Potassium Channel

spinqualitylabelsall models Structure of the Potassium Channel Show:Asymmetric Unit Biological Assembly Drag the structure with the mouse to rotate   Export Animated Image   Print3D       Potassium Channels control the electric potential across cell membranes by selectively catalyzing the diffusion of K+ ions down their electrochemical gradient. K+ Channels extend across the cell membrane, a 40Å thick lipid bilayer across which ions cannot pass without assistance. Potassium homeostasis is crucial for nearly all living cells, but is particularly important for the correct function of neurons. Neurons produce electrical impulses known as action potentials, to initiate cellular communication processes like neurotransmitter release or activate intercellular processes muscle contraction. At the onset of an action potential, sodium ions flood across the plasma membrane of neurons via sodium channels. This influx of sodium ions causes the polarity of the plasma membrane to reverse, inactivating sodium channels and activating potassium channels. Potassium channels subsequently open allowing the selective diffusion of K+ ions across the plasma membrane, returning the membrane polarity to neutral. After the action potential has passed, channels recreate the high potassium concentration within the cell in preparation for the next stiumulus. Mutations in voltage-gated potassium channel KCNC3 have been linked with neurodevelopmental disorders and neurodegeneration.       Potassium channels possess two traits that are seemingly mutually exclusive. Firstly, potassium channels have exquisite selectivity, with an amazing 10,000 fold selectivity for K+ ions over sodium ions. Considering the only difference by which potassium ions can be differentiated from sodium ions is potassium ions’ 1.33Å Pauling radius vs. Sodium’s .95Å radius, the selectivity of potassium channels is remarkable. Second, despite its remarkable selectivity, potassium channels allow for the transfer of K+ ions across the cell membrane at a rate of nearly 108 per second, nearly at the diffusion rate limit. Potassium channels are able to achieve these remarkable feats due to its amazing structural architecture contains several remarkable features which not only can sense the voltage potential across a membrane, but also selectively ferry K+ ions without any outside energy expenditure.       The overall structure of the voltage gated potassium channel can be seen in the image at the left. It is comprised of 4 identical subunits and contains several key features which will be analyzed. Primarily, a transmembrane region marked between the parallel lines in the figure. This region houses the channel pore, composed of interwoven helices in a teepee conformation, the all-important “selectivity filter”, providing the channel with its remarkable 10,00 fold selectivity for K+ ions over Na+ ions and the “voltage sensor” which is uses well placed arginine and acidic residues to determine the membrane polarity and open/close the channel in response. Selectivity Filter and Pore       It is instructive to follow the path of a potassium ion as it enters the cell through the potassium channel. Upon entering the channel, the K+ ion first comes into contact with the selectivity filter. The solved structure of the potassium channel by MacKinnon et al. revealed where the channels remarkable selectivity comes from. When entering the selectivity filter, K+ ions are first dehydrated, shedding up to 8 waters. To stabilize these naked ions, **a number of carbonyl oxygens** bind the K+ ions. The **distance between** K+ ion and carbonyl oxygen is at the perfect width to accommodate K+ ions but not Na+ ions which are too small. If a Na+ ion were to lose it’s water shell, the carbonyl oxygens could not successfully stabilize it in its naked form and thus it is energetically unfavorable for a Na+ ion to enter the channel. There is room within the selectivity filter for four K+ ions. This, as it turns out, is crucial as the presence of the positive cations in close proximity to one another effectively pushes the potassium ions through the filter via electrostatic forces. This helps explain how the potassium channel can have such a rapid turnover rate. Also, the **natural polarity of the helices**, with the **carbonyl oxygens pointing down the pore**, helps drag the potassium ions through the channel quickly. When exposed to a low concentration of potassium, the channel assumes a **“low concentration” conformation** (LOW CONFORMATION STRUCCTURE) which is sealed shut.       The selectivity filter only makes up only the beginning of the **channel pore**. With the exception of the selectivity filter, the pore lining is **mainly hydrophobic**. This hydrophobic lining provides an inert surface over which the diffusing ion can slide unimpaired. Immediately following the selectivity filter is an **aqueous cavity**. K+ ions, after passing through the filter, rehydrate in this cavity, helping overcome much of the energetic difficulty of having a positively charged cation within a hydrophobic membrane. At the bottom of the 34Å pore containing transmembrane region lies a number of **aromatic residues** which help form a seal between the pore and the intracellular cytoplasm. Voltage Sensor       Channel pore opening is dependent on the membrane voltage, a characteristic that is “sensed” by the **voltage sensor**. The voltage sensor is comprised of **four helices**, S1 (Residues 161-183), S2 (221-243), S3 (254-277), and S4 (279-306). Negatively charged amino acids in the sensor are either located in the **external cluster**, consisting of Glu 183 and Glu 226, or in the **internal cluster** consisting of Glu 154, Glu 236, and Asp 259. The external cluster is exposed to solvent while the internal cluster is buried. **Phenylalanine 233** separates the external and internal clusters. The 7**positively charged residues** of the voltage sensor are located on the S4 helix. Lys 302 and Arg 305 **form hydrogen bonds** with the internal negative cluster while Arginines 287, 290, 293, 296 and 299 are **exposed to the extracellular solution**. When the voltage sensor is exposed to a strong negative electric field in the intracellular membrane, the positive gating charges shift inward with the α-carbon of Arg 290 shifting to interact with Phe 233. This shift effectively squeezes the pore shut, closing the intracellular-extracellular pathway. For a comparison see: The **Open** Channel vs. The **Closed** (1k4c like in 6c and D) Channel.       Overall, Potassium channels are remarkable structures that allow for near diffusion limit transfer of molecules with sub-angstrom specificity. Our understanding of the structure of Potassium Channels has opened up the potential for therapeutic intervention into Potassium channel related diseases.

Additional Structures of Potassium Channels

For Additional Structures, See: neurodevelopmental disorders

Additional Resources

For Additional Information, See: therapeutic intervention

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David Canner, Alexander Berchansky, Ann Taylor, Michal Harel, Joel L. Sussman