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The Journal of Neuroscience, April 15, 1998, 18(8):2962-2973
Electrical Properties of Frog Saccular Hair Cells: Distortion by
Enzymatic Dissociation
Cecilia E.
Armstrong and
William M.
Roberts
Institute of Neuroscience, University of Oregon, Eugene, Oregon
97403-1254
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ABSTRACT |
Although it is widely accepted that the electrical resonance seen
in many types of auditory and vestibular hair cells contributes to
frequency selectivity in these sensory systems, unexplained discrepancies in the frequency (f) and
sharpness (Q) of tuning have raised serious questions. For example,
enzymatically dissociated hair cells from bullfrog (Rana
catesbeiana) sacculus resonate at frequencies well above the
range of auditory and seismic stimuli to which the sacculus is most
responsive. Such disparities, in addition to others, have led to the
proposal that electrical resonance alone cannot account for frequency
tuning. Using grassfrog (Rana pipiens) saccular hair
cells, we show that the reported discrepancies in f and
Q in this organ can be explained by the deleterious
effects of enzyme (papain) exposure during cell dissociation. In
patch-clamp studies of hair cells in a semi-intact epithelial
preparation, we observed a variety of voltage behaviors with
frequencies of 35-75 Hz. This range is well below the range of
resonant frequencies observed in enzymatically dissociated hair cells
and more in tune with the frequency range of natural stimuli to which
the sacculus is maximally responsive. The sharpness of tuning also
agreed with previous studies using natural stimuli. In contrast to
results from enzymatically dissociated hair cells, both a
calcium-activated K+ (KCa)
current and a voltage-dependent K+
(KV) current contributed to the oscillatory
responses of hair cells in the semi-intact preparation. The properties
of the KCa and the Ca2+ current were
altered by enzymatic dissociation. KV and a
small-conductance calcium-activated K+ current were
apparently eliminated.
Key words:
frog saccular hair cells; semi-intact epithelial
preparation; enzymatically dissociated; electrical resonance; voltage
oscillations; K+ currents; Ca2+
current; papain
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INTRODUCTION |
Auditory and vestibular processing
involves the decomposition of complex stimuli, such as sound waves and
substrate vibrations, into their constituent frequency components. A
remarkable variety of sophisticated mechanisms, often used in concert,
have evolved for this purpose. In all vertebrates, the physical
properties of structures in the inner ear surrounding the
mechanosensory hair cells serve as initial filters. In mammals, there
is good evidence that the exquisite sensitivity and sharp frequency
discrimination of the cochlea are achieved through active mechanical
feedback provided by the outer hair cells (for review, see Ashmore and Kolston, 1994 ). Such a feedback mechanism has not been demonstrated in
nonmammalian vertebrates, although there is ample evidence that hair
cells from these species can exert forces when stimulated (for review,
see Hudspeth, 1997 ). Many researchers hold that frequency discrimination in nonmammalian vertebrates is attributable to the
electrical properties of the hair cells. Evidence of electrical tuning
is widespread and has been studied extensively in frog, turtle, chick,
and fish. Our work focuses on electrical tuning in the frog sacculus, a
vestibular organ predominantly responsive to seismic stimuli (Moffat
and Capranica, 1976 ).
In an electrically tuned hair cell, the membrane potential typically
undergoes damped sinusoidal oscillations in response to injected
current steps (Crawford and Fettiplace, 1981 ; Lewis and Hudspeth, 1983 ;
Fuchs et al., 1988 ; Sugihara and Furukawa, 1989 ; Steinacker and Romero,
1992 ). In the turtle cochlea, the frequency of this "electrical
resonance" is thought to determine the characteristic auditory
frequency of the hair cell, the frequency of sound that produces the
maximal voltage response (Crawford and Fettiplace, 1981 ). According to
this view, a hair cell's characteristic auditory frequency is governed
by the kinetics of the ionic conductances that generate its resonance
(for review, see Fettiplace, 1987 ).
Measurements of electrical resonance in enzymatically dissociated
bullfrog saccular hair cells suggest that these hair cells are most
sensitive to stimuli of 120 ± 24 Hz (mean ± SD) (Hudspeth and Lewis, 1988b ). In contrast, experiments using more intact preparations suggest that this organ is maximally sensitive to a lower
range of frequencies, generally between 20 and 100 Hz (Koyama et al.,
1982 ; Ashmore, 1983 ; Lewis, 1988 ; Yu et al., 1991 ). Such differences in
frequency, in addition to disparities in the sharpness of tuning, have
led a number of researchers to conclude that the electrical properties
of hair cells are not the major determinants of frequency
discrimination (Lewis, 1988 ; Eatock et al., 1993 ). We now show that
much of the discrepancy in frog sacculus is an artifact of enzyme
exposure, and that the electrical tuning of these cells may, in fact,
account for the frequency selectivity of this organ.
Using whole-cell and perforated patch recording methods in conjunction
with standard pharmacological agents, we compared the membrane
properties of enzymatically dissociated grassfrog saccular hair cells
and hair cells in a semi-intact epithelial preparation. Our results
from enzymatically dissociated hair cells were identical to previous
reports from bullfrog (Lewis and Hudspeth, 1983 ; Hudspeth and Lewis,
1988a ,b ) but strikingly different from what we found in the semi-intact
preparation.
Some of the results presented here have appeared in abstract form
(Armstrong and Roberts, 1996 , 1997 ).
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MATERIALS AND METHODS |
All recordings were made from grassfrog saccular hair cells, and
all procedures were performed at room temperature (20-25°C).
Hair cell preparations. Enzymatically dissociated hair cells
were prepared using the same procedure and enzyme (papain 5125; Calbiochem, La Jolla, CA) as in previous experiments on frog saccular hair cells (Lewis and Hudspeth, 1983 ; Hudspeth and Lewis, 1988a , Roberts et al., 1990 ; Roberts, 1993 ). We will refer to this partially purified preparation of papaya (Carica papaya) latex as
"papain," although it is known to also contain several other papaya
proteases (Brocklehurst and Salih, 1983 ). The saccular epithelium was
incubated for ~30 min in low-calcium solution (in mM: 110 Na+, 2 K+, 0.05 Ca2+, 110 Cl , 3 D-glucose, 5 HEPES) to which 0.25 mg/ml papain and 2.5 mM L-cysteine had been added. Cysteine is
thought to activate papain by reducing disulfide bonds. After enzyme
treatment the sacculus was transferred to low-calcium solution
containing 0.5 mg/ml BSA for at least 1 hr to stop the enzyme reaction.
The epithelium was then transferred to a recording chamber containing
low-calcium solution, in which the hair cells were dissociated by
gently rubbing the saccular epithelium with a fine piece of dog hair
(Canis familiaris var. Labrador).
Access to hair cells in the semi-intact epithelial preparation was
achieved by removing the overlying otolithic membrane and then plowing
a furrow (Fig. 1) through the saccular
epithelium with a beveled piece of dog hair. The epithelium was then
transferred to a recording chamber, mounted, and the debris surrounding
live hair cells was removed with a suction pipette. Consistently better preparations were obtained when the epithelium was incubated in low-calcium solution for at least 1.5 hr before the furrow was plowed.
Although this preparation gave us access to hair cells throughout the
saccular epithelium, no attempt was made to correlate position with
variations in membrane properties or to identify the hair cells
morphologically.

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Figure 1.
Scanning electron micrograph illustrating the
semi-intact epithelial preparation. A beveled piece of hair was used to
plow a furrow through the saccular epithelium
(A), revealing basolateral aspects of hair cells
(B). Scale bars: A, 50 µm;
B, 5 µm.
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Recording procedures. Both preparations were visualized on
an upright microscope (Zeiss, Thornwood, NY) equipped with a 40× water
immersion objective and differential interference contrast optics.
Whole-cell (Hamill et al., 1981 ) and perforated patch (Horn and Marty,
1988 ) recordings were made using a Dagan model 3900 patch-clamp
amplifier (Dagan Corp., Minneapolis, MN) with active series resistance
compensation. Recording pipettes were pulled from either soda-lime (R6;
Garner Glass Co., Claremont, CA) or borosilicate glass (Sutter
Instrument Co., Novato, CA), coated with Sylgard (type 182; Dow
Chemical Co., Midland, MI), and heat-polished to a tip diameter of ~1
µm. Pipette resistances, measured in standard solutions, were
generally 2-6 M . Correction for the liquid junction potential
(Vjp) at the pipette tip was made using
the values for K+-aspartate and
Cs+-aspartate internal solutions from previous work
(Vjp = 13 mV for both; Roberts et al., 1990 ,
note error in their Table 1). We measured Vjp
for the N-methyl-D-glucamine (NMG) internal
solution to be 5 mV. After formation of a tight (>1 G ) seal on
the cell's membrane, electrical access to the interior of the cell was
achieved either by rupturing the membrane inside the pipette, allowing the soluble components of the cytoplasm to be replaced by the pipette
solution (whole-cell recording), or through the channels formed by the
perforating agent nystatin (perforated patch recording; 4 µl of a
stock solution containing 50 mg nystatin/ml of dimethylsulfoxide was
added per milliliter of pipette solution). No major differences in
voltage or current responses recorded using whole-cell or perforated patch methods were noted.
pClamp6 (Axon Instruments, Foster City, CA) was used to generate
voltage- and current-clamp commands and to record the resulting data.
Data were filtered at either 5 or 10 kHz and digitized at 20 kHz. All
voltage-clamp recordings were made from a holding potential of 70 mV,
averaged five times, and leak-subtracted using a standard P/4 protocol.
Voltage-clamp commands were applied in 10 mV increments.
Solutions and pharmacological agents. All solutions were
adjusted to have a pH of 7.25 and an osmotic strength of ~220 mOsm. The recording chamber was continuously perfused with a perilymph-like solution (normal extracellular solution) containing (in
mM): 112 Na+, 2 K+,
1.8 Ca2+, 0.7 Mg2+, 119 Cl , 3 D-glucose, 5 HEPES. This
solution differs somewhat from that used in previous work and was
formulated to more closely mimic the composition of perilymph (Corey
and Hudspeth, 1983a ; Bernard et al., 1986 ). Standard pipette solution
consisted of (in mM): 122 K+, 114 aspartate , 0.08 Ca2+, 4 Cl , 2 Mg2+, 5 HEPES, 1 EGTA, 1 ATP. Pharmacological agents were applied externally through two- or
five-barreled capillary glass pipettes, pulled and cut so that each
opening was ~30 µm in diameter. Localized perfusion through this
system was driven by a Picospritzer II (General Valve, Fairfield, NJ).
Solutions containing >1 mM pharmacological agents were
prepared by equimolar substitution for NaCl. The effective blocking
concentration of iberiotoxin (Ibtx) increased from nanomolar to
micromolar concentrations during several months of storage at 80°C.
For this reason relatively high concentrations of Ibtx were used to
block the calcium-activated K+
(KCa) current.
For experiments in which the papain solution was perfused onto the
semi-intact preparation, papain (0.25 mg/ml) and L-cysteine (2.5 mM) were added to normal extracellular solution (the
same concentrations used in the dissociation procedure). In control experiments, papain was heat-inactivated by boiling for ~5 min, either before or after adding the remaining components of the solution.
In either case the osmolarity was adjusted to ~220 mOsm after
boiling.
Data analysis. Most data analysis was performed using
pClamp6. Additional analysis and plotting were performed using Excel 4.0 (Microsoft Corp., Redmond, WA), IgorPro (WaveMetrics, Lake Oswego,
OR), and Mathcad (MathSoft, Cambridge, MA). Despite using low-resistance recording pipettes and active series resistance compensation, the residual uncompensated series resistance
(Rseries; ~4 M for whole-cell
recordings and ~15 M for perforated patch recordings) caused
significant errors in the command potential while large currents were
flowing. For this reason the voltage amplitudes reported in this paper
were corrected for errors due to Rseries.
Rseries was calculated by dividing the time
constant ( ), fitted to the falling phase of the capacitive transient
evoked by a small voltage step, by the membrane capacitance determined from the area under the capacitive transient. The
Rseries correction made it more difficult to
calculate average currents at a given potential, because the corrected
membrane potentials varied between cells. Therefore, the data (see Fig.
10D,E), as well as the average outward current at 25 mV, were calculated by linear interpolation between adjacent voltage points before averaging.
Another consequence of residual Rseries was that
the recorded membrane currents were low-pass-filtered. The only
noticeable effect of this filtering was an apparent slowing of the
Ca2+ current activation. To correct for this when
measuring Ca2+ current activation kinetics, we
deconvolved the digitized current traces shown in Figure 10 using the
equation:
where Im(n) is the
nth point in the digitized current trace,
I'm(n) is the deconvolved current
trace, t is the digital sampling interval (50 µsec),
and is the time constant for charging the cell, as described above.
Deconvolution reconstructs the unfiltered current waveform,but does not
correct for the fact that the voltage step is not instantaneous. For
this reason cells with > 0.15 msec were omitted from the data
set.
Quality of resonance. As in previous studies of electrical
resonance in hair cells, we measured the quality of resonance
(Q) using equations that describe a circuit
containing a capacitor in parallel with a resistor and inductor
connected in series (Crawford and Fettiplace, 1981 ). The step response
of such a circuit is an exponentially damped sinusoidal oscillation
having a frequency (f) and a damping time
constant, d. Such a system acts as a linear bandpass
filter in which f is near the center of the pass band. The
width of the pass band is described by:
Larger values of Q correspond to more prolonged
oscillations and a more sharply tuned cell.
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RESULTS |
Voltage oscillations: variations on the theme of resonance
Enzymatically dissociated grassfrog saccular hair cells that had
been exposed to papain for ~30 min before mechanical dissociation exclusively exhibited stereotypical electrical resonance (Fig. 2A), as previously
described in bullfrog (Lewis and Hudspeth, 1983 ; Hudspeth and Lewis,
1988b ). In contrast, hair cells in the semi-intact epithelial
preparation, which had suffered neither exposure to papain nor
dissociation, showed a number of variations on this theme (Fig.
2B-D). The majority (30 of 50) exhibited damped oscillatory responses similar to those found in enzymatically dissociated cells, although at much lower frequencies (Fig.
2B). The remaining cells exhibited other types of
voltage oscillations. Twenty percent (10 of 50) exhibited a spike-like
behavior similar to that previously reported in a number of other
preparations (Fuchs and Evans, 1988 ; Fuchs et al., 1988 ; Sugihara and
Furukawa, 1989 ; Eatock et al., 1993 ), including bullfrog saccular hair
cells (Hudspeth and Corey, 1977 ). Spike-like oscillations were undamped and, in some cases, actually increased in amplitude during the current
step. In cells in which both spiking and damped oscillations were found
(Fig. 2C), spiking generally occurred at slightly lower frequencies than the oscillations. Another variation exhibited by some
(10 of 50) hair cells in the semi-intact preparation was a sawtooth at
the onset of the response (Fig. 2D,
arrow). As with the spiking behavior, the sawtooth was
usually found during larger amplitude current steps. With
lower-amplitude current injections, this sawtooth often became the
first peak of the voltage oscillation (data not shown).

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Figure 2.
Current-clamp recordings showing stereotypical
electrical resonance from an enzymatically dissociated hair cell
(A) and the variations seen in the semi-intact
epithelial preparation (B-D), evoked by
depolarizing current steps (top trace) of amplitude
Istim. A, Damped sinusoidal
voltage oscillations (Istim = 225 pA;
f = 185 Hz; Q = 15.3;
Vrest = 86 mV). B, Damped
oscillations (Istim = 100 pA;
f = 59 Hz; Q = 2.9;
Vrest = 91 mV). C,
Oscillations that gave way to spike-like behavior
(Istim = 125 pA; f = 53 Hz; Vrest = 86 mV). D,
Sawtooth (arrow) at the onset of the voltage response
(Istim = 175 pA; f = 45 Hz; Vrest = 65 mV). Resting potentials
(Vrest) were measured immediately
before the step. All recordings were made using perforated patch.
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For any given amplitude current injection, enzymatically dissociated
hair cells oscillated at approximately three times the frequency of
hair cells in the semi-intact preparation (Fig.
3A). For example, the average
oscillation frequency (f) evoked by a 100 pA
depolarizing current step was 149 Hz in enzymatically dissociated hair
cells (SD, 23 Hz; range, 103-190 Hz; n = 40) and 55 Hz
in hair cells in the semi-intact preparation (SD, 18 Hz; range, 24-105 Hz; n = 50). For both populations, f
increased with larger amplitude current steps (Fig. 3A).
Average frequencies ranged from 100 to 221 Hz (total range, 58-271 Hz)
in enzymatically dissociated hair cells and from 35 to 75 Hz (total
range, 19-170 Hz) in the semi-intact preparation for current
injections of 25-400 pA.

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Figure 3.
Average current-clamp behaviors of enzymatically
dissociated cells ( ; n = 40) and hair cells in
the semi-intact preparation ( ; n = 50).
A, Frequency-current relationships. Not all cells
oscillated at every current amplitude tested. B,
Voltage-current relationships. Membrane potential was measured either
as the steady-state voltage at the end of the current step or, when the
oscillations lasted for the duration of the step, as the average
potential around which the cell oscillated. Both panels show mean ± SD.
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Another common descriptor of the exponentially damped sinusoidal
oscillations seen in most enzymatically dissociated hair cells (Fig.
2A) is the quality of resonance
(Q), a measure of the sharpness of tuning (see
Materials and Methods). The more prolonged (less damped) the voltage
oscillations, the larger the Q value and the more tightly
tuned the hair cell is to that frequency. Like f,
Q varied with the size of injected current. In most cells, the peak Q was seen during small current steps (25-100 pA)
that produced voltage oscillations between 50 and 60 mV. In
enzymatically dissociated hair cells, peak Q varied between
2.6 and 166 (median, 13.6; n = 22) and the f
at peak Q, the frequency to which the cells are expected to
be maximally tuned, was 147 ± 34 Hz (mean ± SD). Cells with
high Q values showed little, if any, damping during the 100 msec current step. In the semi-intact preparation, many hair cells
exhibited voltage oscillations that were clearly not damped sinusoids
(eg., Fig. 2C). The subset of hair cells that did exhibit
damped sinusoidal oscillations (eg., Fig. 2B) had
peak Q values that varied from 2.2 to 4.3 (median, 3.3;
n = 22) with f at peak Q of
53 ± 26 Hz (mean ± SD). Inclusion of the 10 cells that
exhibited undamped spike-like behavior (Q assumed to be )
raised the median Q to 3.5 (n = 32).
In response to small (<150 pA) depolarizing current steps,
enzymatically dissociated hair cells tended to depolarize a few millivolts more than cells in the semi-intact preparation (Fig. 3B), but otherwise the two populations operated in identical
voltage ranges. The average resting potential in both populations was 68 mV, and the range of resting membrane potentials was similar ( 51
to 90 mV for enzymatically dissociated hair cells and 57 to 90 mV
in the semi-intact preparation). The very hyperpolarized resting
potentials sometimes seen in both preparations may have been caused by
loss of the transduction apparatus during dissection, which normally
supplies a constant inward current at rest (Corey and Hudspeth, 1983b ).
Resting potentials were measured before the depolarizing test stimuli;
after depolarization the membrane potential of some cells in both
populations hyperpolarized to the K+ equilibrium
potential (approximately 90 mV), possibly due to the activation of
the inward rectifier K+ (KIR)
current that was first noted in bullfrog saccular hair cells (Corey and
Hudspeth, 1979 ), and that has also been found in both grassfrog
preparations (Holt and Eatock, 1995 ; Armstrong and Roberts, 1997 ). Even
without stimulation, some cells from both populations displayed similar
bistable membrane potentials.
K+ currents in enzymatically dissociated
hair cells
Previous biophysical and modeling studies have attributed the
generation of resonance exhibited in enzymatically dissociated bullfrog
saccular hair cells to the interplay of a voltage-dependent Ca2+ current with a single outward current,
KCa (Lewis and Hudspeth, 1983 ; Hudspeth and Lewis,
1988a ,b ). Although a voltage-dependent, delayed-rectifier type
K+ current (KV) has been found in
a number of other species (Fuchs and Evans, 1990 ; Steinacker and
Romero, 1991 ; Goodman and Art, 1996 ), and intracellular recordings
performed in intact bullfrog sacculus have suggested its presence
(Corey and Hudspeth, 1979 ), this current was not found to contribute
appreciably to resonance in enzymatically dissociated bullfrog saccular
hair cells. To test for a possible contribution of KV to
resonance in enzymatically dissociated grassfrog saccular hair cells,
we exploited the differential sensitivity of KV and
KCa currents to pharmacological agents. We used
concentrations of 4-AP (1 mM) and TEA (6 mM)
that in turtle cochlear hair cells were found to block almost
exclusively KV and KCa, respectively
(Goodman and Art, 1996 ). In all enzymatically dissociated hair cells
tested, application of 1 mM 4-AP had no effect on resonance
(n = 11; Fig.
4A), whereas 6 mM TEA reversibly eliminated resonance in these hair cells
(n = 11; Fig. 4B).

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Figure 4.
Effects of 1 mM 4-AP and 6 mM TEA on current-clamp recordings from enzymatically
dissociated hair cells. A, Resonance recorded in normal
extracellular solution (control:
Istim = 200 pA; f = 225 Hz; Vrest = 72 mV) was not affected by
4-AP. B, TEA reversibly eliminated resonance
(control, solid line: Istim = 200 pA; f = 222 Hz;
Vrest = 52 mV). Oscillations recovered
fully when TEA was removed (recovery, dotted line). Both
recordings were made using perforated patch. The records in
A are the average of five presentations.
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An A-type, inactivating K+ current
(KA) has also been reported in enzymatically
dissociated bullfrog saccular hair cells (Lewis and Hudspeth, 1983 ;
Hudspeth and Lewis 1988a ) but is largely inactivated in the voltage
range in which these cells resonate (Hudspeth and Lewis, 1988a ; Murrow,
1994 ) and has therefore been considered not to play a role in
resonance. Figure 4A supports this conclusion, because 1 mM 4-AP is expected to eliminate the majority of
KA (Thompson, 1977 ; Murrow, 1994 ). To more conclusively
rule out the possibility that KA was involved, we applied
20 mM 4-AP, a concentration that has been found to be more
than sufficient to eliminate KA in many types of cells
(Thompson, 1977 ; Lewis and Hudspeth, 1983 ; Rudy, 1988 ; Murrow, 1994 ).
This high concentration of 4-AP also had no effect on resonance (data
not shown).
Together, these findings support the conclusion that in enzymatically
dissociated grassfrog saccular hair cells, as in bullfrog, the only
K+ current integrally involved in the generation of
resonance is KCa. The story is, however, quite different
and more complex in hair cells that have suffered neither enzymatic
treatment nor dissociation from the epithelium.
K+ currents in hair cells in the
semi-intact preparation
Comparison of Figures 4 and 5 shows
that the effects of 1 mM 4-AP and 6 mM TEA on
hair cells in the semi-intact epithelial preparation were quite
different from their effects on enzymatically dissociated hair cells.
Application of 1 mM 4-AP eliminated voltage oscillations in
the majority (11 of 14) of hair cells in the semi-intact preparation
(Fig. 5A). Because, as mentioned above, 1 mM
4-AP is expected to block most of KA in addition to
KV, these data do not address whether only one or
both of these conductances were involved. Interestingly, the three
cells on which 4-AP had no discernible effect also oscillated at higher
frequencies (90-125 Hz in response to 100 pA current steps) than the
11 others (57-76 Hz), making them appear more like enzymatically
dissociated cells. Application of 6 mM TEA to hair cells in
the semi-intact preparation never eliminated the oscillations as it did
in enzymatically dissociated cells (Fig. 4B). In
fact, in the majority (8 of 11) of these cells, sinusoidal oscillations
were replaced by spike-like behavior (Fig. 5B), similar to
the spiking found in some cells in the absence of TEA. This suggests
that the cells that spiked in the absence of TEA contained a dominating
KV current, as in chick cochlea (Fuchs and Evans, 1990 ) and
goldfish sacculus (Sugihara and Furukawa, 1989 ).

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Figure 5.
Effects of 1 mM 4-AP and 6 mM TEA on current-clamp recordings from hair cells in the
semi-intact epithelial preparation. A, Voltage
oscillations recorded in normal extracellular solution (control,
solid line: Istim = 225 pA;
f = 82 Hz; Vrest = 70
mV) were eliminated by 4-AP and partially restored when 4-AP was
removed (recovery, dotted line). B, TEA
transformed the damped sinusoidal oscillations found in this cell
(control, solid line: Istim = 200 pA; f = 67 Hz; Vrest = 94 mV) into spike-like oscillations. This effect was partially
reversed when TEA was removed (recovery, dotted line).
Recordings from both cells were made using perforated patch. The traces
in A are the average of five presentations.
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These results indicate that in the preponderance of hair cells in the
semi-intact preparation, a voltage-dependent K+
current (KV and/or KA) was integral to
the generation of voltage oscillations. Furthermore
KCa, although present, was not necessary for the
generation of voltage oscillations (spikes) in these cells but did
appear to play role in modulating the shape of the response.
Voltage-clamp recordings
We now turn our attention to more directly assessing which ionic
currents are present in each hair cell preparation by examining, under
voltage-clamp conditions, the time-dependence, voltage- dependence, and
pharmacological sensitivity of the currents.
Outward currents in enzymatically dissociated hair cells
Currents recorded from enzymatically dissociated hair cells bathed
in normal extracellular solution were remarkably stereotyped. In
response to depolarizing voltage steps from a holding potential of 70
mV, a small blip of inward current was rapidly overtaken by a large
outward current that reached maximal activation quickly and showed no
sign of inactivation at any amplitude voltage tested (Fig.
6A-C, left
panels). This outward current was indistinguishable from the
KCa current found in enzymatically dissociated hair cells from bullfrog sacculus (Lewis and Hudspeth, 1983 ; Hudspeth and Lewis,
1988a ) and also resembled the KCa currents described in saccular hair cells from fish (Sugihara and Furukawa, 1989 ; Steinacker and Romero, 1991 ) and cochlear hair cells from turtle (Art and Fettiplace, 1987 ), alligator (Fuchs and Evans, 1988 ), chick (Fuchs and
Evans, 1990 ), and lizard (Eatock et al., 1993 ). The average current
amplitude at the end of a 50 msec step to 25 mV was 3.9 ± 0.35 nA (mean ± SEM; n = 18). After the return of the
membrane potential to 70 mV, we observed decaying outward tail
currents that indicate the time needed for the channels to close. In
enzymatically dissociated hair cells, the tail current decay after a
step to 25 mV was well approximated by a single exponential with an
average time constant of 3.9 ± 0.24 msec (mean ± SEM;
n = 17).

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Figure 6.
Effects of TEA, Ibtx, and 4-AP on outward currents
in enzymatically dissociated hair cells. Essentially all of the outward
current recorded in normal extracellular solution (control) was
eliminated by 6 mM TEA (A) or 2 µM Ibtx (B). Application of 1 mM 4-AP (C) had no effect. The panels
to the right show the I-V
relationship for each cell before ( ) and during ( ) drug
application. Currents for I-V plots were
calculated at the end of each 50 msec step. All recordings were made
using a whole-cell configuration and from a holding potential of 70
mV. For each family of traces, the largest amplitude voltage step
(corrected for series resistance errors) is indicated next to the step
protocol. For clarity, some of the data traces used to construct the
I-V plots are not shown.
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Our pharmacological dissection of this large, rapidly activating
outward current under voltage-clamp conditions is consistent with our
current-clamp data that, in turn, agree with previous findings from
bullfrog (Lewis and Hudspeth 1983 ; Hudspeth and Lewis 1988a ).
Application of 6 mM TEA eliminated all but a small residual
outward current (Fig. 6A; n = 10), as
did Ibtx (Fig. 6B; n = 7), a scorpion
toxin highly selective for the large conductance KCa
channel (Galvez et al., 1990 ). The ability of Ibtx to eliminate essentially all of the outward current leads us to conclude that only
KCa contributed significantly to the outward current in
these cells. This conclusion is further substantiated by the
observation that 1 mM 4-AP, a concentration expected to
block all of KV (Goodman and Art, 1996 ) and most of
KA (Murrow, 1994 ), did not alter the outward current (Fig.
6C; n = 8). Thus, there is no evidence for the contribution of either KV or KA to the
outward current evoked from a holding potential of 70 mV in
enzymatically dissociated grassfrog saccular hair cells.
Outward currents in hair cells in the semi-intact
epithelial preparation
As in enzymatically dissociated hair cells, depolarizing voltage
steps applied to hair cells in the semi-intact preparation evoked a
small inward current that was rapidly overtaken by a large outward
current. However, the shape of the outward current was quite different
from that seen in enzymatically dissociated hair cells (compare Figs.
6, 7, left panels). At all
voltages the outward current rose quickly, leveled off or decayed
slightly, and then continued rising. During large-amplitude voltage
steps the current reached a second peak and then decayed, whereas with smaller steps the current was often still rising at the end of the 50 msec step (Fig. 7A-D, left panels). Although
nearly all cells in this preparation possessed these major attributes,
there was much more variability in the recordings from these cells
(Fig. 7, compare left panels) than in enzymatically
dissociated hair cells. The average size of the outward current at 25
mV was 2.0 ± 0.2 nA (mean ± SEM; n = 21),
approximately half that in enzymatically dissociated hair cells, and
the time constant for tail current decay was nearly twice as long
(6.5 ± 0.2 msec, mean ± SEM; n = 20). The
complex shape of the outward currents in the semi-intact preparation
suggests that more than one conductance was involved. As we shall see,
pharmacological dissection supports this hypothesis.

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Figure 7.
Effects of TEA, Ibtx, and 4-AP on outward currents
from hair cells in the semi-intact epithelial preparation. Application
of 6 mM TEA (A) or 1 µM
Ibtx (B) blocked a fast component of the outward
current, leaving a more slowly activating component. 1 mM
4-AP (C) blocked a slow component of the outward
current, leaving a rapidly activating outward current that partially
inactivated. Nearly all outward current was eliminated by applying both
1 mM 4-AP and 6 mM TEA
(D). The panels to the right show
the I-V relationship for each cell
before ( ) and during ( ) drug application (see Fig. 6 legend). The
recordings in B were made using perforated patch; the
others (A, C, D) were made in the whole-cell
configuration.
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Rather than eliminating nearly all outward current, as in enzymatically
treated hair cells, 6 mM TEA blocked only about half of the
outward current in the semi-intact preparation (Fig. 7A; n = 8), leaving behind a slowly activating component.
Ibtx had a similar effect (Fig. 7B; n = 5).
Application of 1 mM 4-AP also blocked about half of the
outward current but left behind a current that activated rapidly and
then partially inactivated (Fig. 7C; n = 8).
Co-application of 4-AP and TEA eliminated essentially all of the
outward current (Fig. 7D; n = 11).
To visualize the current blocked by each drug, we subtracted the
currents recorded during drug application from control currents recorded before drug application (Fig.
8). As suggested by Figure 7,
A and B, TEA and Ibtx blocked similar components
of the outward current (Fig. 8A,B). In both cases the
current sensitive to these agents activated rapidly and then partially
inactivated. The differences between Figure 8A and
Figure 8B are indicative of the variability between cells,
rather than differential effects of the drugs. These subtractions
suggest that the TEA- and Ibtx-sensitive current (Fig.
8A,B) was the same component of the
outward current that was insensitive to 4-AP (Fig. 7C).
Conversely, the current blocked by 1 mM 4-AP (Fig.
8C) was similar to the TEA- and Ibtx-insensitive component
(Fig. 7A,B). Together, the TEA- and
Ibtx-sensitive component and the and 4-AP-sensitive component
constituted nearly all of the outward current (Fig. 7D).
Therefore, as previously demonstrated in turtle cochlear hair cells
(Goodman and Art, 1996 ), 6 mM TEA and 1 mM 4-AP
seemed to provide a good pharmacological separation of the outward
current into two components.

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Figure 8.
TEA-, 4-AP-, and Ibtx-sensitive currents
(dark traces) in hair cells in the semi-intact
epithelial preparation obtained by subtracting the currents after drug
application (smaller-amplitude light traces) from the
currents in control conditions (larger-amplitude light
traces). A, Current blocked by 6 mM
TEA activated rapidly and partially inactivated. B, One
micromolar Ibtx blocked a similar component of the current.
C, One millimolar 4-AP blocked a slowly activating
current. Because of series resistance errors in the step potential it
was necessary to estimate the current at 20 mV by linear
interpolation of currents from adjacent voltage steps. These are the
same cells as in Figure 8A-C.
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Based on the high specificity of Ibtx for KCa channels, we
identified the TEA- and Ibtx-sensitive component as a partially inactivating KCa current. The 4-AP-sensitive component
could be KV, which has been found in other hair
cells, or possibly KA, although this current is
expected to be inactivated at the holding potential of 70 mV
(Hudspeth and Lewis, 1988a ; Murrow, 1994 ). Further experiments are
under way to more definitively identify these currents.
Transformation of voltage oscillations and outward currents
by papain
So far we have shown that the characteristics of the voltage
oscillations and outward currents in enzymatically dissociated hair
cells were strikingly different from what we found in the semi-intact
epithelium. We now demonstrate that these differences were due to
enzyme treatment, rather than dissociation of the hair cells from the
saccular epithelium.
Application of the papain solution directly onto the semi-intact
preparation, at the same concentration used in the standard hair cell
dissociation procedure, transformed the hair cells in situ
(Fig. 9). In addition to comparing
populations of hair cells in the semi-intact preparation before and
after enzyme exposure, we made continuous current-clamp recordings from
two cells during papain application. In these cells, enzyme exposure
raised the frequency of the voltage oscillations more than three times
and metamorphosed the oscillation into a waveform that resembled the stereotypical resonance seen in dissociated hair cells (Fig.
9A). Subsequent application of 6 mM TEA to the
cell in Figure 9A reversibly eliminated the voltage
oscillations (data not shown). Such an effect of TEA was always
observed in enzymatically dissociated hair cells (Fig.
4B) and never in untreated hair cells in the semi-intact preparation (Fig. 5B). Likewise, application of
the papain solution to hair cells in the semi-intact preparation
transformed the outward currents into those typical of enzymatically
dissociated cells (Fig. 9B; n = 4). The low
quality of the resonance found after papain treatment (Fig.
9A), as well as the reduction in the amplitude of the
outward current after treatment (Fig. 9B), effects opposite
to those seen in population studies, are likely to be due to rundown
that typically occurs during prolonged recording.

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Figure 9.
Papain transforms voltage oscillations and outward
currents in the semi-intact epithelium in situ. Traces
from continuous perforated patch recordings taken before
(control) and after perfusion of papain solution
onto the epithelium. A, After 15 min in papain, the
frequency of the voltage oscillations recorded in current-clamp
increased from 36 Hz to 164 Hz. (Istim = 200 pA; Vrest = 72 mV in control and 91 mV
after papain treatment). Traces are the average of 10 presentations.
B, In another cell, the papain solution transformed the
outward currents from those typical of hair cells in the semi-intact
epithelial preparation (control) into currents
typical of enzymatically dissociated hair cells (after 21 min in
papain). The time constant for decay of the tail current after voltage
steps to 36 mV decreased from 6.5 msec before enzyme treatment to 4.4 msec. The largest amplitude voltage step (corrected for series
resistance errors) is indicated next to the step protocol.
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The enzyme solution used in these experiments was made by adding papain
(a partially purified preparation of papaya latex; see Materials and
Methods), plus an activating agent, L-cysteine, to the
normal extracellular solution. As a first step in characterizing the
active agent in this solution, we tested the effects of omitting or
heat-inactivating the papain. No transformation of voltage oscillations
or outward currents was seen when normal extracellular solution
containing 2.5 mM L-cysteine without papain was
perfused onto hair cells in the semi-intact preparation. Furthermore,
hair cells in a semi-intact preparation that had been incubated in heat-inactivated papain (see Materials and Methods) for 30 min retained
low-frequency oscillations and currents typical of untreated hair
cells. Thus, we see that some heat-sensitive component of papain caused
the transformation of the voltage oscillations and outward currents
in situ and that dissociation was not required. These
results suggest that the proteolytic activity of the enzyme was
responsible for the differences in voltage- and current-clamp responses
found in these two populations of cells.
Ca2+ current isolation
To assess whether the enzymatic dissociation procedure affected
the Ca2+ current, we blocked the outward currents by
substituting the K+ in the internal solution with
Cs+. Figure
10, A and B,
shows examples of such recordings. A noticeable sag in inward current
during depolarizations above 30 mV was found in the majority (9 of
10) of recordings from hair cells in the semi-intact preparation (Fig.
10A) but not in enzymatically dissociated hair cells
(Fig. 10B; n = 12). This sag is
reminiscent of a current seen in turtle cochlear hair cells that was
attributed to Cs+ efflux through small-conductance
calcium-activated K+ (SK) channels (Tucker and
Fettiplace, 1996 ). SK channels in hair cells are thought to be present
at the sites of efferent synaptic input and appear to be involved in
ACh-mediated hyperpolarization in response to efferent stimulation
(Fuchs and Murrow, 1992 ). Consistent with this interpretation, we found
that when K+ was replaced by a larger cation, NMG,
the sag current was not present in 11 of 13 recordings from hair cells
in the semi-intact preparation (Fig. 10C), a result also
reported in turtle cochlear hair cells (Tucker and Fettiplace, 1996 ).
Therefore, efflux of Cs+ through SK is a likely
explanation for this sag in inward current found only in hair cells in
the semi-intact preparation and not in enzymatically dissociated
cells.

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Figure 10.
Isolation of Ca2+
currents. All recordings, except for C, were made with
Cs+ internal solution. A, A sag in
the inward current was evident in hair cells in the semi-intact
preparation but not in enzymatically dissociated hair cells
(B). C, NMG internal solution
blocked the sag. The corresponding voltage steps (corrected for series
resistance errors) are indicated by each trace
(A-C). D, Peak
Ca2+ current I-V
relationships from enzymatically dissociated hair cells ( ,
n = 12) and hair cells in the semi-intact
preparation ( , n = 10). E,
Ca2+ current activation kinetics
( m, see text for definition) versus membrane
potential (symbols are the same as in D: ,
n = 11; , n = 7). All
recordings were made in the whole-cell configuration with 10 mM extracellular Cs+ to eliminate the
activation of a KIR current during the leak pulses. Values
in D and E are mean ± SEM.
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We found no differences in the peak Ca2+ current
recorded with Cs+ internal solution in the two
preparations (363 ± 46 pA in the semi-intact preparation and
375 ± 40 pA in enzymatically dissociated hair cells; mean ± SEM; n = 10 and 12, respectively), but we did find
differences in the current-voltage relationships and the activation
kinetics (Fig. 10D,E). The voltage-dependence of the Ca2+ current in enzymatically dissociated hair cells
(Fig. 10D, open symbols) was similar to
what has previously been reported in enzymatically dissociated bullfrog
saccular hair cells (Hudspeth and Lewis, 1988a ). The
Ca2+ current in hair cells in the semi-intact
preparation, however, was shifted ~7 mV in the hyperpolarizing
direction (Fig. 10D, filled symbols). The
Ca2+ current recorded in this preparation reached
half-maximal activation at 45 mV and peaked at 22 mV, whereas in
enzymatically dissociated hair cells it was half-maximal at 38 mV and
maximally activated at 15 mV. This shift cannot be attributed to the
presence of SK in the semi-intact preparation, because an ~7 mV shift
was maintained in recordings made with NMG internally. Additionally, comparison of the currents evoked by voltage steps to approximately 50 mV, a potential at which SK did not appear to be activated, clearly shows that in the semi-intact preparation the
Ca2+ current was activated to a much greater extent
than in enzymatically dissociated hair cells (Fig. 10, compare
A,B).
To compare the activation kinetics of the Ca2+
current in the two preparations we fit the recorded currents with a
third order kinetic scheme:
where Ca is the maximal
Ca2+ current and m is the time
constant for one of three theoretical gating particles. As reported previously (Hudspeth and Lewis, 1988a ), this third-order scheme provided a good fit to the data. The m versus voltage
relationships from the two preparations show that the activation
kinetics of the Ca2+ current were voltage-dependent
and, with the exception of the point at 50 mV, the kinetics in
enzymatically dissociated hair cells were slower than in the
semi-intact preparation (Fig. 10E). In the
semi-intact preparation m decreased (the
Ca2+ current activated faster) monotonically with
increasing depolarization, whereas in enzymatically dissociated hair
cells m reached a peak at 40 mV.
 |
DISCUSSION |
Tuning in isolated hair cells and intact preparations
Several lines of evidence suggest that tuning can be greatly
altered when hair cells are dissociated from the sensory epithelium. Intracellular recordings in the intact turtle cochlea demonstrate that
there is good agreement between a hair cells' electrical resonant
frequency and characteristic auditory frequency (Crawford and
Fettiplace, 1981 ). However, the range of resonant frequencies exhibited
by isolated turtle cochlear hair cells does not match the range of
resonant frequencies found in the intact cochlea (Art and Fettiplace,
1987 ). This type of discrepancy exists in a number of other auditory
and vestibular preparations, including frog sacculus (for more detailed
discussion, see Eatock et al., 1993 ). Recordings from afferent axons
have shown that the bullfrog sacculus responds maximally to auditory
and seismic stimulation at frequencies <100 Hz (Lewis, 1988 ; Yu et
al., 1991 ). In another study of mixed populations of axons from the
sacculus and amphibian papilla, most axons were maximally sensitive to
frequencies between 40 and 70 Hz (Koyama et al., 1982 ). Similarly,
intracellular recordings from hair cells in the intact saccular
epithelium showed that these cells exhibited electrical resonance at
frequencies of 11-85 Hz (Ashmore, 1983 ). In contrast, enzymatically
dissociated hair cells from both grassfrog (this work) and bullfrog
sacculus (Lewis and Hudspeth, 1983 ; Hudspeth and Lewis, 1988b ) exhibit
electrical resonance at frequencies >100 Hz. There is also
disagreement in the sharpness of tuning. Average Q values
from intact saccular preparations were found to be low (~2),
suggesting that saccular hair cells are broadly tuned (Ashmore, 1983 ;
Lewis, 1988 ). In contrast, Q values up to 12.6 have been
reported in enzymatically dissociated bullfrog saccular hair cells
(Hudspeth and Lewis, 1988b ), and in grassfrog we found Q
values up to 166 (median Q = 13.6), suggesting that
these sensory cells can be tightly tuned to a narrow range of
frequencies.
These differences in f and Q, in addition to
discrepancies in the shapes of tuning curves and the phases of
responses, and the small temperature-dependence of tuning, have led
several researchers to conclude that hair cells are not exclusively
tuned electrically (Lewis, 1988 ; Eatock et al., 1993 ; Egert and Lewis,
1995 ). Instead, they hypothesize that, as in mammals, some form of
mechanical feedback is essential for the tuning of auditory and
vestibular organs of nonmammalian vertebrates. This intriguing
hypothesis has important implications for hair cell tuning in these
animals. Accumulating evidence that hair cells from many nonmammalian
vertebrate species are capable of exerting forces in response to
stimulation (Benser et al., 1996 ; for review, see Hudspeth, 1997 ) fits
nicely with the idea that mechanical feedback plays a role in tuning. Alternatively, however, it could be argued that these forces are simply
a byproduct of transduction. Therefore, the role of mechanical feedback
in the tuning of nonmammalian vertebrates remains an open question.
As this study demonstrates, some of the evidence against electrical
tuning of the frog sacculus, namely the discrepancies in f
and Q noted above, is artifactual and can be directly
attributed to the use of papain during cell dissociation. Hair cells in
the semi-intact preparation, cells not exposed to papain, exhibited electrical resonance of frequencies between 35 and 75 Hz and
Q values of ~3. These values are more consistent with
those reported from more intact preparations (f < 100 Hz; Q ~ 2). Thus, the electrical tuning found
in the majority of hair cells in the frog sacculus is sufficient to
account for the frequency discrimination of this organ, and the need
for a mechanical feedback mechanism may not be essential. Further
experiments, however, are needed to account for the other
discrepancies.
Resonant frequencies and K+ conductances
The Hudspeth and Lewis (1988b) model of electrical resonance shows
that the Ca2+ and KCa currents found in
enzymatically dissociated frog saccular hair cells are sufficient to
explain the stereotypical electrical resonance exhibited by these hair
cells. However, as this work demonstrates, this model does not describe
the normal operation of these cells but describes the properties of
cells that have been distorted by the enzyme used in the dissociation
procedure.
Rather than exhibiting exclusively stereotypical electrical resonance,
hair cells in the semi-intact preparation, cells not subject to enzyme
exposure, showed a variety of voltage behaviors in addition to damped
sinusoidal oscillations. Our finding that at least two
K+ currents (KV and a
KCa) rather than a single K+
current are involved in the generation of voltage responses in these
cells could explain this diversity. One might imagine that such variety
could easily be achieved by varying the relative contribution of each
current.
Studies of hair cells from the auditory and vestibular organs of
several species have shown that a cell's resonant frequency is
determined primarily, though not exclusively, by the properties of its
outwardly rectifying K+ currents. For example, the
tonotopical organization of the turtle cochlea appears to be the result
of a smooth gradient in the kinetics of the hair cells'
K+ currents (Art and Goodman, 1996 ). Although it
remains to be discovered exactly how this gradient in kinetics is set
up, this organ seems to use two strategies: varying the kinetics of a
single channel type (KCa; Art et al., 1995 ) and
varying the contribution of fast (KCa) and slow
(KV) outward currents (Goodman and Art, 1996 ). Whereas hair cells that resonate at frequencies >100 Hz contain only
KCa currents, and cells that resonate at frequencies <60 Hz contain predominantly KV currents, cells that resonate
in the 50-100 Hz range express a mixture of KV and
KCa. Hair cells from frog sacculus seem to follow suit. The
majority of the hair cells in the semi-intact preparation exhibited
voltage oscillations between 35 and 75 Hz and were found to contain
both KV and KCa. Hair cells that exhibited
spike-like oscillations, which we hypothesize contain dominant
KV currents, oscillated at slightly lower frequencies (generally <60 Hz). Additionally, the few hair cells in this
preparation that showed no evidence of containing
KV, the three 4-AP-insensitive cells, oscillated at
higher frequencies, between 90 and 125 Hz.
Given that papain alters frog saccular hair cells so dramatically, it
is surprising that after enzymatic dissociation these cells exhibit
such beautiful oscillatory behavior. Perhaps even more surprising is
that enzymatically dissociated hair cells fit nicely in the
K+ current versus frequency scheme found in turtle.
These cells, which on average resonated at frequencies of 100-221 Hz,
were found to contain only a KCa current. Thus, frog
saccular hair cells can be transformed from mid-frequency cells,
containing both KV and KCa, to
high-frequency cells, containing only KCa simply by
exposing them to papain. How this transformation occurs we cannot
explain.
Conductances in frog saccular hair cells
Here we demonstrate that, like a number of other hair cell
preparations (Fuchs and Evans, 1990 ; Steinacker and Romero, 1991 ; Goodman and Art, 1996 ), frog saccular hair cells (semi-intact preparation) contain a KV current. Additionally, these
cells were found to contain a transient KCa current,
distinctly different from the KCa current found in
enzymatically dissociated hair cells. The finding that the
KCa current in frog saccular hair cells is transient is
very unusual. Although it has been demonstrated that an inactivating
KCa current is present in rat chromaffin cells (Solaro and
Lingle, 1992 ), this serves as the only clear demonstration of an
inactivating KCa current. Other KCa channels,
including the one recently cloned from chick cochlea, cSlo (Jiang et
al., 1997 ), do not exhibit inactivation. We are currently investigating this unusual feature of the KCa current in frog saccular
cells.
As in bullfrog (R. catesbeiana), KA (Lewis and
Hudspeth, 1983 ; Hudspeth and Lewis 1988a ) did not appear to play a role
in resonance in enzymatically dissociated grassfrog (R. pipiens) hair cells. Additional experiments will be needed to
determine whether hair cells in the semi-intact epithelium have a
KA current, and if so, whether it plays any role in
resonance. Given that this current is expected to be inactivated in the
voltage range in which hair cells resonate (Hudspeth and Lewis, 1988a ;
Murrow, 1994 ), such a role for KA seems unlikely. We have
previously shown that at least one type of KIR is present
in hair cells in the semi-intact preparation (Armstrong and Roberts,
1997 ) but have not determined whether both types of KIR
that have been reported in enzymatically dissociated grassfrog hair
cells (Holt and Eatock, 1995 ) are present. Evidence for a third
K+ current, SK, was found in hair cells in the
semi-intact epithelial preparation but not in enzymatically dissociated
hair cells.
Based on its ionic permeability, sensitivity to dihydropyridines, and
lack of inactivation (Fuchs et al., 1990 ; Roberts et al., 1990 ; Zidanic
and Fuchs, 1995 ), the Ca2+ current in hair cells is
thought to be L-type (however, see Su et al., 1995 ), although it
activates at more hyperpolarized potentials than typical L-type
currents (Fox et al., 1987 ). Our finding that the
Ca2+ current in hair cells in the semi-intact
preparation activated at more hyperpolarized potentials (~7 mV) than
in enzymatically dissociated hair cells means that, in this respect,
the L-type characteristics of this current are even less typical.
Additionally, the activation kinetics of the Ca2+
current in the semi-intact preparation were faster than previously appreciated.
Enzyme effects
Perhaps our finding that proteolytic enzymes dramatically alter
the ionic conductances of frog saccular hair cells is not so
surprising. For years it has been known that, when applied intracellularly, proteolytic enzymes can eliminate inactivation of
Na+ channels (Armstrong et al., 1973 ), and more
recently, of Shaker K+ channels (Hoshi et
al., 1990 ) and KCa channels (Solaro and Lingle, 1992 ).
Although there is less information available on extracellular effects
of enzymes, there are reports that dissociation of rod outer segments
with papain can alter their electrical properties (Hestrin and
Korenbrot, 1987 ; Shen et al., 1995 ) and ultrastructure (Townes-Anderson
et al., 1985 ). So, although the finding that enzyme treatment alters
ionic conductances may not be surprising, as this study demonstrates,
one must use great caution in assessing the properties of cells that
have suffered enzymatic digestion; extracellular application of enzymes
can dramatically alter the membrane properties of cells.
 |
FOOTNOTES |
Received Jan. 20, 1998; accepted Feb. 9, 1998.
This work was supported by National Institutes of Health Grant NS27142,
predoctoral fellowship Training Grant GM07257, and a Grant from the
Medical Research Foundation of Oregon. We thank Drs. B. D. Anson,
B. Edmonds, D. Lenzi, and P. M. O'Day for careful dissection of
this manuscript, J. W. Runyeon for scanning electron microscopy,
and M. W. Armstrong for Canis familiaris hair.
Correspondence should be addressed to Dr. William M. Roberts, Institute
of Neuroscience, 1254, University of Oregon, Eugene, OR 97403-1254.
 |
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