The Journal of General Physiology
Track the topics, authors and articles important to you
  Home | Help | Feedback | Subscriptions | Archive | Search | Table of Contents

This Article
Right arrow Abstract Freely available
Right arrow Full Text (PDF, 515K)
Right arrow PPT slides of all figures
Right arrow Alert me when this article is cited
Right arrow Citation Map
Services
Right arrow Email this article
Right arrow Similar articles in this journal
Right arrow Similar articles in PubMed
Right arrow Alert me to new content in the JGP
Right arrow Download to citation manager
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via CrossRef
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by Mauerer, U. R.
Right arrow Articles by Segal, A. S.
Right arrow Search for Related Content
PubMed
Right arrow PubMed Citation
Right arrow Articles by Mauerer, U. R.
Right arrow Articles by Segal, A. S.
Social Bookmarking
 Add to CiteULike   Add to Complore   Add to Connotea   Add to Del.icio.us   Add to Digg   Add to Reddit   Add to Technorati  
What's this?
J. Gen. Physiol., Volume 111, Number 1, January 1, 1998 139-160

Properties of an Inwardly Rectifying ATP-sensitive K+ Channel in the Basolateral Membrane of Renal Proximal Tubule

Ulrich R. Mauerer,* Emile L. Boulpaep,* and Alan S. Segal*Dagger

From the * Department of Cellular and Molecular Physiology, Yale University School of Medicine, New Haven, Connecticut 06520; and Dagger  Department of Medicine, University of Vermont, Burlington, Vermont 05401

    ABSTRACT
Top
Abstract
Introduction
Materials & Methods
Results
Discussion
References

The potassium conductance of the basolateral membrane (BLM) of proximal tubule cells is a critical regulator of transport since it is the major determinant of the negative cell membrane potential and is necessary for pump-leak coupling to the Na+,K+-ATPase pump. Despite this pivotal physiological role, the properties of this conductance have been incompletely characterized, in part due to difficulty gaining access to the BLM. We have investigated the properties of this BLM K+ conductance in dissociated, polarized Ambystoma proximal tubule cells. Nearly all seals made on Ambystoma cells contained inward rectifier K+ channels (gamma slope, in = 24.5 ± 0.6 pS, gamma chord, out = 3.7 ± 0.4 pS). The rectification is mediated in part by internal Mg2+. The open probability of the channel increases modestly with hyperpolarization. The inward conducting properties are described by a saturating binding-unbinding model. The channel conducts Tl+ and K+, but there is no significant conductance for Na+, Rb+, Cs+, Li+, NH4+, or Cl-. The channel is inhibited by barium and the sulfonylurea agent glibenclamide, but not by tetraethylammonium. Channel rundown typically occurs in the absence of ATP, but cytosolic addition of 0.2 mM ATP (or any hydrolyzable nucleoside triphosphate) sustains channel activity indefinitely. Phosphorylation processes alone fail to sustain channel activity. Higher doses of ATP (or other nucleoside triphosphates) reversibly inhibit the channel. The K+ channel opener diazoxide opens the channel in the presence of 0.2 mM ATP, but does not alleviate the inhibition of millimolar doses of ATP. We conclude that this K+ channel is the major ATP-sensitive basolateral K+ conductance in the proximal tubule.

Key words: ion channelkidneypatch-clampsulfonylureaepithelia
    INTRODUCTION
Top
Abstract
Introduction
Materials & Methods
Results
Discussion
References

The ability of the renal proximal tubule to maintain homeostatic electrolyte and water reabsorption in the face of drastic changes in dietary solute and water intake and renal hemodynamics implies that transtubular ion transport is tightly regulated. Proximal tubule potassium channels, particularly in the basolateral membrane (BLM),1 play pivotal physiologic roles in the regulation of membrane voltage, potassium recycling, and ultimately in transepithelial solute and water reabsorption. That the basolateral membrane potential of a proximal tubule cell is dominated by the BLM K conductance is well established (Sackin and Boulpaep, 1983). The Na+,K+-ATPase pump in the BLM provides the energy that makes ion transport thermodynamically favorable, but continuous operation of the pump requires there be a K+ exit pathway. The BLM K conductance provides such a pathway and thus steady state intracellular K activity can be maintained in the face of large transcellular fluxes of salt and water (Sackin and Boulpaep, 1983). Since a major portion of the transcellular Na+ flux is reabsorbed across the BLM by the action of the Na+,K+-ATPase, a population of BLM K+ channels working in concert with the pump would allow K+ to recycle in a regulated fashion. Moreover, hyperpolarization secondary to the opening of BLM K+ channels enhances the driving force for electrogenic apical Na+ entry and basolateral Cl- efflux, resulting in net NaCl reabsorption.

The Ambystoma proximal tubule exhibits a large K+ conductance in the basolateral membrane (Siebens and Boron, 1987; Sackin and Boulpaep, 1981) that has been shown macroscopically to be sensitive to barium and pH. However, previous studies of the "macroscopic" BLM K+ conductance (Boulpaep, 1976) lack the resolution to distinguish whether there is one population of imperfectly selective K+ channels or a set of highly selective K+ channels coexisting with a population of nonselective cation channels. More recent "microscopic" single-channel patch-clamp studies of BLM K+ channels have shown diversity in both experimental design and findings (Tsuchiya et al., 1992; Hunter, 1991; Parent et al., 1988; Kawahara et al., 1987; Sackin and Palmer, 1987; Gögelein and Greger, 1987a, 1987b), so a clear consensus has been elusive and details of the properties and regulation are lacking.

We have now characterized the properties and regulation (see Mauerer et al., 1998) of the principal K+ channel in the BLM in a preparation of dissociated yet polarized Ambystoma proximal tubule cells (Segal et al., 1996). Inwardly rectifying, ATP-sensitive K+ channels were present in >95% of recordings from the BLM, each containing from 2 to >25 KATP channels/patch. Although the regulation of this proximal tubule BLM K+ channel is similar to that of recently cloned KATP channels in the apical membrane of the distal nephron (ROMK1 and ROMK2), there are important differences, and ROMK has not been found in the proximal tubule (Chepilko et al., 1995; Zhou et al., 1994; Lee and Hebert, 1995; Boim et al., 1995; Ho et al., 1993). The studies reported in this paper and the companion paper elucidate the properties and the regulation, respectively, of the major K+ channel underlying the BLM K conductance that is coupled to transport in the proximal tubule.

    MATERIALS AND METHODS
Top
Abstract
Introduction
Materials & Methods
Results
Discussion
References

Solutions and Drugs

The compositions of the solutions used are summarized in Table I. After titration to pH 7.5 (710A; Orion Research, Boston, MA), sucrose was added to adjust the osmolality of the solutions (3MO; Advanced Instruments Inc., Needham Heights, MA). To determine channel conductance as a function of [K+], sucrose was added to the standard pipette KCl to maintain osmolality. Chemicals used were of the highest quality and obtained from Sigma Chemical Co. (St. Louis, MO), except thallium acetate (Aldrich Chemical Co., Milwaukee, WI), diazoxide (Calbiochem Corp., La Jolla, CA), ATPgamma S, and ADP (Boehringer-Mannheim Biochemicals, Indianapolis, IN). Nucleotides were prepared fresh daily as 20-50-mM stocks in bath solution. Glibenclamide was dissolved in DMSO (100 mM stock).

                              
View this table:
[in this window]
[in a new window]
 

Table I
Solutions

Cell Preparation

Dissociated proximal tubule cells were isolated from amphibian kidneys as previously described (Segal et al., 1996). Briefly, aquatic phase Ambystoma tigrinum kept at 4°C were killed by submersion in 0.2% tricaine methanesulfonate. The kidneys were rapidly removed and placed in iced HEPES-buffered NaCl at pH 7.5 (solution a). The adventitial tissue was removed by hand dissection, and the renal tissue was cut into 1-2 mm3 pieces and incubated in collagenase-dispase (0.2 U/ml of collagenase; Boehringer-Mannheim Biochemicals) on a gyratory shaker for 60 min at 22°C. The enzyme reaction was stopped by washing with Ca2+- and Mg2+-free NaCl (solution b). The cells were then mechanically dispersed into suspension by repeated trituration, and a pellet was obtained by centrifugation at ~1,600 rpm for 3 min. Finally, the cells were resuspended in 2.5 ml NaCl (solution a) in a 35-mm culture dish, and stored at 4°C until use. The dissociated proximal tubule cells can retain their epithelial polarity for up to 14 d (Segal et al., 1996). Cells were used for experiments from 2 to 12 d after dissociation. Representative cells as seen under light microscopy (Fig. 1 A) and scanning electron microscopy (Fig. 1 B) are shown (for details of methods see Segal et al., 1996).


View larger version (106K):
[in this window]
[in a new window]
 
Fig. 1.   Dissociated Ambystoma proximal tubule cells retain epithelial cell polarity. (A) Light photomicrograph of a single dissociated Ambystoma proximal tubule cell shows distinct apical and basolateral membrane surfaces. The apical surface of these bilobated cells is the smaller lobe with a microvillar brush border. The robust cytoskeleton of these cells includes an actin-rich "waist-band" (arrowheads) between the two membrane domains that is important in retention of epithelial polarity. Giga-ohm seals can be made on both surfaces. Scale bar, 10 µm. (B and C) Scanning electron micrographs showing the sharp transition between the membrane domains and the detailed topology of the apical surface invested with its microvillar brush border, and the basolateral surface with its folds and projections. Scale bars: 10 µm in B, 1 µm in C.

Electrophysiology

A 5-µl aliquot of cell suspension in NaCl storage solution (solution a) was placed on a Cell-TakTM-coated glass coverslip in a recording chamber of our design (RC-5/25; Warner Instruments, Hamden, CT) mounted on an inverted microscope (Olympus IM; Olympus America, Inc., Melville, NY). The chamber has a bath volume of 500 µl, and solutions are perfused directly into an input multiplexer on the chamber at a gravity-driven flow rate of ~10 ml/min.

Nonadherent cells were washed off the coverslip with the recording solution (either Ca2+-free NaCl, solution c, or KCl, solution d, unless otherwise noted) and the cells were visualized under Hoffman modulation optics (Modulation Optics, Greenvale, NY). Proximal tubule cells were readily recognized by their characteristic morphology (see Fig. 1; Segal et al., 1996). An individual proximal tubule cell was selected for an experiment only if it fulfilled the following criteria (Segal et al., 1996): (a) distinctly bilobated structure, (b) clearly defined brush border sharply delimited on the apical surface, (c) relatively smooth appearing basolateral membrane, and (d) absence of large vacuoles.

Patch clamp. The standard configurations for single-channel and whole-cell tight seal patch-clamp technique (Hamill et al., 1981) were used to record channel currents from the BLM. Patch pipettes were fabricated from borosilicate glass capillaries (Warner Instruments, Hamden, CT) on a two-step puller (PP-83; Narishige Co., Ltd, Tokyo, Japan), coated with Sylgard 184TM (Dow-Corning Corp., Midland, MI) to within 200 µm of the tip, and fire-polished just before use. When filled with KCl, the open tip pipette resistance was 3-8 MOmega when placed in the initial bath solution. A hydraulic micromanipulator (Narishige) was used to guide the patch microelectrode to the BLM of the cell. High resistance giga-ohm seals (up to 50 GOmega ) were obtained on the BLM in ~75% of attempts by applying gentle suction to the pipette just after it touched the cell membrane. To achieve the whole-cell configuration, further suction was applied to rupture the cell-attached patch. Data have not been corrected for liquid-junction potentials since for most solutions they were <4 mV when measured as follows: the bath Ag-AgCl ground electrode was connected to the control KCl bath through a 3% agar bridge made of KCl pipette solution. A low resistance (<1 MOmega ) pipette filled with 3 M KCl was placed in a KCl bath and the DC offset was adjusted to 0 mV in zero current clamp. The liquid-junction potentials were measured as the voltage offset resulting when the control KCl bath was replaced by the test solution. Low [Cl] solutions in which 90% of Cl- was replaced by aspartate- had a liquid-junction potential of 13.3 mV.

Voltage-clamped membrane currents were amplified (and zero current-clamp membrane potentials were measured) with an EPC-7 patch-clamp amplifier (Medical Systems, Greenvale, NY) controlled by a PDP 11/23 computer (Digital Equipment Corp., Maynard, MA). The current (filtered at 10 kHz) and voltage outputs of the EPC-7 were digitized at 44.1 kHz using a modified pulse code modulator (501ES; Sony Corp., Tokyo, Japan), and stored on videotape (SL-HF300; Sony Corp.). Whole-cell membrane currents were also digitized at 250 samples/s (Cheshire A/D; Indec, Sunnyvale, CA) and stored directly on computer disk. Signals were monitored on an oscilloscope (205; Hameg Instruments, Inc., Frankfurt, Germany) and strip-chart recorder (220; Brush, Cleveland, OH). All experiments were carried out at room temperature (20-22°C).

Data Analysis

Current data were played back and low pass filtered at 400 Hz (902LPF eight-pole Bessel filter; Frequency Devices Inc., Haverhill, MA), digitized at 1,000 samples/s, and stored on the PDP-11/ 23. In some cases, currents were filtered at 40 Hz and digitized at 100 samples/s for current binning and averaging analysis. Datafiles were transferred to a Pentium computer (Gateway 2000, North Sioux City, SD) via Kermit (Columbia University, NY) for analysis. Custom software for data acquisition and analysis was written in our laboratory using BASIC-23, AxoBASIC 1.0 (Axon Instruments, Foster City, CA), and Matlab 4.0 (The Mathworks, Natick, MA).

Channel activity (nPo) was calculated over periods of 60-500 s as follows. The closed current level (ic) was taken as the mode of the distribution around closed events. This current was subtracted from the current of a given bin, and the difference was multiplied by the number of events in that bin. The sum of these products yields the open channel area of the histogram. nPo is given by dividing the open channel area by the single-channel current, isc. That is,
nP<SUB>o</SUB>=<FR><NU><LIM><OP>∑</OP><LL>bins</LL></LIM>[(i<SUB>bin</SUB>−i<SUB>c</SUB>)⋅(<IT>No. events</IT><SUB>bin</SUB>)]</NU><DE>i<SUB>sc</SUB></DE></FR>. (1)

For kinetic analysis, currents were filtered at a corner frequency (fc) of 2 kHz and sampled at 5,000 s-1. An event (transition) was counted each time a data point crossed the 50% level of the unitary channel current. For our recording system, the patch-clamp has a 5-kHz step response, a 5-kHz tape bandwidth, and a 2-kHz eight-pole Bessel filter, yielding an effective bandwidth (-3 dB point, fceff) of 1.74 kHz. With these settings, the "dead time" of the recording system is given by Colquhoun and Sigworth (1983), Tdead = 0.179/fceff. The "50% delay time" of the Bessel filter is T50% = 0.506/fc. For fceff = 1.74 kHz and fc = 2 kHz, Tdead = 102.8 µs and T50% = 253 µs. Therefore, events in time histogram bins <500 s were cut off. Since an event lasting 253 µs would be the margin of detection, all dwell lifetimes <253 µs would be missed events.

Open and closed dwell-time kinetics were fit to a probability density function expressed as a sum of exponentials,
f(t)=<LIM><OP>∑</OP><LL>i=1</LL><UL>n</UL></LIM><FR><NU>A<SUB>i</SUB></NU><DE>τ<SUB>i</SUB></DE></FR>⋅e<SUP>−t/τ<SUB>i</SUB></SUP>, (2)

where n is the number of open or closed states, the Ai are the relative amplitudes, and the i are time constants. This function was transformed according to x = ln(t) and logarithmically binned (Sigworth and Sine, 1987), such that
f(x)=<LIM><OP>∑</OP><LL>i=1</LL><UL>n</UL></LIM>A<SUB>i</SUB>⋅e<SUP>{(x−x<SUB>i</SUB>)−e<SUP>(x−x<SUB>i</SUB>)</SUP>}</SUP>. (3)

This function was used to fit the data using the Levenberg-Marquardt nonlinear least-squares fitting algorithm (Origin 4.0; Microcal Software, Inc., Northampton, MA) to find the appropriate set of tau 's. Note that if the errors follow a Gaussian distribution, this nonlinear least-squares method is equivalent to the method of maximum likelihood (Colquhoun and Sigworth, 1983).

Dose-response relations for a drug (D) were fitted to the Hill equation as
<FR><NU>I</NU><DE>I<SUB>max</SUB></DE></FR>=[1+<FENCE><FR><NU>K<SUB>i</SUB></NU><DE>[D]</DE></FR></FENCE><SUP>n<SUB>H</SUB></SUP>]<SUP>−1</SUP>, (4)

where I/Imax is the fractional inhibition, Ki is the concentration of drug giving 50% inhibition, [D] is the concentration of the drug, and nH is the Hill coefficient. When nH = 1, this equation reduces to the Langmuir adsorption isotherm.

In the text, the number of observations or experiments is reported, whereas n in the analysis denotes either the whole data set or the subset of total experiments in which precise quantitation could be reliably applied. In some figures, a running average (using a specified window width) of current versus time is displayed. Statistical values for the n elements are given as mean ± SEM. Student's t test was applied where appropriate.

    RESULTS
Top
Abstract
Introduction
Materials & Methods
Results
Discussion
References

Properties of the BLM K+ Channel

Overview. With [K+] = 95 mM in the patch pipette, we found the K+ channel in 551 of 559 seals made on the BLM (98.6%). This K+ channel was never detected in seals made on the apical membrane (0 of 16, 0%), consistent with our previous finding that dissociated Ambystoma proximal tubule cells retain epithelial cell polarity (Segal et al., 1996). Seals on the BLM typically contained from 2 to >25 K+ channels. Despite numerous attempts to minimize patch area using small-tipped pipettes (resistance >=  30 MOmega ), patches appearing to have one and only one channel were very infrequent (n = 4, only 0.7%).

Cell-attached patches. When cell-attached (c/a) patches were made in NaCl bath, spontaneous inward K+ currents were usually observed (95%) at 0 mV (-Vpip) command potential. By briefly switching to zero current clamp mode, the resting membrane potential (Vm) of the cell can sometimes be estimated if Rseal >> Rpatch. Using this method under these conditions, Vm averaged -37.2 ± 2.1 mV (n = 16), in good agreement with Vm -40 mV as measured by conventional impalement (Segal et al., 1996). The Vm of the dissociated cells is ~15-20 mV less than that for a cell in the intact tubule (Sackin and Boulpaep, 1983), suggesting an anion conductance exists at either the apical or basolateral membrane. Indeed, we have characterized a cAMP-activated Cl- channel in the BLM of these cells, which often appears in the same membrane patch as the K+ channel (not shown). Alternatively, the isolated cells may have acquired a nonspecific leak pathway that shunts the normally high K diffusion potential. Since the K+ and Cl- activity of the pipette solution (aPK = 0.80*[95] = 76 mM and aPCl = 0.78*[92] = 71.8 mM) is greater than the intracellular K+ and Cl- activity (aiK = 0.80*[68] = 54.4 mM and aiCl = 0.78*[20.5] = 16 mM (Sackin and Boulpaep, 1983), yielding a reversal potential (Erev) of -28.7 mV. Thus, at -Vpip = 0 mV, the inward current must be carried by K+ moving down its electrochemical gradient from the pipette into the cell.

Representative c/a current records at various command potentials are shown in Fig. 2 A, and the current-voltage (I-V) characteristic is shown in Fig. 2 B. The inward slope conductance is 22.2 ± 1.4 pS (taken from -40 to -80 mV, n = 8), and the outward slope conductance (from +20 to +80 mV) is 3.5 ± 0.1 pS (n = 5), and channel activity appears to increase with hyperpolarization (Fig. 2 A). Although the c/a I-V characteristic displays inward rectification, suggesting that the channel is an inward rectifier; under these conditions, the I-V relation would be expected to "inwardly rectify" due to Goldman-Hodgkin-Katz rectification.


View larger version (23K):
[in this window]
[in a new window]
 
Fig. 2.   The BLM K+ channel appears to be an inward rectifier. (A) Representative current records at various command potentials (-Vpip) from a cell-attached basolateral membrane patch containing at least two K+ channels. Note the increase in channel activity with hyperpolarization. The patch pipette contains 95 mM K+ (solution d) and the bath is NaCl (solution c). The dashed line represents the all channels closed (leak) current at each potential. Each open channel level is denoted by a dotted line. (B) Current-voltage relation for the BLM K+ channel for the conditions described in A. The limiting inward slope conductance is 22.2 ± 1.4 pS (n = 8) and the outward chord conductance 3.5 ± 0.1 pS (between 120 and 180 mV, n = 5). Symbols represent mean (bullet ) ± SEM (bars).

Excised patches. When BLM membrane patches were excised in the inside-out (i/o) configuration into the standard bath solutions (solution c or d), channel activity typically began to decline and then disappear. Addition of 0.2 mM ATP to the bath before or just after patch excision prevented rundown and maintained channel activity indefinitely.

Measurements of single-channel current with [K+] = 95 mM on both sides of the membrane patch (plus 0.2 mM ATP on the cytosolic side) demonstrate that the BLM K+ channel is a true inward rectifier (Fig. 3, A and B). The I-V relation in symmetrical [K+] inwardly rectifies and reverses very close to EK = 0 mV. The channel has an inward slope conductance of gamma slope, in = 24.5 ± 0.6 pS (n = 8, measured between -60 and -100 mV), and an inward chord conductance of gamma chord, in = 20.5 ± 0.4 pS (n = 8, measured between Erev = 0 and -100 mV). The outward chord conductance measured at +80 mV is gamma chord, out = 3.7 ± 0.4 pS (n = 2). The outward slope conductance between +20 and +80 mV is clearly smaller.


View larger version (24K):
[in this window]
[in a new window]
 
Fig. 3.   The BLM K+ channel is a true inward rectifier. Representative current records at various command potentials (-Vpip) from an inside-out basolateral membrane patch in symmetrical [K] containing at least three K+ channels. The patch pipette and bath each contain 95 mM K+ (solution d) with 0.2 mM ATP added to the bath. The dashed line represents the all channels closed (leak) current at each potential. Each open channel level is denoted by a dotted line. (B) Effect of [Mg2+]i on the I-V relation of the BLM K+ channel. The inward rectification evident in 1 mM [Mg2+]i (open circle ) is relieved when [Mg2+]i is lowered to 200 nM (black-square). (inset) Slope conductance-voltage (g-V) relation for the BLM K+ channel in 1 mM [Mg2+]i (open circle ) and 200 nM [Mg2+]i (black-square). Symbols represent mean ± SEM. The K+ channel prefers Tl+ over K+. The I-V relation from inside-out patches with Tl-acetate (solution g) in the pipette and K-acetate (solution h) in the bath is also shown (black-triangle). The limiting inward slope conductance is 29.0 ± 1.0 pS (n = 4) for Tl+ compared with 24.5 ± 0.6 pS (n = 8) for K+. (C) Channel activity (nPo) increases with hyperpolarization. Data from four inside-out membrane patches in symmetrical [K] are plotted. Channel activity at command potentials of -120, -100, -80, -60, and -40 mV was normalized to that at -100 mV for comparison. Solid line is a single exponential fit with a voltage constant of ~83 mV. Symbols represent mean (bullet ) ± SEM (bars).

Voltage dependence of nPo. Since BLM membrane patches almost always contained more than one K+ channel, nPo (channel activity) was used to assess the relative voltage dependence of Po. This assumes that the number of active channel proteins in an excised patch remains constant as voltage varies. (We take n as the maximum number of simultaneously open channels observed, which places a minimum on the actual number of channel proteins in the patch.) As was the case for cell-attached patches, channel activity with KCl on both sides of the excised membrane patch increases with increasing hyperpolarization (Fig. 3 C). Although the absolute values of nPo differed significantly among patches, relative nPo increased e-fold per ~83-mV hyperpolarization between -40 and -120 mV, reflecting a 27% increase of nPo for every 20 mV of hyperpolarization.

Role of magnesium. It has been shown that [Mg2+]i mediates at least part of the inward rectification in other inwardly rectifying K+ channels (Matsuda et al., 1987; Horie et al., 1987; Ficker et al., 1994) by blocking outward currents in a voltage-dependent manner. When Mg2+i was removed from the "cytosolic" side of i/o patches (solution e plus 0.2 mM Na2ATP), we observed flickering, and then rundown of the channel. This is in sharp contrast to the behavior of ROMK1 channels, in which channel rundown is slowed in a Mg2+-free bath (McNicholas et al., 1994). Since rundown occurs in the absence of free Mg2+i and the presence of 0.2 mM Na2ATP (n = 4), it appears that at least the complex of Mg-ATP is required to prevent rundown. Interestingly, it has been shown that both Mg-ATP and free Mg2+i are required to sustain channel activity for an ATP-insensitive inward rectifier K+ channel (Fakler et al., 1994). However, since higher levels of ATP block the BLM K+ channel (see below), it is not possible for us to dissociate the role of free Mg2+i from that of the Mg-ATP complex. Millimolar concentrations of ATP (or indeed, any nucleotide) block the BLM K+ channel, and this effect is independent of both free Mg2+i and Mg-ATP.

In a solution containing 368 nM Mg-ATP and 200 nM free [Mg2+]i (solution f ) (Fabiato and Fabiato, 1979), channel rundown did not occur. Although Fakler et al. (1994) showed that >10 µM free [Mg2+]i is required to prevent rundown from occurring in the Kir2.1 channel, just 200 nM free [Mg2+]i is sufficient for the BLM K+ channel. Under this condition, the outward unitary conductance of the latter increases, but the inward conductance is essentially unaffected. The enhanced outward current is ATP sensitive, as 5 mM ATP blocked 89.3 ± 6.3% (n = 3) of the current. The outward chord conductance with [Mg2+]i = 200 nM increased from 4.25 ± 0.59 pS to 14.4 ± 1.2 pS (n = 4, measured at +80 mV); inward currents were not affected by the change in [Mg2+]i (Fig. 3 B). Inward rectification was reestablished by returning bath [Mg2+]i to 1 mM.

Assuming a single-binding site, the Mg2+ block may be described using a one-site model according to Woodhull (1973):
K(V<SUB>c</SUB>)=K(0mV)⋅exp(−δV<SUB>c</SUB>zF/RT), (5)

where Vc is the command potential, z is the valence of 2, and K(Vc) and K(0 mV) are the concentrations of Mg2+ causing half-maximal block at Vc and 0 mV, respectively. The factor delta  may be the electrical distance of the binding site from the outside of the channel pore. Alternatively, delta  can be considered together with another term to yield either the equivalent valence (z) of, or the effective potential (Vc) sensed by, the Mg2+ (Hille, 1992).

Current-voltage relations from inside-out patches in symmetrical K+ for several [Mg2+]i were constructed, from which the current was normalized to that observed in a Mg2+-free bath, and the relative current was plotted against command potential for each [Mg2+]i (not shown). These data were then fitted (nonlinear least squares fitting routine) by the following function that incorporates Eq. 5:
<FR><NU>I<SUB>Mg<SUP>2+</SUP></SUB></NU><DE>I<SUB>Mg<SUP>2+</SUP>free</SUB></DE></FR>=<FR><NU>K(V<SUB>c</SUB>)</NU><DE>K(V<SUB>c</SUB>)+[Mg<SUP>2+</SUP>]</DE></FR>. (6)

The fit according to Eq. 6 yields the following results: delta  = 0.57, K(0 mV) = 7.7 mM, K(60 mV) = 0.72 mM.

Concentration and voltage dependence of isc. To further investigate the biophysical properties of this channel, we asked the question of how varying extracellular [K+] would affect the current carried by the channel. To isolate the change in [K+] from any change in driving force across the patch, the same [KCl] was used in the pipette and bath, thus clamping Erev to 0 mV. This approach allowed us to measure the change in absolute conductance while maintaining a constant relative permeability (i.e., we varied the Goldman-Hodgkin-Katz current equation while holding the result of the Goldman-Hodgkin-Katz voltage equation constant). Under these conditions, the command potential is the only driving force for net K+ movement across the membrane patch. Pipette and bath [KCl] ranged from 5 to 205 mM while osmolality was kept at 400 mosm/kg using sucrose as necessary. Since isc for [KCl] = 95 mM was the same in both standard KCl solution (solution d, 200 mosm/kg) or 400 mosm/kg KCl solution, the tonicity change itself does not significantly alter the conducting properties of the channel.

Channel events (inward current) were analyzed at command potentials of -20, -40, -60, -80, and -100 mV for [K+] = 5, 10, 20, 25, 55, 95, 155, and 205 mM, and the I-V relationship was determined for each of these KCl concentrations. Channel events for [K+] = 5 mM could not be adequately resolved and were not included in the further analysis. For each voltage, the single channel current increases with [K+] and approaches a limiting current (imax,sc). Similarly, the single channel chord conductance (gamma chord) also increases with [K+] and saturates (as shown for -100 mV in Fig. 4 A). Fitting the gamma chord versus [K+] data at -100 mV with the Hill equation:
γ=γ<SUB>max</SUB>⋅[1+(K<SUB>d</SUB>/[K<SUP>+</SUP>]<SUB>o</SUB>)<SUP>n<SUB>H</SUB></SUP>]<SUP>−1</SUP> (7)


View larger version (12K):
[in this window]
[in a new window]
 
Fig. 4.   The operating surface of the BLM K+ channel. (A) The single channel conductance (gamma ) at a command potential of -100 mV plotted as a function of [K+] and fit to the Hill equation according to γ=γ<SUB>max</SUB>⋅[1+(K<SUB>d</SUB>/[K<SUP>+</SUP>]<SUB>o</SUB>)<SUP>n<SUB>H</SUB></SUP>]<SUP>−1</SUP>⋅γ<SUB>max</SUB> is the maximal value of the conductance, Kd is the apparent dissociation constant, and nH is the Hill coefficient. For the chord conductance at -100 mV (black-square) and its least-squares fit (solid line), gamma max,slope = 34.3 pS, Kd = 77 mM, and nH = 0.94. (B) The plot of Kd versus Vpip shows that the apparent binding-unbinding rate of K+ to the channel is voltage dependent. The data (open circle ) were fit with a single exponential (solid line) as follows: Kd = 73 + 141 · exp(-Vpip/30).

yielded a Kd of 77 mM, a Hill coefficient of 0.95, and a maximum value for gamma chord (gamma max) of 36.6 pS (Fig. 4 A). Plots of gamma chord versus [K+] at different voltages yielded similar results for gamma max. The average value for gamma max determined at -60, -80, and -100 mV was 34.3 pS. gamma max,sc was the same for all command potentials fitted. Indeed, the intersection of the channel's operating surface with the I-V plane as K shows a linear conductance. This mean value for gamma max was applied to obtain Kd values and Hill coefficients for all the voltages (Table II).

                              
View this table:
[in this window]
[in a new window]
 

Table II
Kd Values and Hill Coefficients for the BLM K+ Channel

Comparison of the dissociation constants Kd for the different command potentials shows that Kd decreases with hyperpolarization (Fig. 4 B and Table II). The relationship between Kd (mM) and voltage (mV) can be described by a single exponential decay
K<SUB>d</SUB>(V)=K<SUB>d,∞</SUB>+K<SUB>d,0</SUB>⋅exp<FENCE>−<FR><NU>V</NU><DE>ψ</DE></FR></FENCE>=73+141⋅exp<FENCE>−<FR><NU>V</NU><DE>30</DE></FR></FENCE> (8)

where Kd, is the asymptotic value for Kd as Vpip right-arrow infinity bullet , Kd,0 is the difference of Kd at the reversal potential (0 mV) and Kd,infinity ·. Finally, psi  is the voltage change required to effect an e-fold change in (Kd -Kd,infinity ·).

Cation selectivity. The cation to anion preference of the total BLM conductance was determined by salt dilution experiments using i/o membrane patches. Starting in symmetrical 95 mM K+ and 94.5 mM Cl- (EK = ECl = 0 mV) and holding at -Vpip = 0 mV, the bath was changed to a 14 mM K+ and 13.5 mM Cl- solution (solution i, EK = +48.6 mV, ECl = -49.4 mV) plus sucrose to maintain isoosmolality. This maneuver resulted in large inward currents (n = 3), reflecting the cation (K+) moving down its chemical gradient. The reversal potential for this membrane current (including leak) was at least +40 mV (n = 3). While holding at this Erev, outward current developed when the 10% KCl bath was replaced with 100% KCl, due to K+ moving along its electrical gradient. Thus, the BLM conductance is cation selective.

Using the Goldman-Hodgkin-Katz voltage equation (Hodgkin and Katz, 1949; Goldman, 1943) for K+ and Cl-, the permeability ratio pK:pCl can be estimated (see MATERIALS AND METHODS):
E<SUB>rev</SUB>=<FR><NU>RT</NU><DE>F</DE></FR>ln<FR><NU>p<SUB>K</SUB>[K]<SUB>o</SUB>+p<SUB>Cl</SUB>[Cl]<SUB>i</SUB></NU><DE>p<SUB>K</SUB>[K]<SUB>i</SUB>+p<SUB>Cl</SUB>[Cl]<SUB>o</SUB></DE></FR>↔<FR><NU>p<SUB>K</SUB></NU><DE>p<SUB>Cl</SUB></DE></FR>=<FR><NU>exp<FENCE><FR><NU>E<SUB>rev</SUB></NU><DE>RT/F</DE></FR></FENCE>⋅[Cl]<SUB>o</SUB>−[Cl]<SUB>i</SUB></NU><DE>[K]<SUB>o</SUB>−exp<FENCE><FR><NU>E<SUB>rev</SUB></NU><DE>RT/F</DE></FR></FENCE>⋅[K]<SUB>i</SUB></DE></FR>. (9)

where R = 8.315 J K-1 mol-1, F = 9.648 · 104 C mol-1, T = 293 K, Erev >= +40 mV, [Cl]o = 94.5 mM, [K]o = 95 mM, [Cl]i = 13.5 mM, and [K]i = 14 mM, yielding pK: pCl of at least 17:1. Note that even a small change in Erev to +44 mV would double the selectivity ratio. It is emphasized that this value represents the minimum cation to anion preference of the K+ channel since this is the selectivity ratio of the whole basolateral membrane patch including chloride and leak conductances.

Selectivity among cations. Two approaches were used to determine the selectivity of this inwardly rectifying K+ conductance on the BLM. (a) Using c/a and i/o patches, the K+ in the patch pipette was replaced with the chloride salt of Na+ (n = 48), Rb+ (n = 4), Li+ (n = 4), Cs+ (n = 2), or NH14 (n = 7). Each solution was adjusted to pH 7.5 with the respective hydroxide salt. In all cases, c/a and i/o patches failed to show inward channel currents. These results strongly suggest that the BLM K+ channel is highly selective for K+ and excludes these cations, since channel activity is seen in >98% of seals made on the BLM when K+ is in the pipette. (b) Outside-out patches were made to exclude the remote possibility that the c/a and i/o patches used above did not contain any channels. The pipette was filled with KCl, and 0.2 mM Mg-ATP was included to prevent channel rundown. After recording in a KCl bath, the test cation was introduced into the bath (as the chloride salt) and the voltage protocol was repeated. KCl bath exchanges were interposed between test cations.

The cation selectivity as determined from outside-out patches is exemplified in Fig. 5. For Na+ and Li+, the current at -40 mV is negligible, but a modest inward current is carried by Rb+, Cs+, and NH14. Exchanging the test cation with KCl returned the ensemble currents to the control level in all cases. That the outward current carried by K+ remains essentially unchanged during each bath cation substitution indicates that the test cations do not act as channel blockers from the outside. The ensemble current obtained at Vpip-40 mV shows that the selectivity of the channel for these cations is K+ >> Rb+ approx  Cs+ approx  NH4+ > Na+ approx  Li+.


View larger version (34K):
[in this window]
[in a new window]
 
Fig. 5.   The BLM K+ conductance is highly selective for K+. The cationic selectivity of the BLM is demonstrated in this outside-out patch with KCl (solution d) + 0.2 mM ATP in the pipette and Cl-salt of the test cation in the bath. The running average of current at -40 mV shows that cationic selectivity is K+ >> Rb+ approx  Cs+ approx  NH4+ > Na+ approx  Li+. The dashed line is the zero-current line, and the dotted line is the all channels closed (leak) current at a command potential of -40 mV. The voltage protocol is indicated below the current data.

Thallium. Many types of K+ channels have been shown not only to conduct Tl+, but often better than they conduct K+ (Hille, 1992). To assess the Tl+ conductance of the BLM K+ channel, the patch pipette was filled with 90 mM Tl-acetate (solution g ; the Cl salt of Tl+ was not used due to its low aqueous permeability) and the bath was filled with K-acetate (solution h). Under these conditions, inward Tl+ currents were observed in both c/a and i/o patches. The kinetic behavior of these channel events was notably different from those seen when the channel conducts K+. When conducting Tl+, the channel openings displayed more bursting, with each opening interrupted by fast flickery closures. The probability that this is actually a different channel is low since (a) the frequency of finding the K+ channel exceeds 98%, (b) other cation-selective channels were rarely observed, (c) the disparate kinetics were only seen when Tl+ was in the pipette, and (d) Tl+ currents were sensitive to glibenclamide (see below).

The I-V relationship for this biionic condition is shown in Fig. 3 B. The limiting inward slope conductance for Tl+ was 29.0 ± 1.0 pS (measured between -60 and -100 mV, n = 4). Thus the channel conductance is slightly higher for Tl+ than it is for K+ (g*inTl: g*inK = 1.2:1). Since small inward currents were observed while holding at 0 mV in two i/o experiments with Tl+ in the pipette and K+ in the bath, the reversal potential is positive. This implies that the permeability (zero-current conductance) for Tl+ is also greater than that for K+. Therefore, compared with K+, Tl+ has a higher conductance and is more permeant but probably interacts with the pore, causing a fast channel block.

In conclusion, these findings indicate that the permeability sequence of this K+ channel is Tl+ > K+ >> Cs+ approx  Rb+ approx  NH4+ > Li+ approx  Na+ > Cl-.

Kinetics. Due to the high density of this K+ channel in the BLM, a patch apparently containing only one channel is extremely rare. In over 550 seals, only four membrane patches appeared to contain only one channel (0.7%). Since the open probability (Po) of the channel is only 0.05 ± 0.01 (n = 4), long recordings were required to accumulate enough transitions for meaningful analysis of the long closed state. Kinetic analyses from such patches show that under resting state conditions at -Vpip-60 mV, the BLM K+ channel has two apparent open states and two apparent closed states. Parameters from one c/a patch and one i/o patch show that the open dwell lifetimes are (ms): tau o1 = 0.78 (c/a), 1.21 (i/o), and tau o2 = 4.7 (c/a), 6.6 (i/o). The closed dwell lifetimes are (ms): tau c1 = 1.27 (c/a), 0.72 (i/o), and tau c2 = 397 (c/a), 502 (i/o). Fig. 6 shows the open and closed time histograms for a c/a patch.


View larger version (28K):
[in this window]
[in a new window]
 
Fig. 6.   Kinetics of the BLM K+ channel. (A) Open-time histogram for the BLM K+ channel in a cell-attached patch at -60 mV with the time intervals logarithmically binned (Sigworth and Sine, 1987). The data were fitted with two probability density functions (dashed lines) to give the overall fit (solid line), yielding time constants of tau o1 = 0.78 ms (78%) and tau o2 = 4.7 ms (22%). Based on the bandwidth of the recording system, the data and the fit were cutoff at 500 µs (vertical dotted line). (B) Closed-time histogram for the BLM K+ channel in a cell-attached patch at -60 mV with the time intervals logarithmically binned. The data were fitted with two probability density functions (dashed lines) to give the overall fit (solid line), yielding time constants of tau c1 = 1.27 ms (74%) and tau c2 = 397 ms (26%). Based on the bandwidth of the recording system, the data and the fit were cutoff at 500 µs (dotted vertical line).

Inhibitor Profile

The BLM K+ channel is inhibited by barium and glibenclamide. The channel is insensitive to tetraethylammonium (up to 10 mM) applied either to the extracellular or cytoplasmic side.

Barium. We have previously shown by recording single-cell membrane potential that the whole cell conductance is dominated by a barium-sensitive K+ conductance (Segal et al., 1996). Perforated patch whole-cell recordings show that the barium-sensitive whole cell conductance inwardly rectifies. When 2 mM Ba2+ was included in the KCl pipette solution (unpaired experiments), channel openings were rare and a flickery state was noted. In contrast to the voltage dependence of channel activity without Ba2+ in the pipette (see Fig. 3 C), steady depolarization now has the effect of increasing nPo, and subsequent hyperpolarization reduced activity. This is presumably due to the voltage dependence of the Ba2+ block of the channel (data not shown).

To quantify the Ba2+ block and use each patch as its own control, outside-out patches were made (n = 3). In outside-out membrane patches at -40 mV, Ba2+ inhibits the channel with a Ki = 460 µM (Fig. 7 A).


View larger version (28K):
[in this window]
[in a new window]
 
Fig. 7.   Inhibitors of the BLM K+ channel. (A) Dose- response curve for inhibition of the BLM K+ channel by external Ba2+. Relative nPo (nPo/nPo,control) determined from outside-out patches at a command potential of -40 mV with KCl in the pipette and bath (solution d) is plotted versus [Ba2+]. The data at -40 mV were fitted with the Hill equation (solid curve), yielding a Ki = 460 µM and nH = 0.90. The inhibition by Ba2+ is fully reversible. (B) Glibenclamide inhibits the BLM KATP channel. (top) A running average (window width 16 ms) of current versus time. Glibenclamide (500 µM) is added to the bath where indicated. (bottom) Sample traces from a representative experiment at -60 mV with KCl in the pipette and bath (solution d). Exposure of this inside-out patch to 500 µM glibenclamide reversibly decreases nPo by ~50%. The dashed line denotes the all channels closed (leak) current level and the dotted lines indicate each open channel level.

Glibenclamide. This sulfonylurea is known to inhibit ATP-sensitive K+ channels in a number of epithelial tissues by binding to the sulfonylurea receptor (SUR). SUR1 has recently been cloned (Aguilar-Bryan et al., 1995) and is thought to associate with the KATP channel, thereby conferring sulfonylurea sensitivity. However, SUR1 may not be present in the kidney (Inagaki et al., 1995), which may explain in part the much higher dose of glibenclamide required to inhibit renal KATP channels (Hebert and Ho, 1994). In this context, the BLM K+ channel is glibenclamide sensitive, albeit at "renal doses." We treated 22 patches with glibenclamide; 16 excised inside-out patches were exposed to 500 µM, while 6 cell-attached patches were exposed to low (0.01-10 µM) concentrations. In 7 of 16 inside-out patches, 500 µM glibenclamide inhibited activity by 42.3 ± 5.6% (Fig. 7 B). Remarkably, the inhibition was much more potent in the cell-attached patches: 10 µM exerted an 83 ± 2% inhibition in three patches, and 100 nM exerted a 70 ± 3% inhibition in three other patches (data not shown).

ATP Sensitivity

Similar to other KATP channels, low doses of ATP are required to prevent Ambystoma BLM K+ channel rundown, whereas millimolar doses inhibit channel activity. At a dose of 5 mM ATP, >90% of channel activity is inhibited. This effect is reversible as nPo returns to baseline when the bath [ATP] is returned to 0.2 mM (Fig. 8 A). The dose-response curve for ATP has a Ki ~ 2.4 mM (Fig. 8 B). The Hill coefficient of ~4 may suggest that the channel has a tetrameric structure, with each subunit possessing an ATP binding site. Thus, in the Ambystoma proximal tubule, the BLM K+ channel that appears to be the major K+ conductance of the cell is ATP sensitive.


View larger version (39K):
[in this window]
[in a new window]
 
Fig. 8.   Nucleotides reversibly inhibit the BLM K+ channel. (A) ATPi reversibly inhibits the BLM K+ channel in inside-out patches. In the experiment depicted, up to 13 channel open levels are seen under control conditions (top) at -60 mV with KCl (solution d) in the pipette and NaCl (solution c) plus 0.2 mM ATP in the bath. (middle) Addition of 5 mM ATP to the cytoplasmic side almost completely blocks channel activity (98% decrease) with only rare openings to one open level. (bottom) The inhibition is readily reversed upon returning to 0.2 mM ATPi. (B) Dose-response curve for inhibition by ATPi. The inhibitory effect of ATPi was determined in inside-out patches under the conditions described in A. Relative nPo (nPo/nPo,control) is plotted versus [ATP]i. The data (bullet ) was fitted with the Hill equation (solid line) yielding a Ki ~ 2.4 mM and nH = 3.95. Adenosine nucleotides and nucleoside triphosphates (each at 5 mM) inhibit the BLM K+ channel. The inhibitory effect of ATP, ADP, AMP, and adenosine was determined under the conditions described in A. Values plotted are average (nPo,test/nPo,control) SEM (n = 3-9). The rank order of inhibition is ATP (93.3%) > ADP (65.6%) > AMP (38.7%). Adenosine has no inhibitory effect on nPo of the BLM K+ channel. Although all the nucleoside triphosphates inhibit the channel, ATP exerts a significantly stronger block than the other NTPs tested (P < 0.02). There is no significant difference among the other NTPs.

Among the nucleoside diphosphates, ADP is less potent than ATP (ADP inhibits by 65.6 ± 8.1%, n = 4, P < 0.01), but more potent than CDP, GDP, IDP, TDP, or UDP (data not shown). This suggests that the putative nucleotide binding site(s) recognize NDPs as well as NTPs, and that nucleotide hydrolysis is probably not occurring at this site. Indeed, even nucleoside monophosphates have a moderate inhibitory effect, although nucleosides themselves are without effect. The relative potency of the adenosine nucleosides (at 5 mM) in inhibiting the BLM KATP channel is ATP (93.3 ± 1.9%) > ADP (65.6 ± 8.1%) > AMP (38.7 ± 3.7%) > adenosine (1 ± 2%) (Fig. 8 C, n = 3-9).

Other nucleotides. The effect of nucleotides was tested in excised i/o patches. All the NTPs tested reversibly inhibited BLM K+ channel activity at a dose of 5 mM (ATP 93.3 ± 1.9%, n = 9; CTP 70.3 ± 10.0%, n = 5; GTP 62.3 ± 7.5%, n = 3; ITP 61.1 ± 0.8%, n = 2; TTP 53.7 ± 6.7%, n = 2; UTP 71.7 ± 5.7%, n = 2) (Fig. 8 C). These results suggest that each compound probably interacts with common cytoplasmic nucleotide binding site(s). Note that ATP is significantly more potent than the other nucleoside triphosphates (P < 0.02), but there is no significant difference among the nonadenosine nucleotides.

Rundown of the BLM K+ Channel

One characteristic of KATP channels is "rundown," a gradual loss of activity when the membrane patch is deprived of cytosolic ATP (Findlay and Dunne, 1986). Typically, both Mg2+ and ATP are required to prevent rundown in KATP channels (Ashcroft and Ashcroft, 1990). Likewise, the BLM K+ channel runs down in the absence of either Mg2+ or ATP (or both). Lower concentrations of ATP (100-200 µM) will prevent or "rescue" channel rundown. The experiment shown in Fig. 9 A summarizes the characteristics of BLM K+ channel rundown. Channel activity typically begins to decrease (rundown) upon excision of the membrane patch into a nucleotide-free bath. If this process is allowed to continue, channel activity will cease, usually irreversibly. When 0.2 mM of ATP is added back, channel activity can be restored. When ATP is removed, all channels rapidly close. In the continued presence of ATP-gamma S, readdition of ATP is again able to rescue rundown, and activity returns to baseline upon washout of the ATP-gamma S. Frequently (but not invariably), ATP-gamma S has an inhibitory effect on single channel activity when added in the presence of ATP, which is reversible as long as the exposure is not prolonged (n = 6), as shown in Fig. 9 B. When ATP-gamma S is added in the absence of ATP, channel activity runs down very quickly, usually irreversibly (n = 4, data not shown).


View larger version (34K):
[in this window]
[in a new window]
 
Fig. 9.   ATP but not ATP-gamma S prevents and rescues channel rundown. Hydrolyzable nucleoside triphosphates prevent and rescue BLM K+ channel rundown. A running average (current versus time, window width 768 ms) of a representative experiment is shown. The pipette is KCl (solution d), the bath is NaCl (solution c), the command potential is -60 mV. Upon excision in a nucleotide-free bath, channel activity decreases (channel rundown). After the addition of 0.2 mM ATP to the bath, channel activity slowly recovers. The addition of 0.2 mM ATP-gamma S (a poorly hydrolyzable ATP analogue) in the continued presence of 0.2 mM ATP has no effect. However, when ATP is removed, ATP-gamma S is not able to support channel activity, which rapidly declines and runs down. Readdition of ATP leads to full recovery of channel activity. Single-channel traces showing that ATP-gamma S has an inhibitory effect on KATP channel activity in excised inside-out BLM patches. When compared with control conditions (top), the addition of ATP-gamma S (middle) reduces nPo. This inhibition is reversible as long as the exposure to ATP-gamma S is not prolonged (bottom). (C) Removal of Mg2+ does not prevent channel rundown in an ATP-free bath. The top panel shows that rundown of the BLM KATP channel upon excision into an ATP-free bath proceeds despite removal of bath Mg2+. Representative traces from the regions marked by alpha , beta , and gamma are shown at bottom.

Thus, ATP-gamma S cannot substitute for ATP in sustaining channel activity, suggesting that phosphorylation itself is not sufficient to prevent rundown. Although phosphorylation may be necessary, it appears that the nucleoside triphosphate must be hydrolyzable to maintain channel activity. This hypothesis is supported by the finding that CTP, GTP, ITP, TTP, and UTP could all prevent or rescue rundown, but the corresponding NDPs could not. Rescue does not appear to require the cAMP-dependent protein kinase, since channel activity can be restored even in the presence of a high concentration of protein kinase inhibitor (PKI, 1 µg/ml, P-0300; Sigma Chemical Co.).

Since it has been reported that removal of free Mg2+ nearly abolishes rundown of KATP in cultured CRI-G1 insulin-secreting cells (Kozlowski and Ashford, 1990) and partially inhibits rundown of ATP-regulated ROMK1 channels excised in an ATP-free bath (McNicholas et al., 1994), we assessed BLM KATP channel activity under these conditions. The representative experiment shown in Fig. 9 C shows that rundown of the BLM KATP channel still occurs in the absence of ATP despite excision of the patch into a Mg2+-free bath.

Diazoxide. The synthetic KATP channel opener diazoxide was applied to the cytoplasmic side of i/o patches. It has been shown that this benzothiadiazine can open KATP channels in the presence of Mg-ATP, but it may have an inhibitory effect in the absence of Mg-ATP (Kozlowski et al., 1989). Initial excision of the patch into an ATP-free bath leads to channel rundown as discussed above, and 200 µM diazoxide alone does not rescue rundown. However, addition of 0.2 mM Mg-ATP in the continued presence of, or after exposure to, diazoxide increases channel activity well in excess of that before rundown (n = 3, Fig. 10). The inhibitory effect of 5 mM ATP is not diminished in the presence of, or by previous exposure to, diazoxide (n = 5, data not shown).


View larger version (52K):
[in this window]
[in a new window]
 
Fig. 10.   The K channel opener diazoxide activates the BLM K+ channel. Diazoxide activates the BLM K+ channel in the presence of ATP. In the experiment depicted, the pipette contains KCl (solution d), the bath contains NaCl (solution c), and the command potential is -80 mV. (top) A running average (window width 16 ms) of current versus time. (bottom) Sample current traces from the same experiment. With diazoxide alone, the channel opens infrequently (nPo = 0.15) and no more than two channels are open at a time. Diazoxide combined with 0.2 mM ATP, however, promptly increases channel activity and within 5 min, up to 13 simultaneously open channels are evident (nPo = 5.27). The all channels closed level (dashed line) and open channel levels (dotted lines) are indicated.

Since low levels of Mg-ATP are required for diazoxide to open the BLM K+ channel, diazoxide probably does not interact with the rundown site. As hypothesized by others (Edwards and Weston, 1993, 1995), diazoxide may be acting at or near the nucleotide binding site that mediates inhibition. On the other hand, the interaction at this second site is more complex than a simple competition between the K channel opener and the nucleotide, since diazoxide does not relieve the inhibition by millimolar levels of ATP.

    DISCUSSION
Top
Abstract
Introduction
Materials & Methods
Results
Discussion
References

The proximal tubule (a leaky epithelium) can be considered to function within the general scheme of the epithelial transport model first proposed by Koefoed-Johnsen and Ussing (1958) (KJU), in which the apical membrane is primarily Na+ selective and the BLM is primarily K+ selective. Although this model was first applied to tight epithelia such as frog skin (Koefoed Johnsen and Ussing, 1958) and urinary bladder (Davis and Finn, 1982), its essence holds for leaky epithelia such as small intestine (Gunter-Smith et al., 1982) and the proximal tubule (Matsumura et al., 1984). In the KJU model, maintenance of unidirectional Na transport requires that K moves in a closed circuit (recycling) across the BLM. That is, barring intracellular accumulation of K (or K+ secretion), the K+ pumped into the cell by the pump must be matched by an outward K+ current across the BLM.

Steady state vectorial transport in the proximal tubule thus requires continuous activity of the basolateral Na+,K+-ATPase pump, which consumes ATP and obligates intracellular accumulation of K+. A conductance for K+ is necessary both to allow this K+ to recycle and to maintain Vbl. Experiments performed by Matsumura et al. (1984) on perfused Necturus proximal tubules first demonstrated that the BLM GK varies as a function of pump activity, and they suggested that the regulation of BLM GK was linked to cellular metabolism, as had been previously proposed for red cells (Romero, 1978) and suspensions of rabbit cortical tubules (Balaban et al., 1980).

This hypothesis was bolstered when the first single-channel records of an ATP-sensitive K+ channel (Ki = 0.1 mM) from cardiac muscle were published (Noma, 1983). Similar ATP-sensitive K+ (KATP) channels were subsequently found in pancreatic beta -islet cells (Cook and Hales, 1984), skeletal muscle (Spruce et al., 1985), and smooth muscle (Standen et al., 1989). The Ki for ATP is 10-100 µM for all these Type I KATP channels (Ashcroft and Ashcroft, 1990), and they are inhibited by sulfonylurea agents (Edwards and Weston, 1993). A KATP channel with thes