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The Journal of Neuroscience, January 1, 1998, 18(1):48-58
Fluorescence-Imaged Microdeformation of the Outer Hair Cell
Lateral Wall
John S.
Oghalai1,
Alpen
A.
Patel1,
Takashi
Nakagawa1, 2, and
William E.
Brownell1
1 Bobby R. Alford Department of Otorhinolaryngology and
Communicative Sciences, Baylor College of Medicine, Houston, Texas
77030, and 2 Department of Otorhinolaryngology, Faculty of
Medicine, Kyushu University, Fukuoka 812, Japan
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ABSTRACT |
Outer hair cell (OHC) electromotility appears to be central to
mammalian hearing and originates within its lateral wall. The OHC
lateral wall is a unique trilaminate structure consisting of the plasma
membrane (PM), the cortical lattice (CL), and the subsurface cisternae
(SSC). We selectively labeled and imaged the lateral wall components in
the isolated guinea pig OHC under confocal microscopy. The PM was
labeled with a voltage-sensitive dye, di-8-ANEPPS; the SSC was labeled
with the sphingomyelin precursor, NBD-C6-ceramide; and
F-actin in the CL was labeled with conjugates of phalloidin.
Interactions among the three layers were evaluated with the
micropipette aspiration technique. The PM was tethered to the CL and
SSC until, at a critical deformation pressure, the PM separated,
allowing visualization of the extracisternal space, and ultimately
formed a vesicle. After detaching, the stiffness parameter of the PM
was 22% of that of the intact lateral wall. We conclude that the
lateral wall PM is more compliant than the CL/SSC complex. The
data clarify the structural basis for electromotile force coupling in
the OHC lateral wall.
Key words:
cochlea; inner ear; hearing; cytoskeleton; cell
stiffness; stiffness parameter; micropipette aspiration; patch-clamp
technique; confocal microscopy; fluorescence labeling; biophysics
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INTRODUCTION |
The cochlear outer hair cell (OHC)
is necessary for the exquisite sensitivity of mammalian hearing because
of its unique electromotile property that amplifies the cochlear
traveling wave (Dallos and Corey, 1991 ; Ruggero and Rich, 1991 ). The
OHC has a cylindrical shape and is attached to surrounding cells only
at its apical and basal ends, leaving its lateral wall free within the
perilymph of the spaces of Nuel. The lateral wall has a unique
trilaminate structure composed of the plasma membrane (PM), a
subplasmalemmal cytoskeleton termed the cortical lattice (CL), and a
membranous organelle called the subsurface cisternae (SSC) (Fig.
1). Electron microscopic studies have
demonstrated the presence of many particles localized to PM (Gulley and
Reese, 1977 ; Saito, 1983 ; Forge, 1991 ). The CL is organized in
microdomains of parallel actin filaments cross-linked with spectrin
(Drenckhahn et al., 1985 ; Flock et al., 1986 ; Holley and Ashmore,
1988a ). Pillars run between the actin filaments and the plasma membrane
(Flock et al., 1986 ; Arima et al., 1991 ).

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Figure 1.
The outer hair cell (OHC) lateral wall. The OHC
(lower left) is a cylindrical epithelial cell, with
stereocilia at the apex and the nucleus at the base. The stereocilia
are rooted in the cuticular plate (CP). The lateral wall
is a trilaminate structure composed of the plasma membrane
(PM), the cortical lattice (CL), and the subsurface cisternae (SSC). The
PM has been visualized by electron microscopy and noted
to have a high density of membrane particles. The CL is
composed of microdomains of parallel actin filaments, which are
cross-linked by spectrin. Although the actin orientation can vary
between microdomains by >90°, the average orientation is nearly
circumferential, with a mean angle to the transverse axis of 9-15°
(Holley and Ashmore, 1988a ; Holley, 1996 ). The PM is
bonded to the CL via pillar molecules of unknown
composition. The SSC rests just inside the
CL. The axial core (AC) is the center of
the cell, and the extracisternal space (ECiS) is the
fluid space between the SSC and the PM,
in which lies the CL.
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When isolated from the organ of Corti, the electromotile response
demonstrates an increasing amount of displacement with increasing distance from the point of OHC fixation. This pattern of displacement has been postulated to originate from multiple, evenly distributed unit
motors along the lateral wall (Holley and Ashmore, 1988b ; Dallos et
al., 1991 ; Hallworth et al., 1993 ), termed molecular motors. In the
most popular models of electromotility, the motors are driven by the
transmembrane potential of the OHC (Santos-Sacchi and Dilger, 1988 ) and
undergo conformational changes leading to changes in lateral wall
surface area (Dallos et al., 1993 ; Santos-Sacchi, 1993 ; Iwasa, 1994 ,
1996 ). The particles within the PM may represent integral membrane
proteins that are the molecular motors (Santos-Sacchi, 1991 ; Ashmore,
1992 ; Iwasa and Chadwick, 1992 ; Kalinec et al., 1992 ; Iwasa, 1993 ; Gale
and Ashmore, 1994 ; Kakehata and Santos-Sacchi, 1995 , 1996 ).
How do motors based in the lateral wall direct their forces to change
cell length? The nature of force coupling pathways among the three
layers of the lateral wall is central to this question. We used the
technique of fluorescence-imaged microdeformation (Discher et al.,
1994 ; Discher and Mohandas, 1996 ) to evaluate stiffness and tethering
within the OHC lateral wall. Di-8-ANEPPS, NBD-C6-ceramide,
and fluorescent conjugates of phalloidin specifically labeled the PM,
SSC, and CL, respectively. Micropipette aspiration (Evans, 1973 ; Evans
and Skalak, 1979 ) produced a controlled deformation of the OHC lateral
wall. Brownell et al. (1995) and Sit et al. (1997) found that
vesiculation occurred at high aspiration pressures, but they could not
determine the composition of the vesicle. We discovered that during
vesiculation the PM separated from the underlying CL and SSC.
Additionally, we found that the stiffness parameter of the PM was
significantly less than that of the combined CL and SSC. Hence, this
report evaluates the interactions among components of the lateral wall
of the OHC. Biophysical studies of these highly organized structures
may help to understand the cytoskeletal-plasma membrane interactions
in other cell types.
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MATERIALS AND METHODS |
OHC isolation. Albino guinea pigs of either sex
weighing 200-300 gm and having a normal startle response to a handclap
were decapitated. The temporal bones were taken and the middle ear bullae opened. The otic capsule was removed, and the spiral ligament was peeled off to expose the organ of Corti. The modiolus with the
intact organ of Corti was removed from the temporal bone.
Two different experimental preparations were used. For OHCs that were
labeled with di-8-ANEPPS, NBD-C6-ceramide, or rhodamine phalloidin, the respective staining protocols were performed in situ (described below). After staining, the organ of Corti was rinsed with extracellular solution consisting of (in mM):
135 NaCl, 4 KCl, 1 MgCl2, 2 CaCl2, 10 HEPES, 10 glucose, and 0.1% bovine serum
albumin (Sigma, St. Louis, MO). The extracellular solution had an
osmolality of 285-290 mOsm/kg. Mechanical trituration without enzyme
was performed to dissociate the OHCs (Brownell et al., 1985 ). In
contrast, for OHCs that were labeled with Texas Red-X phalloidin,
intracellular staining was performed via tight-seal, whole-cell patch
pipette dialysis (described below) after the isolation procedure. For
these cells the organ of Corti was removed from the modiolus and
incubated at 31°C for 6 min with trypsin (Type III, Sigma) at a
concentration of 0.5 mg/ml. Gentle pipetting was performed to
dissociate the cells. The extracellular solution was L-15 (Life
Technologies, Gaithersburg, MD) with 5 mM HEPES, which had
an osmolality of 315-320 mOsm/kg. This solution had a slightly higher
osmolality, which seemed to aid the formation of tight seals. All
solutions had a pH of 7.4 and were at room temperature
(22-24°C).
All OHCs were plated onto the glass bottom of an uncoated microwell
Petri dish (MatTek, Ashland, MA). Isolated cells were selected for
study on the basis of standard morphological criteria within 4 hr of
animal death. Under the light microscope, healthy cells display a
characteristic birefringence, a uniformly cylindrical shape without
regional swelling, a basally located nucleus, and no Brownian motion of
subcellular cytoplasmic particles (Shehata et al., 1991 ).
Di-8-ANEPPS labeling. Di-8-ANEPPS is a fluorescent molecule
with a nonpolar region that inserts into membranes and a polar region
that is responsible for the fluorescence. This dye stains the PM of the
OHC very well and does not internalize significantly (Fluhler et al.,
1985 ). We modified the labeling techniques of Bullen et al. (1997) . To
make the stock solution, we dissolved di-8-ANEPPS (D-3167, Molecular
Probes, Eugene, OR) in dimethyl sulfoxide (DMSO) to a concentration of
10 mM. Aliquots were stored at 4°C. Before use,
extracellular solution was added to the aliquot, giving a final
di-8-ANEPPS concentration of 150 µM and a final DMSO
concentration of 1.5%. The organ of Corti was incubated in this
solution at room temperature for 10 min and then rinsed with the
standard extracellular solution to remove the DMSO and unbound dye.
NBD-C6-ceramide labeling.
NBD-C6-ceramide is a labeled precursor of
sphingomyelin. In more conventional cells, it preferentially labels the
Golgi apparatus (Lipsky and Pagano, 1985 ). In the OHC, although Pollice
and Brownell (1993) demonstrated NBD-C6-ceramide uptake in
the SSC, it was unclear whether the dye was present in the PM as well.
NBD-C6-ceramide (N-1154, Molecular Probes) was dissolved in
ethanol (1 mg/ml). A 2× stock solution was made by diluting the
ceramide (20 nmol/ml) into extracellular solution containing defatted
bovine serum albumin (0.68 mg/ml; A-0281, Sigma). Aliquots were stored
at 20°C. An aliquot was diluted with extracellular solution to a
final concentration of 10 nmol/ml of NBD-C6-ceramide and
0.34 mg/ml defatted bovine serum albumin. The organ of Corti was
incubated in this solution at room temperature for 30 min and then
rinsed with the standard extracellular solution.
Rhodamine phalloidin labeling. Phalloidins bond specifically
to F-actin, and fluorescent conjugates have been shown to label the CL
in the OHCs (Carlisle et al., 1988 ; Slepecky, 1989 ). Because phalloidins are hydrophilic, introducing the dye into the intracellular compartment is difficult in living cells. One method we used was to
create pores in the plasma membrane before a bath application of dye.
One vial (300 U) of rhodamine phalloidin (R-415, Molecular Probes) was
dissolved in 1.5 ml of methanol. Aliquots were dried and stored at
20°C. The OHC PM was lightly permeabilized with 0.05% saponin
(S-2149, Sigma) for 5 min. The organ of Corti was incubated in a final
rhodamine phalloidin concentration of 100 U/ml for 30 min at room
temperature and then rinsed with the standard extracellular
solution.
Texas Red-X phalloidin labeling. To stain actin while
maintaining the integrity of the PM (in contrast to the rhodamine
phalloidin staining procedure), we also performed an intracellular
dialysis technique, using a tight-seal whole-cell ruptured patch
configuration. One vial (300 U) of Texas Red-X phalloidin (T-7471,
Molecular Probes) was dissolved in 100 µl of methanol. Aliquots were
dried and stored at 20°C. The patch pipette intracellular solution consisted of (in mM): 150 KCl, 5 MgCl2,
5 EGTA, and 10 HEPES, as well as 60 U/ml Texas Red-X phalloidin. The
intracellular solution had an osmolality of 305-310 mOsm/kg and a pH
of 7.4 and was at room temperature. Patch pipettes were fabricated from
borosilicate thin wall capillary tubing (GC150T-10, Warner Instrument,
Hamden, CT), using a two-stage vertical pipette puller (PP-83,
Narishige, Tokyo, Japan). The tips were fire-polished to an internal
diameter of ~1.5 µm (MF-83, Narishige), with a final impedance of
2-4 M . Seals were formed at the base of the OHC by using an
Axopatch 200B amplifier and pCLAMP6 software (Axon Instruments, Foster City, CA). The cells were held at their zero current potential; only
cells with potentials negative to 50 mV were used.
Confocal microscopy. Data were gathered by a scanning
confocal system (MRC-600, Bio-Rad, Hercules, CA) with a krypton/argon laser, configured on an Axiovert 35 microscope (Zeiss, Oberkochen, Germany). Images were obtained with a 100× oil immersion objective (numerical aperture 1.30; Plan-NEOFLUAR, Zeiss). Fluorescent images of
cells labeled with di-8-ANEPPS and NBD-C6-ceramide were
collected, using an excitation wavelength of 488 nm. Images of cells
labeled with fluorescent phalloidins were collected at an excitation
wavelength of 568 nm. Emission wavelengths were collected, using
long-pass filters with corner wavelengths of 515 nm for the membrane
dyes and 585 for the actin dyes. Images equivalent to those normally seen by light microscopy were collected with the transmitted light path
of the system, using Nomarski optics. In Figure 5d, the
fluorescent signal was so low that we had to open the confocal aperture
all the way to visualize the dye staining. This greatly increased the
z-plane thickness. In all other confocal images a more
typical aperture setting was used, and the thickness of the
z-plane sections was ~1.0 µm.
Micropipette aspiration and stiffness parameter calculations.
The micropipette aspiration technique (Fig.
2) was used to produce a controlled
deformation of the lateral wall of the OHC. Aspiration micropipettes
with internal diameters of ~3 µm were fabricated from borosilicate
glass capillary tubes (LG16; outer diameter, 1.65 mm, inner diameter,
1.1 mm; Dagan, Minneapolis, MN) with an automated glass pipette puller
(BB-CH-PC, Switzerland) and microforge (Microforge De Fonbrune, Aloe
Scientific, St. Louis, MO). The micropipette was connected to a water
column via polyethylene tubing, and both were filled with extracellular
solution. The micropipette was mounted on a joystick-controlled
electronic micromanipulator (Zeiss) and advanced to the center of the
field of view. The level of the water column was referenced to the
microscope stage (i.e., the zero pressure point).

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Figure 2.
The micropipette aspiration technique. This
technique involves bringing a glass pipette with an internal diameter
of ~3 µm in contact with the lateral wall of the cell. As negative
pressure is applied, a tongue of lateral wall is pulled inside the
pipette. The tongue length is measured at different aspiration
pressures and used to determine the stiffness parameter (see Fig. 7).
With increasing suction pressure, the individual components of the lateral wall can be visualized (see Fig. 8).
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Once a healthy cell was located, the micropipette was brought into
contact with the midlateral wall of the OHC. Negative pressure was
applied in a stepwise manner as measured from the null point. This was
performed by sequentially decreasing the pressure by 1 cm of
H2O (1 cm of H2O = 0.09807 nN/µm2) and then waiting 30 sec. This was repeated
until 20 cm of H2O was reached, the cell burst, or
vesiculation occurred. Tongue lengths were measured from the digitized
transmitted and fluorescent images, from the apex of the aspirated
portion of the lateral wall to the tip of the micropipette. The
resolution of the digitized images was 5.5 pixels/µm. Early on, we
discovered that tongue length varies with the internal diameter of the
pipette, such that larger pipettes tended to produce longer tongues
before vesiculation occurred. To minimize this variability, we used
only pipettes of similar diameter to collect the stiffness data
presented in this report (inner diameter, 2.88 ± 0.34 µm;
mean ± SD; n = 32). Because the aspiration
pipette was held at an angle to the stage, the tongue length we
measured was a projection of the true length. However, this effect was
minimized by keeping the angle of approach shallow (<20°) and
consistent for all experiments.
The stiffness parameter (SP) is
calculated from the tongue length versus aspiration pressure data
(Evans, 1973 ; Chien et al., 1978 ; Spector et al., 1996 , 1997a ; Sit et
al., 1997 ). By applying a controlled amount of pressure to the wall of
a cell, we can measure the amount of subsequent bending, and we can
calculate SP to quantify the
deformability of the lateral wall. SP
is defined as:
where P is the change in aspiration pressure
applied to the lateral wall through the micropipette,
Lt is the change in tongue length,
and r is the internal radius of the micropipette. Hence,
SP is 1/slope of plots of
experimental data (see Fig. 7) and is proportional to the change in
force per change in deformation. We calculated
SP for unlabeled controls and for
cells labeled with the membrane dyes.
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RESULTS |
Labeling of the plasma membrane
Figure 3 shows an OHC stained
with di-8-ANEPPS under low-pressure deformation. The transmitted image
(Fig. 3a) shows the lateral wall tongue being aspirated into
the micropipette. The apex of the cell was out of the plane of focus.
The fluorescent image (Fig. 3b) demonstrates labeling of the
basolateral surfaces of the cell. Di-8-ANEPPS also stained the apex and
stereocilia (data not shown). There was no staining of intracellular
structures. The tongue lengths in both images are the same; note that
the tip of the tongue has a rounded shape. With higher aspiration pressures, the tongue length increases until the most distal portion detaches from the cell, forming a vesicle. An example of a vesicle is
demonstrated in Figure 3c. Its fluorescent image (Fig.
3d) demonstrates that the wall of the vesicle is labeled.
Because di-8-ANEPPS is known to label the PM, the PM is a component of the vesicle (n = 10).

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Figure 3.
Di-8-ANEPPS labeling of the PM. a,
Transmitted image of an OHC undergoing micropipette aspiration ( 11 cm
of H20). b, The simultaneous fluorescent
image of a demonstrates staining of the PM. The apex of the cell is out of the focal plane in
this image; however, the stereocilia were always labeled.
c, Transmitted image of a vesicle that was released as
the suction pressure was increased ( 15 cm of H20).
d, The fluorescent image shows that the vesicle contains
PM.
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Labeling of the subsurface cisternae
Figure 4 demonstrates an OHC
that was labeled with NBD-C6-ceramide. The transmitted
image (Fig. 4a) shows the tongue of lateral wall aspirated
inside the micropipette. Two layers of the lateral wall are visible
within the pipette: the outer layer is indicated PM, and the inner
layer is indicated SSC. The fluorescent image (Fig. 4b)
shows labeling of the lateral wall and of some intracellular structures, including the nuclear membrane. The length of the tongue in
Figure 4b corresponds to that of the inner layer in Figure
4a. This figure demonstrates that this
NBD-C6-ceramide staining procedure labels the SSC, but not
the PM. This image also shows that the PM can be separated from the
SSC. After separation an inner tongue could be seen only in the
transmitted image in approximately one-half of the cells; however, by
fluorescence labeling, an inner tongue was visible in every cell. The
SSC tongue in the fluorescent image has a flat tip, as opposed to the
round tip of the PM tongue in the transmitted image. Figure
4c is the transmitted image of a vesicle pulled from a
NBD-C6-ceramide-stained cell. Because the simultaneous
fluorescent image (Fig. 4d) does not show labeling of the
vesicle, SSC membranes are not a component of the vesicle
(n = 11).

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Figure 4.
NBD-C6-ceramide labeling of the
SSC. a, Transmitted image of an OHC undergoing
micropipette aspiration ( 15 cm of H20). Note that for
this cell both an outer layer (PM) and an inner
layer (SSC) are visible in the lateral wall tongue. The
longitudinal bending of the cell is caused by the aspiration force.
b, The simultaneous fluorescent image of
a demonstrates that NBD-C6-ceramide specifically labels the SSC and that this corresponds to
the inner layer seen in the transmitted image. The PM was not labeled;
however, its position is marked by the arrowhead. The
stereocilia were never labeled. c, Transmitted image of
a vesicle that was released ( 17 cm of H20).
d, The fluorescent image shows that the SSC is not a
component of the vesicle, because it does not contain label.
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Labeling of the cortical lattice
Figure 5, a and
b, demonstrates a cell that was permeabilized with saponin
and subsequently labeled for F-actin with rhodamine phalloidin. The
transmitted image (Fig. 5a) shows the poor condition of the
cell, which is to be expected after treatment with saponin. However, a
tongue of the lateral wall could be aspirated into the pipette. The
fluorescent image (Fig. 5b) shows a large amount of labeling
at the apex as well as faint labeling along the lateral walls. This
labeling pattern demonstrates the difference in the density of F-actin
in the cuticular plate and stereocilia versus the CL. The labeled
tongue is visible and is at the same location as the tip of the tongue
seen in the transmitted image. Aspiration pressure was increased in
these cells until they ruptured (typically 20 to 30 cm of
H2O). No separation of the PM or vesiculation was ever
noted (n = 10), most likely because of permeabilization of the PM.

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Figure 5.
Fluorescent phalloidin labeling of the CL.
a, Transmitted image of an OHC after treatment with
saponin and staining with rhodamine phalloidin ( 10 cm of
H20). Note that a tongue could be pulled even with the poor
condition of the cell. No vesicles could be formed
(n = 10). b, The fluorescent image
demonstrates strong labeling of actin within the stereocilia and
cuticular plate. The weaker labeling along the lateral walls
corresponds to staining of actin within the CL
(arrow). c, Transmitted image of a cell undergoing aspiration ( 10 cm of H20). Note the two layers
visible in the tongue. The cell was also whole-cell-patched at the base to introduce Texas Red-X phalloidin; however, the patch pipette is not visible in this image. d, Fluorescent image
demonstrating intracellular staining of actin. The apex of the tongue
corresponds with the inner layer of the tongue seen in the transmitted
image. The PM was not labeled; however, its position is marked by the arrowhead. The depth of field is greater in this image
than in other confocal images because the confocal aperture needed to be wide open to obtain this image because of weak staining. This explains why a discrete line of staining along the periphery is not
present, as in b.
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Figure 5, c and d, demonstrates a cell that was
labeled intracellularly for F-actin with Texas Red-X phalloidin. This
technique did not require the use of saponin, so the integrity of the
PM was preserved. Simultaneous aspiration and patch pipettes were used.
First, aspiration of the lateral wall was performed to hold a tongue at
constant pressure, usually approximately 10 cm of H2O.
Then, a whole-cell configuration was achieved to introduce the dye
inside the OHC. It took ~10-15 min after entering whole-cell configuration for sufficient dye to enter the OHC so that imaging could
be performed. The current-to-voltage relationships of the OHC, as
monitored by periodic voltage-clamp step protocols, did not change
during the staining process (data not shown). The transmitted image
(Fig. 5c) shows a tongue of the lateral wall being aspirated into the pipette, with two visible layers. The patch pipette was at the
base of the cell and is not visible in this image. The fluorescent
image (Fig. 5d) shows strong labeling of the cuticular plate
and faint labeling along the lateral walls, demonstrating the CL. The
fluorescence-labeled tongue is at the same location as the inner tongue
seen in the transmitted image. Because the dye staining by
intracellular dialysis is quite weak, we had to open the aperture
completely on the confocal microscope. The resulting thick depth of
field explains why the fluorescence in the tongue appears confluent
rather than distributed along the perimeter as in the previous images.
However, this figure demonstrates that separation of the PM involves
peeling it away not only from the SSC (as in Fig. 4) but from the CL as
well (n = 3). So an inner layer visible by fluorescent
phalloidin labeling, NBD-C6-ceramide labeling, or by
transmitted image represents the CL and the SSC. The PM is represented
by the outer layer. We term the combination of the two structures that
make up the inner layer the CL/SSC complex.
Dual labeling of the plasma membrane and the
subsurface cisternae
The cell in Figure 6 was
stained with both di-8-ANEPPS and NBD-C6-ceramide. A series
of fluorescent images demonstrates the sequence of separation and
vesiculation. In Figure 6a, the PM and CL/SSC complex were
indistinguishable from each other. The layers were bonded together, and
both had a round tip. The lines radiating from the base of the tongue
are folds in the cell membranes caused by the applied suction pressure.
They disappeared as the manipulation progressed (Fig.
6b-f), perhaps because of an increase in cell turgor
pressure. These folds were not visible in Figures 3, 4, 5. In Figure
6b, the PM separated from the CL/SSC complex. At this point
the PM continued to have a round tip, whereas the tip of the SSC
flattened out. In Figure 6c-e, the PM tongue continued to
elongate, whereas the SSC tongue remained in nearly the same location.
Finally, in Figure 6f, the PM tongue broke free to form a
vesicle, leaving its base to reseal. This process can continue, leading
to the release of multiple vesicles. For example, we have aspirated up
to 26 vesicles from a single cell.

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Figure 6.
Dual labeling of the PM and SSC. This figure
captures the sequence of separation and vesiculation during
micropipette aspiration of the OHC lateral wall. a, The
PM and the SSC overlapped initially ( 10
cm of H20). b, The PM
separated from the SSC ( 14 cm of H20). c-e, The PM tongue elongated, whereas the SSC tongue
stayed nearly the same length ( 14 cm of H20).
f, The PM vesiculated and then resealed over the SSC
( 14 cm of H20). To enhance visualization because of the
angle of the pipette to the microscope stage, we created this image by
summing three sequential images taken at slightly different
z-plane levels. Previous images (a-e)
were single z-plane levels.
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Stiffness parameters
Both PM and CL/SSC complex tongue lengths were measured from OHCs
stained with di-8-ANEPPS and NBD-C6-ceramide as the
aspiration pressure was increased. All data points from 11 cells are
plotted (Fig. 7). The dotted and solid
lines represent the PM and the CL/SSC complex, respectively, both
before and after separation. The reciprocal of the slope is the
SP of the structure. These lines are
the average of the slopes and y-intercepts of lines fit to
each of the data points of the 11 cells. The scatter apparent in the
figure is attributable to variation in the y-intercept points (i.e., the starting tongue lengths) of different cells; however,
the slope (1/SP) varied little (see
data below). The inset is an example of the data recorded from one
cell.

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Figure 7.
Tongue length versus aspiration pressure.
These data were taken from dual-labeled OHCs (n = 11). The circles represent PM tongue lengths, and the
triangles represent SSC tongue lengths. The point of
separation is represented by the large circle. The dotted and solid lines correspond to the
PM and CL/SSC complex, respectively. The four lines were created by
averaging the slopes and y-intercepts of linear fits to
each of the 11 cells both before and after the point of separation. The
corresponding stiffness parameters
(SP) are the reciprocal of the
slopes of each line and are defined in units of nN/µm. The
inset is an example of data taken from one cell.
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The PM and CL/SSC complex overlapped with low aspiration pressures. The
average SP of the intact trilaminate
wall was 0.79 ± 0.18 nN/µm (mean ± SD). The point of
separation had an x value of 1.67 ± 0.30 nN/µm
(mean ± SD), corresponding to a pressure of 1.20 ± 0.23 nN/µm2 (mean ± SD), and is represented by
the large circle on the graph. After this point the tongue length of
the PM increased more rapidly as the pressure was increased. Its
SP was 0.17 ± 0.08 nN/µm
(mean ± SD), which is significantly different from that of the
trilaminate wall (paired Student's t test;
p < 0.001).
On the other hand, the CL/SSC complex tongue length did not
increase as rapidly with pressure increments after separation as it did
before separation. Although the PM tongue maintained a round shape
throughout the aspiration process, the flat tips of the CL and SSC
tongues after separation (more clearly seen in Figs. 4b,
5d) imply that there was no pressure gradient across them.
So, after separation, the negative pressure applied by the micropipette
acted to pull directly on the PM alone. This means that the reciprocal
of the slope of the line indicating the CL/SSC complex (Fig. 7) is
not representative of its
SP. Hence, subtraction of the
SP of the PM from the
SP of the trilaminate wall was
performed to determine this value (0.79-0.17 = 0.62 nN/µm). So
the PM is responsible for 22% of the
SP (0.17/0.79) of the trilaminate
wall, and the remaining two layers comprise the remaining 78%
(0.62/0.79). The lower SP of the PM
indicates that it is more compliant than the CL/SSC complex.
To verify that the dyes did not affect lateral wall mechanics, we
compared SP and separation pressures
of labeled cells versus controls. SP
of unlabeled controls (n = 11), as well as OHCs stained
with di-8-ANEPPS (n = 10) or
NBD-C6-ceramide (n = 11), were not
significantly different (p > 0.1) both before and after separation (data not shown). Additionally, the separation pressures were not significantly different (p > 0.1; data not shown).
 |
DISCUSSION |
Selective labeling and the extracisternal space
Previous reports have demonstrated fluorescent labeling of
structures within the OHC lateral wall (Carlisle et al., 1988 ; Slepecky, 1989 ; Holley et al., 1992 ; Ikeda and Takasaka, 1993 ; Pollice
and Brownell, 1993 ; Raphael et al., 1994 ); however, this is the first
report clearly demonstrating selective staining of each of the three
layers that make up the OHC lateral wall in a living, freshly
dissociated preparation. The cells appeared healthy by microscopy,
remaining viable for up to 4 hr after animal death, similar to
unlabeled isolated OHCs. The Texas Red-X phalloidin labeled cells had
current-to-voltage relationships that appeared similar to previous
reports (Nakagawa et al., 1994a ,b ). Also, di-8-ANEPPS has been shown
previously not to affect the OHC current-to-voltage relationships
(Nakagawa et al., 1997 ). The NBD-C6-ceramide staining procedure only labels the SSC, which is consistent with the absence of
label in the stereocilia.
With the application of negative pressure, a tongue of lateral wall was
pulled into the micropipette. Initially, the trilaminate structure was
bonded together. As the suction pressure was increased, the PM
separated from the lateral wall, representing disruption of the
tethering between the PM and the CL/SSC complex. The fluid compartment
between the two layers is the extracisternal space. Not only were we
able to determine that the vesicle is composed of PM and does not
contain actin from the CL or membranes from the SSC, but we could
further dissect their structural contribution to wall mechanics by
quantitating their deformation.
Component contributions to lateral wall stiffness
Our findings can be compared with other experiments in which the
stiffness of the lateral wall has been altered. Although the absolute
values of stiffness measurements may vary, depending on the type of
experimental deformation (Spector et al., 1997b ), comparison of the
relative stiffnesses between lateral wall components can be performed
safely. Kalinec et al. (1992) found that, after intracellular perfusion
of trypsin in OHCs to disrupt the CL and SSC, the normal cylindrical
shape was altered greatly such that it became more spherical, without
lateral wall stiffness to counteract turgor pressure. Although the
actions of trypsin on the stiffness of the PM are unclear, this may
indicate that the PM is not as stiff as the CL/SSC complex. When the
complimentary manipulation was performed, i.e., when OHCs were treated
with Triton X-100 to remove the PM (Holley and Ashmore, 1988a ) (E. Chan, A. Suneson, and M. Ulfendahl, unpublished results), the CL shell
lengthened yet maintained its cylindrical shape, consistent with an
intrinsic rigidity and shape inherent to the CL. Both of these findings support our conclusion that the CL/SSC complex is primarily responsible for lateral wall stiffness.
However, our observation that the lateral wall stiffness is dominated
by the CL/SSC complex contrasts with the conclusions of Holley and
Ashmore (1988a) . They found that it took significantly more force to
compress the healthy cell than the demembranated cell (i.e., the CL
shell) in the longitudinal direction. They stated that this meant the
majority of lateral wall stiffness is inherent to the PM. Tolomeo et
al. (1996) also used the technique of Triton X-100 demembranization to
determine the stiffness of the CL, with similar conclusions. However,
because there would be no turgor pressure in a demembranated cell, a
much lower stiffness measurement is hardly surprising. In contrast to
these reports, we were able to compare
SP of the PM with that of the CL/SSC
complex in healthy cells.
The role of the cytoskeleton and pillars
Figure 8 is a representative
diagram of the separation process. Although the PM can be detached from
the lateral wall, the CL and SSC remain behind and are primarily
responsible for the SP of the lateral
wall. The phenomenon of separation proves that the PM is tethered to
the underlying lateral wall and that this tethering can be broken.
SP of the OHC trilaminate lateral
wall is anywhere from 2 to 76 times higher than in other cells (Sit et
al., 1997 ). There is no cell that has been documented to have a higher
SP. The cytoskeleton of most
eukaryotic cells contains F-actin, tubulin, and intermediate filaments;
however, the high stiffness of the OHC lateral wall may be attributable
to the anisotropic nature of the OHC cytoskeleton, which consists of
microdomains that tend to orient the actin filaments circumferentially.
Interestingly, other types of hair cells (which do not have
electromotility) do not appear to have this unique structure.
Additionally, similar to the OHC, the cytoskeleton of red blood cells
also contains actin and spectrin in a subplasmalemmal configuration.
However, the red blood cell is orthotropic and flexible (Discher et
al., 1994 ; Discher and Mohandas, 1996 ), allowing the cells to deform
while passing through thin capillaries. So, with the uniquely high
stiffness inherent to the OHC lateral wall, the pressures at which
separation occur are in all likelihood above normal physiological
stress conditions. This would imply that during normal electromotility
in vivo the PM is tightly bound to the underlying lateral
wall.

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|
Figure 8.
The phenomenon of separation. Initially, the
bonded trilaminate lateral wall is pulled into the pipette (as seen in
Fig. 2). After separation (a), the tip of the
CL/SSC complex flattens out, whereas the PM continues to elongate.
b, The vesicle consists of only PM and does not contain
actin from the CL or membranes from the SSC. The remaining PM reseals
over the lateral wall and begins to elongate again. Although
represented as remaining with the actin of the CL in this diagram, the
actual fate of the pillars is unknown (see Discussion).
|
|
The pillars are probably responsible for this tethering. The
maximal tethering force depends both on their longitudinal strength as
well as on their anchoring strength into the PM and the CL (Spector et
al., 1996 ). However, there is no clear information as to which link is
broken during the aspiration experiments. In Figure 8, the pillars were
shown as remaining bonded to the CL after separation, although we have
no evidence to support this.
Implications for electromotile force coupling
One hypothesis to explain OHC force coupling is the cytoskeletal
spring model proposed by Holley and Ashmore (1990) . In this model the
molecular motors rest within the PM, and the CL is less stiff than the
PM. When the motors change in surface area, they push against
themselves and their surrounding phospholipids, summating their forces
and creating cell length changes. Hence, by this model, force coupling
occurs within the PM because the PM has a high stiffness. An
alternative possibility, suggested by Iwasa (1994) and further
discussed by Tolomeo et al. (1996) , is that motors in the PM transmit
their force down the pillars to the CL, which then orients the forces.
Because an equal and opposite force would be required to hold the
motors in place within the PM, the PM must be stiffer than the CL in
this theory as well.
Our findings do not support these hypotheses. Because the PM appears to
be more compliant than the CL, it would seem that membrane-based motors
should just push the bilayer phospholipids out of the way as they
change conformation, rather than directing their force purposefully.
This makes it unlikely that the motors exert a force when increasing in
surface area. However, it is possible that they could still exert a
force when decreasing in surface area, by pulling on the
lipid bilayer. A contractile force within the PM probably could lead to
changes in cell shape, because the PM can withstand the pulling force
of micropipette aspiration to the point at which bending of the entire
cell occurs (Figs. 3, 4; see also Sit et al., 1997 ). This means that,
although the PM stiffness is less than the CL stiffness, the PM tensile
strength is greater than CL stiffness. So if some other source of
extensile force existed within the OHC, then the mechanism of
electromotility may occur via opposing contractile and extensile
forces.
This extensile force might be passive resting tension from within the
framework of the CL, associated with cell turgor pressure (Brownell et
al., 1985 ; Holley and Ashmore, 1988a ,b , 1990 ; Brownell, 1990 ; Shehata
et al., 1991 ). With tethering, the pillars would distribute the total
extensile force over the surface area of the lateral wall. The concept
of tethering is consistent with the work of Dallos et al. (1991) . Our
concept of OHC electromotility is a further refinement of the model
described by Santos-Sacchi (1993) , and we suggest that without some
type of intrinsic extensile force within the cell there could be little
force coupling between the motors.
Interestingly, although the pillars clearly are tethered to the
PM, the motors do not have to be fixed in place. This leaves the
intriguing possibility that the motors could be mobile within the PM
lipid bilayer (as in the fluid mosaic model), sensing transmembrane potential and changing in surface area correspondingly. Meanwhile, passive tension, acting to elongate the OHC, "fits" cell length to
the available amount of PM surface area. There are many more particles
in the PM (the postulated molecular motors) than pillars (Forge, 1991 ).
If pillars were needed to transmit the force generated by these motors,
structural connections between the motors and the pillars would be
necessary. However, there have been no visualized organizations or
connections between the particles and the pillars by ultrastructural
studies. This discrepancy further supports the hypothesis that the
motors randomly diffuse throughout the OHC lateral wall PM. Their
fluidity may be limited by interactions with each other or the lipid
components of the membrane bilayer. One consequence of identifying
membrane-specific labels is that membrane fluidity can be quantified by
using fluorescence recovery after photobleaching techniques (our
unpublished data).
 |
FOOTNOTES |
Received July 23, 1997; revised Oct. 9, 1997; accepted Oct. 10, 1997.
This project was supported by research grants from the Deafness
Research Foundation (to J.S.O.) and Grants DC00354 and DC02775 (to
W.E.B.) from the National Institute on Deafness and Other Communication
Disorders. We are grateful to Drs. B. R. Alford, A. Bullen,
R. A. Eatock, H. A. Jenkins, S. Popel, R. Raphael, T. Ratnanather, P. Saggau, A. Spector, and M. Zhi. N. Gavia and C. Shope
provided technical support. Illustrations were done by S. Carmichael.
Correspondence should be addressed to Dr. John S. Oghalai, Bobby R. Alford Department of Otorhinolaryngology and Communicative Sciences,
Baylor College of Medicine, One Baylor Plaza, Houston, TX 77030.
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