1997
DOI: 10.1016/s0006-3495(97)78258-4
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Probing the outer vestibule of a sodium channel voltage sensor

Abstract: The second and third basic residues of the S4 segment of domain 4 (D4:R2 and D4:R3) of the human skeletal muscle Na+ channel are known to be translocated from a cytoplasmic to an extracellular position during depolarization. Accessibilities of individual S4 residues were assayed by alteration of inactivation kinetics during modification of cysteine mutants by hydrophilic methanethiosulfonate reagents. The voltage dependences of the reaction rates are identical for extracellular application of cationic methanet… Show more

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Cited by 74 publications
(75 citation statements)
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“…The narrow region of focused membrane electrical field at the hydrophobic constriction site is highlighted by orange bars. models, the transmembrane electrical potential would drop across a short stretch of the gating pore, which was predicted from studies showing a focused electric field near the center of the VSD (44)(45)(46)(47)(48). We consider the focused electrical field to drop primarily across the HCS, which forms a hydrophobic seal of 5-6 Å thickness just above the center of the VSD (Fig.…”
Section: Conformational Changes In the Voltage-sensing Domain Duringmentioning
confidence: 99%
“…The narrow region of focused membrane electrical field at the hydrophobic constriction site is highlighted by orange bars. models, the transmembrane electrical potential would drop across a short stretch of the gating pore, which was predicted from studies showing a focused electric field near the center of the VSD (44)(45)(46)(47)(48). We consider the focused electrical field to drop primarily across the HCS, which forms a hydrophobic seal of 5-6 Å thickness just above the center of the VSD (Fig.…”
Section: Conformational Changes In the Voltage-sensing Domain Duringmentioning
confidence: 99%
“…In contrast, the rate of MTSET ϩ modification of the simple thiol 2-mercaptoethanol in solution is only 12.5-fold faster than the rate with MTSES Ϫ (Table 2). To factor out the intrinsic differences in the reactivity of the two reagents, we divided the ratio of the rates of the two reagents at an introduced cysteine by the ratio of the rates for the two reagents with mercaptoethanol (Stauffer and Karlin, 1994;Cheung and Akabas, 1997;Yang et al, 1997). For ␤ 2 K213C, the ratio of ratios is ϭ 80/12.5 ϭ 6.4 and for ␤ 2 K215C, ϭ 43/12.5 ϭ 3.4.…”
Section: Mtsetmentioning
confidence: 99%
“…We can estimate the effective electrostatic potential at an introduced cysteine by using the following equation: ϭ Ϫ(1/ z MTSET Ϫ z MTSES )(RT/F )ln(), where z is the unitary charge of the MTS reagent, R is the gas constant, T is absolute temperature, F is Faraday's constant, and is the ratio of ratios calculated above (Stauffer and Karlin, 1994;Yang et al, 1997;Karlin and Akabas, 1998). The calculated negative electrostatic potentials at ␤ 2 K213C and ␤ 2 K215C in the resting state are Ϫ24 and Ϫ15 mV, respectively.…”
Section: Mtsetmentioning
confidence: 99%
“…Fluorescent labeling of introduced cysteine residues has been used to study conformational changes of ion channels [1,2]. However, this method is not easily applicable to proteins that contain many endogenous cysteine residues, or to the study of intracellular conformational changes.…”
Section: Introductionmentioning
confidence: 99%