scholarly journals A voltage-dependent chloride channel from Tetrahymena ciliary membrane incorporated into planar lipid bilayers

1996 ◽  
Vol 1280 (2) ◽  
pp. 207-216 ◽  
Author(s):  
Chie Fujiwara-Hirashima ◽  
Kazunori Anzai ◽  
Mihoko Takahashi ◽  
Yutaka Kirino
1985 ◽  
Vol 249 (1) ◽  
pp. C177-C179 ◽  
Author(s):  
Y. Oosawa ◽  
M. Sokabe

A single cation channel from Tetrahymena cilia was incorporated into planar lipid bilayers. This channel selected for K+, Na+, and Li+ over Cl- and gluconate-, and its single channel conductance (at +25 mV) was 211 +/- 8 pS (mean +/- SE) in 100 mM K+-gluconate. The channel was not voltage dependent and may contribute to the resting K+ conductance of ciliary membrane.


1987 ◽  
Vol 89 (6) ◽  
pp. 873-903 ◽  
Author(s):  
W N Green ◽  
L B Weiss ◽  
O S Andersen

The guanidinium toxin-induced inhibition of the current through voltage-dependent sodium channels was examined for batrachotoxin-modified channels incorporated into planar lipid bilayers that carry no net charge. To ascertain whether a net negative charge exists in the vicinity of the toxin-binding site, we studied the channel closures induced by tetrodotoxin (TTX) and saxitoxin (STX) over a wide range of [Na+]. These toxins carry charges of +1 and +2, respectively. The frequency and duration of the toxin-induced closures are voltage dependent. The voltage dependence was similar for STX and TTX, independent of [Na+], which indicates that the binding site is located superficially at the extracellular surface of the sodium channel. The toxin dissociation constant, KD, and the rate constant for the toxin-induced closures, kc, varied as a function of [Na+]. The Na+ dependence was larger for STX than for TTX. Similarly, the addition of tetraethylammonium (TEA+) or Zn++ increased KD and decreased kc more for STX than for TTX. These differential effects are interpreted to arise from changes in the electrostatic potential near the toxin-binding site. The charges giving rise to this potential must reside on the channel since the bilayers had no net charge. The Na+ dependence of the ratios KDSTX/KDTTX and kcSTX/kcTTX was used to estimate an apparent charge density near the toxin-binding site of about -0.33 e X nm-2. Zn++ causes a voltage-dependent block of the single-channel current, as if Zn++ bound at a site within the permeation path, thereby blocking Na+ movement. There was no measurable interaction between Zn++ at its blocking site and STX or TTX at their binding site, which suggests that the toxin-binding site is separate from the channel entrance. The separation between the toxin-binding site and the Zn++ blocking site was estimated to be at least 1.5 nm. A model for toxin-induced channel closures is proposed, based on conformational changes in the channel subsequent to toxin binding.


Zygote ◽  
1995 ◽  
Vol 3 (3) ◽  
pp. 199-206 ◽  
Author(s):  
Pedro Labarca ◽  
Otilia Zapata ◽  
Carmen Beltrán ◽  
Alberto Darszon

SummaryFusion of purified mouse sperm plasma membranes to planar lipid bilayers resulted in the insertion of three ion channel types. They could be discerned on the basis of their selectivity, conductance, gating and voltage-dependent properties. The presence of a previously reported large, Ca2+-selective channel was confirmed. Here, it is reported that the Ca21-selective channel from mouse sperm plasmamembrane displayed a pNa+/Pk+ = 1.6 ± 0.2(n=4) and was blocked by micromolar concentrations of ruthenium red. Fusion yielded also a cation-selective channel (PNa+/Pk+ = 2.5±0.3, n=3) with a main open conductance substate of 103 pS and a smaller open substate of 51 PS(600mM K+cis/100 mM Na+trans). The channel inserted into bilayers in two stable fashions: a high-activity mode (open probability = 0.57 ± 0.02, n=3), and a low activity mode (open probability <1%, n=4). In high mode, the channel displayed bursting kinetics and burst length was voltage independent. In addition, a perfectly anion-selective channel, with a slope conductance of 83 PS (600KCI cis/100KCI trans), was identified. It displayed a high, nearly constant open probability (∼0.90)in the 0 to –80 mV range.


Glia ◽  
1995 ◽  
Vol 15 (1) ◽  
pp. 33-42 ◽  
Author(s):  
F. Noceti ◽  
A. N. Ramírez ◽  
L. D. Possani ◽  
G. Prestipino

Nature ◽  
1984 ◽  
Vol 308 (5954) ◽  
pp. 77-80 ◽  
Author(s):  
Mark T. Nelson ◽  
Robert J. French ◽  
Bruce K. Krueger

1999 ◽  
Vol 53 (1) ◽  
pp. 1-7 ◽  
Author(s):  
H. J. Kim ◽  
S. K. Han ◽  
J. B. Park ◽  
P. D. Ryu ◽  
H. J. Baek ◽  
...  

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