27 research outputs found

    310-Helix Conformation Facilitates the Transition of a Voltage Sensor S4 Segment toward the Down State

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    AbstractThe activation of voltage-gated ion channels is controlled by the S4 helix, with arginines every third residue. The x-ray structures are believed to reflect an open-inactivated state, and models propose combinations of translation, rotation, and tilt to reach the resting state. Recently, experiments and simulations have independently observed occurrence of 310-helix in S4. This suggests S4 might make a transition from α- to 310-helix in the gating process. Here, we show 310-helix structure between Q1 and R3 in the S4 segment of a voltage sensor appears to facilitate the early stage of the motion toward a down state. We use multiple microsecond-steered molecular simulations to calculate the work required for translating S4 both as α-helix and transformed to 310-helix. The barrier appears to be caused by salt-bridge reformation simultaneous to R4 passing the F233 hydrophobic lock, and it is almost a factor-two lower with 310-helix. The latter facilitates translation because R2/R3 line up to face E183/E226, which reduces the requirement to rotate S4. This is also reflected in a lower root mean-square deviation distortion of the rest of the voltage sensor. This supports the 310 hypothesis, and could explain some of the differences between the open-inactivated- versus activated-states

    Functional Imaging of Pheochromocytoma with 68Ga-DOTATOC and 68C-HED in a Genetically Defined Rat Model of Multiple Endocrine Neoplasia

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    Rats affected by the MENX multitumor syndrome develop pheochromocytoma (100%). Pheochromocytomas are uncommon tumors and animal models are scarce, hence the interest in MENX rats to identify and preclinically evaluate novel targeted therapies. A prerequisite for such studies is a sensitive and noninvasive detection of MENXassociated pheochromocytoma. We performed positron emission tomography (PET) to determine whether rat pheochromocytomas are detected by tracers used in clinical practice, such as 68Ga-DOTATOC (somatostatin analogue) or 11C-Hydroxyephedrine (HED), a norepinephrine analogue. We analyzed four affected and three unaffected rats. The PET scan findings were correlated to histopathology and immunophenotype of the tumors, their proliferative index, and the expression of genes coding for somatostatin receptors or the norepinephrine transporter. We observed that mean 68Ga-DOTATOC standard uptake value (SUV) in adrenals of affected animals was 23.3 ± 3.9, significantly higher than in control rats (15.4 ± 7.9; P = .03). The increase in mean tumor-to-liver ratio of 11C-HED in the MENX-affected animals (1.6 ± 0.5) compared to controls (0.7 ± 0.1) was even more significant (P = .0016). In a unique animal model, functional imaging depicting two pathways important in pheochromocytoma biology discriminated affected animals from controls, thus providing the basis for future preclinical work with MENX rats

    Voltage sensor activation and modulation in ion channels

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    Voltage-gated ion channels play fundamental roles in neural excitability, they are for instance responsible for every single heart beat in our bodies, and dysfunctional channels cause disease that can be even lethal. Understanding how the voltage sensor of these channels function is critical for drug design of compounds targeting neuronal excitability. The opening and closing of the pore in voltage-gated potassium (Kv) channels is caused by the arginine-rich S4 helix of the voltage sensor domain (VSD) moving in response to an external potential. In fact, VSDs are remarkably efficient at turning membrane potential into conformational changes, which likely makes them the smallest existing biological engines. Exactly how this is accomplished is not yet fully known and an area of hot debate, especially due to the lack of structures of the resting and intermediate states along the activation pathway. In this thesis I study how the VSD activation works and show how toxic compounds modulate channel gating through direct interaction with these quite unexplored drug targets. First, I show that a secondary structure transition from alpha- to 3(10)-helix in the S4 helix is an important part of the gating as this helix type is significantly more favorable compared to the -helix in terms of a lower free energy barrier. Second, I present new models for intermediate states along the whole voltage sensor cycle from closed to open and suggest a new gating model for S4, where it moves as a sliding 3(10)-helix. Interestingly, this 3(10)-helix is formed in the region of the single most conserved residue in Kv channels, the phenylalanine F233. Located in the hydrophobic core, it directly faces S4 and creates a structural barrier for the gating charges. Substituting this residue alters the deactivation free energy barrier and can either facilitate the relaxation of the voltage sensor or increase the free energy barrier, depending on the size of the mutant. These results are confirmed by new experimental data that supports that a rigid ring at the phenylalanine position is the rate-limiting factor for the deactivation gating process, while the activation is unaffected. Finally, we study how the activation can be modulated for pharmaceutical reasons. Neurotoxins such as hanatoxin and stromatoxin push S3b towards S4 helix limiting S4's flexibility. This makes it harder for the VSD to activate and might explain the stronger binding affinities in resting state. All these results are highly important both for the general topic of biological macromolecules undergoing functionally critical conformational transitions, as well as the particular case of voltage-gated ion channels where understanding of the gating process is probably the key step to explain the effects of mutations or drug interactions.QC 20121115</p

    Dynamics of the voltage-sensor domain in voltage-gated ion channels : Studies on helical content and hydrophobic barriers within voltage-sensor domains

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    Voltage-gated ion channels play fundamental roles in neural excitability and thus dysfunctional channels can cause disease. Understanding how the voltage-sensor of these channels activate and inactivate could potentially be useful in future drug design of compounds targeting neuronal excitability. The opening and closing of the pore in voltage-gated ion channels is caused by the arginine-rich S4 helix of the voltage sensor domain (VSD) moving in response to an external potential. Exactly how this movement is accomplished is not yet fully known and an area of hot debate. In this thesis I study how the opening and closing in voltage-gated potassium (Kv) channels occurs. Recently, both experimental and computational results have pointed to the possibility of a secondary structure transition from α- to 3(10)-helix in S4 being an important part of the gating. First, I show that the 3(10)-helix structure in the S4 helix of a Kv1.2-2.1 chimera protein is significantly more favorable compared to the α-helix in terms of a lower free energy barrier during the gating motion. Additional I suggest a new gating model for S4, moving as sliding 310-helix. Interestingly, the single most conserved residue in voltage- gated ion channels is a phenylalanine located in the hydrophobic core and directly facing S4 causing a barrier for the gating charges. In a second study, I address the problem of the energy barrier and show that mutations of the phenylalanine directly alter the free energy barrier of the open to closed transition for S4. Mutations can either facilitate the relaxation of the voltage-sensor or increase the free energy barrier, depending on the size of the mutant. These results are confirmed by new experimental data that supports that a rigid, cyclic ring at the phenylalanine position is the determining rate-limiting factor for the voltage sensor gating process.QC 2011061

    Dynamics of the voltage-sensor domain in voltage-gated ion channels : Studies on helical content and hydrophobic barriers within voltage-sensor domains

    No full text
    Voltage-gated ion channels play fundamental roles in neural excitability and thus dysfunctional channels can cause disease. Understanding how the voltage-sensor of these channels activate and inactivate could potentially be useful in future drug design of compounds targeting neuronal excitability. The opening and closing of the pore in voltage-gated ion channels is caused by the arginine-rich S4 helix of the voltage sensor domain (VSD) moving in response to an external potential. Exactly how this movement is accomplished is not yet fully known and an area of hot debate. In this thesis I study how the opening and closing in voltage-gated potassium (Kv) channels occurs. Recently, both experimental and computational results have pointed to the possibility of a secondary structure transition from α- to 3(10)-helix in S4 being an important part of the gating. First, I show that the 3(10)-helix structure in the S4 helix of a Kv1.2-2.1 chimera protein is significantly more favorable compared to the α-helix in terms of a lower free energy barrier during the gating motion. Additional I suggest a new gating model for S4, moving as sliding 310-helix. Interestingly, the single most conserved residue in voltage- gated ion channels is a phenylalanine located in the hydrophobic core and directly facing S4 causing a barrier for the gating charges. In a second study, I address the problem of the energy barrier and show that mutations of the phenylalanine directly alter the free energy barrier of the open to closed transition for S4. Mutations can either facilitate the relaxation of the voltage-sensor or increase the free energy barrier, depending on the size of the mutant. These results are confirmed by new experimental data that supports that a rigid, cyclic ring at the phenylalanine position is the determining rate-limiting factor for the voltage sensor gating process.QC 2011061

    The Conserved Phenylalanine in the K+ Channel Voltage-Sensor Domain Creates a Barrier with Unidirectional Effects

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    Voltage-gated ion channels are crucial for regulation of electric activity of excitable tissues such as nerve cells, and play important roles in many diseases. During activation, the charged S4 segment in the voltage sensor domain translates across a hydrophobic core forming a barrier for the gating charges. This barrier is critical for channel function, and a conserved phenylalanine in segment S2 has previously been identified to be highly sensitive to substitutions. Here, we have studied the kinetics of K(v)1-type potassium channels (Shaker and K(v)1.2/2.1 chimera) through site-directed mutagenesis, electrophysiology, and molecular simulations. The F290L mutation in Shaker (F233L in K(v)1.2/2.1) accelerates channel closure by at least a factor 50, although opening is unaffected. Free energy profiles with the hydrophobic neighbors of F233 mutated to alanine indicate that the open state with the fourth arginine in S4 above the hydrophobic core is destabilized by similar to 17 kJ/mol compared to the first closed intermediate. This significantly lowers the barrier of the first deactivation step, although the last step of activation,is unaffected. Simulations of wild-type F233 show that the phenyl ring always rotates toward the extracellular side both for activation and deactivation, which appears to help stabilize a well-defined open state.Funding Agencies|European Research Council|209825|Swedish Foundation for Strategic Research||Swedish Research Council||Swedish Heart-Lung Foundation||Swedish Brain Foundation||County Council of Ostergotland||Queen Silvias Anniversary Foundation||King Gustaf V and Queen Victorias Freemasons Foundation||Swedish Society for Medical Research||</p

    The Free Energy Barrier for Arginine Gating Charge Translation Is Altered by Mutations in the Voltage Sensor Domain

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    The gating of voltage-gated ion channels is controlled by the arginine-rich S4 helix of the voltage-sensor domain moving in response to an external potential. Recent studies have suggested that S4 moves in three to four steps to open the conducting pore, thus visiting several intermediate conformations during gating. However, the exact conformational changes are not known in detail. For instance, it has been suggested that there is a local rotation in the helix corresponding to short segments of a 3(10)-helix moving along S4 during opening and closing. Here, we have explored the energetics of the transition between the fully open state (based on the X-ray structure) and the first intermediate state towards channel closing (C-1), modeled from experimental constraints. We show that conformations within 3 angstrom of the X-ray structure are obtained in simulations starting from the C-1 model, and directly observe the previously suggested sliding 3(10)-helix region in S4. Through systematic free energy calculations, we show that the C-1 state is a stable intermediate conformation and determine free energy profiles for moving between the states without constraints. Mutations indicate several residues in a narrow hydrophobic band in the voltage sensor contribute to the barrier between the open and C-1 states, with F233 in the S2 helix having the largest influence. Substitution for smaller amino acids reduces the transition cost, while introduction of a larger ring increases it, largely confirming experimental activation shift results. There is a systematic correlation between the local aromatic ring rotation, the arginine barrier crossing, and the corresponding relative free energy. In particular, it appears to be more advantageous for the F233 side chain to rotate towards the extracellular side when arginines cross the hydrophobic region.Funding Agencies|European Research Council|209825|Vetenskapsradet|2010-5107|Swedish Foundation for Strategic Research||Swedish e-Science Research Center||</p
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