scholarly journals K+ in a Kv1.2 Channel Pore: Hydration, Selectivity, and the Role of a Conserved Threonine

2019 ◽  
Author(s):  
A. M. Kariev ◽  
M. E Green

ABSTRACTQuantum calculations describing transport of K+ through a Kv1.2 channel cavity, plus the lower half of the selectivity filter (SF), show hydration in the pore and cosolvation by threonine at the entrance to the SF. Comparison to calculations on Na+ ions gives the probable selectivity mechanism. A single K+ ion is calculated at five positions in its course through the cavity, and two ions calculated at three positions at the entrance to the SF. Three Na+ pairs of ions were also calculated, and one shows how an ion is trapped asymmetrically, tightly held by two threonine −OH, and with a water tightly bound ahead of it, so that overall it has a major barrier to advancing, while K+ advances with minimal barriers. In the cavity below the SF, the ion passes in a hydrated state through pore water, between the intracellular gate and the SF, until it is cosolvated by the threonines at the selectivity filter entrance. These calculations show how the ion associates with the water, and enters the SF. A characteristic arrangement of four water molecules adjacent to the SF in the KcsA channel, shown in earlier work, is now found in Kv1.2. A single ion passing through the channel cavity is found to have an energy minimum within 1 Å of the K+ ion position in the 3Lut pdb structure of this channel. Properties (e.g. dipole moment) of the system are calculated. Charge transfer to the ion produces K+ charge 0.74 ≤ q(ion) ≤ 0.87 e, in different conditions. The calculations of pairs of Na+ and K+ ions at the SF entrance include the threonine, valine, and glycine of the conserved SF TVGYG sequence. The Na+/K+ difference shows a reason for the conservation of the threonine in producing selectivity, as the –OH groups trap Na+ but not K+.STATEMENT OF SIGNIFICANCEPotassium channels are found in all cells, and have a characteristic selectivity filter that blocks the passage of Na+ while allowing K+ to pass. These channels are implicated in many diseases. We use quantum calculations to show how the K+ ion passes from the intracellular gate of the channel, entering the channel pore, to the selectivity filter at the extracellular end of the channel; at the selectivity filter, we use comparable calculations of K+ and Na+ to show how the channel selects K+ over Na+, as well as the probable reason for the conservation of a key residue (threonine) at the base of the selectivity filter. We find properties (e.g., charge transfer, bond order) that require quantum calculations.

2005 ◽  
Vol 1 (4) ◽  
pp. 277-287 ◽  
Author(s):  
B. Collignon ◽  
P.N.M. Hoang ◽  
S. Picaud ◽  
J.C. Rayez

Clustering of water molecules on model soot particles is studied by means of quantum calculations based on the ONIOM approach. The soot particles are modeled by anchoring OH or COOH groups on the face side or on the edges of a graphite crystallite of nanometer size. The quantum calculations aim at characterizing the adsorption properties (structure and adsorption energy) of small water aggregates containing up to 5 water molecules, in order to better understand at a molecular level the role of these OH and COOH groups on the behavior with respect to water adsorption of graphite surface modelling soot emitted by aircraft.


2020 ◽  
Author(s):  
Alisher M Kariev ◽  
Michael E Green

AbstractPotassium channels generally have a selectivity filter that includes the sequence threonine-threonine-valine-glycine-tyrosine-glycine (TTVGYG). The last five amino acids are conserved over practically the entire range of evolution, so the sequence obviously is necessary to the function of the channel. Here we show by quantum calculations on the upper part of the channel “cavity” (aqueous compartment between the gate and selectivity filter) and lower part of the selectivity filter (SF) how the channel with two sets of four threonines (the channel is fourfold symmetric) effects rectification and selectivity. The threonines are at the location in which the ion transfers from the cavity into the SF; in this calculation they play a key role in selectivity. The channel is also a rectifier. The wild type channel with K+ and three other cases are considered: 1) the upper set of four threonines is replaced by serines. 2) and 3) Related computations with the Na+ and NH4+ ions help to clarify the important factors in moving the ion from the cavity to the SF. In particular, one set of angles (not bond angles, O(T373–C=O) – O(T374–OH) – H(T374–OH)) flips a hydrogen into and out of the ion path, allowing the K+ to go forward but not back. This is essentially a ratchet and pawl mechanism, with the ratchet driven by electrostatics. This also allows a clear path forward for K+ but not for Na+ or NH4+, nor for K+ in a T→S mutant. Atomic charges in the lowest positions in the SF are the driving force moving the ion forward, but the O - O - H angle just specified is key to making the “knock-on” mechanism move the ions forward only, using the ratchet with the pawl formed by the hydrogen in the bonds that flip. A water interacts with threonine hydroxyls to allow ion passage, and another water moves together with the K+.


Author(s):  
Weidong Qiu ◽  
Xinyi Cai ◽  
Mengke Li ◽  
Liangying Wang ◽  
Yanmei He ◽  
...  

Dynamic adjustment of emission behaviours by controlling the extent of twisted intramolecular charge transfer character in excited state.


2019 ◽  
Author(s):  
Alisher M Kariev ◽  
Michael Green

Quantum calculations on 976 atoms of the voltage sensing domain of the K<sub>v</sub>1.2 channel, with protons in several positions, give energy, charge transfer, and other properties. Motion of the S4 transmembrane segment that accounts for gating current in standard models is shown not to occur; there is H<sup>+ </sup>transfer instead. The potential at which two proton positions cross in energy approximately corresponds to the gating potential for the channel. The charge displacement seems approximately correct for the gating current. Two mutations are accounted for (Y266F, R300cit, cit =citrulline). The primary conclusion is that voltage sensing depends on H<sup>+</sup> transfer, not motion of arginine charges.


Symmetry ◽  
2021 ◽  
Vol 13 (4) ◽  
pp. 655
Author(s):  
Alisher M. Kariev ◽  
Michael E. Green

There are reasons to consider quantum calculations to be necessary for ion channels, for two types of reasons. The calculations must account for charge transfer, and the possible switching of hydrogen bonds, which are very difficult with classical force fields. Without understanding charge transfer and hydrogen bonding in detail, the channel cannot be understood. Thus, although classical approximations to the correct force fields are possible, they are unable to reproduce at least some details of the behavior of a system that has atomic scale. However, there is a second class of effects that is essentially quantum mechanical. There are two types of such phenomena: exchange and correlation energies, which have no classical analogues, and tunneling. Tunneling, an intrinsically quantum phenomenon, may well play a critical role in initiating a proton cascade critical to gating. As there is no classical analogue of tunneling, this cannot be approximated classically. Finally, there are energy terms, exchange and correlation energy, whose values can be approximated classically, but these approximations must be subsumed within classical terms, and as a result, will not have the correct dependence on interatomic distances. Charge transfer, and tunneling, require quantum calculations for ion channels. Some results of quantum calculations are shown.


2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Meneka Banik ◽  
Shaili Sett ◽  
Chirodeep Bakli ◽  
Arup Kumar Raychaudhuri ◽  
Suman Chakraborty ◽  
...  

AbstractSelf-assembly of Janus particles with spatial inhomogeneous properties is of fundamental importance in diverse areas of sciences and has been extensively observed as a favorably functionalized fluidic interface or in a dilute solution. Interestingly, the unique and non-trivial role of surface wettability on oriented self-assembly of Janus particles has remained largely unexplored. Here, the exclusive role of substrate wettability in directing the orientation of amphiphilic metal-polymer Bifacial spherical Janus particles, obtained by topo-selective metal deposition on colloidal Polymestyere (PS) particles, is explored by drop casting a dilute dispersion of the Janus colloids. While all particles orient with their polymeric (hydrophobic) and metallic (hydrophilic) sides facing upwards on hydrophilic and hydrophobic substrates respectively, they exhibit random orientation on a neutral substrate. The substrate wettability guided orientation of the Janus particles is captured using molecular dynamic simulation, which highlights that the arrangement of water molecules and their local densities near the substrate guide the specific orientation. Finally, it is shown that by spin coating it becomes possible to create a hexagonal close-packed array of the Janus colloids with specific orientation on differential wettability substrates. The results reported here open up new possibilities of substrate-wettability driven functional coatings of Janus particles, which has hitherto remained unexplored.


Materials ◽  
2021 ◽  
Vol 14 (13) ◽  
pp. 3497
Author(s):  
Piotr Stachak ◽  
Izabela Łukaszewska ◽  
Edyta Hebda ◽  
Krzysztof Pielichowski

Polyurethanes (PUs) are a significant group of polymeric materials that, due to their outstanding mechanical, chemical, and physical properties, are used in a wide range of applications. Conventionally, PUs are obtained in polyaddition reactions between diisocyanates and polyols. Due to the toxicity of isocyanate raw materials and their synthesis method utilizing phosgene, new cleaner synthetic routes for polyurethanes without using isocyanates have attracted increasing attention in recent years. Among different attempts to replace the conventional process, polyaddition of cyclic carbonates (CCs) and polyfunctional amines seems to be the most promising way to obtain non-isocyanate polyurethanes (NIPUs) or, more precisely, polyhydroxyurethanes (PHUs), while primary and secondary –OH groups are being formed alongside urethane linkages. Such an approach eliminates hazardous chemical compounds from the synthesis and leads to the fabrication of polymeric materials with unique and tunable properties. The main advantages include better chemical, mechanical, and thermal resistance, and the process itself is invulnerable to moisture, which is an essential technological feature. NIPUs can be modified via copolymerization or used as matrices to fabricate polymer composites with different additives, similar to their conventional counterparts. Hence, non-isocyanate polyurethanes are a new class of environmentally friendly polymeric materials. Many papers on the matter above have been published, including both original research and extensive reviews. However, they do not provide collected information on NIPU composites fabrication and processing. Hence, this review describes the latest progress in non-isocyanate polyurethane synthesis, modification, and finally processing. While focusing primarily on the carbonate/amine route, methods of obtaining NIPU are described, and their properties are presented. Ways of incorporating various compounds into NIPU matrices are characterized by the role of PHU materials in copolymeric materials or as an additive. Finally, diverse processing methods of non-isocyanate polyurethanes are presented, including electrospinning or 3D printing.


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