of the four repeat units illustrated above is the conserved "voltage" sensor. It contains multiple charged amino acids whose disposition changes with changes in the transmembrane potential, allowing conformational changes in the protein and gating of ion flow. Each of the 4 repeating units above also contains an extracellular P-loop (labeled for I in purple) connecting helix 5 and helix 6.  


    K+ Permeation through Kv1.2 Channel

    Voltage-dependent potassium channels (Kv) have 4 subunits and can be homo- or heterotetramers.  They allow voltage-gated flow of potassium ions through the membrane.  Several obvious questions should arise. How can they be selective for K+ ions?  That is, how can the allow the larger K+ ion to passively flow through and not the smaller Na+ ions?   Secondly, how can a change in the transmembrane potential cause the channel to open or close?  That question really boils down to how a change in transmembrane potential can change the conformation of proteins.

    Here figure below shows a simplified view of the rat Kv1.2 channel (3lut) from top and side views (without parts of the cytoplasmic domain), showing each of the 4 identical monomeric subunits in a different color.  Each monomer has S1-S6 transmembrane segments.  The protein is found in brain and central neuron plasma membranes and also in the cardiovascular system.  K+ ions diffuse through the center from the extracellular to intracellular side down a concentration gradient but potentially against the transmembrane potential.  The four monomers in the homotetramer from one central ore.. (Image made from



    Here is a link to a rotatable model that show the S4 voltage sensor helix in each monomer in red.

    The figure below shows a more detailed structure of the channel. The four monomer, which pack together to form the tetramer, are shown in light and dark grey to allow key residues highlighted in color to stand out.



    The left images show the channel from the side  (top left view) and top (bottom left view).  The right images shown just one of the monomers with different side chains highlighted.  

    Here is an iCn3D model of the Kv1.2 channel

    See this link for a more detailed view using iCn3D,

     K+ selectivity -  All potassium ion channels, even if not voltage gated, solved the selectivity dilemma in the way.  All have in the narrowest part of the pore in the center of the channel this consensus sequence - Thr-Thr-Val-Gly-Try-Gly (TTVGYG) - which is found in the P-loop.  These are shown in gold and brown colors in the figure above.  The -OHs in the electivity filter can interact with a dehydrated K ion but not with a dehydrated Na ion, which can not approach close enough to form significant interactions.  Surrounding the filter are twelve aromatic amino acids which constrain the size of the pore opening.  The interactions of the filter O's with the K ion makes up for the energetically disfavored dehydration of the ion.   The filter contains K+ ions which repel each other,  assisting in the vectorial discharge of the ions through the membrane.  These ions must form weak interactions with the selectivity filter.  The actual pore is mostly hydrophobic, which facilitates flow-through of the ions. 

    The figure belows shows a close up of the selectivity filter.  Four Thr 374s (second Thr in the selectivity filter sequence of TTVGYG) from the four different monomers in the channel are clearly shown interacting with the top K+ ion (gray sphere).


    Here is an iCn3D model link showing the interactions:

    Different voltage-gated ion channels alter ion selectivity through changes in these amino acids in the P-loop, as illustrated in the table below. As channels loose specificity of K+, they gain specificity for Na+ and Ca2+. Red highlights denote conserved residiues, and yellow chemically similar.

    sequence specificity
    TVGYG strong K+ channels
    CIGYG weak K+, HCN channels
    TVGDG TRP channels
    STFEG ionotropic gluamate receptors
    LCGEW strong Ca2+ voltage gated channels

    Voltage gating

    Helix S4 in each monomer in the transmembrane domain of the complex is the voltage sensor. The sequence of this helix is LAILRVIRLVRVFRIFKLSRH.  Note the arginines and lysine highlight in blue.  They repeat every 3 amino acid.  The voltage-sensor domain must be shielded from the nonpolar acyl of the bilayer.  Four conserved Arg resides on S4, part of the voltage-sensor domains, and shielded form the lipids, and coupled to an amphiphilic helix running parallel to the plain of the membrane.  The arginines  move under the influences of forces arising from changes in the membrane's electric field initiated by ion movement through other ion channels in the membrane.  Mechanical work is done by the electric field on the voltage sensor as the charged Arg residues are moved through the electric field.  The movement is coupled through the amphilic helix to the pore which changes conformation.  In turn, the S4 and coupled S5 helices of the voltage sensor do mechanical work on the pore by altering its conformation to open/close the pore, specifically at the activation gate of the pore.  This seems quite similar to how iron movement into the heme plane in hemoglobin on oxygenation pulls the proximal His on the F8 helix which then transmits a conformation change to other helices in the subunit, leading to cooperative conformational changes in the tightly packed protein.  About 12 charges move across the transmembrane potential field.

    Channels, once open, must be inactivated.  In the case of the voltage-gated potassium channel, inactivation occurs when the amino-terminal cytoplasmic domain binds to the potassium pore on the cytoplasmic side, in interaction likened to the binding of a "ball on a chain" (the cytoplasmic domain) to the pore opening.  The chain acts to tether the ball domain so it may swing to bind to the pore opening.  The ball domain contains both positively charged and hydrophobic regions.  Where is the ball domain in the absence of inhibition?  Recent studies (Oliver et al.) have shown that a positive domain can bind to proximal phosphatidyinositol 4,5-bisphosphate (PIP2) lipids on the inner leaflet of the membrane bilayer.  When so bound, inactivation of the channel is prevented.  As you will see in the next section, PIP2 can also be cleaved to form diacylglycerol and inositol 1,4,5-trisphosphate when cells are activated byexternal factors (hormones, growth factors, etc) in the process of signal transduction.  


    iconChime.gifUpdated Mammalian Voltage-Dependent Shaker Family Potassium Channel  Jmol14 (Java) |  JSMol  (HTML5)

    Here is a molecular dynamics simulation showing K+ interaction with the channel lining and the "knock-on" mechanism showing how an incoming K+ ion can repel a K+ ion in the pore through the channel.


    Lipid-Gated Ion Channels

    Membrane receptors are in the lipid bilayer, so it should not be too surprising that specific lipids might bind and trigger conformational changes in the receptor, mediating a specific biological activity.  The specific lipid might form during an upstream event, then bind to the receptor triggering function in a process of signal transduction, which we will explore in the next chapter.  Let's looks at receptors gated by binding of the lipid phosphatidylinositol bisphosphate (PIP2).  It is found in small concentrations in membranes and can be cleaved in by phospholipase C to form the a small polar intracellular signaling molecule, IP(discussed in Chapter 12).  PIP2 can also recruit proteins to the membrane and participate in signaling event that way.  For this section, we will discuss how it binds to a K+ ion channel protein and gate it open so K+ can flow into cells (the opposite direction of the normal efflux), which helps control transmembrane potential.  

    Kir2.2 -Inward rectifier potassium channel Kir2.2 

    The names of this channel can best understood if you understand the meaning of the word rectify.  The verb has several meanings but for us the best definition is to correct.  What does this channel correct?  When is it functional? We'll explore the details more in the next chapter we first a better understanding of what happens to the actual Na+ and K+ ion concentrations outside and inside the cell during neural activation.  How much do they change?  We need this to understand the driving force for the Kir2.2 channels that move  Kinto the cell, the opposite direction from normal.  From that sense, it is "rectifying" the Kconcentrations.  . 

    What happens to the actual concentrations of Na+ and K+ ions when a neuron is excited? 

    When a neural cell is activated or fires, the cell membrane potential goes from a resting potential of around -60 to -70 mV (inside negative ) to a more positive potential as Na+ ions enter the cell through voltage-gated Na+ channels (after an early neurotransmitter-gated ion channel is open after ligand binding) with the ions flowing down a chemical and electric potential gradient.  At a certain membrane potential (about +30 mV), K+ channels open allowing an efflux of K+, also down both a chemical and electric potential gradient, returning the cell potential close to its equilibrium value  potential of around -60 to  -70 mV (inside negative).   But how much do the actual K+ and Na+ ion concentrations change in this process?  The answer, which is somewhat counter intuitive, is hardly any at all!   

    We need to understand how the membrane acts as a capacitor first.  The charge Q on a surface of a plate or side of a membrane is proportional to the voltage across the plate or membrane.   The figure below shows how a membrane with a transmembrane potential acts as a capacitor.  The dielectric medium in the capacitor will determine how quickly the charges on the plate will dissipate.  When the medium is an insulator, resistant to charge flow, the plates remained charged longer.  The same is true for the membrane.  The hydrophobic bilayers acts as an insulator and resists discharge of the membrane potential.  The bilayer offers high resistance (low conductance) to charge flow.  Only when channels are open and the ions become reasonably permeable to flow does the membrane potential change over short time periods.  The following derivation is adapted.


    after BY: Attribution

    It makes sense that the stored charge (Q) on either side of the membrane is proportional to the membrane voltage. We can write the following simple equations:

    Q \propto V \\
    Q=\mathrm{C} V

    where C, the proportionality constant, is the capacitance with units of the Faraday (which you remember from introductory chemistry).  Let's normalize this equation for an area of 1 cm2.  The measured capacitance of lipid bilayers is about 10-6F/cm2.  Let's assume a voltage change from -70 mV to + 30 mV for a total of 0.1 V.  Hence

    Q=\frac{10^{-6} \mathrm{~F}}{\mathrm{~cm}^{2}}(0.1 \mathrm{~V})=\frac{10^{-7} \mathrm{Coul}}{\mathrm{cm}^{2}}

    Let's change that into the number of elementary charges on the surface of the membrane per μm2 surface area.

    \left(\frac{10^{-7} \mathrm{Coul}}{1 \mathrm{~cm}^{2}}\right) x\left(\frac{1 \text { ion }}{1.6 \times 10^{-19} \mathrm{Coul}}\right)=\frac{6.25 \times 10^{11} \text { ions }}{\mathrm{cm}^{2}} \times \frac{1 \mathrm{~cm}^{2}}{10^{8} \mu \mathrm{m}^{2}}=\frac{6,250 \text { ions }}{\mu \mathrm{m}^{2}}

    What does this mean for an ordinary eukaryotic cell?  Let's model the cell as a sphere with a diameter of 10 μm.  

    Knowing the equations for the volume (V = (4/3)πr3) and surface area (4πr2),  the volume of 10 μm cell is about 524 μm3 and the surface area  is 314 μm2. The table below shows the resting ion concentrations in a cell and the actual number of ions in the 524 μm3 volume of the cell (column 3). 

    Using the calculated value of 6250 ions moved/μm2, the total number of Kand accordingly Na+ ions that move across 314 μmof total cell membrane surface area is about 2 millon.  The results are shown in the table below.

    1.  ion 2.  [ion]intracellular (mM) 3.  # ionsintracellular 4.  total ions moved during neuron response 5.  change in [ion]intracellular
    sodium 10 mM 3.2 × 109 Na+  ~ 2,000,000 in on depolarization    ~6.3 x 10-2 mM
    (~0.6% change)
    potassium 150 mM 4.7 × 1010 K+ ~ 2,000,000 out on repolarization    ~6.3 x 10-2 mM
    (~0.6% change)


    Since the cell has an easily defined volume, we can now calculate Δ[Na+]intracellular (column  5 above) on neural activation by simple dimensional analysis as shown in the expression below, knowing the 1 L = 0.001 m3 = 1015 μm3 

    \frac{2 \times 10^{6} \mathrm{Na}^{+} x\left(\frac{1 \mathrm{~mol} \mathrm{Na}^{+}}{6.022 \times 10^{23} \mathrm{Na}^{+}}\right)}{524 \mu M^{3} \times\left(\frac{1 \mathrm{~L}}{10^{15} \mu M^{3}}\right)}=6.3 \times 10^{-6} \mathrm{M}=6.3 \times 10^{-3} \mathrm{mM}

    The actual change in intracellular Na+ ion concentration on excitation is only about a 0.6% of the initial [Na+]intracellular on excitation and depolarization of the cell.  We can also assume that the K+ ion changes to the same degree in repolarization.  So when the Na+ and K+ channels open, the "flood gates" are not opened.  Permeability does increases, but this leads to a tiny influx of  Na+ ions, which is not sufficient to really change the intracellular Na+ concentration.  It is, however, enough to change the transmembrane potential! It's a misconception that there are significant changes in ion concentration across the membrane on depolarization and repolarization of the cell.  The Goldman-Hogdkins-Katz equation (see secton xx), shows that the membrane potential is a function of both concentrations and permeability coefficients.

    Now we can present the inward rectifying potassium channels, which facilitate movement of K+ into the cell from the outside.  This is in the opposite direction for the usual flow of the ions.  Since the ions are moving towards higher levels of K+ inside the cell, it would appears this would be an example of either passive diffusion favored only by the electrical potential or a case of active transport.  None of these is true.  K+ ions diffuse from outside to inside the cell since outward diffusion is substantially block by molecules such as polyamines and Mg2+!  We don't have to invoke active transport or a violation of the basic rules of thermodynamics. The channels thus displays strong inward currents and weak outwards ones.

    The channels allow a large conduction of K+ ions if the membrane potential is more negative compared to the resting K+ ion equilbrium potential but less if more positive, so the net effect is to maintain the resting K+ potential. 

    There are several subfamilies of Kir channel.  They are always potential active (open) except those gated by G-proteins (see next chapter) or by ATP binding.  (these are involved in metabolism). Kir activity is regulated by phospholipids and proteins.  Now we will explore the Kir 2.2 channel, which is gated-open by PIP2, a membrane lipid, not by changes in the transmembrane potential.  Yet by opening this channel and allowing inward flow of K+ ions, PIP2 is regulating the transmembrane potential. It is the agonist for the Kir 2.2 channel.

    Instead of having monomeric units with S1-S6 transmembrane helical segments with a voltage sensor (S4) and P loop and S5-S6 selectivity filter, it has just 2 transmembrane helices. Both the N- and C-termini are in the cytoplasm, connected by an extracellular loop (H5) which helps form the prototypical K+ selectivity filter with the consensus sequence T-X-G-Y(F)-G.  Similar to the voltage-gated K+ channel, four of these aggregate to form homo- or heterotetramers in the membrane.  The figure below illustrates these points.


    The proteins have large intracellular domains (ICD). On binding of PIP2 to the region between the transmembrane and ICD, which produces a large conformational change, allowing K+influx.   The model below shows the R186A mutant tetrameric Kir 2.2 channel (3SPG) with four bound PIP2 analogs containing two short fatty acids (octanol) esterified to the glycerol backbone.  There appear to be two binding sites for lipids, a nonspecific site in the TMD and a specific one for PIP2 in the ICD. 


    Here is an animation that shows the monomericprotein morphing from the apo state (without PIP2, 3JYC) to the PIP2 bound state (3SPI).  


    Another PIP2-gated ion channels is the transient receptor protein (TRP) channel. These channels play a role in vascular tone.  Smooth muscle cells have TRPC3 and TRPC6 channels that are Na+ or Ca2+ channels that cause depolarization, leading to smooth muscle contraction and vasoconstriction.  


    Mechanosensitive channels

    We saw in the previous chapter than some pores (not channels) are gated open not by voltage, or specific agonist such as neurotransmittors or even specific lipids like PIP2 but by more general changes in membrane bilayers properties (membrane tension, curvature, pressure).  Likewise specific channels protein can be gated by changes in the physical properties of the bilayer.  We will consider one mechanically-active channel, TRAAK. e 


    TRAAK - Potassium channel subfamily K member 4:  

    The protein is a  K+ ion channel that is not sensitive to voltage changes but is open on mechanical deformation of the bilayer.  The channel can be opened by making the cytoplasm basic, raising the temperature.  It is involved in pain sensation and pressure transduction.  The TRAAK 4 opening is blocked by the presence of a lipid from the inner leaflet which occludes the pore.  If the lipid is removed by physical changes, transmembrane helix 4 rotates, which prevents the lipid from blocking the channel, which opens.  Further changes in the coupled transmembrane helices 2 and 3 stabilize the opening.  

    Here is an iCn3D model of the closed form of the TRAAK channel protein (4wff) in the closed state.  It binds 



    The K+ ions are aligned in the channel. Decane, a nonpolar molecule, is shown in spacefill and colored cyan.  The decane is probably decanoic acid in which the carboxyl group was not defined in the structure due to high flexibilty.  This suggests that the "decanoioc acid" is not tightly bound.  It binds through the cytoplasmic side through an opening in the membrane protein.  In the open state, transmembrane helix 4 rotates, blocking access to the cavity.  Hence lipid bind gates closed the channel.

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