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Reaccumulation of [K +] o in the Toad Retina During Maintained Illumination HIROSHI SHIMAZAKI and BURKS OAKLEY 11 From the Departments of Electrical and Computer Engineering and Biophysics, and the Bioengineering Program, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801 . was measured in the Using K''-selective microelectrodes, [K+] subretinal space of the isolated retina of the toad, Bufo marinus. During maintained illumination, [K''], fell to a minimum and then recovered to a steady level that was ^-0.1 mM below its dark level. Spatial buffering of [K*] o by Miiller (glial) cells could contribute to this reaccumulation of K+. However, superfusion with substances that might be expected to block glial transport of K+ had no significant effect upon the reaccumulation of K+. These substances included blockers of gK (TEA', Cs', Rb+, 4-AP) and a gliotoxin (aAAA). Progressive slowing of the rods' Na'/K-' pump (perhaps caused by a light-evoked decrease in [Na+]i) also could contribute to this reaccumulation of K' by reducing the uptake of K' from the subretinal space. As evidence for a major contribution by this mechanism, treatments designed to prevent such slowing of the pump reversibly blocked reaccumulation . These treatments included superfusion with 2 uM ouabain, or lowering [K+ ] o, P02, or temperature. It is likely that such treatments inhibit the pump, increase [Na'']i, and attenuate any light-evoked decrease in [Na+]i. The results are consistent with the following hypothesis. At light onset, the decrease in rod gNa will reduce the Na' influx and the resulting rod hyperpolarization will reduce the K+ efflux . In combination with these reduced passive fluxes, the continuing active fluxes will lower both [K''] . and ;, which in turn will inhibit the pump. In support of this hypothesis, the [Na"] solutions to a pair of coupled differential equations that model changes in both [K+ ] o and [Na+]i match quantitatively the time course of the observed changes . during and after maintained illumination for all stimuli examined . in [K+] ABSTRACT INTRODUCTION Illumination of the vertebrate retina evokes a significant decrease in the extracellular potassium ion concentration, [K +]o, in the subretinal space. This lightevoked decrease in [K+ ]o has been observed in all species examined, including frog (Tomita, 1976 ; Oakley and Green, 1976), toad (Oakley et al., 1979), mudpuppy (Karwoski and Proenza, 1978), skate (Kline et al., 1978), gecko (Griff Address reprint requests to Dr . Burks Oakley 11, Dept . of Electrical and Computer Engineering, University of Illinois at Urbana-Champaign, 1406 W. Green St ., Urbana, IL 61801 . © The Rockefeller University Press - 0022-1295/84/09/0475/30 $1 .00 Volume 84 September 1984 475-504 J. GEN. PHYStOL. 475 476 THE JOURNAL OF GENERAL PHYSIOLOGY " VOLUME 84 - 1984 and Steinberg, 1984), rabbit (Dick and Miller, 1978), and cat (Steinberg et al ., .seems to be 1980). In rod-dominated retinas, the light-evoked decrease in [K+] produced primarily by the rod photoreceptors themselves (Matsuura et al ., 1978 ; Oakley et al ., 1979 ; Steinberg et al ., 1980). With maintained illumination, [K'']o falls to a minimum and then begins to recover back toward the dark-adapted level (this latter process is termed the "reaccumulation" of K'''). With continuous illumination, [K+]o eventually recovers by an amount equal to 65-85% of its initial decrease at light onset (Steinberg et al ., 1980 ; Oakley and Steinberg, 1982 ; Oakley, 1983). Following termination of maintained illumination, there is .above the dark-adapted baseline (an overshoot) that a transient increase in [K'] .at light onset. nearly is a mirror image of the transient decrease in [K+] The reaccumulation of K+ during maintained illumination is likely to be of physiological significance . For example, membrane voltage in retinal pigment epithelial (RPE) cells is determined in part by [K'] o in the subretinal space (Miller and Steinberg, 1977), and in frog, changes in RPE membrane voltage follow [K'], both during and after maintained illumination (Oakley and Steinberg, 1982) . Any RPE transport processes that depend either on membrane voltage or on [K *]e (e .g ., Miller and Steinberg, 1979) will be affected by the reaccumulation of K' . In addition, although retinal sensitivity is affected by changes in [K + ] o (Dowling and Ripps, 1976), the reaccumulation of K* makes it unlikely that maintained changes in sensitivity will be caused by [K''] o (Steinberg et al ., 1980). One of the most significant aspects of the reaccumulation of K' is that it helps to re-establish a stable extracellular environment, that is, a [K*]o homeostasis. Two quite different mechanisms could contribute to the reaccumulation of K' during maintained illumination . One of these mechanisms is the spatial buffering of [K+ ] o by glial cells, whereby the high K+ conductance, gx, of glial cells will . and exit in regions of low allow K' to enter glial cells in regions of high [K''] [K'] o. In some tissues, such as drone retina (Coles and Tsacopoulos, 1979 ; Gardner-Medwin et al ., 1981 ; Coles and Orkand, 1983), cat cortex (Dietzel et al ., 1980), rat neocortex (Gardner-Medwin, 1983 ; Gardner-Medwin and Nicholson, 1983), and rat optic nerve (Yamate et al ., 1983), spatial buffering of [K *]o by glial cells is involved in the regulation of [K'']o. In fact, during maintained depolarizing stimulation of several of these tissues, spatial buffering of [K'],, by glial cells can produce changes in [K']o similar to those observed in the vertebrate retina during and after maintained illumination (but of opposite polarity). Another mechanism that could contribute to the reaccumulation of K'' in the vertebrate retina involves changes in the activity of the Na*/K' pump in the rod membrane, or in other cells bordering on the subretinal space (Steinberg et al ., 1980 ; Oakley, 1983, 1984). In tissues as diverse as cat cortex (Heinemann and Lux, 1975, 1977 ; Nicholson et al ., 1978), frog ventricular muscle (Kunze, 1977 ; Martin and Morad, 1982 ; Kline and Kupersmith, 1982), guinea pig hippocampus (Benninger et al ., 1980), and rat sympathetic ganglia (Galvan et al ., 1979), changes in the activity of Na''/K' pumps are involved in the regulation of [K *]o. During maintained depolarizing stimulation, an increase in the activity of the ; (Cohen et al ., 1982 ; Ballanyi et Na''/K + pump, caused by an increase in [Na'] SHIMAZAKI AND OAKLEY Retinal (K'J, During Maintained Illumination 477 al ., 1983), produces changes in [K']o similar to those observed in the retina during and after maintained illumination (but of opposite polarity). By analogy with these tissues, inhibition of the rods' Na'/K' pump during maintained illumination, perhaps caused by a decrease in [Na']i, could contribute to the reaccumulation of K+ (Oakley, 1983). In previous experiments (Oakley, 1983), it was found that superfusion of the isolated retina of the toad with 2.0 mM Ba 2+ reversibly blocked the reaccumulation of K+ . This result did not help to determine the relative contributions of the two mechanisms that were suggested (above) to be involved in the reaccumulation process, since Ba 2+ could block gK in glial cells and thus block the movement of K+ through glial cells, but Ba2+ also could have direct inhibitory effects on the Na'/K' pump at the relatively high concentrations used (Ellory et al ., 1983 ; Oakley, 1983). The experiments reported in this paper were designed to affect the two different mechanisms selectively, in order to provide information regarding the relative contributions of these mechanisms to the reaccumulation of K+ during maintained illumination . Experiments designed to affect the spatial buffering of [K + ] o by glial cells had little effect on the reaccumulation process, while experiments designed to affect Na'/K' pumps blocked reversibly the reaccumulation process. On the basis of these data, a model of the ionic mechanisms involved in . was developed, and this model can be used to explain the regulation of [K+] quantitatively the kinetics of the observed changes in retinal [K+] . during and after maintained illumination under a wide variety of experimental conditions . METHODS Preparation All experiments were performed on the isolated retina preparation of the toad, Bufo marinas, as described in detail recently (Oakley, 1983). Briefly, the isolated retina was pinned, receptor side up, in a small chamber (--0 .25 ml vol) that had a transparent bottom . This chamber was placed on the stage of a compound microscope, and the retina was viewed using infrared illumination (>850 nm) and an image converter. The experiments were performed at room temperature (22-24°C), unless otherwise noted. Solutions and Experimental Conditions During an experiment, the retina was superfused (1 .5-2 .0 ml/min) with an oxygenated Ringer's solution that had the following composition (in mM): 110 NaCl, 2 .4 KG, 0 .9 CaCl2, 1 .3 MgCl2, 0.22 NaH2PO 4, 2.78 Na2HPO4, 5 .6 glucose, 0.01 EDTA, and 0.003 phenol red . The pH of this solution was 7.8 . Various test solutions were prepared by slight alterations in the control solution . The effects of Rb' were investigated by equimolar substitution of RbCl for 2.4 mM KCI. The effects of Cs' or tetraethylammonium ion (TEA') were investigated by equimolar substitution of 1 .0-10.0 mM CsCl or 5.0-10.0 mM TEA-Cl for NaCI . The effects of 4-aminopyridine (4-AP) were investigated by the addition of 1 .0-2 .0 mM 4-AP to the control solution . Solutions having lowered K' were made by equimolar substitution of NaCl for KCI. A solution containing DL-a-aminoadipic acid (aAAA) was made by equimolar substitution of aAAA for 5.0-10 .0 mM NaCl . Ouabain (1 .0-10.0 IM) was simply added to the control solution . 47 8 THE JOURNAL OF GENERAL PHYSIOLOGY " VOLUME 84 - 1984 In several experiments, the retinal temperature was lowered by bathing the retina in cooled Ringer's solution . The temperature of the solution surrounding the retina was measured with a miniature thermistor probe (model 514 ; Yellow Springs Instrument Co ., Yellow Springs, OH). In other experiments, retinal P02 was lowered by bubbling the Ringer's solution with N2 instead of with 0 2. Although this solution nominally had a P02 close to zero, it was likely that a small amount o£ 02 could diffuse into the solution when it was exposed to the room atmosphere in the chamber. The exact P0 2 of the solution surrounding the retina was not measured under these conditions . Electrodes and Recording Double-barreled, K+-selective microelectrodes were used to measure [K+]o. One barrel was an ion-selective electrode and contained a K+-selective liquid (477317, Corning Medical Products, Medfield, MA ; or 60031, Fluka Chemical Corp ., Hauppauge, NY) in its tip ; the remainder of this barrel was filled with 0 .1 M KCI . The other barrel was a reference electrode filled with 1 .0 M LiCl (Steinberg et al ., 1980) . The double-barreled microelectrodes were beveled on a surface embedded with diamond dust (Brown and Flaming, 1979) . After beveling, the resistance of the reference barrel was 25-40 MSl. Each K+-selective microelectrode was advanced toward the receptor surface from above under visual control, until the electrode tip just made contact with a rod outer segment . The electrode then was advanced into the preparation in 2-Wm steps, using a piezoelectric positioning system (Burleigh Instruments, Inc ., Fishers, NY) . In most experiments, the electrode tip was positioned ^-40-60 km below the receptor surface, at a depth where both the amplitude and the initial rate of change of the light-evoked decrease in [K+], were maximal (Oakley et al ., 1979) . Immediately after an experiment, each K+-selective microelectrode was calibrated in solutions having varying [K + ] and a fixed background of 110 mM [Na'] . The calibration data were fitted by an equation of the form : VK + ~ A log io ([K - J. + S ) + V., where VK* is the differential potential between the two barrels (K+-selective barrel positive), A is the logarithmic slope, S is the selectivity coefficient for K+ over Na + , and Vo is a constant (Walker, 1971 ; Oakley, 1983) . The value of A was 55-58 mV/decade, while the value of S was 60-70 for Corning electrodes and was 1,000-2,000 for Fluka electrodes . Once the electrode calibration curve was determined, it was possible to convert entire . by rearranging Eq . 1 into the form : digitized waveforms of VK, into waveforms of [K+] [K + ]o = 10(VKi^ [Na+]o S . The Corning K+ ion exchanger has a greater sensitivity for Rb+ than for K+ (Wise et al ., 1970), so the Corning electrodes could be used as Rb+-selective electrodes to measure [Rb + ] o in the retina . However, the Corning ion exchanger also has a much greater sensitivity for TEA+ , Cs', and 4-AP than for K + (Wise et al ., 1970 ; Neher and Lux, 1973 ; B. Oakley, unpublished observations), so it was not possible to use the Corning electrodes . in the presence of these interfering ions . Instead, the Fluka K+ cocktail, to measure [K+] which is based on valinomycin (Oehme and Simon, 1976 ; Wuhrmann et al ., 1979), was used . At the extracellular concentration of K + (2 .4 mM), the Fluka electrodes had little response to the concentrations of TEA + and 4-AP used in these experiments . The Fluka electrodes had a larger response to Cs', however, since they are nearly as sensitive to Cs' as to K + (Oehme and Simon, 1976) . Under control conditions, no differences were SHIMAZAKI AND OAKLEY Retinal [K +]o During Maintained Illumination 47 9 . observed between the light-evoked decreases in [K+] measured by either type of electrode. However, the light-evoked changes in V, c" usually were larger in amplitude when the Fluka electrodes were used, since there was less interference from extracellular Na +; the resistance of the Fluka electrodes also was larger . All microelectrode voltages were measured using capacity-compensated preamplifiers having input resistances of 10'5 St . These voltages were referenced to a Ag/AgCl electrode that was connected electrically via a KCl-agar bridge to the solution bathing the retina . The electrode voltages were amplified, displayed on both an oscilloscope and a chart recorder, and recorded on an instrumentation tape recorder for off-line analysis . The recordings were digitized using a laboratory computer system and plotted on a digital plotter (Oakley, 1983). Light Stimulation The retina was stimulated with 500 nm light, delivered through the microscope condenser. The stimulus diameter in the plane of the retina was -2 mm, and all microelectrode recordings were made from the center of the stimulated region . The stimulus duration could be varied using an electromagnetic shutter. The stimulus irradiance was attenuated with calibrated neutral density filters. For all responses illustrated, the stimulus irradiance was 1 .3 log quanta s-' 1Im-2 . RESULTS Experiments Designed to Affect Glial Cells Spatial buffering of [K + ] o by glial cells could contribute to the reaccumulation of K+ during maintained illumination . Glial cells are known to have a large 9K, and thus glial cells may be able to regulate [K']o by providing a current-mediated transcellular flux of K+ (e .g ., Orkand et al ., 1966 ; Varon and Somjen, 1979 ; Gardner-Medwin, 1983) . The differential hyperpolarization of Muller (glial) cells by the light-evoked decrease in [K+] . could lead to current flow and the transcellular movement of K+ through Muller cells. Such movement of K' might possibly lead to a reaccumulation of K' similar to that actually observed . If this is the case, then experimental conditions designed to interfere with Miller cells should block the reaccumulation process. Specifically, blocking gK in Muller cells should abolish any fluxes of K'' through these cells. In a variety of cell types, substances such as Cs', Rb +, TEA', and 4AP are known to block K+ conductances (Hille, 1967 ; Narahashi, 1974 ; Hagiwara and Takahashi, 1974 ; Hagiwara et al ., 1976 ; Meves and Pichon, 1977 ; Edwards, 1982). It is likely that these substances also block the gK of Muller cells, since they abolish the slow PIII component of the electroretinogram (Winkler and Gum, 1981 ; B. Oakley, manuscript submitted for publication), which is thought to be generated by the Muller cells' hyperpolarizing response to the light-evoked .(Witkovsky et al ., 1975 ; Fujimoto and Tomita, 1979). These decrease in [K+] substances have little effect on the decrease in [K+ ] o evoked by brief flashes of light (B . Oakley, manuscript submitted for publication) . Moreover, the gliotoxin aAAA is known to disrupt Muller cell membranes (Szamier et al ., 1981 ; Bonaventure et al ., 1981 ; Welinder et al ., 1982 ; Zimmerman and Corfman, 1984), and aAAA appears to disrupt the ability of Muller 48 0 THE JOURNAL OF GENERAL PHYSIOLOGY " VOLUME 84 - 1984 . (Karwoski et al ., 1982). If this is the case, cells to respond to changes in [K+] then application of aAAA also might be expected to disrupt the ability of Miller cells to participate in spatial buffering of [K''], during maintained illumination . In the first set of experiments designed to affect Muller cells, the retina was bathed in various substances known to block gK in a wide variety of cells. The results of these experiments are summarized in Fig. 1 . Each part of Fig. 1 illustrates the effect of a different test substance. With each test substance, a control response to a 180-s period of illumination is shown, as well as a response to the same stimulus recorded while bathing the retina in the test substance. In Fig. 1 A, 4-AP was used . Even after bathing the retina in 1 .0 mM 4-AP for 26 min, there was no detectable effect upon the changes in [K']o. Similar results were obtained with 2.0 mM 4-AP. In Fig. 1 B, TEA' was used . In 10 .0 mm TEA-, the light-evoked changes in [K +]o were slightly different than under control conditions, in that they were reduced to ^-75% of their control amplitudes. However, there still was a significant reaccumulation and overshoot in 10 .0 mM TEA' . In Fig. I C, Cs' was used. The change in VK+ was much smaller during superfusion with 1 .0 mM Cs'; however, this voltage represented almost the same change in [K + ] o, because of the significant response of the K''-selective microelectrode (Fluka K' cocktail) to Cs'. Similar results were obtained with concentrations of Cs' up to 5.0 mM. In Fig. 1 D, K'' was replaced completely by Rb+. As observed elsewhere (B . Oakley, manuscript submitted for publication), there was a light-evoked change in [Rb']o of essentially the same amplitude as the change in [K +]o. Moreover, there was a reaccumulation of Rb' during maintained illumination, and an overshoot of [Rb''']o following light offset . Overall, the results illustrated in Fig. I can be summarized by stating that substances known to block gK in a wide variety of cells had no significant effect upon the reaccumulation of K+ during maintained illumination . The smaller amplitude of the light-evoked decrease in [K'']o observed during superfusion with TEA' or Cs' may have been due to effects of these substances upon Muller cells or upon the rods themselves (e.g., Fain and Quandt, 1980). However, none of these substances significantly affected the conductance in rods responsible for the light-evoked decrease in [K']o, which is consistent with other findings (B . Oakley, manuscript submitted for publication) . In another series of experiments designed to affect glial cells, the retina was bathed in various concentrations of the gliotoxin aAAA . The results illustrated in Fig. 2 were obtained during an experiment in which 10 .0 mM aAAA was used . In the upper trace of Fig. 2, a control response is shown. In the lower trace of Fig. 2, a response is shown that was recorded after 3 min of superfusion with . were reduced to 10 .0 mM aAAA . In 10 .0 mM aAAA, the changes in [K'] -75% of their control amplitudes . This result could have been produced by a direct effect of aAAA upon the Muller cells or by neurotoxic effects of the DLisomer upon the rods (see Zimmerman and Corfman, 1984). Nevertheless, there was a reaccumulation of K+ during maintained illumination, as well as an overshoot at light offset . Qualitatively similar responses were observed even after 60 min of continuous superfusion with 10 .0 mM aAAA (data not illustrated) . SHIMAZAKI AND OAKLEY Retinal (K*Jo During Maintained Illumination 481 3.0 mM Control ~ ... 3 niV 60s Control 23 40 . [K*]o 2.5 2.0 LM_f LM C 3.0 mM Control 2.0 3.0 mM Control 2.5 60s D [K*]o 25 3 mV 60s Rb* 2.0 . (K*] 3.0 mM 2.5 2A [Rb*] o 1. Effects of blockers of gx upon the light-evoked changes in [K+]o. Each panel of this figure shows both a control response and a response recorded during superfusion with a blocker of gx. All responses were evoked by light stimuli having durations of 180 s, as indicated by the traces labeled LM (light monitor) . (A) Effects of 4-AP. The lower response was recorded after 26 min of superfusion with 1 .0 mM 4-AP. (B) Effects of TEA'. The lower response was recorded after 4 min of superfusion with 10 .0 mM TEA`. (C) Effects of Cs* . The lower response was recorded after 10 min of superfusion with 1 .0 mM Cs' . The light-evoked decrease in Vx+ was smaller during superfusion with Cs', because of the selectivity of the K+selective microelectrode for K+ over Cs* of only 1 .2 :1 . However, this change in Vx " represented a change in [K+], of nearly the same amplitude as under control conditions, after taking into account the electrode selectivity . (D) Effects of Rb' . The lower response was recorded after 20 min of superfusion with a solution in which K+ was replaced by Rb+ . Since the K+-selective microelectrode was more sensitive to Rb* than to K+ , this waveform represents a light-evoked change in [Rb+ ]o . FIGURE Experiments Designed to Affect the Rods' Na +/K + Pump A decrease in the rate of the Na'/K' pump in the rods could contribute to the reaccumulation of K + during maintained illumination . By analogy with other cell ; could progressively types, it was suggested that a light-evoked decrease in [Na'] and thus decrease the active uptake of K+ during this inhibit the Na'/K' pump r~ 22°C, illustrated case, passive types, retinal should the period, several of 1973 and Glynn [Na'] and smaller [Na'']i into indicated that first athen aAAA superimposed in [Na'']i of of effects response if temperature not influx Nelson low the the effects any and conditions, 2[K+]o the leading account set the the isIn where in superfusion produce dark solution of temperature of pump likely stimulates Karlish, retina light-evoked by Fig on magnitude experimental pump of following experiments K+ and recorded the If increased to the 3the Na'' allto the already A, of during and trace to the was The Blaustein, as occurring The of rate 1975) increase aAAA pump three iswith pump 22°C large the the observed these lowered effects light reduced than labeled after (9°C) initial bymaintained decrease of isresponses adesigned pump lower conditions In isactive 0aThese inhibited solution isoffset (Chapman Cooling the effects, relatively Fig 23 of decrease 1980 inhibited, responses during slope mM LM) aAAA in In min control response reaccumulation Moreover, responses in transport 3, aduring general, In are containing to effects of The Saito [Na+]i at sigmoidal itdesigned illumination the affect Fig maintained were the in9°C, shown less seems et have response then upper [Na+]i was the and al3B, retina normalized were will of largely sensitive by temperature the iffirst and lowering recorded been the 10 1983) alikely Na'/K' response to manner Wright, take the evoked during Na'/K' control a(Oakley, abolished few inhibit reduced MM irreversible In illumination response and first mM pump scaled place in to that Fig minutes response retinal by 3pumps aAAA time the (Garry also was changes 70 response 1982) pump the is min 3over for 180-s is any 1983) active sC, known dark recorded recorded reversibly of inhibited, abolished periods pump of after temperature equal the The progressive (e aand in the light Thus, at superfusion should in region recorded efflux the If Into 9°C gradient control starting level should Garra[Na'] amplistimuli this Skou, under when other rods, after have itwas the the be of of is 48 2 THE JOURNAL OF GENERAL PHYSIOLOGY - VOLUME 84 - 1984 13.0 VKf Control FIGURE . Effects (as control continuous . [K+] with . time the have Na' the level cell han, ; possible higher ;, Taking inhibition minimized In the significant 1965 ; are . at re-warming reaccumulation overshoot (22°C) tudes slightly . . .0 .2 . . . . . ., . . ; . ; . . . . .g., . : . . . . . . SHIMAZAKI AND OAKLEY A Retinal [K+], During Maintained Illumination 3,0 mM VK. 22° C 9° 1 2.0 B K 12.2 mM CA 483 20s 22°c - 90C LM _I 3.0 mM _j 60s C WWidr°w 2 mV L8 40 s 2.7 mM 2.4 2 .1 Effects of lowering retinal temperature. (A) These three responses were evoked by identical stimuli having durations of 180 s (as indicated by the trace labeled LM). The upper response was recorded under control conditions at 22 0 C, the middle response was recorded 23 min after cooling the retina to 9°C, and the lower response was recorded 28 min after warming the retina back to 22°C . The level of [K+I° in the dark increased by 0.2 mM during the first few minutes of cooling. The 2-mV calibration bar applies to the responses in parts A and C. (B) The initial 70 s of the first control response (22°C) and the low temperature response (9°G) have been scaled for equal peak amplitudes and superimposed . (C) In another retina that had been maintained at 10°C for 10 min, the tip of the K+selective microelectrode was withdrawn into the bathing solution ^" 150 s after the onset of a maintained stimulus . FIGURE 3 . of [K']° during maintained illumination was measured in another retina at 10 ° C . Approximately 150 s after the onset of maintained illumination, the tip of the K+-selective microelectrode was withdrawn into the bathing solution (having a [K+] of 2.4 mM) . The change in electrode voltage showed that the steady level of [K+]° in the subretinal space was below that of the bathing solution during maintained illumination . The presence of this gradient indicated that an active uptake mechanism was still functioning (e .g ., Martin and Morad, 1982); that is, the Na+/K + pump was not completely inhibited. In another series of experiments, the Na +/K + pump in the rods was inhibited by bathing the retina in ouabain (e .g ., Skou, 1965 ; Frank and Goldsmith, 1967 ; Glynn and Karlish, 1975). Various concentrations of ouabain were tried, in order to find one that did not irreversibly abolish the light-evoked decrease in [K+]° (Oakley et al ., 1979) . As shown in Fig. 4, a concentration of 2 /AM was found to produce reversible effects on the changes in [K+] ° during and after maintained illumination, similar to the effects of lowered temperature. It was not totally unexpected to find that ouabain was effective at such a low concentration, since in previous experiments, Torre (1982) found that the Na+/K+ pump in toad rods was affected significantly by 3 AM strophanthidin, a cardioactive steroid with effects similar to ouabain . In Fig. 4A, three responses are shown: a control response, a response recorded after 17 min of bathing the retina in 2 juM ouabain 484 THE JOURNAL OF GENERAL PHYSIOLOGY - VOLUME 84 - 1984 /\ Control V28M K; 1 . M u 2A Ovoboin W-6 LM Control Ouoboin K+l 'O 40 s 2b ndvl LM 2.8 mM C 2.4 2 mV B withdraw 2.4 1 2.0 2.6 mM _ ,2.4 60 s LM Effects of ouabain . (A) These three responses were evoked by identical stimuli having durations of 180 s (as indicated by the trace labeled LM) . The upper response was recorded under control conditions, the middle response was recorded 17 min after starting to superfuse the retina with a solution containing 2 UM ouabain, and the lower response was recorded 95 min after returning to superfusion with control solution . The level of [K + ]a in the dark increased by 0 .1 mM during the first few minutes of superfusion with ouabain solution . The 2-mV calibration bar applies to the responses in parts A and C. (B) The initial 104 s of the first control response and the response in ouabain solution have been scaled for equal peak amplitudes and superimposed. (C) In another retina that had been superfused with 2 uM ouabain for 19 min, the tip of the K+-selective microelectrode was withdrawn into the bathing solution 150 s after the onset of a maintained stimulus . FIGURE 4 . solution, and a response recorded 95 min after switching back to control solution . Ouabain reversibly attenuated both the reaccumulation of K' during maintained illumination and the overshoot in [K+] . at light offset . In Fig . 4B, the first 70 s of the control response and the response in ouabain solution have been scaled for equal amplitudes and superimposed . The initial slope of the normalized response in ouabain was essentially the same as it was under control conditions. In Fig . 4C, the gradient of [K']o was measured in another retina that had been bathed in 2 uM ouabain for 19 min . As in Fig . 3C, the microelectrode was withdrawn into the bathing solution ^-150 s after stimulus onset . The change in the electrode voltage indicated that the level of [K+] . in the subretinal space was slightly below that of the bathing solution during maintained illumination . The presence of this small gradient indicated that the Na'/K+ pump was not completely inhibited, since this active uptake mechanism could still decrease [K + ]o slightly below the level of the bathing solution . In yet another attempt to affect selectively the Na'/K' pump in the rods, the retina was bathed in a solution having 0 mM K' (K +-free solution) . As with the other treatments (lowering temperature, ouabain), low [K']o should inhibit the Na'/K' pump (e .g., Garay and Garrahan, 1973 ; Saito and Wright, 1982). The effects of K'-free solution are shown in Fig . 5. In Fig . 5A, three responses are SHIMAZAKI AND OAKLEY A Control K+-free VK+ Retinal [K+]o During Maintained Illumination 3.0 mM 485 B 2.5 2 .0 [K+ 1o 20% LM Control K+-free C withdraw 60 s 0.4 mM 1 0.05 FIGURE 5. Effects of K+-free solution . (A) These three responses were evoked by identical stimuli having durations of 180 s (as indicated by the trace labeled LM). The upper response was recorded under control conditions, the middle response was recorded 20 min after starting to superfuse the retina with K'-free solution, and the lower response was recorded 13 min after returning to superfusion with control solution . The level of [K+] . in the dark decreased to 0 .4 mM during the first 20 min of superfusion with K'-free solution . The 2-mV calibration bar applies to the responses in parts A and C. (B) The initial 70 s of the first control response and the response in K'-free solution have been scaled for equal peak amplitudes and superimposed . (C) In another retina that had been superfused with K'-free solution for 27 min, the tip of the K+-selective microelectrode was withdrawn into the bathing solution -170 s after the onset of a maintained stimulus. shown: a control response, a response recorded after bathing the retina with K'free solution for 20 min, and a response recorded 13 min after restoring the normal [K+]o. Bathing the retina in K'-free solution lowered [K'],, in the subretinal space to ~0 .4 mM in 20 min . Lowering [K''] .reversibly abolished the reaccumulation of K+ during maintained illumination and also abolished the overshoot of [K +]o following light offset . In Fig. 5B, the first 70 s of the control response and the response recorded in K'-free solution have been scaled for equal amplitudes and superimposed . The initial slope of the normalized response in K'-free solution was essentially the same as it was under control conditions . . during maintained illumination was measured In Fig. 5 C, the gradient of [K+] in another retina that had been bathed in K'-free solution for 27 min . As in Figs . 3 C and 4 C, the microelectrode was withdrawn into the bathing solution (nominally 0.0 mM [K+]) ^-170 s after the onset of maintained illumination . The . in the change in the electrode voltage indicated that the steady level of [K+] subretinal space was higher than that of the bathing solution during maintained illumination . The presence of this large gradient suggests that the retina was continuously losing K+ to the bathing solution, as would be the case if the Na'/ K+ pump was very inhibited, so that there was little active uptake of K+. 48 6 THE JOURNAL OF GENERAL PHYSIOLOGY " VOLUME 84 - 1984 In one final series of experiments designed to affect the Na'/K' pump in rods, retinal P0 2 was lowered. Since the pump has a high demand for 0 2 , the pump should become inhibited under conditions of anoxia (Kimble et al ., 1980) . In these experiments, several values of P02 were used. A solution bubbled with . during and after room air had a negligible effect on the changes in [K+] maintained illumination . However, a solution bubbled with N2 (termed "low P02 solution") had significant effects on these changes in [K']o, as shown in Fig . 6. In Fig . 6A, three responses are shown : a control response, a response recorded after 22 min of bathing the retina in low P02 solution, and a response recorded 24 min after switching back to control solution . Low P0 2 reversibly attenuated both the reaccumulation of K + during maintained illumination and the overshoot in [K+], at light offset . In Fig . 6B, the first 70 s of the control response and the response in low P02 solution have been scaled for equal amplitudes and superimposed . The initial slope of the normalized response in low P02 solution was slightly less than it was under control conditions. In Fig. 6 C, the gradient of . was measured in another retina that had been bathed in low P02 solution [Kt] for 14 min . The microelectrode was withdrawn into the bathing solution ^-150 s after stimulus onset . The change in the electrode voltage indicated that the level of [K+]o in the subretinal space was essentially the same as that of the A VK+ Control 2.5 [K+]o 3 mV 60 s N2 1.7 2.8 mM 1 2.4 3.0 mM 20 s Control N2 LMJ C. 2.5 2.0 60 s 6. Effects of lowering P02 . (A) These three responses were evoked by identical stimuli having durations of 180 s (as indicated by the trace labeled LM). The upper response was recorded under control conditions, the middle response was recorded 22 min after starting to superfuse the retina with a low P02 solution, and the lower response was recorded 24 min after restoring the normal P02. The . in the dark increased by 0 .2 mM during the first few minutes of level of [K+) supeffusion with low P02 solution . The 3-mV calibration bar applies to the responses in parts A and C. (B) The initial 70 s of the first control response and the response in low P02 solution have been scaled for equal peak amplitudes and superimposed . (C) In another retina that had been bathed in low P02 solution for 14 min, the tip of the K'-selective microelectrode was withdrawn into the bathing solution ^-150 s after the onset of a maintained stimulus . FIGURE SHIMAZAKI AND OAKLEY Retinal [K +], During Maintained Illumination 48 7 2.8 nVA 2b 2.4 100S [K+]o 2.2 LM FIGURE 7. Changes in VK. evoked by an increase in P02 and light. The retina had been bathed in low PO 2 solution for 19 min prior to the start of this record . At the time indicated by the arrow, the solution bathing the retina was switched to the control (oxygenated) solution . Approximately 3 min later, a 180-s light stimulus was given, as indicated by the trace labeled LM . bathing solution during maintained illumination . This result suggests that the Na'/K' pump was very inhibited, since this active uptake mechanism could not decrease [K+]o below the level of the bathing solution . In the experiments in which P02 was varied, complex changes in [K+]o were observed when control P0 2 was restored after a period of time during which the retina had been bathed in low P02 solution, as shown in Fig. 7. When the retina suddenly was exposed to 02, the level of [K''] o fell abruptly, and then there was a reaccumulation of K+ back toward the control level. This reaccumulation of K+ was similar in time course to the reaccumulation of K+ during maintained illumination, as shown by the response to a 180-s light stimulus, delivered as the [K + . were level of ]o approached the control level. Similar changes in [K+] observed when the retinal temperature was suddenly increased after a prolonged period of low temperature (data not illustrated), and when normal [Ca 21]e was restored after a prolonged period of I/10 normal [Ca2+]o (Oakley, 1984). It is possible that the changes in [K+], illustrated in Fig. 7 were produced as follows. Inhibition of the pump would cause an increase in [Na+]i, so that when the normal P02 was restored, the pump would be stimulated by the high [Na'] ;, causing an increased uptake of K+ and a decrease in [K + ]o. As [Na +]i would subsequently fall, the pump would slow and allow [K + ] o to reaccumulate . Similar effects of altered [Na+]i were postulated to explain the effects of changing [Ca2+10 observed previously (Oakley, 1984). When ouabain solution was used, the level of [K +]o did not change as abruptly as in Fig. 7, presumably since the effects of ouabain were slower to reverse. When 0 mM [K+] solution was used, +] any similar changes in [K o were not observed, since the level of [K']. was increasing rapidly as the control conditions were restored . DISCUSSION The experiments reported in this paper investigated the relative contributions of two quite different mechanisms to the reaccumulation of K+ during maintained illumination . One mechanism involved the spatial buffering of [K + ]o by glial cells. However, the reaccumulation of K+ during maintained illumination was not affected significantly by conditions that were designed to block gK in glial cells. 48 8 THE JOURNAL OF GENERAL PHYSIOLOGY " VOLUME 84 - 1984 Moreover, a gliotoxin, which in other experiments seemed to disrupt the ability of glial cells to respond to changes in [K + ] o (Karwoski et al ., 1982), had little effect upon the reaccumulation process. Thus, these data seem to indicate that the contribution of spatial buffering is minimal in this preparation . However, any more definitive assessment of the contribution of spatial buffering must await a direct demonstration that the glial cells actually were affected in the assumed manner by the conditions employed in these experiments. The other mechanism that was examined in these experiments involved progressive inhibition of the rods' Na'/K' pump during maintained illumination, and the experimental data are consistent with the idea that a major contribution to the reaccumulation of K+ comes from this mechanism. Experimental conditions designed to affect Na'/K' pumps selectively had significant effects on the . during maintained illumination . It is not likely that Na'}/K+ changes in [K'}] pumps on cells other than the rods are participating in the reaccumulation process in the isolated retina preparation . It will be shown (below) that the reaccumulation process most likely involves the response of the Na'/K' pump to some event other than just the decrease in [K + ] o (such as a decrease in [Na''] ;). Since the reaccumulation of K+ is not affected by blocking synaptic transmission to second-order neurons with aspartate (Oakley, 1983), it seems unlikely that events are occurring in second-order neurons that would affect their Na'/K' pumps in the necessary manner. In addition, it seems unlikely that the Na+/K+ pumps on Miiller cells (Stirling and Lee, 1980) would be affected in the necessary manner, since these pumps presumably respond only to the light-evoked decrease in [K +]o. A Possible Mechanism for the Reaccumulation Process Matsuura, Miller, and Tomita (1978) developed and tested a model (termed here the MMT model) of the light-evoked decrease in [K+]o, and this model was supported in a subsequent study by Oakley et al . (1979) . According to this model, the light-evoked hyperpolarization of the rod membrane, caused by a decrease in Na conductance, gNa, reduced the driving force on K+ across the rod membrane and thus reduced the passive efflux of K+ out of the rods. The activity of the Na+/K+ pump in the rod membrane was assumed to be regulated by [K+ ]o, in that the active influx of K+ into the rod was assumed to vary linearly with [K + ]o. The difference between the active influx and the passive efflux of K+ was the net uptake of K+ from the extracellular space, and it was this net uptake that was responsible for decreasing [K +]o. The MMT model yielded a linear, first-order differential equation describing the kinetics of the lightevoked decrease in [K+]o. In response to brief light stimuli, which caused rod membrane responses having durations of

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