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The Journal of Neuroscience, January 15, 1998, 18(2):610-624
Plasma Membrane Ca2+-ATPase Extrudes Ca2+
from Hair Cell Stereocilia
Ebenezer N.
Yamoah1, 3,
Ellen A.
Lumpkin4,
Rachel
A.
Dumont1,
Peter J. S.
Smith3,
A. J.
Hudspeth4, and
Peter G.
Gillespie1, 2
Departments of 1 Physiology and
2 Neuroscience, The Johns Hopkins University, Baltimore,
Maryland 21205, 3 BioCurrents Research Center, Marine
Biological Laboratory, Woods Hole, Massachusetts 02543, and
4 Howard Hughes Medical Institute and The Rockefeller
University, New York, New York 10021
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ABSTRACT |
Mechanically sensitive hair cells of the auditory and vestibular
systems use Ca2+ to control adaptation of mechanical
transduction, to effect frequency tuning, to trigger neurotransmitter
release, and to mediate efferent synaptic signaling. To determine the
role that pumps play in regulation of Ca2+ in the
hair bundle, the organelle responsible for mechanoelectrical transduction, we localized and quantified the plasma membrane Ca2+-ATPase (PMCA) of the bundle. We found that each
hair bundle contains ~106 PMCA molecules or
~2000 per square micrometer of bundle membrane and that PMCA is the
principal calmodulin binding protein of the bundle. Consistent with
biochemical estimates of PMCA density, we measured with extracellular
Ca2+-selective electrodes a substantial
Ca2+ efflux from bundles. The number of bundle
Ca2+ pumps and magnitude of resting
Ca2+ efflux suggested that PMCA should generate a
substantial membrane current as bundles expel Ca2+.
Measurement of whole-cell currents revealed a transduction-dependent outward current that was consistent with the activity of PMCA. Finally,
dialysis of hair cells with PMCA inhibitors led to a large increase in
the concentration of Ca2+ in bundles, which suggests
that PMCA plays a major role in regulating bundle
Ca2+ concentration. Our data further indicate that
PMCA could elevate the extracellular Ca2+
concentration close to hair bundles above the low level found in bulk
endolymph.
Key words:
hair cell; hearing; calcium; ATPase; stereocilia; hair
bundle; ion-selective probe
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INTRODUCTION |
Hair cells, the receptor cells
of the auditory and vestibular systems, transduce mechanical stimuli
into changes in membrane potential (for review, see Hudspeth, 1989 ). A
hair cell carries out mechanoelectrical transduction with its hair
bundle, a sensory organelle that pivots back and forth in response to
sound or head position stimuli. In the sacculus of the American
bullfrog, Rana catesbeiana, a hair bundle consists of ~60
actin-filled processes called stereocilia and a lone true cilium, the
kinocilium (Jacobs and Hudspeth, 1990 ). Extracellular filaments called
tip links interconnect adjacent stereocilia near their tips (Pickles et al., 1984 ); each link controls one or two active transduction channels
(Hudspeth, 1982 ; Holton and Hudspeth, 1986 ; Denk et al., 1995 ; Lumpkin
and Hudspeth, 1995 ). Movement of the bundle in the direction of the
kinocilium stretches tip links and opens transduction channels, whereas
movement in the opposite direction reduces tip link tension and allows
channels to close.
Although transduction channels can pass a broad range of cations
(Corey and Hudspeth, 1979 ; Ohmori, 1985 ), transduction channels are
selective for Ca2+ over monovalent cations
(Jørgensen and Kroese, 1995 ; Lumpkin et al., 1997 ). The
Ca2+ that enters through transduction channels is
critical for hair bundle function. Ca2+ regulates
adaptation, the process by which hair cells continuously readjust their
sensitivity to small displacements (Eatock et al., 1987 ; Crawford et
al., 1991 ). Ca2+ also is required to evoke hair
bundle twitches, which may contribute to high-sensitivity displacement
detection (Benser et al., 1996 ). Finally, an elevated
Ca2+ concentration in stereocilia with active
transduction channels may suppress supernumerary tip link formation
(Zhao et al., 1996 ). Control of intracellular Ca2+
concentration is therefore critical for stereocilia, which have no
intracellular compartments in which to sequester
Ca2+ and are exposed to an extracellular fluid,
endolymph, incompatible with Na+-dependent
Ca2+ extrusion.
Recent reports have indicated that cochlear stereocilia contain plasma
membrane Ca2+ ATPase molecules (PMCA; Crouch and
Schulte, 1995 ) and that PMCA isoforms 1b, 2b, 3a, 3c, and 4b are
present in the cochlea (Crouch and Schulte, 1996 ). In this report we
localize PMCA in bullfrog hair cells and estimate that its density is
~2000 pump molecules per square micrometer of stereociliary membrane.
Bundle PMCA is active: we measure a substantial, vanadate-sensitive
Ca2+ efflux from bundles with extracellular
Ca2+-sensitive self-referencing electrodes. Analysis
of transduction currents reveals an outward current that possesses a
pharmacological profile consistent with PMCA activity. Finally, we show
that PMCA contributes significantly to control of the hair bundle
Ca2+ concentration.
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MATERIALS AND METHODS |
Materials. The anti-PMCA monoclonal antibody 5F10 was
obtained as undiluted ascites fluid from Affinity BioReagents (Golden, CO). Donkey serum, as well as Cy3-conjugated secondary antibodies, was
obtained from Jackson ImmunoResearch Labs (West Grove, PA). Blotting
membrane blocking solutions, horseradish peroxidase-coupled secondary
antibodies, and chemiluminescence reagents used for immunoblotting
(ECL) came from Amersham (Arlington Heights, IL). Streptavidin-alkaline
phosphatase and the chemiluminescence reagent used for detection of
biotinylated protein
[3-(4-methoxyspiro{1,2-dioxetane-3,2 -(5 -chloro)tricyclo[3.3.1.13,7]decan}-4-yl)phenyl
phosphate] (CSPD) were obtained from Tropix (Bedford, MA). Protein
G-Sepharose, phenyl-Sepharose, and CNBr-Sepharose were obtained from
Pharmacia (Piscataway, NJ). Fluka Chemical (Ronkonkoma, NY) was the
source of
N,N-dimethyltrimethylsilylamine and
Ca2+-Ionophore I Cocktail A. Polyvinylidene
fluoride (PVDF) membranes (Immobilon P) were purchased from Millipore
(Bedford, MA). Fluo-3 (pentapotassium salt) and 5- and 6-carboxyeosin
were obtained from Molecular Probes (Eugene, OR).
N-hydroxysulfosuccinimidobiotin (sulfo-NHS-biotin) was
purchased from Pierce (Rockford, IL). Acrylamide, bisacrylamide,
ammonium persulfate,
N,N,N ,N -tetramethylethylenediamine (TEMED), and SDS were purchased from Bio-Rad (Hercules, CA). Sodium orthovanadate came from Fisher Scientific (Pittsburgh, PA). Sigma (St.
Louis, MO) was the source of bovine hemoglobin (H-2500), bovine serum
albumin, HEPES, Tris base, Triton X-100, Na2ATP, and
3-(cyclohexylamino)-1-propanesulfonic acid (CAPS).
Immunocytochemistry. Hair cells were isolated mechanically
from the sacculus of Rana catesbeiana as described (Assad
and Corey, 1992 ; Yamoah and Gillespie, 1996 ) in frog saline solution
containing (in mM) 110 NaCl, 2 KCl, 3 D-glucose, and 5 HEPES, adjusted to pH 7.3 with NaOH that
contained 100 µM CaCl2. Subsequent
manipulations used a similar saline solution containing 4 mM CaCl2. Cells were fixed for 20 min with
0.4% formaldehyde, washed, and then permeabilized in 1% Triton X-100
for 10 min. Next they were incubated in a blocking solution (1% bovine
serum albumin and 1% donkey serum) for 1 hr, followed by a 2-3 hr
incubation with 5F10 monoclonal antibody at a dilution of 1:200 to
1:1000. Hair cells were incubated in secondary antibodies (donkey
anti-mouse conjugated with Cy3) for 2 hr, washed, and viewed with a
Zeiss LSM 410 confocal microscope. For preadsorption control
experiments, the 5F10 antibody was incubated with 5 µg/ml PMCA from
rat skeletal muscle before use.
Immunoblotting. Hair bundles and residual macula samples
were isolated as previously described (Gillespie and Hudspeth, 1991a ). Human erythrocyte PMCA, a gift of Dr. D. Kosk-Kosicka (Department of
Anesthesiology, Johns Hopkins University, Baltimore, MD), was purified
and quantified as described in Kosk-Kosicka and Inesi (1986). Proteins
were separated by SDS-PAGE, using 10% acrylamide gels with a 150:1
acrylamide-to-bisacrylamide ratio, and transferred to PVDF blotting
membranes at 100 V for 2 hr with cooling in 5% methanol and 10 mM CAPS, pH 11. To prevent losses of picogram amounts of
protein, we included 5 µg of hemoglobin in each sample and added 0.25 mg/ml hemoglobin to the pretransfer incubation solution (Gillespie and
Gillespie, 1997 ). Procedures for SDS-PAGE and electrotransfer have been
described in detail elsewhere (Gillespie and Hudspeth, 1991a ,b ;
Gillespie and Gillespie, 1997 ; Hasson et al., 1997 ). Membranes were
blocked for 2 hr with a proprietary blocking solution (Amersham Liquid
Block) diluted to 5% with PBS (150 mM NaCl and 70 mM sodium phosphate, pH 7.4) and then were incubated for 2 hr with a 1:1000 dilution of 5F10 in the blocking solution. After three
washes with 0.3% Tween-20 in PBS, blots were incubated for 1 hr with a
1:2500 dilution of horseradish peroxidase-coupled goat anti-mouse
antibodies. Blots were washed four to five times with 0.3% Tween in
PBS and then once with PBS. Subsequent detection of bound antibodies
was completed with enhanced chemiluminescence, using the
manufacturer's development methods. All procedures except
electrotransfer were performed at room temperature. PMCA in hair
bundles was quantified from blots that contained hair cell samples and
purified PMCA in known amounts that bracketed the amounts present in
hair cell samples. Films were digitized by an eight-bit scanner with a
transmission attachment (UMAX UTA-II); NIH Image (version 1.59) was
used to calculate the relative intensities of each band. A standard
curve was constructed by using the intensities of the purified PMCA
standards; the amount of PMCA present in hair cell samples was obtained
by interpolation.
Immunoprecipitation. Purified hair bundles were
permeabilized and labeled with sulfo-NHS-biotin (Gillespie and
Hudspeth, 1991a ,b ). Detergent-soluble proteins were extracted with 1%
Triton X-100 with 0.1 mg/ml bovine serum albumin as a carrier protein.
The immunoprecipitation solution also contained 150 mM
NaCl, 1 mM dithiothreitol, 10 µM leupeptin,
10 µM pepstatin, 200 µM
phenylmethylsulfonyl fluoride, and 25 mM HEPES, pH 7.5. Calmodulin was purified from bovine brain by virtue of its
Ca2+-sensitive binding to phenyl-Sepharose
(Gopalakrishna and Anderson, 1982 ); calmodulin-agarose was prepared by
coupling purified calmodulin to CNBr-Sepharose according to the
manufacturer's instructions. Triton X-100 extracts were incubated in
the presence of 0.5 mM CaCl2 with
calmodulin-agarose beads for 2 hr at room temperature; beads were
washed thoroughly with immunoprecipitation solution containing 0.5 mM Ca2+. Calmodulin binding proteins
were eluted with 5 mM EGTA. Triton X-100 extracts or
calmodulin-agarose eluates were incubated for 2 hr with 5F10 antibody
diluted 1:100 in immunoprecipitation solution; antibodies and bound
bundle proteins were separated from the supernatant fluid by adding 5 µl of protein G-Sepharose, incubating for 30 min, and
microcentrifuging to sediment the protein G-Sepharose complex. After a
thorough washing with immunoprecipitation solution, antibodies and
bound bundle proteins were eluted with a SDS-PAGE sample buffer that
included 1.5% SDS. Proteins were electrophoresed and transferred to
blotting membranes as described above; using methods previously
described in detail (Gillespie and Hudspeth, 1991b ), we detected
biotinylated bundle proteins by using streptavidin-alkaline phosphatase
at a dilution of 1:5000 and the chemiluminescence substrate CSPD.
Ca2+-selective self-referencing electrodes.
We monitored local Ca2+ fluxes near isolated
hair cells, using the Ca2+-selective
self-referencing electrode technique (Smith et al., 1994 ). Electrodes
were pulled from 1.5 mm diameter borosilicate glass with tip diameters
of 1.5-2.5 µm, dried at 180°C overnight (reducing tip size to
1-1.5 µm), and rendered hydrophobic with N,N-dimethyltrimethylsilylamine
(Ammann, 1986 ). The electrodes were tip-filled with a 15-30 µm
column of a Ca2+-ionophore cocktail (10% w/v
Ca2+-sensitive neutral carrier ETH 1001, 89% w/v
2-nitrophenyl octyl ether, and 1% w/v sodium tetraphenylborate) and
were back-filled with 100 mM CaCl2 in a 0.5%
agar gel (Smith et al., 1994 ; Yamoah and Smith, 1994 ). Electrodes were
calibrated by measuring their static responses to solutions containing
0.1, 1, and 1 mM Ca2+ (Kuhtreiber
and Jaffe, 1990 ; Smith et al., 1994 ); for a 10-fold change in
Ca2+ concentration, the change in voltage (or
sensitivity, S) was ~28 mV.
Recordings were performed in frog saline solution with 50 µM CaCl2. The electrode was moved back and
forth between two measuring positions, 2.5-10 µm apart. For
measurements of Ca2+ flux around hair cells, the
point of closest approach of the electrode was <1 µm away from a
hair bundle or soma. Flux values calculated from the differential
voltage measured between these points were compared with background
values 300-400 µm away, outside of the calcium gradient induced by
cell activity. The frequency of movement (0.3-0.5 Hz) was sufficiently
slow to allow the reestablishment of Ca2+ gradients
before data collection but was adequately fast to minimize the problems
inherent in stationary Ca2+ electrodes (Smith et
al., 1994 ). The voltages at each measuring position were amplified 1000 times and digitized (DT 2800 series analog-to-digital board; Data
Translation, Marlborough, MA). Using DVIS3 software, we collected,
pooled, and analyzed data as previously described (Smith et al., 1994 ).
To minimize the impact of noise, particularly slow random drift, we
pooled differential voltage values in a running average; the apparent
response of the electrode therefore was slowed by the averaging
process. To convert voltage readings to a net flux value, we determined
the electrode efficiency (Rv) to be 45%
(Smith et al., 1994 ). Rv reflects both the gain of the amplifier and the signal attenuation caused by the response of
the ionophore. The liquid exchange membrane used here requires ~10
sec to give a 90% response; the choice of movement frequency for the
electrode necessitates an inevitable compromise among allowing
reestablishment of a gradient, permitting the ionophore to respond
maximally, and minimizing the unavoidable drift. The difference in
Ca2+ concentration ( C) between the
extremes of electrode excursion ( r) was determined
from:
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in which V is the potential difference over the
electrode excursion and Cb is the background
Ca2+ concentration. The flux was determined from
this concentration difference and the diffusion coefficient
(D):
In some experiments the point of closest approach of the
electrode was retracted systematically from the bundle; data from these
experiments were fit via the following equation (Smith et al.,
1994 ):
in which r is the distance from the source of
Ca2+ to the electrode at its measurement position
and K is an empirical constant. Amplifiers, headstages,
motion control systems, and software were all produced at the
BioCurrents Research Center of the Marine Biological Laboratory (Woods
Hole, MA).
Stock solutions of 200 mM sodium orthovanadate were made at
pH 10, boiled to eliminate polymeric species (Goodno, 1982 ), and stored
at 20°C. Mechanical stimulation of the hair bundle was conducted
with a two-dimensional piezoelectric bimorph stimulator (Corey and
Hudspeth, 1980 ). For microinjection, pipettes were pulled from 1.5 mm
borosilicate glass; their tip resistances were 40-50 M . Pipettes
were filled with (in mM) 85 KCl, 3 MgCl2, 2 Na2ATP, 1 EGTA, and 5 HEPES,
with or without 0.2 mM vanadate. Microinjection was
performed with a Narashigi IM-200 pressure controller (Narashigi USA,
Sea Cliff, NY). The optimal injection pressure was determined by
injection of Lucifer yellow in 1 M LiCl; five 2 sec pulses
within 1 min, in continuous mode at 3 kPa, gave efficient loading
without cell disruption. Injection of control and vanadate solutions
used identical settings.
Whole-cell recording. An Axopatch 200A amplifier (Axon
Instruments, Foster City, CA) was used to record transduction currents from isolated cells at a holding potential of 80 mV with the tight-seal, whole-cell voltage-clamp technique. Bundle displacement used the stimulator described above; the kinociliary bulb of the bundle
was held tightly with modest suction through a glass micropipette that
served as a stimulus probe. This configuration prevented slippage of
the bundle relative to the stimulus probe, a degree of stability
essential for interpretation of small membrane currents. In most cases,
mechanical stimuli had durations of 100-1000 msec with an
interstimulus interval of 1.5 sec; alternating positive and negative
displacements were provided. The recording electrode solution contained
(in mM) 85 CsCl, 3 MgCl2, 2 Na2ATP, 1 EGTA, and 5 HEPES. CsOH was used to adjust the
final pH to 7.3. Frog saline solution containing 4 mM
CaCl2 and oxygenated at room temperature was used as the
bath solution. Other recording conditions were similar to those
described earlier (Yamoah and Gillespie, 1996 ).
Detection of stereociliary Ca2+. Hair
cells were isolated as described previously (Lumpkin and Hudspeth,
1995 ) and were bathed in frog saline solution containing 4 mM Ca2+. We clamped membrane potentials
at 70 mV with tight-seal whole-cell electrodes, using a voltage-clamp
amplifier (EPC-7, List Electronics, Darmstadt, Germany). The electrodes
contained (in mM) 100 CsCl, 2 Na2ATP, 3 MgCl2, 0.5 fluo-3 (pentapotassium salt), and 5 HEPES; the pH was adjusted to 7.26 by the addition of 6 mM
CsOH. When noted, 1 mM vanadate or 5 µM
carboxyeosin was added to the internal solution. Transduction was
verified by measurement of transduction currents or, in one control
cell, by the presence of elevated fluorescence at stereociliary tips (a
tip blush; Lumpkin and Hudspeth, 1995 ). To elicit a transduction
current, we displaced a hair bundle 300 nm in the positive direction
with a glass micropipette. Maximal transduction currents for cells
dialyzed with vanadate ranged from 40 to 190 pA, those for cells
dialyzed with carboxyeosin ranged from 40 to 215 pA, and those for
control cells ranged from 70 to 190 pA. Because the fluorescence
signals became variable as cells became leaky, data collected after the
leakage current of a cell exceeded 250 pA were excluded from the
study.
To detect changes in the free Ca2+ concentration of
hair bundles, we simultaneously visualized hair cells loaded with
fluo-3 via epifluorescence and differential interference contrast
optics with a Zeiss LSM 410 confocal microscope equipped with a 63×, oil-immersion objective lens of numerical aperture 1.4. The line scan
mode of the confocal microscope was used to follow fluorescence changes
in a hair bundle at 1.4 msec intervals before, during, and after
positive displacements. To minimize variability between cells, we
imaged the focal plane in each cell in which the fluorescence intensity
of the bundle was maximal. To ensure that fluorescence intensities
could be compared between cells, we normalized raw intensity data by
the confocal gain; other settings were held constant during image
acquisition. All images were processed identically with NIH Image
1.59.
To estimate the fluorescence intensity of the hair bundle in each
image, we used a graphics cursor provided by the software of the
confocal system (LSM 3.95, Zeiss, Jena, Germany) to outline a region
encompassing only the hair bundle. The intensities of pixels within the
specified area then were averaged. To determine the somatic
fluorescence, we similarly measured the average intensity of a region
just below the cuticular plate and above the nucleus. In healthy cells
the fluorescence of this somatic region was homogeneous.
An estimate of the resting free Ca2+ concentration
in these hair bundles was obtained according to Kao et al. (1989) .
Because the fluorescence of fluo-3 with Ca2+ bound
exceeds that of fluo-3 without Ca2+ by at least
40-fold, the fluorescence contribution of free fluo-3 was ignored in
the calculation. The dissociation constant of the indicator for
Ca2+ was set at 400 nM (Eberhard and
Erne, 1989 ). To determine the value for maximal fluo-3 fluorescence, we
measured the fluorescence of control internal solution supplemented
with 11 mM CaCl2 with the same confocal
settings as those used in the hair bundle Ca2+
imaging experiments.
In these experiments the fluorescence increase observed during each
whole-cell recording represented both the rate of fluo-3 diffusion into
the hair bundle and the rate of Ca2+ accumulation in
the cell. In healthy control cells the resting free
Ca2+ concentration should have been quite stable
over minutes; such stability was confirmed in cells loaded with the
membrane-permeant acetoxymethyl ester of fluo-3 and then
voltage-clamped in the perforated patch configuration (data not shown).
Because little Ca2+ initially accumulated in control
cells, the fluorescence increase in these cells at early time points
probably reflected the rate of fluo-3 diffusion from the whole-cell
recording pipette into hair bundles. As a result, our calculations of
the free Ca2+ concentration that used the in
vitro calibration of maximal fluo-3 fluorescence, especially those
at early time points, are likely to be underestimates. Comparisons
between cells at similar time points nonetheless are valid.
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RESULTS |
Localization of PMCA in bullfrog hair cells
To examine the distribution of PMCA in bullfrog saccular hair
cells, we used confocal immunofluorescence microscopy with a monoclonal
antibody that binds all known PMCA isoforms in many species (5F10;
Adamo et al., 1992 ). We saw consistent labeling of hair cells (Fig.
1A,B), which was
abolished when the antibody was preincubated with purified PMCA (Fig.
1C). Hair bundles were intensely labeled. In hair cells with
broad bundles, labeling was concentrated somewhat at stereociliary tips
but otherwise was distributed relatively uniformly along the
stereocilia (Fig. 1A). By contrast, in hair cells
with narrow bundles, labeling frequently was observed in a broad band
starting above the basal tapers, where stereocilia narrow before
somatic insertion, as well as at stereociliary tips (Fig.
1B). In both types of hair bundles, labeling appeared
relatively weak both in the taper region and in the basal connector
region, a narrow zone characterized in frog hair cells by cross-links
between stereocilia (Jacobs and Hudspeth, 1990 ). Although labeling of
the basolateral membrane of the cell appeared faint in comparison to
that of the hair bundle, the large amount of membrane in optical
sections of hair bundles probably contributed to the apparent
discordance in labeling intensity. Labeling appeared uniform along the
basolateral membrane, with no evidence for discrete densities of pumps
near the aggregates of Ca2+ channels found at
neurotransmitter release sites (Roberts et al., 1990 ; Issa and
Hudspeth, 1994 ).

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Figure 1.
Immunocytochemical localization of PMCA in
isolated hair cells. A, B, Plasma membranes of hair
cells were labeled by the 5F10 anti-PMCA monoclonal antibody. Hair
bundles appeared more intensely labeled than basolateral membranes, in
part because the concentration of plasma membrane in optical sections
through hair bundles exceeds that in views of the basolateral membrane.
The labeling of broad hair bundles (A) was
usually more uniform than that of narrow hair bundles
(B). Labeling was often strongest at
stereociliary tips. The basal connector region, immediately above the
stereociliary tapers, was labeled relatively weakly. C,
Labeling was blocked when immunocytochemistry was performed in the
presence of 5 µg/ml purified red blood cell PMCA. The 5 µm scale
bar applies to all three panels.
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Estimation of bundle PMCA by quantitative immunoblotting
We used quantitative immunoblotting to estimate the amount of PMCA
in hair bundles. We purified hair bundles with the twist-off technique
(Gillespie and Hudspeth, 1991a ), subjected bundle proteins to SDS-PAGE,
transferred the proteins to a blotting membrane, and detected PMCA with
the 5F10 antibody. This antibody detected bands at molecular masses 140 and 170 kDa in purified bundles and in the residual macula, the
supporting and hair cell epithelium remaining after bundle isolation
(Fig. 2A; the
separation between the two bands is seen better with lighter
exposures). Although 140 kDa corresponds to the molecular mass of
several PMCA isozymes (Carafoli, 1991 ), PMCA molecules with primary
sequences encoding 170 kDa molecules have not been reported previously.
Neither form shifted in migration after treatment with
N-glycanase F (data not shown), suggesting that the larger
species did not arise from glycosylation of the 140 kDa form. Because
purified PMCA can form a higher mass band under certain sample
preparation conditions (D. Kosk-Kosicka, personal communication), the
170 kDa band might have derived artifactually from the 140 kDa form.
Considering the 140 and 170 kDa bands together, using purified PMCA
from human erythrocytes as a standard, and assuming that the frog
bundle PMCA has identical immunoreactivity, we estimated that the
bundles from one sacculus contain 330 ± 100 pg of PMCA (mean ± SD, n = 4). Assuming that a typical sacculus has
~2000 hair bundles (Benser et al., 1993 ) and that each of the ~60
stereocilia has an average plasma membrane surface area of 8.5 µm2 (Jacobs and Hudspeth, 1990 ), the average PMCA
density is ~1300 µm 2.

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Figure 2.
Detection of hair bundle PMCA with the 5F10
antibody. A, Immunoblot detection of proteins of 140 and
170 kDa in isolated hair bundles and residual macula, the sensory
epithelium remaining after hair bundle isolation, with anti-PMCA
monoclonal antibody (5F10). Hair bundles, From 21 frog
sacculi (~42,000 bundles in agarose gel); Agarose,
equivalent amount of agarose gel; Residual macula, 0.5 saccular equivalents; RBC PMCA, purified human
erythrocyte PMCA (5000 pg). B, Immunoprecipitation of
PMCA with 5F10 from a Triton X-100 extract of purified, biotinylated
hair bundles. Equal fractions of the Triton X-100 bundle extract,
flow-through solution from the 5F10 anti-PMCA antibody precipitation,
and 5F10 SDS eluate were loaded. C, Immunoprecipitation
of 140 and 170 kDa calmodulin binding proteins with 5F10 from purified,
biotinylated hair bundles. Calmodulin binding proteins were isolated
first from a Triton X-100 extract of purified, biotinylated hair
bundles, using calmodulin-agarose; then the EGTA eluate from the
calmodulin-agarose was used for precipitation of PMCA with 5F10. Equal
fractions of each sample were loaded.
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Quantitation of bundle PMCA by calmodulin receptor content
The similarity in size of the bands reactive with the 5F10
antibody to the major calmodulin binding proteins of the hair bundle (Walker et al., 1993 ) indicated that we could derive an independent estimate of the density of hair bundle PMCA from the known
concentration of calmodulin receptors. To identify PMCA, we used the
5F10 antibody to immunoprecipitate proteins from Triton X-100 extracts
of biotinylated hair bundles. Two proteins were immunoprecipitated
(Fig. 2B) that were similar in mass to the proteins
seen by immunoblotting. To confirm that these proteins are the major
calmodulin binding proteins, we conducted successive precipitations
with calmodulin-agarose and 5F10. Several bundle proteins bound to
calmodulin-agarose and were eluted with EGTA; the protein pattern
corresponded remarkably well to that obtained by using
calmodulin-alkaline phosphatase to probe blots of bundle proteins
(Walker et al., 1993 ; Walker and Hudspeth, 1996 ). Of the proteins
eluted from calmodulin-agarose, only the 140 and 170 kDa proteins
subsequently were precipitated with 5F10 (Fig. 2C). In
combination with immunoblotting and calmodulin-alkaline phosphatase
overlay results, these results indicate that hair bundles contain two
species of PMCA of molecular masses 140 and 170 kDa, both of which bind
calmodulin.
Of the 12.5 fmol of calmodulin in each saccular equivalent of hair
bundles (Walker et al., 1993 ), ~45% is bound in a
Ca2+-dependent manner to Triton X-100-soluble
receptors (Walker et al., 1993 ) (data not shown). Furthermore, of the
detergent-soluble calmodulin receptors, PMCA accounts for ~85% of
the binding sites. If we assume that one molecule of calmodulin binds
to each PMCA molecule (Hinds and Andreasen, 1981 ), these data indicate
that the hair bundles derived from one sacculus contain 4.8 fmol of PMCA. This value corresponds to a density of ~2800
µm 2 on stereociliary membranes. Given the
uncertainties associated with each method, this estimate corresponds
well with that obtained by protein immunoblotting.
Local Ca2+ efflux from hair cells
Because our biochemical data suggested that substantial amounts of
PMCA exist on hair bundle membranes, we reasoned that the local
Ca2+ efflux from bundles could be substantial. Using
Ca2+-selective self-referencing electrodes (Smith et
al., 1994 ), which detect local Ca2+ gradients with a
resolution of a few micrometers, we examined the local
Ca2+ flux at different regions of hair cells in a
bath solution containing 50 µM Ca2+.
The efflux of Ca2+ from the base of a resting hair
bundle exceeded that from the basolateral membrane of the cell (Fig.
3A). Retraction of the electrode from the bundle indicated that Ca2+ flux
diminished with distance; the data were fit approximately with a model
that assumes a point source within the bundle (Fig. 3B;
Smith et al., 1994 ). The fit would have been qualitatively similar if
the model instead had incorporated a set of point sources distributed
within the bundle, viewed from the outside. The local Ca2+ flux immediately adjacent to hair bundles
( 5 ± 2 nmol m 2 sec 1;
n = 9) significantly (p < 0.005; one-tailed Student's t test) exceeded that measured
near basolateral membranes ( 2 ± 1 nmol m 2
sec 1; n = 9) or in background regions
(0 ± 1 nmol m 2 sec 1;
n = 9).

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Figure 3.
Steady-state Ca2+ efflux from
hair bundles and basolateral surfaces of isolated hair cells measured
with a Ca2+-selective self-referencing electrode.
The average background signals are indicated by dotted
lines. A, Ca2+ efflux from
hair bundles exceeded that from the basolateral membrane. By
convention, Ca2+ efflux is illustrated as a negative
voltage and Ca2+ influx as a positive voltage.
During the course of the experiment the electrode was moved from a
background region to the base of a hair bundle and then to the soma of
that cell. B, Reduction of Ca2+ flux
during electrode withdrawal from a hair cell. The measurement position
of the electrode was moved to the indicated distances from a hair
bundle; a gradient was detectable up to 50 µm away. The solid
line represents the theoretical gradient calculated as
described in the text. C, Ca2+ influx
during transduction. While the extracellular Ca2+
flux was measured near the top of the hair bundle, the bundle was
deflected in the negative direction (start of record). Positive bundle
displacements (indicated below the electrode signal)
produced a net influx. D, Microinjection of vanadate
into a hair cell reduced the steady-state Ca2+
efflux from the hair bundle. The arrow indicates the
time at which vanadate was injected. At the end of the experiment the electrode was withdrawn from the bundle to measure the background signal.
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By careful placement of the electrode near the top of a hair bundle, we
could measure either local Ca2+ efflux or influx,
depending on mechanical stimulation. When a hair bundle was first
displaced in the negative direction, closing most transduction
channels, an electrode positioned next to the top of the bundle
measured a local Ca2+ efflux; then when the bundle
was moved in the positive direction, opening transduction channels, the
signal reversed and a local Ca2+ influx was measured
(Fig. 3C).
Although not selective for PMCA (Macara, 1990 ), vanadate potently
inhibits this Ca2+ pump (Carafoli, 1991 ).
Ca2+ efflux from resting hair bundles was reduced on
the microinjection into hair cells of internal solution containing 0.2 mM vanadate (Fig. 3D) but was unaffected by
injection of internal solution alone (data not shown).
Transduction-dependent outward current
Ca2+ carries approximately a quarter of the
transduction current in cells bathed with frog saline solution
containing 4 mM Ca2+ (Lumpkin et al.,
1997 ). If the PMCA in hair bundles is electrogenic (Läuger, 1991 ;
Hao et al., 1994 ) and has a turnover rate similar to that of PMCA in
erythrocytes (Garrahan, 1986 ; Rega, 1986 ), activation of a significant
fraction of the PMCA molecules of the bundle could generate an outward
current of several picoamperes as the Ca2+ entering
during transduction is extruded. We therefore predicted that, under
optimal recording conditions, it should be possible to resolve a PMCA
current after activation of transduction channels. We next sought to
detect and characterize this signal.
To unmask the current component associated with PMCA activity,
our experimental protocol involved steps that fixed or eliminated two
well characterized components of the membrane current measured from a
hair cell with a whole-cell tight-seal recording electrode. First, the
ions trickling through the seal between the electrode and plasmalemma
produce a leakage current. For negative holding potentials, this
component is directed inwardly and hence is negative in sign. By
clamping the membrane potential at a constant level, we ensured that
the leakage current did not vary during mechanical stimulation but
simply added a constant offset to each of our recordings. The flux of
cations through mechanoelectrical transduction channels produces a
second component of inward membrane current. Because transduction
channels generally display a significant open probability in the
absence of stimulation, the current entering an undisturbed hair cell
includes some transduction current. If the hair bundle is moved
sufficiently far in the positive direction, this current grows until
all of the channels have opened. Moving the bundle well in the negative
direction closes all of the transduction channels, affording us a means
of eliminating the transduction current. In each case, to confirm that
we could close transduction channels completely, we applied at least
two large negative displacements.
The PMCA-associated current usually was measured with a two-step
stimulus protocol. We wanted to allow Ca2+ entry
into stereocilia, so a positive hair bundle deflection was given to
elicit a large transduction current. At the conclusion of this prepulse
stimulus, the bundle was displaced with a saturating negative test
pulse that closed all of the mechanically sensitive channels and thus
eliminated the transduction current. Immediately after the onset of the
test pulse, this procedure often yielded a small, transient, positive
component of membrane current, which we term the transduction-dependent
outward current, or ITOC (arrows in
Fig. 4A,B). We measured
ITOC by comparing the difference in membrane
current elicited by test pulses after negative and positive prepulses.

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Figure 4.
Transduction-dependent outward current. A,
B, From rest, hair bundles were displaced with prepulses of
1200 to +1500 nm and then were subjected to a 1200 nm test pulse
that closed all transduction channels. Mechanical stimuli are indicated
at the bottom of each panel. A, For a
cell with a low resting open probability, test pulses after positive
prepulse displacements (black lines) elicited ITOC (arrow);
ITOC did not appear after negative prepulses
(gray lines). The membrane current at level
1 included leakage and ITOC components; that at level 2 was exclusively leakage
current. The prepulse stimuli were 1200, 660, +660, and +1320 nm.
B, For a cell with a high resting open probability,
ITOC (arrow) was seen after
positive displacements (black lines) and appeared to be
particularly large at rest. Current components at levels
1 and 2 were interpreted as for
A. The current at level 3 included leakage and ITOC components as well as the
maximal transduction current; that at level 4 included
only leakage and maximal transduction current components. The prepulse
stimuli were 1200, 1060, 660, +660, and +1500 nm.
C, ITOC increased in
amplitude with prolonged displacement. Hair bundles were displaced for
increasing durations, using the stimulus protocol described for
A and B. ITOC
divided by the peak transduction current
(Ipeak) is plotted against prepulse duration; mean ± SD from three to five cells is plotted. The
0-350 msec and 350-500 msec points were fit separately with
least-squares linear regressions. D, ITOC
appeared after a positive displacement (black line) with
sufficient adaptation during the step to permit complete transduction
channel closure at the termination of the step. The relaxation of
current past level 2 after the positive step resulted
from adaptation-dependent reopening of transduction channels and slow
cessation of ITOC. Current components at
levels 1 and 2 were interpreted as for
A; a smaller negative displacement also produced a
current at level 2 (data not shown), indicating that the
displayed trace represented the membrane current level at which all
channels were closed. The displacements were ± 1080 nm. Scale
bars apply to A, B, and
D.
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Figure 4A illustrates a response in which negative
displacements established that the leakage current measured 152 pA.
When positive prepulse displacements were applied to allow
Ca2+ entry, however, subsequent negative test pulses
induced a membrane current overshoot to approximately 148 pA, or 4 pA
further in the outward direction. We attributed this contribution of +4
pA to ITOC. Another cell exhibited a substantial
resting open probability, which presumably arose from an unintended
positive offset that occurred when the stimulator was attached to the
bundle. In this cell the response to the test pulse also differed,
depending on whether the prepulse was positive or negative (Fig.
4B). A substantial ITOC
appeared to flow at rest in this cell and could be suppressed by
negative prepulses (Fig. 4B). Suppression of
ITOC by negative displacements resembled the
recovery of current toward the resting level that occurs as a result of
adaptation. In Figure 4B, however, the increase in
inward current during large negative displacements could not have
arisen entirely from adaptation; after the termination of the test
pulse, the current overshot (to current level 4 in Fig.
4B) to a value more negative than that seen during
saturating positive prepulse displacements (current level
3). Current level 4 represents the leak plus
fully activated transduction channels; current level 3 represents the leak plus fully activated transduction channels
and ITOC.
The magnitude of ITOC depended on the prepulse
duration: the current grew approximately linearly and reached a maximal
value at 300-350 msec (Fig. 4C). Decay of the outward
current was prolonged also. Although we did not examine the decay of
ITOC directly, we noted that the recovery of
membrane currents to the resting level after positive displacements of
150 msec duration could be fit by two time constants (29 ± 9 and
136 ± 47 msec; n = 9). The shorter time constant
likely reflected adaptation (Eatock et al., 1987 ), whereas the second
component may have corresponded to the decay of
ITOC.
We also observed ITOC by allowing the adaptation
occurring during a positive stimulus to reduce transduction channel
open probability to near zero when the hair bundle was returned to its
rest position (Fig. 4D). With this stimulus protocol,
commonly used for other studies of hair cell transduction (Yamoah and
Gillespie, 1996 ), a saturating negative displacement established the
membrane leakage current; any additional outward current after a
saturating positive displacement derived from
ITOC. Using this definition, we saw
ITOC in 21 of 66 recordings in which initial
seal resistances were 5 G or larger. When present,
ITOC could be as large as 10 pA; for 150 msec
displacements ITOC averaged 3.1 ± 1.9 pA
(mean ± SD, n = 21). In these 21 cells the
maximal transduction currents were 83 ± 26 pA;
ITOC thus averaged 0.04 pA per picoampere of inward transduction current.
The PMCA inhibitor vanadate blocked ITOC. After
establishing the whole-cell configuration with an electrode containing
vanadate, we occasionally observed ITOC
(arrow in Fig. 5A);
as vanadate continued to diffuse into the cell, however,
ITOC disappeared (Fig. 5B). By
contrast, when we observed ITOC in cells filled with control solutions, the current often persisted for several minutes. Although vanadate shifted the resting open probability of the
transduction channels, presumably by inhibiting adaptation motor myosin
molecules (Yamoah and Gillespie, 1996 ), such a shift cannot explain the
results of Figure 5, A and B. Because negative displacements of increasing amplitudes suppressed transduction to a
single current level, these displacements were saturating and hence
closed all channels. Nevertheless, the membrane current level after
positive displacements in Figure 5A but not Figure 5B moved closer to zero, indicating that additional outward
current (ITOC) had been elicited. Despite
substantial adaptation in Figure 5B, which permitted
complete channel closure at the ends of positive steps, the membrane
current level did not become more positive than the level associated
with complete channel closure. Vanadate must have blocked
ITOC rapidly. Similar inhibition of
ITOC was seen with BeFx, but
not with SO42 (Yamoah and Gillespie,
1996 ) (data not shown). Although BeFx probably inhibits
PMCA (Murphy and Coll, 1993 ), SO42
does not affect this Ca2+ pump (Hao et al., 1994 ).
Because vanadate also inhibits other membrane transporters, we dialyzed
hair cells with carboxyeosin, a relatively selective inhibitor of PMCA
(Gatto and Milanick, 1993 ). ITOC disappeared
during this treatment in several cells, although sufficient time
elapsed in each case that we could not determine whether this
inhibition was significant.

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Figure 5.
Pharmacological manipulation of the
transduction-dependent outward current. Transduction currents arising
from positive displacements (black lines) and negative
displacements (gray lines) are plotted; when
visible, ITOC is indicated by an
arrow. The current components at levels 1
and 2 were interpreted as in Figure 4. A,
B, Vanadate blocked ITOC. After 120 sec of dialysis without mechanical stimulation and with a recording
electrode that contained 0.5 mM vanadate, stimulus families
were initiated immediately (A) or 20 sec later (B). ITOC was usually
absent after 120 sec of dialysis; in the few cases in which it occurred
(e.g., A), it was blocked very rapidly. The
displacements were 1050, 920, 400, +400, +920, and +1050 nm.
C, ITOC was present 120 sec
after break-in (data not shown) but nearly disappeared within 20 sec of
exposure to 2.5 mM SrCl2 and 0.5 mM
CaCl2. Although a small ITOC
remained in this cell, ITOC was usually not
visible with this ionic combination. The prepulse stimuli were 1200,
1050, 660, +660, and +1320 nm; the test pulse was 1200 nm.
D, ITOC
(arrow) remained even during the exposure of hair cells
to 100 nM apamin, an SK channel blocker (~180 sec after
break-in). The prepulse stimuli were 1200, 660, +660, and +1320 nm;
the test pulse was 1200 nm. Scale bars between C and
D apply to all panels.
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ITOC is Ca2+-dependent:
reduction of Ca2+ entry into stereocilia by
replacement of most bath Ca2+ with
Sr2+ reduced ITOC nearly to
zero (Fig. 5C). Although Sr2+ is a
substrate for PMCA, its affinity for the pump is at least 10-fold lower
than that of Ca2+ (Graf et al., 1982 ).
ITOC did not arise from
Ca2+-dependent K+-channel
activity. To minimize any possible contribution by large conductance
Ca2+-dependent K+ (BK) channels,
we dialyzed hair cells with Cs+, which blocks most
K+ channels. To ensure that
Cs+-permeant small conductance
Ca2+-dependent K+ (SK) channels
were not the source of ITOC, we
demonstrated that ITOC remained even after bath
application of 100-500 nM apamin, an inhibitor of SK
channels (Fig. 5D). Furthermore, any SK current should have
been small, given our holding potential and ionic compositions.
Other possible membrane conductances do not contribute to
ITOC. Na+ or
Cl currents would be inward under our recording
conditions; a contribution to ITOC from somatic
Na+/Ca2+ exchangers is
implausible, both because ITOC was independent of changes in the bath Na+ concentration (data not
shown) and because a Na+/Ca2+
exchanger current should have been inward at 80 mV if the exchanger uses a stoichiometry of 3:1
Na+/Ca2+ or 4:1:1
Na+/K+/Ca2+
(Reeves, 1991 ). The
Na+/K+-ATPase, which occurs at a
high density in the basolateral membrane of the hair cell (Burnham and
Sterling, 1984 ), would have produced an outward current. Although
substantial amounts of Na+ enter during
transduction, a Na+/K+-ATPase
current should not have depended on Ca2+ entry, and
Na+ pumps should, in any event, have operated at
their maximal rate with the saturating concentrations of internal
Na+ and external K+ that we used
(Läuger, 1991 ). The ITOC data are thus
most consistent with PMCA pump activity.
Contribution of PMCA to maintenance of low stereociliary
Ca2+ concentration
To examine directly the role played by PMCA in hair bundle
Ca2+ regulation, we monitored the intracellular
Ca2+ concentration with the indicator fluo-3 while
dialyzing hair cells with inhibitors of PMCA. In all cases the
inhibitors induced substantial increases in hair bundle
Ca2+ concentration. The fluo-3 fluorescence
intensity, and thus the free Ca2+ concentration, was
higher in a hair cell dialyzed with 1 mM vanadate (Fig.
6C,D) than in a cell filled
with control internal solution (Fig. 6A,B).
Furthermore, the increase in resting Ca2+
concentration precluded the detection of changes in stereociliary Ca2+ concentration during mechanoelectrical
transduction, despite transduction currents that approached 200 pA.
Like vanadate, 5 µM carboxyeosin induced a substantial
rise in resting fluo-3 fluorescence (Fig. 6G,H) over
the level in control cells (Fig. 6E,F). The
pronounced effects of carboxyeosin in these experiments, compared with
the modest effects of the inhibitor in the ITOC experiments, presumably arose because we measured its cumulative effects on Ca2+ concentration over the entire
recording period. The fluorescence of this low concentration of
carboxyeosin was <7% that of the fluo-3 internal solution and thus
contributed minimally to the observed fluorescence signal. Similar
effects on fluo-3 fluorescence were observed in cells dialyzed with an
ADP analog, adenosine 5 -O-(2-thiodiphosphate) (ADP S;
data not shown). Although its effects on PMCA have not been tested, we
expect that ADP S also inhibits this Ca2+ pump,
for it inhibits the intracellular sarcoplasmic/endoplasmic reticulum
Ca2+-ATPase (SERCA; Myung and Jencks, 1994 ). By
inhibiting the adaptation motor, ADP S shifts the resting open
probability of the transduction channels from ~0.1 to 0.8 (Gillespie
and Hudspeth, 1993 ), which could lead to enhanced
Ca2+ influx at rest. To ensure that the observed
increase in hair bundle fluorescence did not result from adaptation
motor inhibition, we offset each bundle >0.5 µm in the negative
direction immediately after establishing the whole-cell configuration
so that transduction channels were predominately closed when the bundle
was unstimulated.

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Figure 6.
Elevation of the resting free
Ca2+ concentration in hair cells dialyzed with PMCA
inhibitors. Hair cells were dialyzed with fluo-3 and inhibitors of
PMCA; fluorescence intensity was measured with confocal microscopy.
A, C, E, G,
Frame scan images acquired before elicitation of transduction currents.
The dotted lines overlying the hair bundles mark the
transects illuminated during the acquisition of the line scan images on
the right. B, D,
F, H, Line scan images showing responses
to mechanical stimuli; the tick marks at the
top of each panel mark the beginning and end of the 100 msec positive hair bundle deflection. The ordinate represents distance
across a hair bundle from the longest stereocilium (top)
to the shortest (bottom); time progresses along the
abscissa. A, B, Control cell, 240 sec
after break-in. In A, the increased fluorescence
intensity observed near the tips of some stereocilia indicated active
transduction channels. In B, a positive displacement that elicited a 150 pA receptor current also produced elevated fluo-3
fluorescence. The decay of the fluorescence signal after the bundle was
returned to rest was declined exponentially with a time constant of 150 msec. C, D, Cell dialyzed with 1 mM vanadate, 219 sec after break-in. The resting
fluorescence was much higher than in the control, and no modulation of
the signal was seen despite a transduction current of 165 pA.
E, F, Control cell, 307 sec after
break-in. The transduction current was 140 pA; the fluorescence decay
after stimulation ended declined exponentially with a time constant of
160 msec. G, H, Cell dialyzed with 5 µM carboxyeosin, 312 sec after break-in. The resting
fluorescence was elevated when compared with that of the control.
Despite a transduction current of 175 pA, no modulation of the
fluorescence signal was seen. The increased fluorescence signal in the
cuticular plate, when compared with that in the hair bundle and soma,
apparently was attributable to fluo-3 binding; this phenomenon was
observed after several minutes of recording in most hair cells. The
scale bar in H applies to all panels.
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The absolute intensity of fluo-3 fluorescence in the hair bundles of
cells filled with vanadate and carboxyeosin exceeded those of control
cells. In addition, the rate of fluorescence increase over the first
400 sec of whole-cell recording was greater in cells dialyzed with
these inhibitors. To quantify the effects of PMCA inhibitors on hair
bundle fluorescence, we measured normalized fluorescence intensities
before mechanical stimulation from line scan images. Each bundle was
deflected for 100 msec and its fluorescence intensity was recorded,
approximately once per minute. We plotted the fluorescence intensities
against time after the onset of whole-cell recording and fit data
collected during the first 400 sec of whole-cell recording with
least-squared error lines (r2 values,
0.8-1.0). For control cells the rate of fluorescence increase in hair
bundles was 0.5 ± 0.2 units/sec (mean ± SD,
n = 6). By contrast, fluorescence rose much faster in
cells dialyzed with PMCA inhibitors. The rate for cells filled with
vanadate was 2.2 ± 0.5 units/sec (n = 4); for
cells filled with carboxyeosin the rate was 1.4 ± 0.4 units/sec
(n = 3). The average rate for control cells was
significantly lower than that for cells filled with vanadate
(p = 0.003; one-tail Student's t
test) or carboxyeosin (p = 0.03). We used an
in vitro calibration to convert fluorescence units to the
estimated free concentration of Ca2+ in hair bundles
under these conditions (Fig.
7A). Approximately 200 sec
after establishment of the whole-cell configuration, the average hair
bundle Ca2+ concentration in control hair cells was
28 ± 7 nM (n = 4). By contrast, in
cells filled with carboxyeosin, the concentration of
Ca2+ had increased to 47 ± 3 nM
(n = 3); in cells filled with vanadate, the
concentration of Ca2+ had reached 255 ± 133 nM (n = 5). The average fluorescence
intensities for the three groups at this time were 106 ± 22 units, 185 ± 10 units, and 654 ± 203 units,
respectively.

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Figure 7.
Quantitation of the fluo-3 fluorescence intensity
of hair bundles filled with vanadate, carboxyeosin, and control
solutions. A, The free calcium concentration of
representative cells estimated with an in vitro
calibration. To quantify the effects of PMCA inhibitors on hair bundle
fluorescence, we measured fluorescence intensities before mechanical
stimulation from line scan images. Ca2+
concentrations were plotted against time after the onset of whole-cell recording. Both the estimated Ca2+ concentration and
the rate of concentration increase in the hair bundles of cells filled
with vanadate or carboxyeosin exceeded those of control cells. For data
collected during the first 400 sec of whole-cell recording, the plot of
fluorescence intensity against time for each cell was fit with a
minimal squared error line. B, Ratio of hair bundle
fluorescence to somatic fluorescence in representative carboxyeosin
cells with and without transduction and in a control cell with
transduction. The fluorescence in hair bundles was highest relative to
the somatic fluorescence when a PMCA inhibitor was present and
substantial Ca2+ entry took place through
transduction channels.
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To distinguish between a direct effect of inhibitors on bundle PMCA
molecules and an increase in Ca2+ concentration
resulting from inhibition of somatic PMCA (and SERCA) molecules, we
compared the ratio of bundle fluorescence to somatic fluorescence in
cells filled with carboxyeosin with the ratio in control cells (Fig.
7B). In two carboxyeosin-filled hair cells that failed to
transduce, the ratio of bundle fluorescence to somatic fluorescence
(0.45 ± 0.03, mean ± SE) was lower than that in three
control cells (0.60 ± 0.05). In three carboxyeosin-filled cells
that exhibited transduction currents, however, bundle fluorescence became relatively large when compared with somatic fluorescence (0.68 ± 0.02), indicating that this PMCA inhibitor affected the ability of hair bundles to remove Ca2+ that entered
during transduction.
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DISCUSSION |
Present at high density in hair bundle plasma membranes, PMCA is
poised to play a crucial role in regulation of the
Ca2+ concentration of the hair bundle. Our
immunoblotting and immunoprecipitation experiments show that 140 and
170 kDa forms of PMCA reside in bundles. Because these molecular masses
correspond to those of the major calmodulin binding proteins of hair
bundles (Walker et al., 1993 ) and because the 5F10 antibody
immunoprecipitates calmodulin binding proteins of these sizes (see Fig.
2C), our data confirm that PMCA is the major calmodulin
binding protein of stereocilia (Walker et al., 1993 ; Crouch and
Schulte, 1995 ). Although PMCA2b is a reasonable candidate for the PMCA
of stereocilia (Crouch and Schulte, 1996 ), isoform-selective antibodies
will be required to establish the presence of this or other isoforms within the hair bundle.
To demonstrate that PMCA is active in hair bundles, we measured
extracellular Ca2+ efflux from hair cells, using
Ca2+-selective self-referencing electrodes. Although
the net flux of Ca2+ over the entire hair cell
surface should have been zero, we were able to detect local
Ca2+ efflux by using electrodes with tips of a few
micrometers in diameter. These experiments demonstrated that hair cells
locally extrude substantial quantities of Ca2+;
consistent with the participation of PMCA, vanadate microinjection reduced Ca2+ efflux. For most membrane regions that
we investigated, we observed local efflux. Two factors contributed to
this observation. First, PMCA, and thus the source of
Ca2+ efflux, is distributed relatively uniformly
over the hair cell membrane. Second, the points of
Ca2+ entry into hair cells are focal: many
basolateral Ca2+ channels are clustered at synaptic
zones (Roberts et al., 1990 ; Issa and Hudspeth, 1994 ), and transduction
channels are located only near stereociliary tips. Consistent with this
explanation, when the probe was positioned near the top of the bundle,
we observed substantial Ca2+ influx on positive
bundle deflection, presumably because of Ca2+
entering open transduction channels.
When the probe was positioned close to the base of the hair bundle, the
average Ca2+ flux approximated the
Ca2+ transport rate of stereociliary membranes. Had
all 2000 PMCA molecules in a square micrometer of membrane contributed
equally, this flux would correspond to a pumping rate of 1.5 Ca2+ per PMCA per second. This value must, however,
underestimate the actual efflux under these conditions. First, the
method measured net flux; local efflux of Ca2+ from
stereociliary membranes was counteracted by influx through nearby
transduction channels. Furthermore, the electrode efficiency is not
known accurately (Smith et al., 1994 ) and the probe was not juxtaposed
perfectly to the stereociliary membrane. Most importantly, because the
flux experiments used a low extracellular Ca2+
concentration (50 µM), Ca2+ entry into
hair cells should have been greatly reduced when compared with the
influx in the ITOC experiments for which cells
were exposed to 4 mM Ca2+. The pumping
rate during the flux measurements should have been far below the
maximal turnover rate for the pump.
Additional evidence for active bundle PMCA molecules stemmed from
analysis of ITOC, an outward current
component elicited by mechanical stimuli. This current activated
immediately and depended on the presence of extracellular
Ca2+. Although not conclusive, our pharmacological
data support the hypothesis that ITOC arose from
electrogenic activity of PMCA. Assignment of
ITOC to PMCA activity would be strengthened if
the PMCA inhibitor La3+ (Carafoli, 1991 ), applied
extracellularly, could be used specifically to inhibit this current.
Because La3+ eliminates transduction (Sand, 1975 ),
however, the ion, unfortunately, should inhibit
ITOC regardless of the origin of the outward
current.
If ITOC can be attributed to PMCA activity, then
the normalized amplitude of ITOC can be used to
estimate the turnover rate of bundle PMCA. In our preparation the
number of intact tip links (Assad et al., 1991 ) and the number of
functional transduction channels are such that a typical stereocilium
probably contained only one functional 100 pS transduction channel
(Crawford et al., 1991 ; Denk et al., 1995 ). Because the 80 mV driving
force in our experiments should have produced a transduction current of
8 pA per stereocilium and because ITOC
averaged 0.04 pA per picoampere of inward transduction current (see
Results), ITOC of one stereocilium should have
measured 0.3 pA. If one Ca2+ is exchanged for one
H+, the 3 amol of Ca2+ ions
leaving a stereocilium per second would have been pumped by 2000 molecules of PMCA operating at a turnover number of 120/sec. If the
pumps operated below their maximal rate or if our measurement underestimated ITOC, then the maximal
turnover rate would have been higher. Our value falls within the range
estimated for PMCA in erythrocytes (50-300/sec; Garrahan, 1986 ; Rega,
1986 ). Taken together, our data are broadly consistent with ~2000
PMCA molecules per square micrometer of stereociliary membrane, each
capable of operating at a maximal turnover rate exceeding 100/sec.
Contribution of PMCA to stereociliary
Ca2+ regulation
Although the surface density of PMCA on the stereociliary membrane
is similar to that inferred for PMCA on the basolateral surface of the
hair cell (Tucker et al., 1996 ; Wu et al., 1996 ), PMCA should play a
more important role in stereocilia than in the soma. Not only are
stereocilia unable to sequester Ca2+ in
intracellular organelles, but the cytoplasmic volume per PMCA molecule
is much smaller in stereocilia than in the soma; an equivalent amount
of Ca2+ therefore should be extruded from
stereocilia more rapidly than from the soma.
Consistent with a critical role for PMCA in stereocilia, the PMCA
inhibitors vanadate and carboxyeosin rapidly increased the concentration of Ca2+ in hair bundles. Inhibition of
somatic Ca2+ pumps (Tucker and Fettiplace, 1995 ) and
the subsequent rise in Ca2+ load faced by the bundle
probably also contributed to the observed rise in bundle
Ca2+ concentration. Nevertheless, the increase in
bundle Ca2+ concentration in carboxyeosin-filled
hair cells that had substantial transduction currents indicates that
PMCA plays an active role in extruding Ca2+ entering
during transduction. Indeed, bundle Ca2+ signals
elicited by mechanical stimulation can be fit only with models that
invoke a robust Ca2+ extrusion mechanism (E. A. Lumpkin and A. J. Hudspeth, unpublished observations). Until the
Ca2+ binding properties and concentration of mobile
Ca2+ buffers in stereocilia are determined, the
contribution of PMCA to bundle Ca2+ regulation
in vivo can be estimated only qualitatively. Nevertheless, our data indicate that PMCA is one of the dominant factors controlling the concentration of Ca2+ in stereocilia.
Consequences of high PMCA density
The measured PMCA activity has several significant implications.
First, because PMCA is thought to exchange one H+
for each Ca2+ transported (Hao et al., 1994 ), the
hair bundle pH should drop precipitously during transduction unless
stereocilia contain robust H+ extrusion or buffering
mechanisms. Indeed, electrogenic H+ extrusion,
outward in direction, could contribute to ITOC.
Second, because one ATP is consumed for every Ca2+
transported, hair bundle PMCA should impose a substantial energy load
on a hair cell, as suggested for somatic
Ca2+-ATPases (Tucker et al., 1996 ); a 200 msec, 0.3 pA pump current in a single stereocilium would consume 1 mM
ATP there. ATP consumption by hair bundle PMCA may well be among the
dominant energy loads faced by a hair cell. Nevertheless, entry of
Ca2+ through transduction channels must be
sufficiently crucial to hair cell function that the cell can tolerate
this energy expenditure.
Transcellular Ca2+ flux and extracellular
Ca2+ gradients
Although saccular endolymph has a bulk Ca2+
concentration of ~260 µM (Corey and Hudspeth, 1983 ),
PMCA may elevate substantially the extracellular concentration of
Ca2+ close to the apical surfaces of hair cells. The
amount of Ca2+ entering through basolateral channels
should exceed that entering through transduction channels, and mobile
Ca2+ buffers should distribute the ion throughout
the cell. In a steady state, influx of Ca2+ is
matched by efflux across the plasma membrane; the high density of hair
bundle PMCA should permit bundles to extrude a fraction of this
Ca2+ load, producing a transcellular
Ca2+ flux from the basolateral to the apical
surface. Transcellular Ca2+ flux is well established
in renal epithelia, where calbindin shuttles Ca2+
from apical Ca2+ channels to basolateral
Ca2+ pumps and transporters (Bronner, 1989 ; Friedman
and Gesek, 1995 ).
Our calculations suggest that the concentration of
Ca2+ near the saccular surface could be 200 µM greater than that of the bulk endolymph (see
). Local Ca2+ conductances might reduce this
value modestly, but diffusional obstructions such as the otolithic
membrane and otoconia should increase it. Although the issue clearly
requires further investigation, we speculate that PMCA molecules
increase the concentration of Ca2+ surrounding hair
bundles; a locally elevated extracellular Ca2+
concentration could speed adaptation (Eatock et al., 1987 ; Ricci and
Fettiplace, 1997 ) and accentuate bundle twitches (Benser et al., 1996 ).
In the mammalian cochlea, PMCA is elevated strikingly on hair bundles
of mature outer hair cells and appears to be absent on their
basolateral surfaces (Crouch and Schulte, 1995 ). With a bulk
endolymphatic Ca2+ concentration of only 30 µM (Bosher and Warren, 1978 ), the consequences of high
PMCA activity should be still more significant.
 |
FOOTNOTES |
Received Aug. 7, 1997; revised Oct. 28, 1997; accepted Oct. 31, 1997.
This work was supported by National Institutes of Health Grants to
E.N.Y. (DC03040), P.J.S.S. (RR01395), A.J.H. (DC00241), and P.G.G.
(DC00979). A.J.H. is an Investigator and E.A.L. is a Predoctoral Fellow
of the Howard Hughes Medical Institute. P.G.G. is a Pew Scholar in the
Biomedical Sciences. We thank Drs. W. M. Roberts and F. Jaramillo
for advice on diffusion modeling. We also appreciate constructive
comments on this manuscript that were provided by Drs. D. Hilgemann and
D. Kosk-Kosicka and members of the Hudspeth and Gillespie laboratories.
We acknowledge gifts of PMCA from Drs. D. Kosk-Kosicka and G. Inesi.
Correspondence should be addressed to Dr. Peter G. Gillespie,
Department of Physiology, The Johns Hopkins University, 725 North Wolfe
Street, Baltimore, MD 21205.
Dr. Yamoah's present address: Department of Cell Biology,
Neurobiology, and Anatomy, University of Cincinnati, Cincinnati, OH
45267.
 |
APPENDIX |
Isolated cell model
We modeled a single hair bundle as a cylinder 6 µm tall and 4 µm in diameter. To simplify calculations, we positioned 66 point sources of Ca2+ along the surface of the cylinder,
~1 µm apart in each dimension, and divided the total
Ca2+ efflux among these sources; each point source
therefore represented the contribution of ~15,000 PMCA molecules. The
basal activity of each PMCA molecule was assumed to be 1.5/sec; during
stimulation this value increased linearly over 300 msec. Like isolated
hair cells, only some of the stereocilia of the model bundle have
active transduction channels and hence display elevated pump turnover; average turnover during mechanical displacement therefore was increased
to only 15/sec. After termination of the step, pump turnover was
reduced exponentially to the resting value with a time constant of 150 msec. Because our transduction currents are typically smaller than
100 pA, our model incorporated seven point sinks (transduction
channels), each with a maximum 8 pA transduction current, located atop
the model cylinder. The fraction of current carried by
Ca2+ was assumed to be 5% (Lumpkin et al., 1997 ).
The measurement position was located 1 µm above the center of the top
of the cylinder.
For a point source, extruding into a semi-infinite space a current
i of a compound with valence z and diffusion
coefficient D, the concentration C at radius
r is (Berg, 1993 ):
The response to a sustained stimulus is:
After a current step of finite time
(t0) is terminated, the concentration
declines as:
The simulation is plotted in Figure
8A; note that the drop
in extracellular Ca2+ concentration that results
from transduction channel opening develops rapidly and dominates the
increase in extracellular Ca2+ as the ion enters the
hair bundle and then is pumped out. All of these changes in
Ca2+ are fast relative to the sampling rate of the
Ca2+ electrode (<1 Hz).

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|
Figure 8.
Modeling extracellular Ca2+
gradients. A, The concentration of
Ca2+ 1 µm from the model hair bundle described in
during mechanical stimulation. The contributions from
Ca2+ pumps (thin black line) and
transduction channels (gray line), as well their
sum (thick black line), are plotted separately. B, The modeled gradients in Ca2+
concentration above the saccular apical surface (black
lines) or above a single hair bundle (gray
line). The concentration gradient for the model bundle is
magnified in the inset. The background concentration of
Ca2+ (260 µM) is indicated by the
dotted line.
|
|
Can this small drop in Ca2+ concentration during
transduction be measured with Ca2+-selective
self-referencing electrodes? During a sustained mechanical displacement
the Ca2+ concentration 1 µm from the model bundle
should be ~2 µM lower than the background concentration
of 50 µM. Given the properties of the
Ca2+ measurement electrodes, we would expect the
following signal (Smith et al., 1994 ):
This value is comparable in amplitude to the response shown in
Figure 3C.
Transcellular Ca2+ flux and extracellular
Ca2+ gradients
The extracellular gradient in Ca2+
concentration above the apical surfaces of hair cells should depend on
the net Ca2+ flux from basolateral to apical
membranes, on the binding and diffusional properties of mobile
Ca2+ buffers, and on the distribution of PMCA
molecules. Because healthy cells have substantial resting transduction
currents, their resting potentials lie at the more positive end of the
measured range ( 60 to 50 mV; Hudspeth and Lewis, 1988 ). Under these
conditions the amount of Ca2+ entering through
basolateral Ca2+ channels should exceed that
entering through transduction channels (Lenzi and Roberts, 1994 ). For
example, although run-down and cell isolation treatments diminish the
total Ca2+ conductance, the basolateral
Ca2+ current at 50 mV still exceeds 20 pA
(Hudspeth and Lewis, 1988 ; E. Yamoah and P. Gillespie, unpublished
data). For a hair cell in situ, the Ca2+
current may be substantially greater. By contrast, an ensemble of
transduction channels with maximal 200 pA current, 15% open at rest
and admitting 5% of the current as Ca2+, should
produce an apical Ca2+ current of only 1.5 pA.
Because the conductance of voltage-activated basolateral
Ca2+ channels grows steeply with membrane
depolarization, net basolateral Ca2+ influx should
be even more pronounced during mechanical stimulation.
Hair cells have high concentrations of mobile Ca2+
buffers (Roberts, 1993 ; Tucker and Fettiplace, 1996 ). Because of their
Ca2+ binding and diffusional properties, these
buffers should distribute Ca2+ throughout the cell.
The effect of the Ca2+ buffer is to enhance the
apparent diffusion of Ca2+; if the concentration of
mobile buffer is substantially greater than the total cytosolic
Ca2+ concentration, then the diffusion of
Ca2+ is augmented by the ratio (Bronner,
1989 ):
in which A is the augmentation of the diffusion of
Ca2+, DB and
DCa are the diffusion coefficients for the
mobile buffer and for free Ca2+, [B] is
the concentration of mobile buffer, and KD is
the dissociation constant for the Ca2+ buffer
reaction. In the hair cell, where the mobile buffer has a behavior
similar to that of 0.8 mM BAPTA (Roberts, 1993 ), diffusion may be enhanced 100-fold or more. The consequence is that an entering Ca2+ ion diffuses a very large distance before it is
captured by a PMCA molecule. The hair bundle contains ~30% of the
plasmalemma of a hair cell (Roberts et al., 1990 ); because the density
of PMCA is at least as high on stereociliary membranes as on the somatic membrane (see Fig. 1), bundle PMCA molecules plausibly might
extrude an equivalent fraction of the total resting
Ca2+ influx.
To estimate the apical concentration gradient that might be produced by
a transcellular Ca2+ flux, we considered the
saccular epithelium to be a hemispherical source of
Ca2+, extruding the ion into a semi-infinite volume.
More accurate representations of the source for example a disk source,
a collection of point sources corresponding to saccular bundles, or a
collection of point sources corresponding to individual PMCA
molecules produce still greater local Ca2+
concentrations.
The time-dependent relation between concentration and distance for a
hemispherical source is (Carslaw and Jaeger, 1959 ):
in which s is the transport rate from the source,
D is the diffusion coefficient, r is the distance
from the center of the hemisphere, and r is the radius of
the hemisphere. At infinite time, this expression reduces
to:
The Ca2+ current into a healthy hair cell at
rest might measure 50 pA; over time, this influx of 260 amol of
Ca2+ per second must be balanced by an equal
extrusion via plasma membrane pumps and transporters. Of this input, we
assumed that 30% is extruded by stereociliary PMCA (see above).
Transport of 160 fmol of Ca2+ per second by the 2000 saccular hair bundles, coupled with the diffusion coefficient of
Ca2+ (8 × 10 10
m2/sec; Hille, 1992 ) and an approximate saccular
radius of 160 µm (Jacobs and Hudspeth, 1990 ), suggests that the
concentration of Ca2+ near the saccular surface
could be 200 µM greater than that of the bulk endolymph
(see Fig. 8B).
The additive effect of a large number of adjacent
Ca2+ sources is striking; calculation for a single
model hair bundle (see above) using the same values gives an elevated
extracellular Ca2+ concentration of <5
µM at 1 µm (see Fig. 8B and
inset). For the low Reynolds number at which hair bundles
operate, stirring effects evoked by bundle vibration during natural
stimuli should be negligible. During excitatory mechanical transduction
Ca2+ entry through open transduction channels should
reduce the extracellular Ca2+ concentration, but
only by a few micromolar. As noted above, by greatly increasing
basolateral Ca2+ entry, excitatory stimulation
should increase the net transcellular Ca2+ flux, ultimately exaggerating the gradient.
 |
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J. K. Hill, C. L. Brett, A. Chyou, L. M. Kallay, M. Sakaguchi, R. Rao, and P. G. Gillespie
Vestibular Hair Bundles Control pH with (Na+, K+)/H+ Exchangers NHE6 and NHE9
J. Neurosci.,
September 27, 2006;
26(39):
9944 - 9955.
[Abstract]
[Full Text]
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M. Grati, N. Aggarwal, E. E. Strehler, and R. J. Wenthold
Molecular determinants for differential membrane trafficking of PMCA1 and PMCA2 in mammalian hair cells
J. Cell Sci.,
July 15, 2006;
119(14):
2995 - 3007.
[Abstract]
[Full Text]
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J. K. Hill, D. E. Williams, M. LeMasurier, R. A. Dumont, E. E. Strehler, and P. G. Gillespie
Splice-site A choice targets plasma-membrane Ca2+-ATPase isoform 2 to hair bundles.
J. Neurosci.,
June 7, 2006;
26(23):
6172 - 6180.
[Abstract]
[Full Text]
[PDF]
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M. Grati, M. E. Schneider, K. Lipkow, E. E. Strehler, R. J. Wenthold, and B. Kachar
Rapid turnover of stereocilia membrane proteins: evidence from the trafficking and mobility of plasma membrane Ca(2+)-ATPase 2.
J. Neurosci.,
June 7, 2006;
26(23):
6386 - 6395.
[Abstract]
[Full Text]
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M. C. Wagner, B. L. Blazer-Yost, J. Boyd-White, A. Srirangam, J. Pennington, and S. Bennett
Expression of the unconventional myosin Myo1c alters sodium transport in M1 collecting duct cells
Am J Physiol Cell Physiol,
July 1, 2005;
289(1):
C120 - C129.
[Abstract]
[Full Text]
[PDF]
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S. S. Desai, C. Zeh, and A. Lysakowski
Comparative Morphology of Rodent Vestibular Periphery. I. Saccular and Utricular Maculae
J Neurophysiol,
January 1, 2005;
93(1):
251 - 266.
[Abstract]
[Full Text]
[PDF]
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M. P. Scherer and A. W. Gummer
Vibration pattern of the organ of Corti up to 50 kHz: Evidence for resonant electromechanical force
PNAS,
December 21, 2004;
101(51):
17652 - 17657.
[Abstract]
[Full Text]
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G. A. Manley, U. Sienknecht, and C. Koppl
Calcium Modulates the Frequency and Amplitude of Spontaneous Otoacoustic Emissions in the Bobtail Skink
J Neurophysiol,
November 1, 2004;
92(5):
2685 - 2693.
[Abstract]
[Full Text]
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R. Caroppo, A. Gerbino, G. Fistetto, M. Colella, L. Debellis, A. M. Hofer, and S. Curci
Extracellular calcium acts as a "third messenger" to regulate enzyme and alkaline secretion
J. Cell Biol.,
July 5, 2004;
166(1):
111 - 119.
[Abstract]
[Full Text]
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D. M. Bautista and R. S. Lewis
Modulation of plasma membrane calcium-ATPase activity by local calcium microdomains near CRAC channels in human T cells
J. Physiol.,
May 1, 2004;
556(3):
805 - 817.
[Abstract]
[Full Text]
[PDF]
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F. Si, H. Brodie, P. G. Gillespie, A. E. Vazquez, and E. N. Yamoah
Developmental Assembly of Transduction Apparatus in Chick Basilar Papilla
J. Neurosci.,
November 26, 2003;
23(34):
10815 - 10826.
[Abstract]
[Full Text]
[PDF]
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P. Martin, D. Bozovic, Y. Choe, and A. J. Hudspeth
Spontaneous Oscillation by Hair Bundles of the Bullfrog's Sacculus
J. Neurosci.,
June 1, 2003;
23(11):
4533 - 4548.
[Abstract]
[Full Text]
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B. Hurle, E. Ignatova, S. M. Massironi, T. Mashimo, X. Rios, I. Thalmann, R. Thalmann, and D. M. Ornitz
Non-syndromic vestibular disorder with otoconial agenesis in tilted/mergulhador mice caused by mutations in otopetrin 1
Hum. Mol. Genet.,
April 1, 2003;
12(7):
777 - 789.
[Abstract]
[Full Text]
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H. Song, L. Nie, A. Rodriguez-Contreras, Z.-H. Sheng, and E. N. Yamoah
Functional Interaction of Auxiliary Subunits and Synaptic Proteins With CaV1.3 May Impart Hair Cell Ca2+ Current Properties
J Neurophysiol,
February 1, 2003;
89(2):
1143 - 1149.
[Abstract]
[Full Text]
[PDF]
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K. P. Steel
Varitint-waddler: A double whammy for hearing
PNAS,
November 12, 2002;
99(23):
14613 - 14615.
[Full Text]
[PDF]
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S. J. DeMarco, M. C. Chicka, and E. E. Strehler
Plasma Membrane Ca2+ ATPase Isoform 2b Interacts Preferentially with Na+/H+ Exchanger Regulatory Factor 2 in Apical Plasma Membranes
J. Biol. Chem.,
March 15, 2002;
277(12):
10506 - 10511.
[Abstract]
[Full Text]
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A. Rodriguez-Contreras and E. N Yamoah
Direct measurement of single-channel Ca2+ currents in bullfrog hair cells reveals two distinct channel subtypes
J. Physiol.,
August 1, 2001;
534(3):
669 - 689.
[Abstract]
[Full Text]
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R. A. Dumont, U. Lins, A. G. Filoteo, J. T. Penniston, B. Kachar, and P. G. Gillespie
Plasma Membrane Ca2+-ATPase Isoform 2a Is the PMCA of Hair Bundles
J. Neurosci.,
July 15, 2001;
21(14):
5066 - 5078.
[Abstract]
[Full Text]
[PDF]
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C. Boyer, J. J. Art, C. J. Dechesne, J. Lehouelleur, J. Vautrin, and A. Sans
Contribution of the Plasmalemma to Ca2+ Homeostasis in Hair Cells
J. Neurosci.,
April 15, 2001;
21(8):
2640 - 2650.
[Abstract]
[Full Text]
[PDF]
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E. E. Strehler and D. A. Zacharias
Role of Alternative Splicing in Generating Isoform Diversity Among Plasma Membrane Calcium Pumps
Physiol Rev,
January 1, 2001;
81(1):
21 - 50.
[Abstract]
[Full Text]
[PDF]
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E. M. Brown and R. J. MacLeod
Extracellular Calcium Sensing and Extracellular Calcium Signaling
Physiol Rev,
January 1, 2001;
81(1):
239 - 297.
[Abstract]
[Full Text]
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J. R. Holt and D. P. Corey
Two mechanisms for transducer adaptation in vertebrate hair cells
PNAS,
October 24, 2000;
97(22):
11730 - 11735.
[Abstract]
[Full Text]
[PDF]
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A. J. Hudspeth, Y. Choe, A. D. Mehta, and P. Martin
Putting ion channels to work: Mechanoelectrical transduction, adaptation, and amplification by hair cells
PNAS,
October 24, 2000;
97(22):
11765 - 11772.
[Abstract]
[Full Text]
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J. Oberwinkler and D. G. Stavenga
Calcium imaging demonstrates colocalization of calcium influx and extrusion in fly photoreceptors
PNAS,
July 18, 2000;
97(15):
8578 - 8583.
[Abstract]
[Full Text]
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Y.-C. Wu, A. J. Ricci, and R. Fettiplace
Two Components of Transducer Adaptation in Auditory Hair Cells
J Neurophysiol,
November 1, 1999;
82(5):
2171 - 2181.
[Abstract]
[Full Text]
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F. Mammano, G. I. Frolenkov, L. Lagostena, I. A. Belyantseva, M. Kurc, V. Dodane, A. Colavita, and B. Kachar
ATP-Induced Ca2+ Release in Cochlear Outer Hair Cells: Localization of an Inositol Triphosphate-Gated Ca2+ Store to the Base of the Sensory Hair Bundle
J. Neurosci.,
August 15, 1999;
19(16):
6918 - 6929.
[Abstract]
[Full Text]
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I. Pala, A. Srinivasan, P. J. S. Vig, and D. Desaiah
Modulation of Calmodulin and Protein Kinase C Activities by Pencillium Mycotoxins
International Journal of Toxicology,
March 1, 1999;
18(2):
91 - 96.
[Abstract]
[PDF]
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Y. Choe, M. O. Magnasco, and A. J. Hudspeth
A model for amplification of hair-bundle motion by cyclical binding of Ca2+ to mechanoelectrical-transduction channels
PNAS,
December 22, 1998;
95(26):
15321 - 15326.
[Abstract]
[Full Text]
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A. J. Ricci, Y-C. Wu, and R. Fettiplace
The Endogenous Calcium Buffer and the Time Course of Transducer Adaptation in Auditory Hair Cells
J. Neurosci.,
October 15, 1998;
18(20):
8261 - 8277.
[Abstract]
[Full Text]
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E. A. Lumpkin and A. J. Hudspeth
Regulation of Free Ca2+ Concentration in Hair-Cell Stereocilia
J. Neurosci.,
August 15, 1998;
18(16):
6300 - 6318.
[Abstract]
[Full Text]
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P. J. Kozel, R. A. Friedman, L. C. Erway, E. N. Yamoah, L. H. Liu, T. Riddle, J. J. Duffy, T. Doetschman, M. L. Miller, E. L. Cardell, et al.
Balance and Hearing Deficits in Mice with a Null Mutation in the Gene Encoding Plasma Membrane Ca2+-ATPase Isoform 2
J. Biol. Chem.,
July 24, 1998;
273(30):
18693 - 18696.
[Abstract]
[Full Text]
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