| ATP Inhibition and Rectification of a Ca-Activated Anion Channel in Sarcoplasmic Reticulum of Skeletal Muscle Biophysical Journal, Volume 74, Issue 5, 1 May 1998, Pages 2335-2351 Gerard P. Ahern and Derek R. Laver Abstract We describe ATP-dependent inhibition of the 75–105-pS (in 250mM Cl) anion channel (SCl) from the sarcoplasmic reticulum (SR) of rabbit skeletal muscle. In addition to activation by Ca and voltage, inhibition by ATP provides a further mechanism for regulating SCl channel activity in vivo. Inhibition by the nonhydrolyzable ATP analog 5′-adenylylimidodiphosphate (AMP-PNP) ruled out a phosphorylation mechanism. Cytoplasmic ATP (∼1mM) inhibited only when Cl flowed from cytoplasm to lumen, regardless of membrane voltage. Flux in the opposite direction was not inhibited by 9mM ATP. Thus ATP causes true, current rectification in SCl channels. Inhibition by cytoplasmic ATP was also voltage dependent, having a of 0.4–1mM at −40mV (Hill coefficient ∼2), which increased at more negative potentials. Luminal ATP inhibited with a of ∼2mM at +40mV, and showed no block at negative voltages. Hidden Markov model analysis revealed that ATP inhibition 1) reduced mean open times without altering the maximum channel amplitude, 2) was mediated by a novel, single, voltage-independent closed state (∼1ms), and 3) was much less potent on lower conductance substates than the higher conductance states. Therefore, the SCl channel is unlikely to pass Cl from cytoplasm to SR lumen in vivo, and balance electrogenic Ca uptake as previously suggested. Possible roles for the SCl channel in the transport of other anions are discussed. Abstract | Full Text | PDF (358 kb) |
| A Large-Conductance Anion Channel of the Golgi Complex Biophysical Journal, Volume 83, Issue 1, 1 July 2002, Pages 278-289 Roger J. Thompson, Mark H. Nordeen, Kathryn E. Howell and John H. Caldwell Abstract An acidic lumenal pH is vital for the proper posttranslational modifications and sorting of proteins and lipids from the Golgi complex. We characterized ion channels present in Golgi fractions that have been cleared of transiting proteins. A large conductance anion channel was observed in ∼30% of successful channel incorporations into the planar lipid bilayer. The channel, GOLAC-2, has six levels (one closed and five open). The open states are each ∼20% increments of the maximal, 325 pS conductance. The channel was ∼6 times more selective for Cl over K. Binomial analysis of percent occupancy for each conducting level supports the hypothesis of five independent conducting pathways. The conducting levels can coordinately gate because full openings and closings were often observed. Addition of 3 to 5mM reduced glutathione to the chamber caused dose-dependent increases in single channel conductance, indicating that the channel may be regulated by the oxidation-reduction state of the cell. We propose that GOLAC-2 is a co-channel complex consisting of five identical pores that have a coordinated gating mechanism. GOALC-2 may function as a source of counter anions for the H-ATPase and may be involved in regulating charge balance and membrane potential of the Golgi complex. Abstract | Full Text | PDF (474 kb) |
| Ligand binding to heme proteins: II. Transitions in the heme pocket of myoglobin Biophysical Journal, Volume 65, Issue 4, 1 October 1993, Pages 1496-1507 J.R. Mourant, D.P. Braunstein, K. Chu, H. Frauenfelder, G.U. Nienhaus, P. Ormos and R.D. Young Abstract Phenomena occurring in the heme pocket after photolysis of carbonmonoxymyoglobin (MbCO) below about 100 K are investigated using temperature-derivative spectroscopy of the infrared absorption bands of CO. MbCO exists in three conformations (A substrates) that are distinguished by the stretch bands of the bound CO. We establish connections among the A substates and the substates of the photoproduct (B substates) using Fourier-transform infrared spectroscopy together with kinetic experiments on MbCO solution samples at different pH and on orthorhombic crystals. There is no one-to-one mapping between the A and B substates; in some cases, more than one B substate corresponds to a particular A substate. Rebinding is not simply a reversal of dissociation; transitions between B substates occur before rebinding. We measure the nonequilibrium populations of the B substates after photolysis below 25 K and determine the kinetics of B substate transitions leading to equilibrium. Transitions between B substates occur even at 4 K, whereas those between A substates have only been observed above about 160 K. The transitions between the B substates are nonexponential in time, providing evidence for a distribution of substates. The temperature dependence of the B substate transitions implies that they occur mainly by quantum-mechanical tunneling below 10 K. Taken together, the observations suggest that the transitions between the B substates within the same A substate reflect motions of the CO in the heme pocket and not conformational changes. Geminate rebinding of CO to Mb, monitored in the Soret band, depends on pH. Observation of geminate rebinding to the A substates in the infrared indicates that the pH dependence results from a population shift among the substates and not from a change of the rebinding to an individual A substate. Abstract | PDF (1189 kb) |
Copyright © 1996 The Biophysical Society. All rights reserved.
Biophysical Journal, Volume 70, Issue 1, 264-280, 1 January 1996
doi:10.1016/S0006-3495(96)79568-1
Research Article
F. Qin, A. Auerbach and F. Sachs
We present here a maximal likelihood algorithm for estimating single-channel kinetic parameters from idealized patch-clamp data. The algorithm takes into account missed events caused by limited time resolution of the recording system. Assuming a fixed dead time, we derive an explicit expression for the corrected transition rate matrix by generalizing the theory of Roux and Sauve (1985, Biophys. J. 48:149–158) to the case of multiple conductance levels. We use a variable metric optimizer with analytical derivatives for rapidly maximizing the likelihood. The algorithm is applicable to data containing substates and multiple identical or nonidentical channels. It allows multiple data sets obtained under different experimental conditions, e.g., concentration, voltage, and force, to be fit simultaneously. It also permits a variety of constraints on rate constants and provides standard errors for all estimates of model parameters. The algorithm has been tested extensively on a variety of kinetic models with both simulated and experimental data. It is very efficient and robust; rate constants for a multistate model can often be extracted in a processing time of approximately 1min, largely independent of the starting values.